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A resistor is a block or material that limits the flow of current. The greater the resistance, the lower the current will be, assuming the same voltage imposed on the resistor. The hydraulic analogy of a resistor would be the pipe with water flowing through it. The wider the diameter of a pipe, the higher the water flow through the pipe, assuming the same pressure difference on the terminals of a pipe.

Resistors have two leads (points of contact) to which the resistor can be connected to an electrical circuit. A symbol for a resistor used in electrical circuit diagrams is shown below.

The endpoints at the left and right sides of the symbol indicate the points of contact for the resistor. The ratio of the voltage to current will always be positive, since a higher voltage on one side of a resistor is a positive voltage, and a current will flow from the positive side to the negative side, resulting in a positive current. If the voltage is reversed, the current is reversed, leading again to a positive resistance.

Resistance is a characteristic of Resistor indicates the measurement of current opposition . Resistance has a symbol R measured in Ohm (Ω) . The ratio of voltage to current is referred to as Ohm’s Law, and is one of the most basic laws that govern electronics.

An ohm is the amount of resistance which passes one ampere of current when a one volt potential is placed across it. (The ohm is actually defined as the resistance which dissipates one watt of power when one ampere of current is passed through it.)

Resistance can vary from very small to very large. A superconductor has zero resistance, while something like the input to an op-amp can have a resistance near 1012 Ω, and even higher resistances are possible.

Resistance converts Electrical Energy into Heat this causes Electric Energy Loss.

NOTE : Resistors which dissipate large amounts of power are cooled so that they are not destroyed, typically with finned heatsinks.

If Electric Energy Supply is Pv and Electric Energy Loss is Pr Then, Electric Energy Delivered is

The ratio of Electric Energy Delivered over Electric Energy Supplied indicates the Efficiency of Electric Power Supply

A manufactured resistor is usually labeled with the nominal value (value to be manufactured to) and sometimes a tolerance. Rectangular resistors will usually contain numbers that indicate a resistance and a multiplier. If there are three or four numbers on the resistor, the first numbers are a resistance value, and the last number refers to the number of zeroes in the multiplier. If there is an R in the value, the R takes the place of the decimal point.

Cylindrical resistors (axial) usually have colored bands that indicate a number and a multiplier. Resistance bands are next to each other, with a tolerance band slightly farther away from the resistance bands. Starting from the resistance band side of the resistor, each colour represents a number in the same fashion as the number system shown above.

Clue : B.B.ROY of Great Britain was a Very Good Worker.
Additional Colours: A gold band in the multiplier position means 0.1, but means a 5% tolerance in the tolerance position. A silver band in the multiplier position means 0.01, but means 10% in the tolerance position.

The resistance R of a component is dependent on its physical dimension and can be calculated using:

If you increase ρ or L you increase the resistance of the material, but if you increase A you decrease the resistance of the material.

Every material has its own resistivity, depending on its physical makeup. Most metals are conductors and have very low resistivity; whereas, insulators such as rubber, wood, and air all have very high resistivity. The inverse of resistivity is conductivity, which is measured in units of Siemens/metre (S/m) or, equivalently. mhos/metre.

In the following chart, it is not immediately obvious how the unit ohm-meter is selected. Considering a solid block of the material to be tested, one can readily see that the resistance of the block will decrease as its cross-sectional area increases (thus widening the conceptual “pipe”), and will increase as the length of the block increases (lengthening the “pipe”). Given a fixed length, the resistance will increase as the cross-sectional area decreases; the resistance, multiplied by the area, will be a constant. If the cross-sectional area is held constant, as the length is increased, the resistance increases in proportion, so the resistance divided by the length is similarly a constant. Thus the bulk resistance of a material is typically measured in ohm meters squared per meter, which simplifies to ohm – meter (Ω-m).

Silver, copper, gold, and aluminum are popular materials for wires, due to low resistivity. Silicon and germanium are used as semiconductors. Glass, rubber, quartz crystal, and air are popular dielectrics, due to high resistivity.

Many materials, such as air, have a non-linear resistance curve. Normal undisturbed air has a high resistance, but air with a high enough voltage applied will become ionized and conduct very easily.

The resistivity of a material also depends on its temperature. Normally, the hotter an object is, the more resistance it has. At high temperatures, the resistance is proportional to the absolute temperature. At low temperatures, the formula is more complicated, and what counts as a high or low temperature depends on what the resistor is made from. In some materials the resistivity drops to zero below a certain temperature. This is known as superconductivity, and has many useful applications.

For all resistors, the change in resistance for a small increase in temperature is directly proportional to the change in temperature.

Current passing through a resistor will warm it up.
Many components have heat sinks to dissipate that heat. The heatsink keeps the component from melting or setting something on fire.

The length of an object is directly proportional to its resistance. As shown in the diagram below, 1 unit cubed of material has 1 ohm of resistance. However, when 4 units are stacked lengthwise and a connection is made to the front and back sides respectively, the total resistance is 4 ohms. This is because the length of the unit is 4, whereas the cross-sectional area remains 1. However, if you were to make connections on the sides, the exact opposite would be true: the cross-sectional area would be 4 and the length 1, resulting in 0.25 ohms total resistance.

Increasing area is the same as having resistors in parallel, so as you increase the area you add more paths for current to take.

The resistance of a material is inversely proportional to its cross-sectional area. This is shown in the diagram below, where 1 unit cubed has one ohm of resistance. However, if 4 units cubed are stacked on top of each other in the fashion such that there is 4 units squared of cross-sectional area, and the electrical connections are made to the front and back such that the connections are on the largest sides, the resultant resistance would be 0.25 ohms.

Additional note: There are two reasons why a small cross-sectional area tends to raise resistance. One is that the electrons, all having the same negative charge, repel each other. Thus there is resistance to many being forced into a small space. The other reason is that they collide, causing “scattering,” and therefore they are diverted from their original directions. (More discussion is on page 27 of “Industrial Electronics,” by D. J. Shanefield, Noyes Publications, Boston, 2001.)

For instance, if you wanted to calculate the resistance of a 1 cm high, 1 cm wide, 5 cm deep block of copper, as shown in the diagram below:

You would first need to decide how it’s oriented. Suppose you want to use it from front to back (lengthwise), like a piece of wire, with electrical contacts on the front and rear faces. Next you need to find the length, L. As shown, it is 5 cm long (0.05 m). Then, we look up the resistivity of copper on the table, 1.6×10-8 Ω-meters. Lastly, we calculate the cross-sectional area of the conductor, which is 1 cm × 1 cm = 1 cm2 (0.0001 m2). Then, we put it all in the formula, converting cm to m:

0.05 m1.6×108 Ωm0.0001 m2=0.08×108 Ωm20.0001 m2{displaystyle {0.05 {mbox{m}}cdot 1.6times 10^{-8} Omega cdot {mbox{m}} over 0.0001 {mbox{m}}^{2}}={0.08times 10^{-8} Omega cdot {mbox{m}}^{2} over 0.0001 {mbox{m}}^{2}}}

Which, after evaluating, gives you a final value of 8.0×10-6 Ω, or 8 microohms, a very small resistance. The method shown above included the units to demonstrate how the units cancel out, but the calculation will work as long as you use consistent units.

Resistors in series are equivalent to having one long resistor. If the properties of two resistors are equivalent, except the length, the final resistance will be the sum of the two construction methods:

This means that the resistors add when in series.

In a parallel circuit, current is divided among multiple paths. This means that two resistors in parallel have a lower equivalent resistance than either of the parallel resistors, since both resistors allow current to pass. Two resistors in parallel will be equivalent to a resistor that is twice as wide:

Since conductances (the inverse of resistance) add in parallel, you get the following equation:

For example, two 4 Ω resistors in parallel have an equivalent resistance of only 2 Ω.

To simplify mathematical equations, resistances in parallel can be represented with two vertical lines “||” (as in geometry). For two resistors the parallel formula simplifies to:

Resistors in parallel are evaluated as if in a mathematical set of “parentheses.” The most basic group of resistors in parallel is evaluated first, then the group in series with the new equivalent resistor, then the next group of resistors in parallel, and so on. For example, the above portion would be evaluated as follows:

Resistors are available as pre-fabricated, real-world components. The behavior of such components deviates from an ideal resistor in certain ways. Therefore, real-world resistors are not only specified by their resistance, but also by other parameters. In order to select a manufactured resistance, the entire range of specifications should be considered. Usually, exact values do not need to be known, but ranges should be determined.

The nominal resistance is the resistance that can be expected when ordering a resistor. Finding a range for the resistance is necessary, especially when operating on signals. Resistors do not come in all of the values that will be necessary. Sometimes resistor values can be manipulated by shaving off parts of a resistor (in industrial environments this is sometimes done with a LASER to adjust a circuit), or by combining several resistors in series and parallel.

Available resistor values typically come with a resistance value from a so called resistor series. Resistor series are sets of standard, predefined resistance values. The values are actually made up from a geometric sequence within each decade. In every decade there are supposed to be

n{displaystyle n}

resistance values, with a constant step factor. The standard resistor values within a decade are derived by using the step factor

i{displaystyle i}

rounded to a two digit precision. Resistor series are named E

n{displaystyle n}

, according to the used value of

n{displaystyle n}

in the above formula.

For example, in the E12 series for

n=12{displaystyle n=12}

, the resistance steps in a decade are, after rounding the following 12 values:

and actually available resistors from the E12 series are for example resistors with a nominal value of 120Ω or 4.7kΩ.

A manufactured resistor has a certain tolerance to which the resistance may differ from the nominal value. For example, a 2kΩ resistor may have a tolerance of ±5%, leaving a resistor with a value between 1.9kΩ and 2.1kΩ (i.e. 2kΩ±100Ω). The tolerance must be accounted for when designing circuits. A circuit with an absolute voltage of 5V±0.0V in a voltage divider network with two resistors of 2kΩ±5% will have a resultant voltage of 5V±10% (i.e. 5V±0.1V). The final resistor tolerances are found by taking the derivative of the resistor values, and plugging the absolute deviations into the resulting equation.

The above mentioned E-series which are used to provide standardized nominal resistance values, are also coupled to standardized nominal tolerances. The fewer steps within a decade there are, the larger the allowed tolerance of a resistor from such a series is. More precises resistors, outside of the mentioned E-series are also available, e.g. for high-precision measurement equipment. Common tolerances, colors and key characters used to identify them are for example:

Resistor manufacturers can benefit from this standardization. They manufacture resistors first, and afterwards they measure them. If a resistor does not meet the nominal value within the defined tolerance of one E-series, it might still fit into a lower series, and doesn’t have to be thrown away, but can be sold as being compliant to that lower E-series standard. Although typically at a lower price.

Series: Resistors that combine in series add the nominal tolerances together.

Parallel: Resistors that combine in parallel have a combined tolerance that is slightly more complex.

Because the purpose of a resistor is to dissipate power in the form of heat, the resistor has a rating (in watts) at which the resistor can continue to dissipate before the temperature overwhelms the resistor and causes it to overheat. When a resistor overheats, the material begins to melt away, which will cause the resistance to increase (usually), until the resistor breaks.

Related to power rating, the operating temperature is the temperature that the resistor can continue to operate before being destroyed.

In order to avoid sparkovers or material breakdown a certain maximum voltage over a resistor must not be exceeded. The maximum voltage is part of a resistor’s specification, and typically a function of the resistor’s physical length, distance of the leads, material and coating.

For example, a resistor with a maximum operating voltage of 1kV can have a length in the area of 2″, while a 0.3″ resistor can operate under up to several tens of volts, probably up to a hundred volts. When working with dangerous voltages it is essential to check the actual specification of a resistor, instead of only trusting it because of the length.

This parameter refers to the constant in which the resistance changes per degree Celsius (units in C-1). The change in temperature is not linear over the entire range of temperatures, but can usually be thought of as linear around a certain range (usually around room temperature). However, the resistance should be characterized over a large range if the resistor is to be used as a thermistor in those ranges. The simplified linearized formula for the affect on temperature to a resistor is expressed in an equation:

Real world resistors not only show the physical property of resistance, but also have a certain capacity and inductance. These properties start to become important, if a resistor is used in some high frequency circuitry. Wire wound resistors, for example, show an inductance which typically make them unusable above 1kHz.

Resistors can be packaged in any way possible, but are divided into surface mount, through hole, soldering tag and a few more forms. Surface mount is connected to the same side that the resistor is on. Through hole resistors have leads (wires) that typically go through the circuit board and are soldered to the board on the side opposite the resistor, hence the name. Resistors with leads are also used in point-to-point circuits without circuit boards. Soldering tag resistors have lugs to solder wires or high current connectors onto.

Usual packages for surface mount resistors are rectangular, referenced by a length and a width in mils (thousands of an inch). For instance, an 0805 resistor is a rectangle with length .08″ x .05″, with contacts (metal that connects to the resistor) on either side. Typical through hole resistors are cylindrical, referenced either by the length (such as 0.300″) or by a typical power rating that is common to the length (a 1/4W resistor is typically 0.300″). This length does not include the length of the leads.

Electronics |
Foreword |
Basic Electronics |
Complex Electronics | Electricity |
Machines |
History of Electronics |
Appendix |

Some different capacitors for electronic equipment

Capacitors are a good example of the fact that even the simplest device can become complicated given 250 years of evolution. (Citation J. Ho, T. R. Jow, St. Boggs, Historical Introduction to Capacitor Technology)[1]

Capacitors, together with resistors, inductors and memristors, belong to the group of “passive components” for electronic equipment. Although in absolute figures the most common capacitors are integrated capacitors, e.g. in DRAMs or in flash memory structures, this article is concentrated on discrete components.


Theory of conventional construction[edit]

A capacitor (historically known as a “condenser”) is a device that stores energy in an electric field, by accumulating an internal imbalance of electric charge. It is made of two conductors separated by a dielectric (insulator). Using the same analogy of water flowing through a pipe, a capacitor can be thought of as a tank, in which the charge can be thought of as a volume of water in the tank. The tank can “charge” and “discharge” in the same manner as a capacitor does to an electric charge. A mechanical analogy is that of a spring. The spring holds a charge when it is pulled back.

When voltage exists one end of the capacitor is getting drained and the other end is getting filled with charge.This is known as charging. Charging creates a charge imbalance between the two plates and creates a reverse voltage that stops the capacitor from charging. As a result, when capacitors are first connected to voltage, charge flows only to stop as the capacitor becomes charged. When a capacitor is charged, current stops flowing and it becomes an open circuit. It is as if the capacitor gained infinite resistance.

You can also think of a capacitor as a fictional battery in series with a fictional resistance. Starting the charging procedure with the capacitor completely discharged, the applied voltage is not counteracted by the fictional battery, because the fictional battery still has zero voltage, and therefore the charging current is at its maximum. As the charging continues, the voltage of the fictional battery increases, and counteracts the applied voltage, so that the charging current decreases as the fictional battery’s voltage increases. Finally the fictional battery’s voltage equals the applied voltage, so that no current can flow into, nor out of, the capacitor.

Just as the capacitor charges it can be discharged. Think of the capacitor being a fictional battery that supplies at first a maximum current to the “load”, but as the discharging continues the voltage of the fictional battery keeps decreasing, and therefore the discharge current also decreases. Finally the voltage of the fictional battery is zero, and therefore the discharge current also is then zero.

This is not the same as dielectric breakdown where the insulator between the capacitor plates breaks down and discharges the capacitor. That only happens at large voltages and the capacitor is usually destroyed in the process. A spectacular example of dielectric breakdown occurs when the two plates of the capacitor are brought into contact. This causes all the charge that has accumulated on both plates to be discharged at once. Such a system is popular for powering tasers which need lots of energy in a very brief period of time.

Theory of electrochemical construction[edit]

Scheme on double layer on electrode (BMD model).
1. IHP Inner Helmholtz Layer
2. OHP Outer Helmholtz Layer
3. Diffuse layer
4. Solvated ions
5. Specifically adsorptive ions (Pseudocapacitance)
6. Solvent molecule.

Besides the conventional static storage of electric energy in an electric field, two other storage principles to store electric energy in a capacitor exist. They are so-called electrochemical capacitors. In contrast to ceramic, film and electrolytic capacitors, supercapacitors, also known as electrical double-layer capacitors (EDLC) or ultracapacitors do not have a conventional dielectric. The capacitance value of an electrochemical capacitor is determined by two high-capacity storage principles. These principles are:

  • electrostatic storage within Helmholtz double layers achieved on the phase interface between the surface of the electrodes and the electrolyte (double-layer capacitance) and the
  • electrochemical storage achieved by a faradaic electron charge-transfer by specifically adsorpted ions with redox reactions (pseudocapacitance). Unlike batteries, in the faradaic redox reactions, the ions simply cling to the atomic structure of an electrode without making or braking chemical bonds, and no or negligibly small chemical modifications are involved in charge/discharge.

The ratio of the storage resulting from each principle can vary greatly, depending on electrode design and electrolyte composition. Pseudocapacitance can increase the capacitance value by as much as an order of magnitude over that of the double-layer by itself.[2]


The capacitance of a capacitor is a ratio of the amount of charge that will be present in the capacitor when a given potential (voltage) exists between its leads. The unit of capacitance is the farad which is equal to one coulomb per volt. This is a very large capacitance for most practical purposes; typical capacitors have values on the order of microfarads or smaller.

Where C is the capacitance in farads, V is the potential in volts, and Q is the charge measured in coulombs. Solving this equation for the potential gives:

Capacitor & Direct Current Voltage (DC)[edit]

Charge Building

When a Capacitor is connected with electricity source V. Charge will build up on each plates of capacitor of the same amount of charge but different in polarity . This process is called Capacitor Charging

Storing Charge

When both plates are charged up to voltage V then there is no difference in voltage between capacitor’s plates and electricity source therefore no current flow in the circuit. This is called Storing Charge

Charge discharge

When the capacitor is connected to ground, current will flow from capacitor to ground until the voltage on capacitor’s plates are equal to zero.

Therefore, a Capacitor is a device that can Build up Charge , Store Charge and Release Charge

Capacitor & Alternating Current Voltage (AC)[edit]




Reactance is defined as the ratio of Voltage over Current


Impedance is defined as the sum of Capacitor’s Resistance and Reactance

Angle of Difference between Voltage and Current[edit]

For Lossless Capacitor

Current will lead Voltage an angle 90 degree

For Lossy Capacitor

Current will lead Voltage an angle θ degree where
Tan θ =

Changing the value of R and C will change the value of Phase Angle, Angular Frequency, Frequency and Time

Capacitor Connection[edit]

Capacitors in Series[edit]

Capacitors in series are the same as increasing the distance between two capacitor plates. As well, it should be noted that placing two 100 V capacitors in series results in the same as having one capacitor with the total maximum voltage of 200 V. This, however, is not recommended to be done in practice, especially with capacitors of different values. In a capacitor network in series, all capacitors can have a different voltage over them.


In a series configuration, the capacitance of all the capacitors combined is the reciprocal of the sum of the reciprocals of the capacitance of all the capacitors.

Capacitors in Parallel[edit]

Capacitors in parallel are the same as increasing the total surface area of the capacitors to create a larger capacitor with more capacitance. In a capacitor network in parallel, all capacitors have the same voltage over them.


In a parallel configuration, the capacitance of the capacitors in parallel is the sum of the capacitance of all the capacitors.

RC Circuit[edit]


An RC circuit is short for ‘Resistor-Capacitor’ circuit. A capacitor takes a finite amount of time to discharge through a resistor, which varies with the values of the resistor and capacitor. A capacitor acts interestingly in an electronic circuit, practically speaking as a combination of a voltage source and a variable resistor.


Below is a simple RC Circuit:
Electronics RC01.PNG

There is a capacitor in parallel with the resistor and current probe. The way the capacitor functions is by acting as a very low resistance load when the circuit is initially turned on. This is illustrated below:
Electronics RC02.PNG

Initially, the capacitor has a very low resistance, almost 0. Since electricity takes the path of least resistance, almost all the electricity flows through the capacitor, not the resistor, as the resistor has considerably higher resistance.
Electronics RC03.PNG

As a capacitor charges, its resistance increases as it gains more and more charge. As the resistance of the capacitor climbs, electricity begins to flow not only to the capacitor, but through the resistor as well:
Electronics RC04.PNG

Once the capacitor’s voltage equals that of the battery, meaning it is fully charged, it will not allow any current to pass through it. As a capacitor charges its resistance increases and becomes effectively infinite (open connection) and all the electricity flows through the resistor.
Electronics RC05.PNG

Once the voltage source is disconnected, however, the capacitor acts as a voltage source itself:
Electronics RC06.PNG

As time goes on, the capacitor’s charge begins to drop, and so does its voltage. This means less current flowing through the resistor:
Electronics RC01.PNG

Once the capacitor is fully discharged, you are back to square one:

If one were to do this with a light and a capacitor connected to a battery, what you would see is the following:

  1. Switch is closed. Light does not light up.
  2. Light gradually becomes brighter and brighter…
  3. Light is at full luminosity.
  4. Switch is released. Light continues to shine.
  5. Light begins to fade…
  6. Light is off.

This is how a capacitor acts. However, what if you changed the values of R1? C1? The voltage of the battery? We will examine the mathematical relationship between the resistor, capacitor, and charging rate below.

Time Constant[edit]

In order to find out how long it takes for a capacitor to fully charge or discharge, or how long it takes for the capacitor to reach a certain voltage, you must know a few things. First, you must know the starting and finishing voltages. Secondly, you must know the time constant of the circuit you have. Time constant is denoted by the Greek letter ‘tau’ or τ. The formula to calculate this time constant is:

So this means that the time constant is how long it takes for a capacitor to charge to 63% of its full charge. This time, in seconds, is found by multiplying the resistance in ohms and the capacitance in farads.

According to the formula above, there are two ways to lengthen the amount of time it takes to discharge. One would be to increase the resistance, and the other would be to increase the capacitance of the capacitor. This should make sense. It should be noted that the formula compounds, such that in the second time constant, it charges another 63%, based on the original 63%. This gives you about 86.5% charge in the second time constant. Below is a table.

Time Constant Charge
1 63%
2 87%
3 95%
4 98%
5 99+%

For all practicality, by the 5th time constant it is considered that the capacitor is fully charged or discharged.

put some stuff in here about how discharging works the same way, and the function for voltage based on time

v(t)=1Ci(t)dt{displaystyle v(t)={frac {1}{C}}int i(t)dt}

Where i(t) is the current flowing through the capacitor as a function of time.

This equation is often used in another form. By differentiating with respect to time:

i(t)=Cdv(t)dt{displaystyle i(t)=C{frac {dv(t)}{dt}}}

Substituting v/r for i(t) and integrating the above equation gives you an equation used to describe the charging and discharging characteristics of RC circuits. A charging characteristic curve exponentially increases from 0% (0 volts) and approaches 100% full (maximum voltage), similarly, a discharge curve starts at the theoretical 100% (maximum voltage) and exponentially falls back to 0% (0 volts).

Common capacitors and their names[edit]

Capacitors are divided into two mechanical groups: Fixed capacitors with fixed capacitance values and variable capacitors with variable (trimmer) or adjustable (tunable) capacitance values.

The most important group is the fixed capacitors. Many got their names from the dielectric. For a systematic classification these characteristics can’t be used, because one of the oldest, the electrolytic capacitor, is named instead by its cathode construction. So the most-used names are simply historical.

The most common kinds of capacitors are:

  • Ceramic capacitors have a ceramic dialectric.
  • Film and paper capacitors are named for their dielectrics.
  • Aluminum, tantalum and niobium electrolytic capacitors are named after the material used as the anode and the construction of the cathode
  • Supercapacitor is the family name for:
    • Double-layer capacitors were named for the physical phenomenon of the Helmholtz double-layer
    • Pseudocapacitors were named for their ability to store electric energy electro-chemically with reversible faradaic charge-transfer
    • Hybrid capacitors combine double-layer and pseudocapacitors to increase power density
  • Seldom-used Silver mica, glass, silicon, air-gap and vacuum capacitors were named for their dielectric.

Capacitors in each family have similar physical design features, but vary, for example, in the form of the terminals.

Overview over the most commonly used fixed capacitors in electronic equipment

In addition to the above shown capacitor types, which derived their name from historical development, there are many individual capacitors that have been named based on their application. They include:

  • Power capacitors, motor capacitors, DC-link capacitors, suppression capacitors, audio crossover capacitors, lighting ballast capacitors, snubber capacitors, coupling, decoupling or bypassing capacitors.

Often, more than one capacitor family is employed for these applications, e.g. interference suppression can use ceramic capacitors or film capacitors.

Specialized devices such as built-in capacitors with metal conductive areas in different layers of a multi-layer printed circuit board and kludges such as twisting together two pieces of insulated wire also exist.


Principle charge storage of different capacitor types and their inherent voltage progression

The most common dielectrics are:

All of them store their electrical charge statically within an electric field between two (parallel) electrodes.

Beneath this conventional capacitors a family of electrochemical capacitors called Supercapacitors was developed. Supercapacitors don’t have a conventional dielectric. They store their electrical charge statically in

and additional electrochemical with faradaic charge transfer

  • with a pseudocapacitance (Pseudocapacitors)
  • or with both storage principles together (Hybrid capacitors).

The most important material parameters of the different dielectrics used and the appr. Helmholtz-layer thickness are given in the table below.

The capacitor’s plate area can be adapted to the wanted capacitance value. The permittivity and the dielectric thickness are the determining parameter for capacitors. Ease of processing is also crucial. Thin, mechanically flexible sheets can be wrapped or stacked easily, yielding large designs with high capacitance values. Razor-thin metallized sintered ceramic layers covered with metallized electrodes however, offer the best conditions for the miniaturization of circuits with SMD styles.

A short view to the figures in the table above gives the explanation for some simple facts:

  • Supercapacitors have the highest capacitance density because of its special charge storage principles
  • Electrolytic capacitors have lesser capacitance density than supercapacitors but the highest capacitance density of conventional capacitors because its thin dielectric.
  • Ceramic capacitors class 2 have much higher capacitance values in a given case than class 1 capacitors because of their much higher permittivity.
  • Film capacitors with their different plastic film material do have a small spread in the dimensions for a given capacitance/voltage value of a film capacitor because the minimum dielectric film thickness differs between the different film materials.

Capacitance and voltage range[edit]

Capacitance ranges vs. voltage ranges of different capacitor types

Capacitance ranges from picofarad to more than hundreds of farad. Voltage ratings can reach 100 kilovolts. In general, capacitance and voltage correlates with physical size and cost.


Capacitor volumetric efficiency increased from 1970 to 2005 (click image to enlarge)

As in other areas of electronics, volumetric efficiency measures the performance of electronic function per unit volume. For capacitors, the volumetric efficiency is measured with the “CV product”, calculated by multiplying the capacitance (C) by the maximum voltage rating (V), divided by the volume. From 1970 to 2005, volumetric efficiencies have improved dramatically.

Overlapping range of applications[edit]

These individual capacitors can perform their application independent of their affiliation to an above shown capacitor type, so that an overlapping range of applications between the different capacitor types exists.

Comparing the three main capacitor types it shows, that a broad range of overlapping functions for many general-purpose and industrial applications exists in electronic equipment.

Capacitor – types and styles[edit]

Ceramic capacitors[edit]

Construction of a Multi-Layer Ceramic Capacitor (MLCC)
Main page: Ceramic capacitor

A ceramic capacitor is a non-polarized fixed capacitor made out of two or more alternating layers of ceramic and metal in which the ceramic material acts as the dielectric and the metal acts as the electrodes. The ceramic material is a mixture of finely ground granules of paraelectric or ferroelectric materials, modified by mixed oxides that are necessary to achieve the capacitor’s desired characteristics. The electrical behavior of the ceramic material is divided into two stability classes:

  • Class 1 ceramic capacitors with high stability and low losses compensating the influence of temperature in resonant circuit application. Common EIA/IEC code abbreviations are C0G/NP0, P2G/N150, R2G/N220, U2J/N750 etc.
  • Class 2 ceramic capacitors with high volumetric efficiency for buffer, by-pass and coupling applications Common EIA/IEC code abbreviations are: X7R/2XI, Z5U/E26, Y5V/2F4, X7S/2C1, etc.

The great plasticity of ceramic raw material works well for many special applications and enables an enormous diversity of styles, shapes and great dimensional spread of ceramic capacitors. The smallest discrete capacitor, for instance, is a “01005” chip capacitor with the dimension of only 0.4 mm × 0.2 mm.

The construction of ceramic multilayer capacitors with mostly alternating layers results in single capacitors connected in parallel. This configuration increases capacitance and decreases all losses and parasitic inductances. Ceramic capacitors are well-suited for high frequencies and high current pulse loads.

Because the thickness of the ceramic dielectric layer can be easily controlled and produced by the desired application voltage, ceramic capacitors are available with rated voltages up to the 30 kV range.

Some ceramic capacitors of special shapes and styles are used as capacitors for special applications, including RFI/EMI suppression capacitors for connection to supply mains, also known as safety capacitors,[9][10] X2Y® capacitors for bypassing and decoupling applications,[11] feed-through capacitors for noise suppression by low-pass filters[12] and ceramic power capacitors for transmitters and HF applications.[13][14]

Features and applications as well as disadvantages of ceramic capacitors
Capacitor type Dielectric Features/applications Disadvantages
Ceramic Class 1 capacitors paraelectric ceramic mixture of Titanium dioxide modified by additives Predictable linear and low capacitance change with operating temperature. Excellent high frequency characteristics with low losses. For temperature compensation in resonant circuit application. Available in voltages up to 15,000 V Low permittivity ceramic, capacitors with low volumetric efficiency, larger dimensions than Class 2 capacitors
Ceramic Class 2 capacitors ferroelectric ceramic mixture of barium titanate and suitable additives High permittivity, high volumetric efficiency, smaller dimensions than Class 1 capacitors. For buffer, by-pass and coupling applications. Available in voltages up to 50,000 V. Lower stability and higher losses than Class 1. Capacitance changes with change in applied voltage, with frequency and with aging effects. Slightly microphonic

Film capacitors[edit]

Main page: Film capacitor

Three examples of different film capacitor configurations for increasing surge current ratings

Film capacitors or plastic film capacitors are non-polarized capacitors with an insulating plastic film as the dielectric. The dielectric films are drawn to a thin layer, provided with metallic electrodes and wound into a cylindrical winding. The electrodes of film capacitors may be metallized aluminum or zinc, applied on one or both sides of the plastic film, resulting in metallized film capacitors or a separate metallic foil overlying the film, called film/foil capacitors.

Metallized film capacitors offer self-healing properties. Dielectric breakdowns or shorts between the electrodes do not destroy the component. The metallized construction makes it possible to produce wound capacitors with larger capacitance values (up to 100 µF and larger) in smaller cases than within film/foil construction.

Film/foil capacitors or metal foil capacitors use two plastic films as the dielectric. Each film is covered with a thin metal foil, mostly aluminium, to form the electrodes. The advantage of this construction is the ease of connecting the metal foil electrodes, along with an excellent current pulse strength.

A key advantage of every film capacitor’s internal construction is direct contact to the electrodes on both ends of the winding. This contact keeps all current paths very short. The design behaves like a large number of individual capacitors connected in parallel, thus reducing the internal ohmic losses (ESR) and parasitic inductance (ESL). The inherent geometry of film capacitor structure results in low ohmic losses and a low parasitic inductance, which makes them suitable for applications with high surge currents (snubbers) and for AC power applications, or for applications at higher frequencies.

The plastic films used as the dielectric for film capacitors are Polypropylene (PP), Polyester (PET), Polyphenylene sulfide (PPS), Polyethylene naphthalate (PEN), and Polytetrafluoroethylene or Teflon (PTFE). Polypropylene film material with a market share of something about 50% and Polyester film with something about 40% are the most used film materials. The rest of something about 10% will be used by all other materials including PPS and paper with roughly 3%, each.[15][16]

Characteristics of plastic film materials for film capacitors
Film material, abbreviated codes
Film characteristics PET PEN PPS PP
Relative permittivity at 1 kHz 3.3 3.0 3.0 2.2
Minimum film thickness (µm) 0.7–0.9 0.9–1.4 1.2 2.4–3.0
Moisture absorption (%) low 0.4 0.05 <0.1
Dielectric strength (V/µm) 580 500 470 650
Commercial realized
voltage proof (V/µm)
280 300 220 400
DC voltage range (V) 50–1,000 16–250 16–100 40–2,000
Capacitance range 100 pF–22 µF 100 pF–1 µF 100 pF–0.47 µF 100 pF–10 µF
Application temperature range (°C) −55 to +125 /+150 −55 to +150 −55 to +150 −55 to +105
ΔC/C versus temperature range (%) ±5 ±5 ±1.5 ±2.5
Dissipation factor (•10−4)
at 1 kHz 50–200 42–80 2–15 0.5–5
at 10 kHz 110–150 54–150 2.5–25 2–8
at 100 kHz 170–300 120–300 12–60 2–25
at 1 MHz 200–350 18–70 4–40
Time constant RInsul•C (s) at 25 °C ≥10,000 ≥10,000 ≥10,000 ≥100,000
at 85 °C 1,000 1,000 1,000 10,000
Dielectric absorption (%) 0.2–0.5 1–1.2 0.05–0.1 0.01–0.1
Specific capacitance (nF•V/mm3) 400 250 140 50

Some film capacitors of special shapes and styles are used as capacitors for special applications, including RFI/EMI suppression capacitors for connection to the supply mains, also known as safety capacitors,[17] Snubber capacitors for very high surge currents,[18] Motor run capacitors, AC capacitors for motor-run applications[19]

Features and applications as well as disadvantages of film capacitors
Capacitor type Dielectric Features/applications Disadvantages
Metallized film capacitors PP, PET, PEN, PPS, (PTFE) Metallized film capacitors are significantly smaller in size than film/foil versions and have self-healing properties. Thin metallized electrodes limit the maximum current carrying capability respectively the maximum possible pulse voltage.
Film/foil film capacitors PP, PET, PTFE Film/foil film capacitors have the highest surge ratings/pulse voltage, respectively. Peak currents are higher than for metallized types. No self-healing properties: internal short may be disabling. Larger dimensions than metallized alternative.
Polypropylene (PP) film capacitors Polypropylene
Most popular film capacitor dielectric. Predictable linear and low capacitance change with operating temperature. Suitable for applications in Class-1 frequency-determining circuits and precision analog applications. Very narrow capacitances. Extremely low dissipation factor. Low moisture absorption, therefore suitable for “naked” designs with no coating. High insulation resistance. Usable in high power applications such as snubber or IGBT. Used also in AC power applications, such as in motors or power factor correction. Very low dielectric losses. High frequency and high power applications such as induction heating. Widely used for safety/EMI suppression, including connection to power supply mains. Maximum operating temperature of 105 °C. Relatively low permittivity of 2.2. PP film capacitors tend to be larger than other film capacitors. More susceptible to damage from transient over-voltages or voltage reversals than oil-impregnated MKV-capacitors for pulsed power applications.
Polyester (PET) film
(Mylar) capacitors
Polyethylene terephthalate, Polyester (Hostaphan®, Mylar®) Smaller in size than functionally comparable polypropylene film capacitors. Low moisture absorption. Have almost completely replaced metallized paper and polystyrene film for most DC applications. Mainly used for general purpose applications or semi-critical circuits with operating temperatures up to 125 °C. Operating voltages up to 60,000 V DC. Usable at low (AC power) frequencies. Limited use in power electronics due to higher losses with increasing temperature and frequency.
Polyethylene naphthalate
(PEN) film capacitors
Polyethylene naphthalate (Kaladex®) Better stability at high temperatures than PET. More suitable for high temperature applications and for SMD packaging. Mainly used for non-critical filtering, coupling and decoupling, because temperature dependencies are not significant. Lower relative permittivity and lower dielectric strength imply larger dimensions for a given capacitance and rated voltage than PET.
Polyphenylene Sulfide (PPS)
film capacitors
Polyphenylene (Torelina®) Small temperature dependence over the entire temperature range and a narrow frequency dependence in a wide frequency range. Dissipation factor is quite small and stable. Operating emperatures up to 270 °C. Suitable for SMD. Tolerate increased reflow soldering temperatures for lead-free soldering mandated by the RoHS 2002/95/European Union directive Above 100 °C, the dissipation factor increases, increasing component temperature, but can operate without degradation. Cost is usually higher than PP.
Polytetrafluoroethylene (PTFE)
(Teflon film) capacitors
Polytetrafluoroethylene (Teflon®) Lowest loss solid dielectric. Operating temperatures up to 250 °C. Extremely high insulation resistance. Good stability. Used in mission-critical applications. Large size (due to low dielectric constant). Higher cost than other film capacitors.
Polycarbonate (PC)
film capacitors
Polycarbonate Almost completely replaced by PP Limited manufacturers
Polystyrene (PS)
film capacitors
Polystyrene (Styroflex) Almost completely replaced by PET Limited manufacturers
Polysulphone film capacitors Polysulfone Similar to polycarbonate. Withstand full voltage at comparatively higher temperatures. Only development, no series found (2012)
Polyamide film capacitors Polyamide Operating temperatures of up to 200 °C. High insulation resistance. Good stability. Low dissipation factor. Only development, no series found (2012)
Polyimide film
(Kapton) capacitors
Polyimide (Kapton) Highest dielectric strength of any known plastic film dielectric. Only development, no series found (2012)

Film power capacitors[edit]

MKV power capacitor, double-sided metallized paper (field-free mechanical carrier of the electrodes), polypropylene film (dielectric), windings impregnated with insulating oil

A related type is the power film capacitor. The materials and construction techniques used for large power film capacitors mostly are similar to those of ordinary film capacitors. However, capacitors with high to very high power ratings for applications in power systems and electrical installations are often classified separately, for historical reasons. The standardization of ordinary film capacitors is oriented on electrical and mechanical parameters. The standardization of power capacitors by contrast emphasizes the safety of personnel and equipment, as given by the local regulating authority.

As modern electronic equipment gained the capacity to handle power levels that were previously the exclusive domain of “electrical power” components, the distinction between the “electronic” and “electrical” power ratings blurred. Historically, the boundary between these two families was approximately at a reactive power of 200 volt-amps.

Film power capacitors mostly use polypropylene film as the dielectric. Other types include metallized paper capacitors (MP capacitors) and mixed dielectric film capacitors with polypropylene dielectrics. MP capacitors serve for cost applications and as field-free carrier electrodes (soggy foil capacitors) for high AC or high current pulse loads. Windings can be filled with an insulating oil or with epoxy resin to reduce air bubbles, thereby preventing short circuits.

They find use as converters to change voltage, current or frequency, to store or deliver abruptly electric energy or to improve the power factor. The rated voltage range of these capacitors is from approximately120 V AC (capacitive lighting ballasts) to 100 kV.[20]

Features and applications as well as disadvantages of film-based power capacitors
Capacitor type Dielectric Features/applications Disadvantages
Metallized paper power capacitors Paper impregnated with insulating oil or epoxy resin Self-healing properties. Originally impregnated with wax, oil or epoxy. Oil-Kraft paper version used in certain high voltage applications. Mostly replaced by PP. Large size. Highly hygroscopic, absorbing moisture from the atmosphere despite plastic enclosures and impregnates. Moisture increases dielectric losses and decreases insulation resistance.
Paper film/foil power capacitors Kraft paper impregnated with oil Paper covered with metal foils as electrodes. Low cost. Intermittent duty, high discharge applications. Physically large and heavy. Significantly lower energy density than PP dielectric. Not self-healing. Potential catastrophic failure due to high stored energy.
PP dielectric,
field-free paper
power capacitors
(MKV power capacitors)
Double-sided (field-free) metallized paper as electrode carrier. PP as dielectic, impregnated with insulating oil, epoxy resin or insulating gas Self-healing. Very low losses. High insulation resistance. High inrush current strength. High thermal stability. Heavy duty applications such as commutating with high reactive power, high frequencies and a high peak current load and other AC applications. Physically larger than PP power capacitors.
Single- or double-sided
metallized PP power capacitors
PP as dielectric, impregnated with insulating oil, epoxy resin or insulating gas Highest capacitance per volume power capacitor. Self-healing. Broad range of applications such as general-purpose, AC capacitors, motor capacitors, smoothing or filtering, DC links, snubbing or clamping, damping AC, series resonant DC circuits, DC discharge, AC commutation, AC power factor correction. critical for reliable high voltage operation and very high inrush current loads, limited heat resistance (105 °C)
PP film/foil power capacitors Impregnated PP or insulating gas, insulating oil, epoxy resin or insulating gas Highest inrush current strength Larger than the PP metallized versions. Not self-healing.

Electrolytic capacitors[edit]

Main page: Electrolytic capacitor

Electrolytic capacitors have a metallic anode covered with an oxidized layer used as dielectric. The second electrode is a non-solid (wet) or solid electrolyte. Electrolytic capacitors are polarized. Three families are available, categorized according to their dielectric.

The anode is highly roughened to increase the surface area. This and the relatively high permittivity of the oxide layer gives these capacitors very high capacitance per unit volume compared with film- or ceramic capacitors.

The permittivity of tantalum pentoxide is approximately three times higher than aluminium dioxide, producing significantly smaller components. However, permittivity determines only the dimensions. Electrical parameters, especially conductivity, are established by the electrolyte’s material and composition. Three general types of electrolytes are used:

  • non solid (wet, liquid)—conductivity approximately 10 mS/cm and are the lowest cost
  • solid manganese oxide—conductivity approximately 100 mS/cm offer high quality and stability
  • solid conductive polymer (Polypyrrole)—conductivity approximately 10,000 mS/cm,[21] offer ESR values as low as <10 mΩ

Internal losses of electrolytic capacitors, prevailing used for decoupling and buffering applications, are determined by the kind of electrolyte.

Some important values of the different electrolytic capacitors
Anode material Electrolyte Capacitance
Max. rated
at 85 °C
ripple current
(roughned foil)
non solid,
e.g. Ethylene glycol,
0.1–2,700,000 600 150 0.05–2.0
Manganese dioxide
0.1–1,500 40 175 0.5–2.5
conductive polymere
(e.g. Polypyrrole)
10–1,500 25 125 10–30
(roughned foil)
non solid
Sulfuric acid
0.1–1,000 630 125
non solid
sulfuric acid
0.1–15,000 150 200
Manganese dioxide
0.1–3,300 125 150 1.5–15
conductive polymere
(e.g. Polypyrrole)
10–1,500 35 125 10–30
Manganese dioxide
1–1,500 10 125 5–20
conductive polymere
(e.g. Polypyrrole)
2.2–1,000 25 105 10–30
1) Ripple current at 100 kHz and 85 °C / volumen (nominal dimensions)

The large capacitance per unit volume of electrolytic capacitors make them valuable in relatively high-current and low-frequency electrical circuits, e.g. in power supply filters for decoupling unwanted AC components from DC power connections or as coupling capacitors in audio amplifiers, for passing or bypassing low-frequency signals and storing large amounts of energy. The relatively high capacitance value of an electrolytic capacitor combined with the very low ESR of the polymer electrolyte of polymer capacitors, especially in SMD styles, makes them a competitor to MLC chip capacitors in personal computer power supplies.

Bipolar electrolytics (also called Non-Polarized capacitors) contain two anodized aluminium foils, behaving like two capacitors connected in series opposition.

Electolytic capacitors for special applications include motor start capacitors,[22] flashlight capacitors[23] and audio frequency capacitors.[24]

Features and applications as well as disadvantages of electrolytic capacitors
Capacitor type Dielectric Features/applications Disadvantages
Electrolytic capacitors
with non solid
(wet, liquid)
Aluminum dioxide
Very large capacitance to volume ratio. Capacitance values up to 2,700,000 µF/6.3 V. Voltage up to 550 V. Lowest cost per capacitance/voltage values. Used where low losses and high capacitance stability are not of major importance, especially for lower frequencies, such as by-pass, coupling, smoothing and buffer applications in power supplies and DC-links. Polarized. Significant leakage. Relatively high ESRTemplate:Dn and ESL values, limiting high ripple current and high frequency applications. Lifetime calculation required because drying out phenomenon. Vent or burst when overloaded, overheated or connected wrong polarized. Water based electrolyte may vent at end-of-life, showing failures like “capacitor plague”
Tantalum pentoxide
Wet tantalum electrolytic capacitors (wet slug)[25] Lowest leakage among electrolytics. Voltage up to 630 V (tantalum film) or 125 V (tantalum sinter body). Hermetically sealed. Stable and reliable. Military and space applications. Polarized. Violent explosion when voltage, ripple current or slew rates are exceeded, or under reverse voltage. Expensive.
[Electrolytic capacitors
with solid [Manganese dioxide]] electrolyte
Aluminum dioxide
Tantalum pentoxide
Niobium pentoxide
Tantalum and niobium with smaller dimensions for a given capacitance/voltage vs aluminum. Stable electrical parameters. Good long-term high temperature performance. Lower ESR lower than non-solid (wet) electrolytics. Polarized. About 125 V. Low voltage and limited, transient, reverse or surge voltage tolerance. Possible combustion upon failure. ESR much higher than conductive polymer electrolytics. Manganese expected to be replaced by polymer.
Electrolytic capacitors
with solid Polymer electrolyte
(Polymer capacitors)
Aluminum dioxide
Tantalum pentoxide
Niobium pentoxide
Greatly reduced ESR compared with manganese or non-solid (wet) elelectrolytics. Higher ripple current ratings. Extended operational life. Stable electrical parameters. Self-healing.[26] Used for smoothing and buffering in smaller power supplies especially in SMD. Polarized. Highest leakage current among electrolytics. Higher prices than non-solid or manganese dioxide. Voltage limited to about 100 V. Explodes when voltage, current, or slew rates are exceeded or under reverse voltage.


Main page: Supercapacitor

Hierarchical classification of supercapacitors and related types

Ragone chart showing power density vs. energy density of various capacitors and batteries

Classification of supercapacitors into classes regarding to IEC 62391-1, IEC 62567and DIN EN 61881-3 standards

Supercapacitors (SC),[27] comprise a family of electrochemical capacitors. Supercapacitor, sometimes called ultracapacitor is a generic term for electric double-layer capacitors (EDLC), pseudocapacitors and hybrid capacitors. They don’t have a conventional solid dielectric. The capacitance value of an electrochemical capacitor is determined by two storage principles, both of which contribute to the total capacitance of the capacitor:[28][29][30]

The ratio of the storage resulting from each principle can vary greatly, depending on electrode design and electrolyte composition. Pseudocapacitance can increase the capacitance value by as much as an order of magnitude over that of the double-layer by itself.[27]

Supercapacitors are divided into three families, based on the design of the electrodes:

  • Double-layer capacitors – with carbon electrodes or derivates with much higher static double-layer capacitance than the faradaic pseudocapacitance
  • Pseudocapacitors – with electrodes out of metal oxides or conducting polymers with a high amount of faradaic pseudocapacitance
  • Hybrid capacitors – capacitors with special and asymmetric electrodes that exhibit both significant double-layer capacitance and pseudocapacitance, such as lithium-ion capacitors

Supercapacitors bridge the gap between conventional capacitors and rechargeable batteries. They have the highest available capacitance values per unit volume and the greatest energy density of all capacitors. They support up to 12,000 Farads/1.2 Volt,[31] with capacitance values up to 10,000 times that of electrolytic capacitors.[27] While existing supercapacitors have energy densities that are approximately 10% of a conventional battery, their power density is generally 10 to 100 times greater. Power density is defined as the product of energy density, multiplied by the speed at which the energy is delivered to the load. The greater power density results in much shorter charge/discharge cycles than a battery is capable, and a greater tolerance for numerous charge/discharge cycles. This makes them well-suited for parallel connection with batteries, and may improve battery performance in terms of power density.

Within electrochemical capacitors, the electrolyte is the conductive connection between the two electrodes, distinguishing them from electrolytic capacitors, in which the electrolyte only forms the cathode, the second electrode.

Supercapacitors are polarized and must operate with correct polarity. Polarity is controlled by design with asymmetric electrodes, or, for symmetric electrodes, by a potential applied during the manufacturing process.

Supercapacitors support a broad spectrum of applications for power and energy requirements, including:

  • Low supply current during longer times for memory backup in (SRAMs) in electronic equipment
  • Power electronics that require very short, high current, as in the KERSsystem in Formula 1 cars
  • Recovery of braking energy for vehicles such as buses and trains

Supercapacitors are rarely interchangeable, especially those with higher energy densities. IEC standard 62391-1 Fixed electric double layer capacitors for use in electronic equipment identifies four application classes:

  • Class 1, Memory backup, discharge current in mA = 1 • C (F)
  • Class 2, Energy storage, discharge current in mA = 0.4 • C (F) • V (V)
  • Class 3, Power, discharge current in mA = 4 • C (F) • V (V)
  • Class 4, Instantaneous power, discharge current in mA = 40 • C (F) • V (V)

Exceptional for electronic components like capacitors are the manifold different trade or series names used for supercapacitors like: APowerCap, BestCap, BoostCap, CAP-XX, DLCAP, EneCapTen, EVerCAP, DynaCap, Faradcap, GreenCap, Goldcap, HY-CAP, Kapton capacitor, Super capacitor, SuperCap, PAS Capacitor, PowerStor, PseudoCap, Ultracapacitor making it difficult for users to classify these capacitors.

Features and applications as well as disadvantages of supercapacitors
Capacitor type Dielectric Features/applications Disadvantages
Helmholtz double-layer plus faradaic pseudo-capacitance Energy density typically tens to hundreds of times greater than conventional electrolytics. More comparable to batteries than to other capacitors. Large capacitance/volume ratio. Relatively low ESR. Thousands of farads. RAM memory backup. Temporary power during battery replacement. Rapidly absorbs/delivers much larger currents than batteries. Hundreds of thousands of charge/discharge cycles. Hybrid vehicles. Recuperation Polarized. Low operating voltage per cell. (Stacked cells provide higher operating voltage.) Relatively high cost.
Hybrid capacitors
Lithium ion capacitors
Helmholtz double-layer plus faradaic pseudo-capacitance. Anode doped with lithium ions. Higher operating voltage. Higher energy density than common EDLCs, but smaller than lithium ion batteries (LIB). No thermal runaway reactions. Polarized. Low operating voltage per cell. (Stacked cells provide higher operating voltage.) Relatively high cost.

Miscellaneous capacitors[edit]

Beneath the above described capacitors covering more or less nearly the total market of discrete capacitors some new developments or very special capacitor types as well as older types can be found in electronics.

Integrated capacitors[edit]

  • Integrated capacitors—in integrated circuits, nano-scale capacitors can be formed by appropriate patterns of metallization on an isolating substrate. They may be packaged in multiple capacitor arrays with no other semiconductive parts as discrete components.[32]
  • Glass capacitors—First Leyden jar capacitor was made of glass, As of 2012 glass capacitors were in use as SMD version for applications requiring ultra-reliable and ultra-stable service.

Power capacitors[edit]

  • Vacuum capacitors—used in high power RF transmitters
  • SF6 gas filled capacitors—used as capacitance standard in measuring bridge circuits

Special capacitors[edit]

  • Printed circuit boards—metal conductive areas in different layers of a multi-layer printed circuit board can act as a highly stable capacitor. It is common industry practice to fill unused areas of one PCB layer with the ground conductor and another layer with the power conductor, forming a large distributed capacitor between the layers.
  • Wire—2 pieces of insulated wire twisted together. Capacitance alues usually range from 3 pF to 15 pF. Used in homemade VHF circuits for oscillation feedback.

Obsolete capacitors[edit]

Features and applications as well as disadvantages of miscellaneous capacitors
Capacitor type Dielectric Features/applications Disadvantages
Air gap capacitors Air Low dielectric loss. Used for resonating HF circuits for high power HF welding. Physically large. Relatively low capacitance.
Vacuum capacitors Vacuum Extremely low losses. Used for high voltage, high power RF applications, such as transmitters and induction heating. Self-healing if arc-over current is limited. Very high cost. Fragile. Large. Relatively low capacitance.
SF6-gas filled capacitors SF6 gas High precision.[33] Extremely low losses. Very high stability. Up to 1600 kV rated voltage. Used as capacitance standard in measuring bridge circuits. Very high cost
Metallized mica (Silver mica) capacitors Mica Very high stability. No aging. Low losses. Used for HF and low VHF RF circuits and as capacitance standard in measuring bridge circuits. Mostly replaced by Class 1 ceramic capacitors Higher cost than class 1 ceramic capacitors
Glass capacitors Glass Better stability and frequency than silver mica. Ultra-reliable. Ultra-stable. Resistant to nuclear radiation. Operating temperature: −75 °C to +200 °C and even short overexposure to +250 °C.[34] Higher cost than class 1 ceramic
Integrated capacitors oxide-nitride-oxide (ONO) Thin (down to 100 µm). Smaller footprint than most MLCC. Low ESL. Very high stability up to 200 °C. High reliability Customized production

Variable capacitors[edit]

Variable capacitors may have their capacitance changed by mechanical motion. Generally two versions of variable capacitors has to be to distinguished

  • Tuning capacitor – variable capacitor for intentionally and repeatedly tuning an oscillator circuit in a radio or another tuned circuit
  • Trimmer capacitor – small variable capacitor usually for one-time oscillator circuit internal adjustment

Variable capacitors include capacitors that use a mechanical construction to change the distance between the plates, or the amount of plate surface area which overlaps. They mostly use air as dielectric medium.

Semiconductive variable capacitance diodes are not capacitors in the sense of passive components but can change their capacitance as a function of the applied reverse bias voltage and are used like a variable capacitor. They have replaced much of the tuning and trimmer capacitors.

Features and applications as well as disadvantages of variable capacitors
Capacitor type Dielectric Features/applications Disadvantages
Air gap tuning capacitors Air Circular or various logarithmic cuts of the rotor electrode for different capacitance curves. Split rotor or stator cut for symmetric adjustment. Ball bearing axis for noise reduced adjustment. For high professional devices. Large dimensions. High cost.
Vacuum tuning capacitors Vacuum Extremely low losses. Used for high voltage, high power RF applications, such as transmitters and induction heating. Self-healing if arc-over current is limited. Very high cost. Fragile. Large dimensions.
SF6 gas filled tuning capacitor SF6 Extremely low losses. Used for very high voltage high power RF applications. Very high cost, fragile, large dimensions
Air gap trimmer capacitors Air Mostly replaced by semiconductive variable capacitance diodes High cost
Ceramic trimmer capacitors Class 1 ceramic Linear and stable frequency behavior over wide temperature range High cost


Discrete capacitors today are industrial products produced in very large quantities for use in electronic and in electrical equipment. Globally, the market for fixed capacitors was estimated at approximately US$18 billion in 2008 for 1,400 billion (1.4 × 1012) pieces.[35] This market is dominated by ceramic capacitors with estimate of approximately one trillion (1 × 1012) items per year.[1]

Detailed estimated figures in value for the main capacitor families are:

All other capacitor types are negligible in terms of value and quantity compared with the above types.

Capacitor – Electrical characteristics[edit]

Series-equivalent circuit[edit]

Series-equivalent circuit model of a capacitor

Discrete capacitors deviate from the ideal capacitor. An ideal capacitor only stores and releases electrical energy, with no dissipation. Capacitor components have losses and parasitic inductive parts. These imperfections in material and construction can have positive implications such as linear frequency and temperature behavior in class 1 ceramic capacitors. Conversely, negative implications include the non-linear, voltage-dependent capacitance in class 2 ceramic capacitors or the insufficient dielectric insulation of capacitors leading to leakage currents.

All properties can be defined and specified by a series equivalent circuit composed out of an idealized capacitance and additional electrical components which model all losses and inductive parameters of a capacitor. In this series-equivalent circuit the electrical characteristics are defined by:

  • C, the capacitance of the capacitor
  • Rinsul, the insulation resistance of the dielectric, not to be confused with the insulation of the housing
  • Rleak, the resistance representing the leakage current of the capacitor
  • RESR, the equivalent series resistance which summarizes all ohmic losses of the capacitor, usually abbreviated as “ESR”
  • LESL, the equivalent series inductance which is the effective self-inductance of the capacitor, usually abbreviated as “ESL”.

Using a series equivalent circuit instead of a parallel equivalent circuit is specified by IEC/EN 60384-1.

Standard values and tolerances[edit]

The “rated capacitance” CR or “nominal capacitance” CN is the value for which the capacitor has been designed. Actual capacitance depends on the measured frequency and ambient temperature. Standard measuring conditions are a low-voltage AC measuring method at a temperature of 20 °C with frequencies of

  • 100 kHz, 1 MHz (preferred) or 10 MHz for non-electrolytic capacitors with CR ≤ 1 nF:
  • 1 kHz or 10 kHz for non-electrolytic capacitors with 1 nF < CR ≤ 10 μF
  • 100/120 Hz for electrolytic capacitors
  • 50/60 Hz or 100/120 Hz for non-electrolytic capacitors with CR > 10 μF

For supercapacitors a voltage drop method is applied for measuring the capacitance value. .

Capacitors are available in geometrically increasing preferred values (E series standards) specified in IEC/EN 60063. According to the number of values per decade, these were called the E3, E6, E12, E24 etc. series. The range of units used to specify capacitor values has expanded to include everything from pico- (pF), nano- (nF) and microfarad (µF) to farad (F). Millifarad and kilofarad are uncommon.

The percentage of allowed deviation from the rated value is called tolerance. The actual capacitance value should be within its tolerance limits, or it is out of specification. IEC/EN 60062 specifies a letter code for each tolerance.

Tolerances of capacitors and their letter codes
E series Tolerance
CR > 10 pF Letter code CR < 10 pF Letter code
E 96 1% F 0.1 pF B
E 48 2% G 0.25 pF C
E 24 5% J 0.5 pF D
E 12 10% K 1 pF F
E 6 20% M 2 pF G
E3 −20/+50% S
−20/+80% Z

The required tolerance is determined by the particular application. The narrow tolerances of E24 to E96 are used for high-quality circuits such as precision oscillators and timers. General applications such as non-critical filtering or coupling circuits employ E12 or E6. Electrolytic capacitors, which are often used for filtering and bypassing capacitors mostly have a tolerance range of ±20% and need to conform to E6 (or E3) series values.

Temperature dependence[edit]

Capacitance typically varies with temperature. The different dielectrics express great differences in temperature sensitivity. The temperature coefficient is expressed in parts per million (ppm) per degree Celsius for class 1 ceramic capacitors or in % over the total temperature range for all others.

Temperature coefficients of some common capacitors
Type of capacitor,
dielectric material
Temperature coefficient
temperature range
Ceramic capacitor class 1
paraelectric NP0
± 30 ppm/K (±0.5 %) −55 to +125 °C
Ceramic capacitor class 2
ferroelectric X7R
±15 % −55 to +125 °C
Ceramic capacitor class 2,
ferroelectric Y5V
+22 % / −82 % −30 to +85 °C
Film capacitor
Polypropylene ( PP)
±2.5 % −55 to +85/105 °C
Film capacitor
Polyethylen terephthalate,
Polyester (PET)
+5 % −55 to +125/150 °C
Film capacitor
Polyphenylene sulfide (PPS)
±1.5 % −55 to +150 °C
Film capacitor
Polyethylene naphthalate (PEN)
±5 % −40 to +125/150 °C
Film capacitor
Polytetrafluoroethylene (PTFE)
? −40 to +130 °C
Metallized paper capacitor (impregnated) ±10 % −25 to +85 °C
Aluminum electrolytic capacitor
±20 % −40 to +85/105/125 °C
Tantalum electrolytic capacitor
±20 % −40 to +125 °C

Frequency dependence[edit]

Most discrete capacitor types have more or less capacitance changes with increasing frequencies. The dielectric strength of class 2 ceramic and plastic film diminishes with rising frequency. Therefore their capacitance value decreases with increasing frequency. This phenomenon for ceramic class 2 and plastic film dielectrics is related to dielectric relaxation in which the time constant of the electrical dipoles is the reason for the frequency dependence of permittivity. The graphs below show typical frequency behavior of the capacitance for ceramic and film capacitors.

For electrolytic capacitors with non-solid electrolyte, mechanical motion of the ions occurs. Their movability is limited so that at higher frequencies not all areas of the roughened anode structure are covered with charge-carrying ions. As higher the anode structure is roughned as more the capacitance value decreases with increasing frequency. Low voltage types with highly-roughened anodes display capacitance at 100 kHz approximately 10 to 20% of the value measured at 100 Hz.

Voltage dependence[edit]

Capacitance may also change with applied voltage. This effect is more prevalent in class 2 ceramic capacitors. The permittivity of ferroelectric class 2 material depends on the applied voltage. Higher applied voltage lowers permittivity. The change of capacitance can drop to 80% of the value measured with the standardized measuring voltage of 0.5 or 1.0 V. This behavior is a small source of non-linearity in low-distortion filters and other analog applications. In audio applications this can be the reason for harmonic distortion.

Film capacitors and electrolytic capacitors have no significant voltage dependence.

Rated and category voltage[edit]

Relation between rated and category temperature range and applied voltage

The voltage at which the dielectric becomes conductive is called the breakdown voltage, and is given by the product of the dielectric strength and the separation between the electrodes. The dielectric strength depends on temperature, frequency, shape of the electrodes, etc. Because a breakdown in a capacitor normally is a short circuit and destroys the component, the operating voltage is lower than the breakdown voltage. The operating voltage is specified such that the voltage may be applied continuously throughout the life of the capacitor.

In IEC/EN 60384-1 the allowed operating voltage is called “rated voltage” or “nominal voltage”. The rated voltage (UR) is the maximum DC voltage or peak pulse voltage that may be applied continuously at any temperature within the rated temperature range.

The voltage proof of nearly all capacitors decreases with increasing temperature. For some applications it is important to use a higher temperature range. Lowering the voltage applied at a higher temperature maintains safety margins. For some capacitor types therefore the IEC standard specify a second “temperature derated voltage” for a higher temperature range, the “category voltage”. The category voltage (UC) is the maximum DC voltage or peak pulse voltage that may be applied continuously to a capacitor at any temperature within the category temperature range.

The relation between both voltages and temperatures is given in the picture right.


Simplified series-equivalent circuit of a capacitor for higher frequencies (above); vector diagram with electrical reactances XESL and XC and resistance ESR and for illustration the impedance Z and dissipation factor tan δ

In general, a capacitor is seen as a storage component for electric energy. But this is only one capacitor function. A capacitor can also act as an AC resistor. In many cases the capacitor is used as a decoupling capacitor to filter or bypass undesired biased AC frequencies to the ground. Other applications use capacitors for capacitive coupling of AC signals; the dielectric is used only for blocking DC. For such applications the AC resistance is as important as the capacitance value.

The frequency dependent AC resistance is called impedance

Z{displaystyle scriptstyle Z}

and is the complex ratio of the voltage to the current in an AC circuit. Impedance extends the concept of resistance to AC circuits and possesses both magnitude and phase at a particular frequency. This is unlike resistance, which has only magnitude.

The magnitude

|Z|{displaystyle scriptstyle |Z|}

represents the ratio of the voltage difference amplitude to the current amplitude,

j{displaystyle scriptstyle j}

is the imaginary unit, while the argument

θ{displaystyle scriptstyle theta }

gives the phase difference between voltage and current.

In capacitor data sheets, only the impedance magnitude |Z| is specified, and simply written as “Z” so that the formula for the impedance can be written in Cartesian form

where the real part of impedance is the resistance

R{displaystyle scriptstyle R}

(for capacitors

ESR{displaystyle scriptstyle ESR}

) and the imaginary part is the reactance

X{displaystyle scriptstyle X}


As shown in a capacitor’s series-equivalent circuit, the real component includes an ideal capacitor

C{displaystyle C}

, an inductance

L(ESL){displaystyle L(ESL)}

and a resistor

R(ESR){displaystyle R(ESR)}

. The total reactance at the angular frequency

ω{displaystyle omega }

therefore is given by the geometric (complex) addition of a capacitive reactance (Capacitance)

XC=1ωC{displaystyle X_{C}=-{frac {1}{omega C}}}

and an inductive reactance (Inductance):

XL=ωLESL{displaystyle X_{L}=omega L_{mathrm {ESL} }}


To calculate the impedance

Z{displaystyle scriptstyle Z}

the resistance has to be added geometrically and then

Z{displaystyle Z}

is given by

to calculate either the peak or the effective value of the current or the voltage.

In the special case of resonance, in which the both reactive resistances

have the same value (

XC=XL{displaystyle X_{C}=X_{L}}

), then the impedance will only be determined by

ESR{displaystyle {ESR}}


Typical impedance curves for different capacitance values over frequency showing the typical form with a decreasing impedance values below resonance and increasing values above resonance. As higher the capacitance as lower the resonance.

The impedance specified in the datasheets often show typical curves for the different capacitance values. With increasing frequency as the impedance decreases down to a minimum. The lower the impedance, the more easily alternating currents can be passed through the capacitor. At the apex, the point of resonance, where XC has the same value than XL, the capacitor has the lowest impedance value. Here only the ESR determines the impedance. With frequencies above the resonance the impedance increases again due to the ESL of the capacitor. The capacitor becomes to an inductance.

As shown in the graph, the higher capacitance values can fit the lower frequencies better while the lower capacitance values can fit better the higher frequencies.

Aluminum electrolytic capacitors have relatively good decoupling properties in the lower frequency range up to about 1 MHz due to their large capacitance values. This is the reason for using electrolytic capacitors in standard or switched-mode power supplies behind the rectifier for smoothing application.

Ceramic and film capacitors are already out of their smaller capacitance values suitable for higher frequencies up to several 100 MHz. They also have significantly lower parasitic inductance, making them suitable for higher frequency applications, due to their construction with end-surface contacting of the electrodes. To increase the range of frequencies, often an electrolytic capacitor is connected in parallel with a ceramic or film capacitor.[36]

Many new developments are targeted at reducing parasitic inductance (ESL). This increases the resonance frequency of the capacitor and, for example, can follow the constantly increasing switching speed of digital circuits. Miniaturization, especially in the SMD multilayer ceramic chip capacitors (MLCC), increases the resonance frequency. Parasitic inductance is further lowered by placing the electrodes on the longitudinal side of the chip instead of the lateral side. The “face-down” construction associated with multi-anode technology in tantalum electrolytic capacitors further reduced ESL. Capacitor families such as the so-called MOS capacitor or silicon capacitors offer solutions when capacitors at frequencies up to the GHz range are needed.

Inductance (ESL) and self-resonant frequency[edit]

ESL in industrial capacitors is mainly caused by the leads and internal connections used to connect the capacitor plates to the outside world. Large capacitors tend to have higher ESL than small ones because the distances to the plate are longer and every mm counts as an inductance.

For any discrete capacitor, there is a frequency above DC at which it ceases to behave as a pure capacitor. This frequency, where

XC{displaystyle X_{C}}

is as high as

XL{displaystyle X_{L}}

, is called the self-resonant frequency. The self-resonant frequency is the lowest frequency at which the impedance passes through a minimum. For any AC application the self-resonant frequency is the highest frequency at which capacitors can be used as a capacitive component.

This is critically important for decoupling high-speed logic circuits from the power supply. The decoupling capacitor supplies transient current to the chip. Without decouplers, the IC demands current faster than the connection to the power supply can supply it, as parts of the circuit rapidly switch on and off. To counter this potential problem, circuits frequently use multiple bypass capacitors—small (100 nF or less) capacitors rated for high frequencies, a large electrolytic capacitor rated for lower frequencies and occasionally, an intermediate value capacitor.

Ohmic losses, ESR, dissipation factor, and quality factor[edit]

The summarized losses in discrete capacitors are ohmic AC losses. DC losses are specified as “leakage current” or “insulating resistance” and are negligible for an AC specification. AC losses are non-linear, possibly depending on frequency, temperature, age or humidity. The losses result from two physical conditions:

  • line losses including internal supply line resistances, the contact resistance of the electrode contact, line resistance of the electrodes, and in “wet” aluminum electrolytic capacitors and especially supercapacitors, the limited conductivity of liquid electrolytes and
  • dielectric losses from dielectric polarization.

The largest share of these losses in larger capacitors is usually the frequency dependent ohmic dielectric losses. For smaller components, especially for wet electrolytic capacitors, conductivity of liquid electrolytes may exceed dielectric losses. To measure these losses, the measurement frequency must be set. Since commercially available components offer capacitance values cover 15 orders of magnitude, ranging from pF (10−12 F) to some 1000 F in supercapacitors, it is not possible to capture the entire range with only one frequency. IEC 60384-1 states that ohmic losses should be measured at the same frequency used to measure capacitance. These are:

  • 100 kHz, 1 MHz (preferred) or 10 MHz for non-electrolytic capacitors with CR ≤ 1 nF:
  • 1 kHz or 10 kHz for non-electrolytic capacitors with 1 nF < CR ≤ 10 μF
  • 100/120 Hz for electrolytic capacitors
  • 50/60 Hz or 100/120 Hz for non-electrolytic capacitors with CR > 10 μF

A capacitor’s summarized resistive losses may be specified either as ESR, as a dissipation factor(DF, tan δ), or as quality factor (Q), depending on application requirements.

Capacitors with higher ripple current

IR{displaystyle I_{R}}

 loads, such as electrolytic capacitors, are specified with equivalent series resistance ESR. ESR can be shown as an ohmic part in the above vector diagram. ESR values are specified in datasheets per individual type.

The losses of film capacitors and some class 2 ceramic capacitors are mostly specified with the dissipation factor tan δ. These capacitors have smaller losses than electrolytic capacitors and mostly are used at higher frequencies up to some hundred MHz. However the numeric value of the dissipation factor, measured at the same frequency, is independent on the capacitance value and can be specified for a capacitor series with a range of capacitance. The dissipation factor is determined as the tangent of the reactance (

XCXL{displaystyle X_{C}-X_{L}}

) and the ESR, and can be shown as the angle δ between imaginary and the impedance axis.

If the inductance

ESL{displaystyle ESL}

 is small, the dissipation factor can be approximated as:

Capacitors with very low losses, such as ceramic Class 1 and Class 2 capacitors, specify resistive losses with a quality factor (Q). Ceramic Class 1 capacitors are especially suitable for LC resonant circuits with frequencies up to the GHz range, and precise high and low pass filters. For an electrically resonant system, Q represents the effect of electrical resistance and characterizes a resonator’s bandwidth

B{displaystyle B}

relative to its center or resonant frequency

f0{displaystyle f_{0}}

. Q is defined as the reciprocal value of the dissipation factor.

A high Q value is for resonant circuits a mark of the quality of the resonance.

Comparization of ohmic losses for different capacitor types
for resonant circuits (Reference frequency 1 MHz)
Capacitor type Capacitance
at 100 kHz
at 1 MHz
tan δ
at 1 MHz
Silicon capacitor[37] 560 400 2,5 4000
Mica capacitor[38] 1000 650 65 4 2500
Class 1
ceramic capacitor (NP0)[39]
1000 1600 160 10 1000

Limiting current loads[edit]

A capacitor can act as an AC resistor, coupling AC voltage and AC current between two points. Every AC current flow through a capacitor generates heat inside the capacitor body. These dissipation power loss

P{displaystyle P}

is caused by

ESR{displaystyle ESR}

and is the squared value of the effective (RMS) current

I{displaystyle I}

The same power loss can be written with the dissipation factor

tanδ{displaystyle tandelta }


The internal generated heat has to be distributed to the ambient. The temperature of the capacitor, which is established on the balance between heat produced and distributed, shall not exceed the capacitors maximum specified temperature. Hence, the ESR or dissipation factor is a mark for the maximum power (AC load, ripple current, pulse load, etc.) a capacitor is specified for.

AC currents may be a:

  • ripple current—an effective (RMS) AC current, coming from an AC voltage superimposed of an DC bias, a
  • pulse current—an AC peak current, coming from an voltage peak, or an
  • AC current—an effective (RMS) sinusoidal current

Ripple and AC currents mainly warms the capacitor body. By this currents internal generated temperature influences the breakdown voltage of the dielectric. Higher temperature lower the voltage proof of all capacitors. In wet electrolytic capacitors higher temperatures force the evaporation of electrolytes, shortening the life time of the capacitors. In film capacitors higher temperatures may shrink the plastic film changing the capacitor’s properties.

Pulse currents, especially in metallized film capacitors, heat the contact areas between end spray (schoopage) and metallized electrodes. This may reduce the contact to the electrodes, heightening the dissipation factor.

For safe operation, the maximal temperature generated by any AC current flow through the capacitor is a limiting factor, which in turn limits AC load, ripple current, pulse load, etc.

Ripple current[edit]

A “ripple current” is the RMS value of a superimposed AC current of any frequency and any waveform of the current curve for continuous operation at a specified temperature. It arises mainly in power supplies (including switched-mode power supplies) after rectifying an AC voltage and flows as charge and discharge current through the decoupling or smoothing capacitor. The “rated ripple current” shall not exceed a temperature rise of 3, 5 or 10 °C, depending on the capacitor type, at the specified maximum ambient temperature.

Ripple current generates heat within the capacitor body due to the ESR of the capacitor. The ESR, composed out of the dielectric losses caused by the changing field strength in the dielectric and the losses resulting out of the slightly resistive supply lines or the electrolyte depends on frequency and temperature. Higher frequencies heighten the ESR and higher temperatures lower the ESR slightly.

The types of capacitors used for power applications have a specified rated value for maximum ripple current. These are primarily aluminum electrolytic capacitors, and tantalum as well as some film capacitors and Class 2 ceramic capacitors.

Aluminium electrolytic capacitors, the most common type for power supplies, experience shorter life expectancy at higher ripple currents. Exceeding the limit tends to result in explosive failure.

Tantalum electrolytic capacitors with solid manganese dioxide electrolyte are also limited by ripple current. Exceeding their ripple limits tends to shorts and burning components.

For film and ceramic capacitors, normally specified with a loss factor tan δ, the ripple current limit is determined by temperature rise in the body of approximately 10 °C. Exceeding this limit may destroy the internal structure and cause shorts.

Pulse current[edit]

The rated pulse load for a certain capacitor is limited by the rated voltage, the pulse repetition frequency, temperature range and pulse rise time. The “pulse rise time”

dv/dt{displaystyle dv/dt}

, represents the steepest voltage gradient of the pulse (rise or fall time) and is expressed in volts per μs (V/μs).

The rated pulse rise time is also indirectly the maximum capacity of an applicable peak current

Ip{displaystyle I_{p}}

. The peak current is defined as:


Ip{displaystyle I_{p}}

is in A;

C{displaystyle C}

in µF;

dv/dt{displaystyle dv/dt}

in V/µs

The permissible pulse current capacity of a metallized film capacitor generally allows an internal temperature rise of 8 to 10 °K.

In the case of metallized film capacitors, pulse load depends on the properties of the dielectric material, the thickness of the metallization and the capacitor’s construction, especially the construction of the contact areas between the end spray and metallized electrodes. High peak currents may lead to selective overheating of local contacts between end spray and metallized electrodes which may destroy some of the contacts, leading to increasing ESR.

For metallized film capacitors, so-called pulse tests simulate the pulse load that might occur during an application, according to a standard specification. IEC 60384 part 1, specifies that the test circuit is charged and discharged intermittently. The test voltage corresponds to the rated DC voltage and the test comprises 10000 pulses with a repetition frequency of 1 Hz. The pulse stress capacity is the pulse rise time. The rated pulse rise time is specified as 1/10 of the test pulse rise time.

The pulse load must be calculated for each application. A general rule for calculating the power handling of film capacitors is not available because of vendor-related internal construction details. To prevent the capacitor from overheating the following operating parameters have to be considered:

  • peak current per µF
  • Pulse rise or fall time dv/dt in V/µs
  • relative duration of charge and discharge periods (pulse shape)
  • maximum pulse voltage (peak voltage)
  • peak reverse voltage;
  • Repetition frequency of the pulse
  • Ambient temperature
  • Heat dissipation (cooling)

Higher pulse rise times are permitted for pulse voltage lower than the rated voltage.

Examples for calculations of individual pulse loads are given by many manufactures, e.g. WIMA[40] and Kemet.[41]

AC current[edit]

Limiting conditions for capacitors operating with AC loads

An AC load only can be applied to a non-polarized capacitor. Capacitors for AC applications are primarily film capacitors, metallized paper capacitors, ceramic capacitors and bipolar electrolytic capacitors.

The rated AC load for an AC capacitor is the maximum sinusoidal effective AC current (rms) which may be applied continuously to a capacitor within the specified temperature range. In the datasheets the AC load may be expressed as

  • rated AC voltage at low frequencies,
  • rated reactive power at intermediate frequencies,
  • reduced AC voltage or rated AC current at high frequencies.

Typical rms AC voltage curves as a function of frequency, for 4 different capacitance values of a 63 V DC film capacitor series

The rated AC voltage for film capacitors is generally calculated so that an internal temperature rise of 8 to 10 °K is the allowed limit for safe operation. Because dielectric losses increase with increasing frequency, the specified AC voltage has to be derated at higher frequencies. Datasheets for film capacitors specify special curves for derating AC voltages at higher frequencies.

If film capacitors or ceramic capacitors only have a DC specification, the peak value of the AC voltage applied has to be lower than the specified DC voltage.

AC loads can occur in AC Motor run capacitors, for voltage doubling, in snubbers, lighting ballast and for power factor correction PFC for phase shifting to improve transmission network stability and efficiency, which is one of the most important applications for large power capacitors. These mostly large PP film or metallized paper capacitors are limited by the rated reactive power VAr.

Bipolar electrolytic capacitors, to which an AC voltage may be applicable, are specified with a rated ripple current.

Insulation resistance and self-discharge constant[edit]

The resistance of the dielectric is finite, leading to some level of DC “leakage current” that causes a charged capacitor to lose charge over time. For ceramic and film capacitors, this resistance is called “insulation resistance Rins“. This resistance is represented by the resistor Rins in parallel with the capacitor in the series-equivalent circuit of capacitors.
Insulation resistance must not be confused with the outer isolation of the component with respect to the environment.

The time curve of self-discharge over insulation resistance with decreasing capacitor voltage follows the formula

With stored DC voltage

U0{displaystyle U_{0}}

 and self-discharge constant

Thus, after

τs{displaystyle tau _{mathrm {s} },}


U0{displaystyle U_{0}}

 drops to 37% of the initial value.

The self-discharge constant is an important parameter for the insulation of the dielectric between the electrodes of ceramic and film capacitors. For example, a capacitor can be used as the time-determining component for time relays or for storing a voltage value as in a sample and hold circuits or operational amplifiers.

Class 1 ceramic capacitors have an insulation resistance of at least 10 GΩ, while class 2 capacitors have at least 4 GΩ or a self-discharge constant of at least 100 s. Plastic film capacitors typically have an insulation resistance of 6 to 12 GΩ. This corresponds to capacitors in the uF range of a self-discharge constant of about 2000–4000 s.[42]

Insulation resistance respectively the self-discharge constant can be reduced if humidity penetrates into the winding. It is partially strongly temperature dependent and decreases with increasing temperature. Both decrease with increasing temperature.

In electrolytic capacitors, the insulation resistance is defined as leakage current.

Leakage current[edit]

The general leakage current behavior of electrolytic capacitors depend on the kind of electrolyte

For electrolytic capacitors the insulation resistance of the dielectric is termed “leakage current”. This DC current is represented by the resistor Rleak in parallel with the capacitor in the series-equivalent circuit of electrolytic capacitors. This resistance between the terminals of a capacitor is also finite. Rleak is lower for electrolytics than for ceramic or film capacitors.

The leakage current includes all weak imperfections of the dielectric caused by unwanted chemical processes and mechanical damage. It is also the DC current that can pass through the dielectric after applying a voltage. It depends on the interval without voltage applied (storage time), the thermic stress from soldering, on voltage applied, on temperature of the capacitor, and on measuring time.

The leakage current drops in the first minutes after applying DC voltage. In this period the dielectric oxide layer can self-repair weaknesses by building up new layers. The time required depends generally on the electrolyte. Solid electrolytes drop faster than non-solid electrolytes but remain at a slightly higher level.

The leakage current in non-solid electrolytic capacitors as well as in manganese oxide solid tantalum capacitors decreases with voltage-connected time due to self-healing effects. Although electrolytics leakage current is higher than current flow over insulation resistance in ceramic or film capacitors, the self-discharge of modern non solid electrolytic capacitors takes several weeks.

A particular problem with electrolytic capacitors is storage time. Higher leakage current can be the result of longer storage times. These behaviors are limited to electrolytes with a high percentage of water. Organic solvents such as GBL do not have high leakage with longer storage times.

Leakage current is normally measured 2 or 5 minutes after applying rated voltage.


All ferroelectric materials exhibit piezoelectricity a piezoelectric effect. Because Class 2 ceramic capacitors use ferroelectric ceramics dielectric, these types of capacitors may have electrical effects called microphonics. Microphonics (microphony) describes how electronic components transform mechanical vibrations into an undesired electrical signal (noise).[43] The dielectric may absorb mechanical forces from shock or vibration by changing thickness and changing the electrode separation, affecting the capacitance, which in turn induces an AC current. The resulting interference is especially problematic in audio applications, potentially causing feedback or unintended recording.

In the reverse microphonic effect, varying the electric field between the capacitor plates exerts a physical force, turning them into an audio speaker. High current impulse loads or high ripple currents can generate audible sound from the capacitor itself, draining energy and stressing the dielectric.[44]

Dielectric absorption (soakage)[edit]

Main page: Dielectric absorption

Dielectric absorption occurs when a capacitor that has remained charged for a long time discharges only incompletely when briefly discharged. Although an ideal capacitor would reach zero volts after discharge, real capacitors develop a small voltage from time-delayed dipole discharging, a phenomenon that is also called dielectric relaxation, “soakage” or “battery action”.

Values of dielectric absorption for some often used capacitors
Type of capacitor Dielectric Absorption
Air and vacuum capacitors Not measurable
Class-1 ceramic capacitors, NP0 0.6%
Class-2 ceramic capacitors, X7R 2.5%
Polypropylene film capacitors (PP) 0.05 to 0.1%
Polyester film capacitors (PET) 0.2 to 0.5%
Polyphenylene sulfide film capacitors (PPS) 0.05 to 0.1%
Polyethylene naphthalate film capacitors (PEN) 1.0 to 1.2%
Tantalum electrolytic capacitors with solid electrolyte 2 to 3%,[45] 10%[46]
Aluminium electrolytic capacitor with non solid electrolyte 10 to 15%
Double-layer capacitor or super capacitors data not available

In many applications of capacitors dielectric absorption is not a problem but in some applications, such as long-time-constant integrators, sample-and-hold circuits, switched-capacitor analog-to-digital converters, and very low-distortion filters, it is important that the capacitor does not recover a residual charge after full discharge, and capacitors with low absorption are specified.[47]
The voltage at the terminals generated by the dielectric absorption may in some cases possibly cause problems in the function of an electronic circuit or can be a safety risk to personnel. In order to prevent shocks most very large capacitors are shipped with shorting wires that need to be removed before they are used.[48]

Energy density[edit]

The capacitance value depends on the dielectric material (ε), the surface of the electrodes (A) and the distance (d) separating the electrodes and is given by the formula of a plate capacitor:

The separation of the electrodes and the voltage proof of the dielectric material defines the breakdown voltage of the capacitor. The breakdown voltage is proportional to the thickness of the dielectric.

Theoretically, given two capacitors with the same mechanical dimensions and dielectric, but one of them have half the thickness of the dielectric. With the same dimensions this one could place twice the parallel-plate area inside. This capacitor has theoretically 4 times the capacitance as the first capacitor but half of the voltage proof.

Since the energy density stored in a capacitor is given by:

thus a capacitor having a dielectric half as thick as another has 4 times higher capacitance but ½ voltage proof, yielding an equal maximum energy density.

Therefore, dielectric thickness does not affect energy density within a capacitor of fixed overall dimensions. Using a few thick layers of dielectric can support a high voltage, but low capacitance, while thin layers of dielectric produce a low breakdown voltage, but a higher capacitance.

This assumes that neither the electrode surfaces nor the permittivity of the dielectric change with the voltage proof. A simple comparison with two existing capacitor series can show whether reality matches theory. The comparison is easy, because the manufacturers use standardized case sizes or boxes for different capacitance/voltage values within a series.

Comparison of energy stored in capacitors with the same dimensions but with different rated voltages and capacitance values
Electrolytic capacitors
NCC, KME series
Ǿ D × H = 16.5 mm × 25 mm[49]
Metallized PP film capacitors
KEMET; PHE 450 series
W × H × L = 10.5 mm × 20.5 mm × 31.5 mm[50]
Capacitance/Voltage Stored Energy Capacitance/Voltage Stored Energy
4700 µF/10 V 235 mWs 1.2 µF/250 V 37.5 mWs
2200 µF/25 V 688 mWs 0.68 µF/400 V 54.4 mWs
220 µF/100 V 1100 mWs 0.39 µF/630 V 77.4 mWs
22 µF/400 V 1760 mWs 0.27 µF/1000 V 135 mWs

In reality modern capacitor series do not fit the theory. For electrolytic capacitors the sponge-like rough surface of the anode foil gets smoother with higher voltages, decreasing the surface area of the anode. But because the energy increases squared with the voltage, and the surface of the anode decreases lesser than the voltage proof, the energy density increases clearly. For film capacitors the permittivity changes with dielectric thickness and other mechanical parameters so that the deviation from the theory has other reasons.[51]

Comparing the capacitors from the table with a supercapacitor, the highest energy density capacitor family. For this, the capacitor 25  F/2.3 V in dimensions D × H = 16 mm × 26 mm from Maxwell HC Series, compared with the electrolytic capacitor of approximately equal size in the table. This supercapacitor has roughly 5000 times higher capacitance than the 4700/10 electrolytic capacitor but ¼ of the voltage and has about 66,000 mWs (0.018 Wh) stored electrical energy,[52] approximately 100 times higher energy density (40 to 280 times) than the electrolytic capacitor.

Long time behavior, aging[edit]

Electrical parameters of capacitors may change over time during storage and application. The reasons for parameter changings are different, it may be a property of the dielectric, environmental influences, chemical processes or drying-out effects for non-solid materials.


Aging of different Class 2 ceramic capacitors compared with NP0-Class 1 ceramic capacitor

In ferroelectric Class 2 ceramic capacitors, capacitance decreases over time. This behavior is called “aging”. This aging occurs in ferroelectric dielectrics, where domains of polarization in the dielectric contribute to the total polarization. Degradation of polarized domains in the dielectric decreases permittivity and therefore capacitance over time.[53][54] The aging follows a logarithmic law. This defines the decrease of capacitance as constant percentage for a time decade after the soldering recovery time at a defined temperature, for example, in the period from 1 to 10 hours at 20 °C. As the law is logarithmic, the percentage loss of capacitance will twice between 1 h and 100 h and 3 times between 1 h and 1,000 h and so on. Aging is fastest near the beginning, and the absolute capacitance value stabilizes over time.

The rate of aging of Class 2 ceramic capacitors depends mainly on its materials. Generally, the higher the temperature dependence of the ceramic, the higher the aging percentage. The typical aging of X7R ceramic capacitors is about 2.5&nbs;% per decade.[55] The aging rate of Z5U ceramic capacitors is significantly higher and can be up to 7% per decade.

The aging process of Class 2 ceramic capacitors may be reversed by heating the component above the Curie point.

Class 1 ceramic capacitors and film capacitors do not have ferroelectric-related aging. Environmental influences such as higher temperature, high humidity and mechanical stress can, over a longer period, lead to a small irreversible change in the capacitance value sometimes called aging, too.

The change of capacitance for P 100 and N 470 Class 1 ceramic capacitors is lower than 1%, for capacitors with N 750 to N 1500 ceramics it is ≤ 2%. Film capacitors may lose capacitance due to self-healing processes or gain it due to humidity influences. Typical changes over 2 years at 40 °C are, for example, ±3 % for PE film capacitors and ±1 % PP film capacitors.

Life time[edit]

The electrical values of electrolytic capacitors with non-solid electrolyte changes over the time due to evaporation of electrolyte. Reaching specified limits of the parameters the capacitors will be count as “wear out failure”.

Electrolytic capacitors with non-solid electrolyte age as the electrolyte evaporates. This evaporation depends on temperature and the current load the capacitors experience. Electrolyte escape influences capacitance and ESR. Capacitance decreases and the ESR increases over time. In contrast to ceramic, film and electrolytic capacitors with solid electrolytes, “wet” electrolytic capacitors reach a specified “end of life” reaching a specified maximum change of capacitance or ESR. End of life, “load life” or “lifetime” can be estimated either by formula or diagrams[56] or roughly by a so-called “10-degree-law”. A typical specification for an electrolytic capacitor states a lifetime of 2,000 hours at 85 °C, doubling for every 10 degrees lower temperature, achieving lifespan of approximately 15 years at room temperature.

Supercapacitors also experience electrolyte evaporation over time. Estimation is similar to wet electrolytic capacitors. Additional to temperature the voltage and current load influence the life time. Lower voltage than rated voltage and lower current loads as well as lower temperature extend the life time.

Failure rate[edit]

The life time (load life) of capacitors correspondents with the time of constant random failure rate shown in the bathtub curve. For electrolytic capacitors with non-solid electrolyte and supercapacitors ends this time with the beginning of wear out failures due to evaporation of electrolyte

Capacitors are reliable components with low failure rates, achieving life expectancies of decades under normal conditions. Most capacitors pass a test at the end of production similar to a “burn in”, so that early failures are found during production, reducing the number of post-shipment failures.

Reliability for capacitors is usually specified in numbers of Failures In Time (FIT) during the period of constant random failures. FIT is the number of failures that can be expected in one billion (109) component-hours of operation at fixed working conditions (e.g. 1000 devices for 1 million hours, or 1 million devices for 1000 hours each, at 40 °C and 0.5 UR). For other conditions of applied voltage, current load, temperature, mechanical influences and humidity the FIT can recalculated with terms standardized for industrial[57] or military[58] contexts.

Additional information[edit]


Capacitors may experience changes to electrical parameters due to environmental influences like soldering, mechanical stress factors (vibration, shock) and humidity. The greatest stress factor is soldering. The heat of the solder bath, especially for SMD capacitors, can cause ceramic capacitors to change contact resistance between terminals and electrodes; in film capacitors, the film may shrink, and in wet electrolytic capacitors the electrolyte may boil. A recovery period enables characteristics to stabilize after soldering; some types may require up to 24 hours. Some properties may change irreversibly by a few per cent from soldering.

Electrolytic behavior from storage or disuse[edit]

Electrolytic capacitors with non-solid electrolyte are “aged” during manufacturing by applying rated voltage at high temperature for a sufficient time to repair all cracks and weaknesses that may have occurred during production. Some electrolytes with a high water content react quite aggressively or even violently with unprotected aluminum. This leads to a “storage” or “disuse” problem of electrolytic capacitors manufactured before the 1980s. Chemical processes weaken the oxide layer when these capacitors are not used for too long. New electrolytes with “inhibitors” or “passivators” were developed during the 1980s to solve this problem.[59][60]
As of 2012 the standard storage time for electronic components of two years at room temperature substantiates (cased) by the oxidation of the terminals will be specified for electrolytic capacitors with non-solid electrolytes, too. Special series for 125 °C with organic solvents like GBL are specified up to 10 years storage time ensure without pre-condition the proper electrical behavior of the capacitors.[61]

For antique radio equipment, “pre-conditioning” of older electrolytic capacitors may be recommended. This involves applying the operating voltage for some 10 minutes over a current limiting resistor to the terminals of the capacitor. Applying a voltage through a safety resistor repairs the oxide layers.

IEC/EN standards[edit]

The tests and requirements to be met by capacitors for use in electronic equipment for approval as standardized types are set out in the generic specification IEC/EN 60384-1 in the following sections.[62]

Ceramic capacitors

  • IEC/EN 60384-8—Fixed capacitors of ceramic dielectric, Class 1
  • IEC/EN 60384-9—Fixed capacitors of ceramic dielectric, Class 2
  • IEC/EN 60384-21—Fixed surface mount multilayer capacitors of ceramic dielectric, Class 1
  • IEC/EN 60384-22—Fixed surface mount multilayer capacitors of ceramic dielectric, Class 2

Film capacitors

  • IEC/EN 60384-2—Fixed metallized polyethylene-terephthalate film dielectric d.c. capacitors
  • IEC/EN 60384-11—Fixed polyethylene-terephthalate film dielectric metal foil d.c. capacitors
  • IEC/EN 60384-13—Fixed polypropylene film dielectric metal foil d.c. capacitors
  • IEC/EN 60384-16—Fixed metallized polypropylene film dielectric d.c. capacitors
  • IEC/EN 60384-17—Fixed metallized polypropylene film dielectric a.c. and pulse
  • IEC/EN 60384-19—Fixed metallized polyethylene-terephthalate film dielectric surface mount d.c. capacitors
  • IEC/EN 60384-20—Fixed metalized polyphenylene sulfide film dielectric surface mount d.c. capacitors
  • IEC/EN 60384-23—Fixed metallized polyethylene naphthalate film dielectric chip d.c. capacitors

Electrolytic capacitors

  • IEC/EN 60384-3—Surface mount fixed tantalum electrolytic capacitors with manganese dioxide solid electrolyte
  • IEC/EN 60384-4—Aluminium electrolytic capacitors with solid (MnO2) and non-solid electrolyte
  • IEC/EN 60384-15—fixed tantalum capacitors with non-solid and solid electrolyte
  • IEC/EN 60384-18—Fixed aluminium electrolytic surface mount capacitors with solid (MnO2) and non-solid electrolyte
  • IEC/EN 60384-24—Surface mount fixed tantalum electrolytic capacitors with conductive polymer solid electrolyte
  • IEC/EN 60384-25—Surface mount fixed aluminium electrolytic capacitors with conductive polymer solid electrolyte


  • IEC/EN 62391-1—Fixed electric double-layer capacitors for use in electric and electronic equipment – Part 1: Generic specification
  • IEC/EN 62391-2—Fixed electric double-layer capacitors for use in electronic equipment – Part 2: Sectional specification – Electric double-layer capacitors for power application

Capacitor symbols[edit]



Capacitors, like most other electronic components and if enough space is available, have imprinted markings to indicate manufacturer, type, electrical and thermal characteristics, and date of manufacture. If they are large enough the capacitor is marked with:

  • manufacturer’s name or trademark;
  • manufacturer’s type designation;
  • polarity of the terminations (for polarized capacitors)
  • rated capacitance;
  • tolerance on rated capacitance
  • rated voltage and nature of supply (AC or DC)
  • climatic category or rated temperature;
  • year and month (or week) of manufacture;
  • certification marks of safety standards (for safety EMI/RFI suppression capacitors)

Polarized capacitors have polarity markings, usually “-” (minus) sign on the side of the negative electrode for electrolytic capacitors or a stripe or “+” (plus) sign, see #Polarity marking. Also, the negative lead for leaded “wet” e-caps is usually shorter.

Smaller capacitors use a shorthand notation. The most commonly used format is: XYZ J/K/M VOLTS V, where XYZ represents the capacitance (calculated as XY × 10Z pF), the letters J, K or M indicate the tolerance (±5%, ±10% and ±20% respectively) and VOLTS V represents the working voltage.


  • 105K 330V implies a capacitance of 10 × 105 pF = 1 µF (K = ±10%) with a working voltage of 330 V.
  • 473M 100V implies a capacitance of 47 × 103 pF = 47 nF (M = ±20%) with a working voltage of 100 V.

Capacitance, tolerance and date of manufacture can be indicated with a short code specified in IEC/EN 60062. Examples of short-marking of the rated capacitance (microfarads): µ47 = 0,47 µF, 4µ7 = 4,7 µF, 47µ = 47 µF

The date of manufacture is often printed in accordance with international standards.

  • Version 1: coding with year/week numeral code, “1208” is “2012, week number 8”.
  • Version 2: coding with year code/month code. The year codes are: “R” = 2003, “S”= 2004, “T” = 2005, “U” = 2006, “V” = 2007, “W” = 2008, “X” = 2009, “A” = 2010, “B” = 2011, “C” = 2012, “D” = 2013, etc. Month codes are: “1” to “9” = Jan. to Sept., “O” = October, “N” = November, “D” = December. “X5” is then “2009, May”

For very small capacitors like MLCC chips no marking is possible. Here only the traceability of the manufacturers can ensure the identification of a type.

Colour coding[edit]

Main page: Electronic color code

As of 2013 Capacitors do not use color coding.

Polarity marking[edit]

Aluminum e-caps with non-solid electrolyte have a polarity marking at the cathode (minus) side. Aluminum, tantalum, and niobium e-caps with solid electrolyte have a polarity marking at the anode (plus) side. Supercapacitor are marked at the minus side.

  1. ab J. Ho, T. R. Jow, S. Boggs, Historical Introduction to Capacitor Technology, PDF [1]
  2. abc Adam Marcus Namisnyk (23 June 2003). “A Survey of Electrochemical Supercapacitor Technology”. Retrieved 2011-06-24. 
  3. WIMA, Characteristics of Metallized Film Capacitors in Comparison with Other Dielectrics [2]
  4. Film Capacitors, TDK Epcos, General technical information
  5. AVX, Dielectric Comparison Chart
  6. Holystone, Capacitor Dielectric Comparison, Technical Note 3
  7. Power Film Capacitors for Industrial Applications, P. Bettacchi, D. Montanari, D. Zanarini, D. Orioli, G. Rondelli, A. Sanua, KEMET Electronics [3]
  8. ab Template:Literatur
  9. General technical information of (RFI/EMI)Noise suppression capacitors on AC mains [4]
  10. Vishay, Capacitors – RFI Class X/Y
  11. X2Y® Technology
  12. Murata, Three-terminal Capacitor Structure, No.TE04EA-1.pdf 98.3.20
  13. Vishay, Ceramic RF-Power Capacitors
  14. Vishay. “Capacitors – RF Power”. Vishay. Retrieved 2013-03-09. 
  15. Passive component magazine, Nov./Dec. 2005, F. Jacobs, Polypropylene Capacitor Film Resin, p. 29 ff [5]
  16. Paumanok Publications, PCInewsletterOct2007cmp Paumanok Publications, Inc.
  17. WIMA, RFI Capacitors
  18. WIMA Snubber Capacitors
  19. Amrad Engeneering Inc., Motor run capacitors
  20. Epcos, Capacitors for power electronics, General technical information
  21. Sanyo, Capacitor lecture POSCAP (Ta) (Basic), Polymerized electrolyte
  22. CDE, Motor Start Capacitors
  23. Rubycon, Aluminum Electrolytic Capacitors for Strobe Flash
  24. Fischer & Tausche, Electrolytic capacitor for audio frequency
  25. Vishay, Wet Electrolyte Tantalum Capacitors, Introduction
  26. Self-healing Characteristics of Solid Electrolytic Capacitor with Polypyrrole Electrolyte, Yamamoto Hideo [6]
  27. abc B. E. Conway (1999). Electrochemical Supercapacitors: Scientific Fundamentals and Technological Applications. Berlin: Springer. ISBN 0306457369. Retrieved 2013, Mai 02.  see also Brian E. Conway in Electrochemistry Encyclopedia: Electrochemical Capacitors — Their Nature, Function and Applications
  28. Template:Cite techreport
  29. Elzbieta Frackowiak, Francois Beguin, PERGAMON, Carbon 39 (2001) 937–950, Carbon materials for the electrochemical storage of energy in Capacitors
  30. Yu.M. Volfkovich, A.A. Mikhailin, D.A. Bograchev, V.E. Sosenkin and V.S. Bagotsky, Studies of Supercapacitor Carbon Electrodes with High Pseudocapacitance, A. N. Frumkin Institute of Physical Chemistry and Electrochemistry, Russian Academy of Sciences, Moscow, Russia, Dr. Ujjal Kumar Sur (Ed.), ISBN 978-953-307-830-4
  31. Elton
  32. IPDiA, 3D Silicon Capacitors
  33. Tettex instruments, SF6 Gas insulated Standard Capacitors
  34. AVX, Performance Characteristics of Multilayer Glass Capacitors
  35. highbeam business, Electronic Capacitors SIC 3675, Industry report
  36. Murata: Basics of capacitors, lesson 2 Includes graph showing impedance as a function of frequency for different capacitor types; electrolytics are the only ones with a large component due to ESR
  37. Siliziumkondensator, Vishay, HPC0603A
  38. Simic Electronics, Chip Mica Capacitors
  39. AVX, NP0, 1000 pF 100 V, 0805, Q >= 1000 (1 MHz), [7]
  40. WIMA, Selection of Capacitors for Pulse Applications
  41. Kemet, General information DC Film Capacitors
  42. Wima,Insulation Resistance
  43. [8], Capacitors for reduced sound emissions.
  44. Kemet, Are your military ceramic capacitors subject to the piezoelectric effect?
  45. Kemet, Polymer Tantalum Chip Capacitors
  47. “Understand Capacitor Soakage to Optimize Analog Systems” by Bob Pease 1982 [10]
  48. * “Modeling Dielectric Absorption in Capacitors”, by Ken Kundert
  49. NCC, KME series
  50. KEMET, series PHE450
  51. Metallized Polypropylene Film Energy Storage Capacitors For Low Pulse Duty, Ralph M. Kerrigan, NWL Capacitor Division [11]
  52. Maxwell HC Series / docs/datasheet_hc_series_1013793.pdf
  53. Template:Literatur
  54. Takaaki Tsurumi & Motohiro Shono & Hirofumi Kakemoto & Satoshi Wada & Kenji Saito & Hirokazu Chazono, Mechanism of capacitance aging under DC-bias field in X7R-MLCCs
    Published online: 23 March 2007, # Springer Science + Business Media, LLC 2007
  55. Christopher England, Johanson dielectrics, Ceramic Capacitor Aging Made Simple [13]
  56. Electrolytic Capacitor Lifetime Estimation, Dr. Arne Albertsen, Jianghai Europe, [14]
  57. IEC/EN 61709, Electric components. Reliability. Reference conditions for failure rates and stress models for conversion
  58. MIL-HDBK-217F Reliability Prediction of Electronic Equipment
  59. J. L. Stevens, T. R. Marshall, A. C. Geiculescu M., C. R. Feger, T. F. Strange, Carts USA 2006, The Effects of Electrolyte Composition on the Deformation Characteristics of Wet Aluminum ICD Capacitors, [15]
  60. Alfonso Berduque, Zongli Dou, Rong Xu, BHC Components Ltd (KEMET), Electrochemical Studies for Aluminium Electrolytic Capacitor Applications: Corrosion Analysis of Aluminium in Ethylene Glycol-Based Electrolytes pdf
  61. Vishay BCcomponents, Introduction Aluminum Capacitors, paragraph “Storage”, Revision: 10-May-12, Document Number: 28356, pdf
  62. IEC/EN/DIN Standards, Beuth-Verlag

Electronics |
Foreword |
Basic Electronics |
Complex Electronics | Electricity |
Machines |
History of Electronics |
Appendix |


An inductor is a passive electronic component dependent on frequency used to store electric energy in the form of a magnetic field. An inductor has the symbol

Inductor diagram.svg


Inductance is the characteristic of the Inductor to generate a magnetic field for a given current. Inductance has a letter symbol L and measured in units of Henry (H).

This section list formulas for inductances in specific situations. Beware that some of the equations are in Imperial units.

The permeability of free space, μ0, is constant and is defined to be exactly equal to 4π×10-7 H m-1.

Basic inductance formula for a cylindrical coil[edit]

The self-inductance of a straight, round wire in free space[edit]

Lself = self inductance / H(?)
b = wire length /m
a = wire radius /m

If you make the assumption that b >> a and that the wire is nonmagnetic (

μr=1{displaystyle mu _{r}=1}

), then this equation can be approximated to

The inductance of a straight wire is usually so small that it is neglected in most practical problems. If the problem deals with very high frequencies (f > 20 GHz), the calculation may become necessary. For the rest of this book, we will assume that this self-inductance is negligible.

Inductance of a short air core cylindrical coil in terms of geometric parameters:[edit]

Multilayer air core coil[edit]

Flat spiral air core coil[edit]

Hence a spiral coil with 8 turns at a mean radius of 25 mm and a depth of 10 mm would have an inductance of 5.13µH.

Winding around a toroidal core (circular cross-section)[edit]

L = inductance / H
μr = relative permeability of core material
N = number of turns
r = radius of coil winding / m
D = overall diameter of toroid / m

Quality of good inductor[edit]

There are several important properties for an inductor that may need to be considered when choosing one for use in an electronic circuit. The following are the basic properties of a coil inductor. Other factors may be important for other kinds of inductor, but these are outside the scope of this article.

Current carrying capacity is determined by wire thickness and resistivity.
The quality factor, or Q-factor, describes the energy loss in an inductor due to imperfection in the manufacturing.
The inductance of the coil is probably most important, as it is what makes the inductor useful. The inductance is the response of the inductor to a changing current.

The inductance is determined by several factors.

Coil shape: short and squat is best
Core material
The number of turns in the coil. These must be in the same direction, or they will cancel out, and you will have a resistor.
Coil diameter. The larger the diameter (core area) the larger the induction.

Coil’s Characteristics[edit]

For a Coil that has the following dimension

Basic Inductor with B-field.svg
Area enclosed by each turn of the coil is A
Length of the coil is ‘l’
Number of turns in the coil is N
Permeability of the core is μ. μ is given by the permeability of free space, μ0 multiplied by a factor, the relative permeability, μr
The current in the coil is ‘i’

The magnetic flux density, B, inside the coil is given by:

We know that the flux linkage in the coil, λ, is given by;


The flux linkage in an inductor is therefore proportional to the current, assuming that A, N, l and μ all stay constant. The constant of proportionality is given the name inductance (measured in Henries) and the symbol L:

Taking the derivative with respect to time, we get:

Since L is time-invariant in nearly all cases, we can write:

Now, Faraday’s Law of Induction states that:

We call

E{displaystyle -{mathcal {E}}}

the electromotive force (emf) of the coil, and this is opposite to the voltage v across the inductor, giving:

This means that the voltage across an inductor is equal to the rate of change of the current in the inductor multiplied by a factor, the inductance. note that for a constant current, the voltage is zero, and for an instantaneous change in current, the voltage is infinite (or rather, undefined). This applies only to ideal inductors which do not exist in the real world.

This equation implies that

  • The voltage across an inductor is proportional to the derivative of the current through the inductor.
  • In inductors, voltage leads current.
  • Inductors have a high resistance to high frequencies, and a low resistance to low frequencies. This property allows their use in filtering signals.

An inductor works by opposing current change. Whenever an electron is accelerated, some of the energy that goes into “pushing” that electron goes into the electron’s kinetic energy, but much of that energy is stored in the magnetic field.
Later when that or some other electron is decelerated (or accelerated the opposite direction), energy is pulled back out of the magnetic field.

Inductor and Direct Current Voltage (DC)[edit]

When a coil of several turns is connected to an electricity source in a closed loop, the current in the circuit induces a magnetic field that has the same properties as a Magnetic Field of a Magnet.

When the current is turned off, the Magnetic Field does not exist.

Conducting Coil is called ElectroMagnet

Inductor and Alternating Current Voltage (AC)[edit]

Inductor’s Voltage[edit]

Inductor’s Current[edit]



Angle Difference Between Voltage and Current[edit]

For Lossless Inductor

The angle difference between Voltage and Current is 90

For Lossy Inductor

Changing the value of L and RL will change the value of Angle of Difference, Angular Frequency, Frequency and Time.

Time Constant[edit]

Quality factor[edit]

Quality factor denoted as Q is defined as the ability to store energy to the sum total of all energy losses within the component

Inductor’s Connection[edit]

Series Connection[edit]

Inductors in Series.svg

Parallel Connection[edit]

Inductors in Parallel.svg

See Also[edit]

A electron moving through space creates a magnetic field that spins around the charge according to the right hand rule. The magnetic field is created by the spin of the moving electron. If the wire is bent in the shape of a ring, when its current is flowing it magnetic field will resemble water flowing through a hose. In order for the ring to have a magnetic field, its magnetic field must first displace the magnetic field that is already there. This is why inductors initially resist any changes in current when a voltage is applied. Over time the magnetic field changes to reflect the magnetic field of the ring and current starts flowing.

Inductors resist changes in current and take time to adjust.

A popular example of inductance is an electromagnet. It is essentially an inductor connected to dc with a piece of metal in its core. The flow of current creates a magnetic flow that mimicks a magnet. The direction of current determines the polarity of the magnet.

The nice thing about electromagnets is the strength of the current determines the strength of the magnetic field, so the more current the more magnetic field. Also reversing the direction of the current switches the polarity of the electromagnet.

This property allows electromagnets to be used as switches. As the current increases the magnet becomes more repulsive to other magnets.

Electromagnets are also used in loudspeakers. You have a voltage that is dependent on distance so as the distance decreases the voltage increases and as the distance increases the voltage decreases. The result is the ability to program the loudspeaker according to a vibration pattern.

Inductors in Series.svg

Consider n inductors in series, as above. The voltage across the whole arrangement (i.e. across the two terminals) must be equal to the sum of the voltages across the individual inductors:

from our definition of inductance, where the voltage is the inductance multiplied by the rate of change of current, we get

where i1 is the current in element 1, and so on. Since the current in every element the series must always be the same (by Kirchhoff’s Current Law), we can see that

where i is the current in the network. Factorising, we get:

If we now call all the element in the series a single, equivalent inductance, Leq, we see that


This means that when in series, the total inductance is just the sum of all the constituent inductances.


Inductors in Parallel.svg

When inductors are in parallel, then each inductor has the same voltage across it, that is, the voltage present at the terminals of the network. This can just be called v. Now, our equation describing the equivalent inductance, Leq, is:

where ieq is the current through the network.

By Kirchhoff’s Current Law, we have

Differentiating with respect to time gives

Now by rearranging the general equation describing inductance in the i’th element, we can obtain, for each term in the above,

Substituting into the equation before, we get


Rearranging, we get

So, therefore:

This is identical to the rule for combining resistors.

An inductor is the electrical equivalent of a flywheel. When you introduce energy to an inductor, the current flows slowly at first, just like a flywheel doesn’t instantly get up to speed. And if you try to stop a flywheel instantly, something will break. If you let current through an inductor, then open the switch, the energy of the inductor must go somewhere – it will arc back across the switch, quickly ruining it – thus the condensor used in coil-type automotive ignition systems: it stores the energy until the inefficiency of the flywheel can turn it into heat.

Inductors are formed of a coil of conductive material. Normally they are made of copper wire, but not always (Example: aluminum wire, or spiral pattern etched on circuit board). The material around and within the coil affects its properties; common types are air-core (only a coil of wire), iron-core, and ferrite core. Iron and ferrite types are more efficient because they conduct the magnetic field much better than air; of the two, ferrite is more efficient because stray electricity cannot flow through it. Ferrite is more expensive but operates at much higher frequencies than iron cores.

Some inductors have more than a core, which is just a rod the coil is formed about. Some are formed like transformers, using two E-shaped pieces facing each other, the wires wound about the central leg of the E’s. The E’s are made of laminated iron/steel or ferrite.

Toroidal inductors are most efficient of all, they are wound around a donut shape which is made of ferrite. They are more difficult to make, because the formed coil cannot be manufactured directly on the toroid – it must be wound onto it.

Important qualities of angf inductor

There are several important properties for an inductor.

  • Current carrying capacity is determined by wire thickness.
  • Q, or quality, is determined by the uniformity of the windings, as well as the core material and how thoroughly it surrounds the coil.
  • Last but not least, the inductance of the coil.

The inductance is determined by several factors.

  • coil shape: short and squat is best
  • core material
  • windings: winding in opposite directions will cancel out the inductance effect, and you will have only a resistor.

(someone add formulas etc. for determining inductance, please.)

In the real world, various factors contribute to non-idealities within inductors.

Nonzero Resistance[edit]

Nearly all common components have wire leads. Inductors specifically have this drawback in addition to the fact that they are typically made from a length of wire which is coiled around some form of material. This wire typically does not have zero resistance. While small lengths of wire made of typical conductive materials, such as copper, larger coils will have a relatively large amount of this wire, leading to an added resistance which may not be neglected. This also becomes true when the potential applied across the inductor increases.

To account for this added resistivity, a non-ideal inductor may be modeled as an ideal inductor in series with a resistor. This resistance may be measured under DC steady-state conditions.

High-frequency considerations[edit]

Although quite small, lead wires do have some amount of self-inductance. This will usually be neglectable except in the case of very small values for inductive components as well as for high frequency design. To account for the inductance added by these wires, one may model such a non-ideal inductor by including series inductors on for each of the two (or more) leading wires coming from the component.

Electronics |
Foreword |
Basic Electronics |
Complex Electronics | Electricity |
Machines |
History of Electronics |
Appendix |


Capacitors and inductors follow similar laws as resistors when it comes to simplification.

Simplifying Capacitor Configurations[edit]

Capacitors in Parallel[edit]

Capacitors in parallel are the same as increasing the total surface area of the capacitors to create a larger capacitor with more capacitance. In a capacitor network in parallel, all capacitors have the same voltage over them.

File:Electronics Capacitorsparallel.png

In a parallel configuration, the capacitance of the capacitors in parallel is the sum of the capacitance of all the capacitors.

Capacitors in Series[edit]

Capacitors in series are the same as increasing the distance between two capacitor plates. As well, it should be noted that placing two 100V capacitors in series results in the same as having one capacitor with the total maximum voltage of 200V. This, however, is not recommended to be done in practice. Especially with capacitors of different values. In a capacitor network in series, all capacitors can have the a different voltage over them.

File:Electronics Capacitorsseries.png

In a series configuration, the capacitance of all the capacitors combined is the sum of the reciprocals of the capacitance of all the capacitors.

Simplifying Inductor Configurations[edit]

An inductor works by opposing current change

Inductors in Parallel[edit]

Each inductor has a decreased amount of current flowing through it.
Take two inductors of the same strength that are in parallel. This divides the current so half the current is flowing through each inductor.

1Leq=1L1+1L2++1Ln{displaystyle {frac {1}{L_{eq}}}={frac {1}{L_{1}}}+{frac {1}{L_{2}}}+cdots +{frac {1}{L_{n}}}}

Inductors in Series[edit]

Inductors in series are just like resistors in series. Simply add them up.

Electronics |
Foreword |
Basic Electronics |
Complex Electronics | Electricity |
Machines |
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Appendix |

Ideal voltage sources[edit]

Voltage Source.svg

An ideal voltage source is a fundamental electronics component that creates a constant voltage between two points regardless of whatever else is connected to it. Since it is ideal, some circuit configurations are not allowed, such as short circuits, which would create infinite current. (I = V / 0)
A water analogy would be a pump with pressure sensors on both sides. The difference in pressure between the in port and out port is constantly measured, regardless of the absolute pressure of each side, and the pump speed is adjusted so that the pressure difference stays constant.
Real voltage sources, such as batteries, power supplies, piezoelectric disks, generators, steam turbines, wall outlets, etc. have an internal source impedance (in series with the ideal voltage source), which is very important to understand.

Ideal current sources[edit]

Current Source.svg

An ideal current source is an electronics component that creates a constant current through a section of circuit, regardless of whatever else is connected to it. Since it is ideal, some circuit configurations are not allowed, such as open circuits, which would create an infinite voltage.
A water analogy would be a pump with a flow meter. It measures the amount of water flowing by per unit time and changes the speed of the pump so that the current flow is constant.
Real current sources, such as batteries, power supplies, piezoelectric disks, generators, etc. have an internal source impedance (in parallel with the source), which is very important to understand.
Real sources generally behave more like voltage sources than current sources, because the internal impedance in series is very low. A current source can be created from a voltage source with a circuit such as a current mirror.

Dependent Sources[edit]

A dependent source is either a voltage or a current source which is dependent upon another value within the circuit, usually another voltage or current. Typically, these are used in circuit modeling and analysis.

There are four main types of such sources.

Voltage-controlled voltage source (VCVS)[edit]

This is a voltage source whose value is controlled by another voltage elsewhere in the circuit. Its output will typically be given as
An example of a VCVS may be an idealized amplifier, where A is the gain of the amplifier.

Current-controlled voltage source (CCVS)[edit]

This is a voltage source whose value is controlled by a current elsewhere in the circuit. Its output is typically given as

Voltage-controlled current source (VCCS)[edit]

This is a current source whose value is controlled by a voltage elsewhere in the circuit. Its output is typically given as

Current-controlled current source (CCCS)[edit]

This is a current source whose value is controlled by a current elsewhere in the circuit. Its output is typically given as
An example of a CCCS is an idealized bipolar junction transistor, which may be thought of as a small current controlling a larger one. Specifically the base current, Ib is the control and the collector current Ic is the output.


A switch is a mechanical device that connects or disconnects two parts of a circuit.

Closed Switch.svg

A switch is a short circuit when it is on.

Open Switch.svg
And it is a open circuit when it is off.

When you turn a switch on it completes a circuit that allows current to flow. When you turn the switch off it creates an air gap (depending on the type of switch), and since air is an insulator no current flows.
A switch is a device for making or breaking an electric circuit.
Usually the switch has two pieces of metal called contacts that touch to make a circuit, and separate to break the circuit. The contact material is chosen for its resistance to corrosion, because most metals form insulating oxides that would prevent the switch from working. Sometimes the contacts are plated with noble metals. They may be designed to wipe against each other to clean off any contamination. Nonmetallic conductors, such as conductive plastic, are sometimes used. The moving part that applies the operating force to the contacts is called the actuator, and may be a rocker, a toggle or dolly, a push-button or any type of mechanical linkage.

Contact Arrangements[edit]

Switches can be classified according to the arrangement of their contacts. Some contacts are normally open until closed by operation of the switch, while normally closed contacts are opened by the switch action. A switch with both types of contact is called a changeover switch.
The terms pole and throw are used to describe switch contacts. A pole is a set of contacts that belong to a single circuit. A throw is one of two or more positions that the switch can adopt. These terms give rise to the following abbreviations.
Electronics Switches.PNG
  • S (single), D (double).
  • T (throw), CO (changeover).
  • CO = DT.

(single|double) pole ((single|double) throw|changeover)

  • SPST = single pole single throw, a simple on-off switch.
  • SPDT = single pole double throw, a simple changeover or on-off-on switch.
  • SPCO = single pole changeover, equivalent to SPDT.
  • DPST = double pole single throw, equivalent to two SPST switches controlled by a single mechanism.
  • DPDT = double pole double throw, equivalent to two SPDT switches controlled by a single mechanism.
  • DPCO = double pole changeover, equivalent to DPDT.
Switches with larger numbers of poles or throws can be described by replacing the “S” or “D” with a number.

Biased Switches[edit]

A biased switch is one containing a spring that returns the actuator to a certain position. The “on-off” notation can be modified by placing parentheses around all positions other than the resting position. For example, an (on)-off-(on) switch can be switched on by moving the actuator in either direction away from the centre, but returns to the central off position when the actuator is released.
The momentary push-button switch is a type of biased switch. This device makes contact when the button is pressed and breaks when the button is released.

Special Types[edit]

Switches can be designed to respond to any type of mechanical stimulus: for example, vibration (the trembler switch), tilt, air pressure, fluid level (the float switch), the turning of a key (key switch), linear or rotary movement (the limit switch or microswitch).
The mercury tilt switch consists of a blob of mercury inside a glass bulb. The two contacts pass through the glass, and are shorted together when the bulb is tilted to make the mercury roll on to them. The advantage of this type of switch is that the liquid metal flows around particles of dirt and debris that might otherwise prevent the contacts of a conventional switch from closing.

Electronics |
Foreword |
Basic Electronics |
Complex Electronics | Electricity |
Machines |
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Appendix |

Ohm’s Law[edit]

Ohm’s law describes the relationship between voltage, current, and resistance.Voltage and current are proportional to the potential difference and inversely proportional to the resistance of the circuit

Voltage (V) is measured in volts (V); Current (I) in amperes (A); and resistance (R) in ohms (Ω).

Ohms law voltage source.svg

In this example, the current going through any point in the circuit, I, will be equal to the voltage V divided by the resistance R.

Ohms law current source.svg

In this example, the voltage across the resistor, V, will be equal to the supplied current, I, times the resistance R.

If two of the values (V, I, or R) are known, the other can be calculated using this formula.

Any more complicated circuit has an equivalent resistance that will allow us to calculate the current draw from the voltage source. Equivalent resistance is worked out using the fact that all resistors are either in parallel or series. Similarly, if the circuit only has a current source, the equivalent resistance can be used to calculate the voltage dropped across the current source.

Kirchoff’s Voltage Law[edit]

Kirchoff’s Voltage Law (KVL):

The sum of voltage drops around any loop in the circuit that starts and ends at the same place must be zero.

Voltage as a Physical Quantity[edit]

  1. Voltage is the potential difference between two charged objects.
  2. Potentials can be added or subtracted in series to make larger or smaller potentials as is commonly done in batteries.
  3. Positive charge flow from areas of high potential to lower potential.
  4. All the components of a circuit have resistance that acts as a potential drop.

Kirchoff’s Current Law[edit]

Kirchoff’s Current Law (KCL):

The sum of all current entering a node must equal the sum of all currents leaving the node.

KCL Example[edit]

Electronics KCL.PNG

I1 + I2 + I3 = 0 ↔ I1 = I2 + I3

Electronics KCL 1.PNG

I1I2I3I4 = 0 ↔ I2 + I3 + I4 = I1

Here is more about Kirchhoff’s laws, which can be integrated here

Consequences of KVL and KCL[edit]

Voltage Dividers[edit]

If two circuit elements are in series, there is a voltage drop across each element, but the current through both must be the same. The voltage at any point in the chain divides according to the resistances. A simple circuit with two (or more) resistors in series with a source is called a voltage divider.


Figure A: Voltage Divider circuit.

Consider the circuit in Figure A. According to KVL the voltage

Vin{displaystyle V_{in}}

is dropped across resistors

R1{displaystyle R_{1}}


R2{displaystyle R_{2}}

. If a current i flows through the two series resistors then by Ohm’s Law.



Similary if

VR1{displaystyle V_{R1}}

is the voltage across

R1{displaystyle R_{1}}


In general for n series resistors the voltage dropped across one of them say

Ri{displaystyle R_{i}}



Voltage Dividers as References[edit]

Clearly voltage dividers can be used as references. If you have a 9 volt battery and you want 4.5 volts, then connect two equal valued resistors in series and take the reference across the second and ground. There are clearly other concerns though, the first concern is current draw and the effect of the source impedance. Clearly connecting two 100 ohm resistors is a bad idea if the source impedance is, say, 50 ohms. Then the current draw would be 0.036 mA which is quite large if the battery is rated, say, 200 milliampere hours. The loading is more annoying with that source impedance too, the reference voltage with that source impedance is

9(100)250=3.6 V{displaystyle {frac {9(100)}{250}}=3.6{mbox{ V}}}

. So clearly, increasing the order of the resistor to at least 1 k

Ω{displaystyle Omega }

is the way to go to reduce the current draw and the effect of loading. The other problem with these voltage divider references is that the reference cannot be loaded if we put a 100 Ω resistor in parallel with a 10 kΩ resistor. When the voltage divider is made of two 10 kΩ resistors, then the resistance of the reference resistor becomes somewhere near 100 Ω. This clearly means a terrible reference. If a 10 MΩ resistor is used for the reference resistor will still be some where around 10 kΩ but still probably less. The effect of tolerances is also a problem; if the resistors are rated 5% then the resistance of 10 kΩ resistors can vary by ±500 Ω. This means more inaccuracy with this sort of reference.

Current Dividers[edit]

If two elements are in parallel, the voltage across them must be the same, but the current divides according to the resistances. A simple circuit with two (or more) resistors in parallel with a source is called a current divider.


Figure B: Parallel Resistors.

If a voltage V appears across the resistors in Figure B with only

R1{displaystyle R_{1}}


R2{displaystyle R_{2}}

for the moment then the current flowing in the circuit, before the division, i is according to Ohms Law.

Using the equivalent resistance for a parallel combination of resistors is

The current through

R1{displaystyle R_{1}}

according to Ohms Law is

Dividing equation (2) by (1)


In general with n Resistors the current

ix{displaystyle i_{x}}


Or possibly more simply


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A node is a section of a circuit which connects components to each other. All of the current entering a node must leave a node, according to Kirchoff’s Current Law. Every point on the node is at the same voltage, no matter how close it is to each component, because the connections between components are perfect conductors. This voltage is called the node voltage, and is the voltage difference between the node and an arbitrary reference, the ground point. The ground point is a node which is defined as having zero voltage. The ground node should be chosen carefully for convenience. Note that the ground node does not necessarily represent an actual connection to ground, it is just a device to make the analysis simpler. For example, if a node has a voltage of 5 Volts, then the voltage drop between that node and the ground node will be 5 Volts.

Note that in real circuits, nodes are made up of wires, which are not perfect conductors, and so the voltage is not perfectly the same everywhere on the node. This distinction is only important in demanding applications, such as low noise audio, high speed digital circuits (like modern computers), etc. If we look at how a particular circuit functions an engineer might be able to select check points that are diametrically opposite of each other, this signifies two points of current crossing over to another point this can be another method in testing a circuit to determine how nodes work.

Nodal Analysis[edit]

Nodal analysis is a formalized procedure based on KCL equations.


  1. Identify all nodes.
  2. Choose a reference node. Identify it with reference (ground) symbol. A good choice is the node with the most branches, or a node which can immediately give you another node voltage (e.g., below a voltage source).
  3. Assign voltage variables to the other nodes (these are node voltages.)
  4. Write a KCL equation for each node (sum the currents leaving the node and set equal to zero). Rearrange these equations into the form A*V1+B*V2=C (or similar for equations with more voltage variables.)
  5. Solve the system of equations from step 4. There are a number of techniques that can be used: simple substitution, Cramer’s rule, the adjoint matrix method, etc.

Complications in Nodal Analysis[edit]

  1. Dependent Current Source
    Solution: Write KVL equations for each node. Then express the extra variable (whatever the current source depends on) in terms of node voltages. Rearrange into the form from step 4 above. Solve as in step 5.
  2. Independent Voltage Source
    Problem: We know nothing about the current through the voltage source. We cannot write KCL equations for the nodes the voltage source is connected to.
    Solution: If the voltage source is between the reference node and any other node, we have been given a ‘free’ node voltage: the node voltage must be equal to the voltage source value! Otherwise, use a ‘super-node’, consisting of the source and the nodes it is connected to. Write a KCL equation for all current entering and leaving the super-node. Now we have one equation and two unknowns (the node voltages). Another equation that relates these voltages is the equation provided by the voltage source (V2-V1=source value). This new system of equations can be solved as in Step 5 above.
  3. Dependent Voltage Source
    Solution: Same as an independent voltage source, with an extra step. First write a super-node KCL equation. Then write the source controlling quantity (dependence quantity?) in terms of the node voltages. Rearrange the equation to be in the A*V1+B*V2=C form. Solve the system as above.


Given the Circuit below, find the voltages at all nodes.
Nodal example.png

node 0:

V0=0V{displaystyle V_{0}=0V,}

(defined as ground node)
node 1:

V1=9V{displaystyle V_{1}=9V,}

(free node voltage)
node 2:

V1V21k=V2V03k+V2V32k{displaystyle {frac {V_{1}-V_{2}}{1k}}={frac {V_{2}-V_{0}}{3k}}+{frac {V_{2}-V_{3}}{2k}}}

node 3:

V2V32k=V3V02k{displaystyle {frac {V_{2}-V_{3}}{2k}}={frac {V_{3}-V_{0}}{2k}}}

which results in the following system of linear equations:

{+11V23V3=54+1V22V3=0{displaystyle left{{begin{matrix}+11V_{2}&-3V_{3}&=&54\+1V_{2}&-2V_{3}&=&0end{matrix}}right.}

therefore, the solution is:

{V0=0.00VV1=9.00VV2=5.68VV3=2.84V{displaystyle left{{begin{matrix}V_{0}=0.00V\V_{1}=9.00V\V_{2}=5.68V\V_{3}=2.84Vend{matrix}}right.}

Another solution with KCL would be to solve node in terms of node 2;

V29V1k+V23k+V24k=0{displaystyle {frac {V_{2}-9V}{1k}}+{frac {V_{2}}{3k}}+{frac {V_{2}}{4k}}=0}

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A ‘mesh’ (also called a loop) is simply a path through a circuit that starts and ends at the same place. For the purpose of mesh analysis, a mesh is a loop that does not enclose other loops.

Mesh Analysis[edit]

Similar to nodal analysis, mesh analysis is a formalized procedure based on KVL equations. A caveat: mesh analysis can only be used on ‘planar’ circuits (i.e. there are no crossed, but unconnected, wires in the circuit diagram.)


  1. Draw circuit in planar form (if possible.)
  2. Identify meshes and name mesh currents. Mesh currents should be in the clockwise direction. The current in a branch shared by two meshes is the difference of the two mesh currents.
  3. Write a KVL equation in terms of mesh currents for each mesh.
  4. Solve the resulting system of equations.

Complication in Mesh Analysis[edit]

1. Dependent Voltage Sources

Solution: Same procedure, but write the dependency variable in terms of mesh currents.

2. Independent Current Sources

Solution: If current source is not on a shared branch, then we have been given one of the mesh currents! If it is on a shared branch, then use a ‘super-mesh’ that encircles the problem branch. To make up for the mesh equation you lose by doing this, use the mesh current relationship implied by the current source (i.e.

I2I1=4mA{displaystyle I_{2}-I_{1}=4mA}


3. Dependent Current Sources

Solution: Same procedure as for an independent current source, but with an extra step to eliminate the dependency variable. Write the dependency variable in terms of mesh currents.


Given the Circuit below, find the currents

I1{displaystyle I_{1}}


I2{displaystyle I_{2}}

The circuit has 2 loops indicated on the diagram. Using KVL we get:

0=91000I13000(I1I2){displaystyle 0=9-1000I_{1}-3000(I_{1}-I_{2})}


0=3000(I1I2)2000I22000I2{displaystyle 0=3000(I_{1}-I_{2})-2000I_{2}-2000I_{2}}

Simplifying we get the simultaneous equations:

0=94000I1+3000I2{displaystyle 0=9-4000I_{1}+3000I_{2}}

0=0+3000I17000I2{displaystyle 0=0+3000I_{1}-7000I_{2}}

solving to get:

I1=3.32mA{displaystyle I_{1}=3.32mA}

I2=1.42mA{displaystyle I_{2}=1.42mA}

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Source Transformation[edit]

Any linear time invariant network of impedances can be reduced to one equivalent impedance. In particular, any network of sources and resistors can be reduced to one ideal source and one resistor, in either the Thevenin or Norton configurations. In this way, a complicated network attached to a load resistor can be reduced to a single voltage divider (Thevenin) or current divider (Norton).

Thevenin norton equivalents.svg

Thevenin and Norton equivalents allow a voltage source in series with a resistor to be replaced by a current source in parallel with that exact same resistor (or vice versa.) This is called a source transformation.

The point to be noted is that the block that is replaced with such an equivalent should be linear and time invariant, i.e. a linear change in the electrical source in that block produces a linear change in the equivalent source, and the behavior can be replicated if the initial conditions are replicated.
The above shown transformation figures are true only if the circuit contains at least one independent voltage or current source. If the circuit comprises only dependent sources then Thevenin (and also Norton) equivalent consists of RTh alone

Thevenin Equivalents[edit]

The Thevenin equivalent circuit of a (two-terminal) network consists of a voltage source in series with a resistor. The Thevenin equivalent will have the same output voltage and current regardless of what is attached to the terminals.

Techniques For Finding Thevenin Equivalents[edit]

  • Network contains no sources (only resistors): The Thevenin resistance is equal to the equivalent resistance of the network. The Thevenin voltage is zero.
  • Basic: Works for any network except one with no independent sources. Find the voltage across the terminals (with positive reference at terminal A) when they are open-circuited. Find the current from terminal A to terminal B when they are short-circuited. Then

The Thevenin voltage source value is equivalent to the open-circuit voltage.

If the network has no dependent sources, the independent sources can be zeroed, and the Thevenin resistance is equal to the equivalent resistance of the network with zeroed sources. Then, find

Voc{displaystyle V_{oc}}


If the network has only dependent sources, either attach a test voltage source to the terminal points and measure the current that passes from the positive terminal, or attach a test current source to the terminal points and measure the voltage difference across the terminals. In both cases you will have values for

Voc{displaystyle V_{oc}}


Isc{displaystyle I_{sc}}

, allowing you to use the

Rth=VocIsc{displaystyle R_{th}={frac {V_{oc}}{I_{sc}}}}

relation to find the Thevenin resistance.

Norton Equivalents[edit]

Norton equivalents can be found by performing a source transformation on the Thevenin equivalent.
The Norton Equivalent of a Thevenin Equivalent consists of a current source,

IN=VthRth{displaystyle I_{N}={frac {V_{th}}{R_{th}}}}

in parallel with

Rth{displaystyle R_{th}}


Thevenin and Norton Equivalent[edit]

Figure 1: Circuit for the determination of Equivalents

The steps for creating the Equivalent are:

1. Remove the load circuit.
2. Calculate the voltage, V, at the output from the original sources.
3. Now replace voltage sources with shorts and current sources with open circuits.
4. Replace the load circuit with an imaginary ohm meter and measure the total resistance, R, looking back into the circuit, with the sources removed.
5. The equivalent circuit is a voltage source with voltage V in series with a resistance R in series with the load.

The Thevenin Equivalent is determined with

R2{displaystyle R_{2}}

as the load as shown in Figure 1. The first step is to open circuit

R2{displaystyle R_{2}}

Then the voltage v is calculated with

R2{displaystyle R_{2}}

open circuited must be calculated. The voltage across

R2{displaystyle R_{2}}


V1{displaystyle V_{1}}

this is because no current flows in the circuit so the voltage across

R2{displaystyle R_{2}}

must be

V1{displaystyle V_{1}}

by KVL.

Since this circuit does not contain any dependent sources, all that needs to be done is for all the Independent Voltage sources to be shorted and for all Independent Current Sources to be open circuited. This results in the circuit shown in Figure 2.

Figure 2: Circuit for the Equivalent Resistance

Now the Thevenin Resistance is calculated looking into the two nodes. The Thevenin resistance is clearly

R1+R3||R4{displaystyle R_{1}+R_{3}||R_{4}}

The Thevenin Equivalent is shown in Figure 3 and

Rth{displaystyle R_{th}}


Vth{displaystyle V_{th}}

have the values shown below.

Figure 3: Equivalent Thevenin Circuit

The Norton Equivalent is created by doing a source transformation using

IN=VthRth{displaystyle I_{N}={frac {V_{th}}{R_{th}}},}


Figure 4: Equivalent Norton Circuit


R2=R1=6kΩ{displaystyle R_{2}=R_{1}=6kOmega }


R3=R4=2kΩ{displaystyle R_{3}=R_{4}=2kOmega }


V1=15V{displaystyle V_{1}=15V}


As a final note if the voltage across

R2{displaystyle R_{2}}

is calculate by Voltage Divider Rule using the Thevenin Equivalent circuit in Figure 3.

If the value of

Rth{displaystyle R_{th}}

form equation 1 is substituted into equation 3.

Now look at Figure 1 and calculate

VR2{displaystyle V_{R2}}

by voltage divider rule it has the same value as equation 4. If the current through

R2{displaystyle R_{2}}

is calculated in Figure 4 by current divider rule.

Substituting equation 2 into 5.

If equation 4 and Ohm’s Law are used to get the voltage across

R2{displaystyle R_{2}}

equation 3 is reached.

Please note: The “||”, a symbol that is used as an operator here, holds higher precedence than the “+” operator. As such, it is evaluated before a sum.

See Norton’s theorem and Thevenin’s theorem for more examples.

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Superposition Principle[edit]

Superposition Illustrative1.svg(a)

Superposition Illustrative2.svg(b)

Superposition Illustrative3.svg(c)

Figure 1: The circuits showing the linearity of resistors.

Most basic electronic circuits are composed of linear elements. Linear elements are circuit elements which follow Ohm’s Law. In Figure 1 (a) with independent voltage source, V1, and resistor, R, a current i1 flows. The current i1 has a value according to Ohm’s Law. Similarly in Figure 1 (b) with independent voltage source, V2, and resistor, R, a current i2 flows. In Figure 1 (c) with independent voltage sources, V1 and V2, and resistor, R, a current i flows. Using Ohm’s Law equation 1 is reached. If some simple algebra is used then equation 2 is reached. But V1/R has a value i1 and the other term is i2 this gives equation 3. This is basically what the Superposition Theorem states.

The Superposition Theorem states that the effect of all the sources with corresponding stimuli on a circuit of linear elements is equal to the algebraic sum of each individual effect. Each individual effect is calculated by removing all other stimuli by replacing voltage sources with short circuits and current sources with open circuits. Dependent sources can be removed as long as the controlling stimuli is not set to zero. The process of calculating each effect with one stimulus connected at a time is continued until all the effects are calculated. If kth stimulus is denoted sk and the effect created by sk denoted ek.

The steps for using superposition are as follows:

1. Calculate the effect of each source in turn with all other independent voltage sources short circuited and independent current sources open circuited.
2. Sum these effects to get the complete effect.

Note: the removal of each source is often stated differently as: replace each voltage source with its internal resistance and each current with its internal resistance. This is identical to what has been stated above. This is because a real voltage source consists of an independent voltage source in series with its internal resistance and a real current source consists of an independent current source in parallel with its internal resistance.

Superposition Example[edit]

Superposition Example.svg

Figure 2: The circuit for the example.

Problem: Calculate the voltage, v, across resistor R1.

Step 1:
Short circuit V2 and solve for v1. By voltage divider rule.

Short circuit V1 and solve for v2. By voltage divider rule.

Step 2:
Sum the effects.

Using equations 5 and 6.


R1=R2=R3=2kΩ{displaystyle R_{1}=R_{2}=R_{3}=2kOmega }


V1=V2=15V{displaystyle V_{1}=V_{2}=15V}


There is a wide array of devices used to test and diagnose electronic equipment. This chapter will attempt to explain the differences and different types of equipment used by electronics technicians and engineers.


An ammeter measures current.Current in electronics is usually measured in mA which are called milliamperes, which are 1/1000s of an ampere.
. The ammeter’s terminals must be in series with the current being measured. Ammeters have a small resistance (typically 50 ohms) so that they only have a small effect on the current.

0 Polímero GFDL.jpg

Basically an ammeter consists of a coil that can rotate inside a magnet, but a spring is trying to push the coil back to zero. The larger the current that flows through the coil, the larger the angle of rotation, the torque (= a rotary force) created by the current being counteracted by the return torque of the spring.
. Usually ammeters are connected in parallel with various switched resistors that can extend the range of currents that can be measured. Assume, for example, that the basic ammeter is “1000 ohms per volt”, which means that to get the full-scale deflection of the pointer a current of 1 mA is needed (1 volt divided by 1000 ohms is 1 mA – see “Ohm’s Law”).
. To use that ammeter to read 10 mA full-scale it is shunted with another resistance, so that when 10 mA flows, 9 mA will flow through the shunt, and only 1 mA will flow through the meter. Similarly, to extend the range of the ammeter to 100 mA the shunt will carry 99 mA, and the meter only 1 mA.


An ohmmeter measures resistance.The two terminals of ohmmeter are each placed on a terminal of the resistance being measured. This resistance should be isolated from other effects. (It should be taken out of a circuit, if it is in one.)

Ohmmeters are basically ammeters that are connected to an internal battery, with a suitable resistance in series. Assume that the basic ammeter is “1000 ohms per volt”, meaning that 1 mA is needed for full-scale deflection. When the external resistance that is connected to its terminals is zero (the leads are connected together at first for calibration), then the internal, variable, resistor in series with the ammeter is adjusted so that 1 mA will flow; that will depend on the voltage of the battery, and as the battery runs down that setting will change. The full scale point is marked as zero resistance. If an external resistance is then connected to the terminals that causes only half of the current to flow (0.5 mA in this example), then the external resistance will equal the internal resistance, and the scale is marked accordingly. When no current flows, the scale will read infinity resistance. The scale of an ohmmeter is NOT linear.Ohmmeters are usually usuful in cheking the short circuit and open circuit in boards.


A voltmeter measures voltage.The voltmeter’s terminals must be in parallel with the voltage being measured. Voltmeters have a large resistance (typically 1 megaohm), so that they only have a small effect on the voltage.

Fluke 87 III True RMS Multimeter.jpg


Digital Multimeter Aka.jpg

A multimeter is a combination device, (usually) capable of measuring current, resistance, or voltage. Most modern models measure all three, and include other features such as a diode tester, which can be used to measure continuity in circuits (emitting a loud ‘beep’ if there is a short).


An oscilloscope, commonly called a ‘scope’ by technicians, is used to display a voltage waveform on a screen, usually graphing voltage as a function of time.

Tektronix 465 oscilloscope.png

Spectrum Analyzer[edit]

Spectrum analyzer shows voltage (or power) densities as function of frequency on radio frequency spectrum. Spectrum analyzer can use analog frequency scanning principle (like radio receiver always changing frequency and measuring receiving amplitude) or digital sampling and FFT (Fast Fourier Transformation).

Spektrumanalysator FSL von Rohde & Schwarz.jpg

Logic analyzer[edit]

A logic analyzer is, in effect, a specialised oscilloscope. The key difference between an analyzer and an oscilloscope is that the analyzer can only display a digital (on/off) waveform, whereas an oscilloscope can display any voltage (depending on the type of probe connected). The other difference is that logic analyzers tend to have many more signal inputs than oscilloscopes – usually 32 or 64, versus the two channels most oscilloscopes provide. Logic analyzers can be very useful for debugging complex logic circuits, where one signal’s state may be affected by many other signals.

Logic probe new.jpg

Frequency counter[edit]

A frequency counter is a relatively simple instrument used to measure the frequency of a signal in Hertz (cycles per second). Most counters work by counting the number of signal cycles that occur in a given time period (usually one second). This count is the frequency of the signal in Hertz, which is displayed on the counter’s display.

Frequency counter.JPG


A voltmeter with extremely high input resistance capable of measuring electrical charge with minimal influence to that charge. Ubiquitous in nucleonics, physics and bio-medical disciplines. Enables the direct verification of charge measured in coulombs according to Q=CV. Additionally, electrometers can generally measure current flows in the femtoampere range, i.e. .000000000000001 ampere.

Signal Generator[edit]

Leader LSG-15 signal generator.jpg

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DC Circuit Analysis[edit]

In this chapter, capacitors and inductors will be introduced (without considering the effects of AC current.) The big thing to understand about Capacitors and Inductors in DC Circuits is that they have a transient (temporary) response. During the transient period, capacitors build up charge and stop the flow of current (eventually acting like infinite resistors.) Inductors build up energy in the form of magnetic fields, and become more conductive. In other words, in the steady-state (long term behavior), capacitors become open circuits and inductors become short circuits. Thus, for DC analysis, you can replace a capacitor with an empty space and an inductor with a wire. The only circuit components that remain are voltage sources, current sources, and resistors.

Capacitors and Inductors at DC[edit]

Electronics DC CLmess 0.PNG
Electronics DC CLmess 1.PNG
Electronics DC CLmess 2.PNG
Electronics R.PNG

DC steady-state (meaning the circuit has been in the same state for a long time), we’ve seen that capacitors act like open circuits and inductors act like shorts. The above figures show the process of replacing these circuit devices with their DC equivalents. In this case, all that remains is a voltage source and a lone resistor. (An AC analysis of this circuit can be found in the AC section.)


If a circuits contains only resistors possibly in a combination of parallel and series connections then an equivalent resistance is determined. Then Ohm’s Law is used to determine the current flowing in the main circuit. A combination of voltage and current divider rules are then used to solve for other required currents and voltages.

Simplify the following:
Electronics R.PNG(a)
Electronics R2S.PNG(b)
Electronics R3S.PNG(c)

Figure 1: Simple circuits series circuits.

The circuit in Figure 1 (a) is very simple if we are given R and V, the voltage of the source, then we use Ohm’s Law to solve for the current. In Figure 1 (b) if we are given R1, R2 and V then we combine the resistor into an equivalent resistors noting that are in series. Then we solve for the current as before using Ohm’s Law. In Figure 1 (c) if the resistors are labeled clockwise from the top resistor R1, R2 and R3 and the voltage source has the value: V. The analysis proceeds as follows.

This is the formula for calculating the equivalent resistance of series resistor. The current is now calculated using Ohm’s Law.

If the voltage is required across the third resistor then we can use voltage divider rule.

Or alternatively one could use Ohm’s Law together with the current just calculated.

Electronics R2P.PNG(a)
Electronics R3P.PNG(b)

Figure 2: Simple parallel circuits.

In Figure 2 (a) if the Resistor nearest the voltage source is R1 and the other resistor R2. If we need to solve for the current i. then we proceed as before. First we calculate the equivalent resistance then use Ohm’s Law to solve for the current. The resistance of a parallel combination is:

So the current, i, flowing in the circuit is, by Ohm’s Law:

If we need to solve for current through R2 then we can use current divider rule.

But it would probably have been simpler to have used the fact that V most be dropped across R2. This means that we can simply use Ohm’s Law to calculate the current through R2. The equation is just equation 1. In Figure 2 (b) we do exactly the same thing except this time there are three resistors this means that the equivalent resistance will be:

Using this fact we do exactly the same thing.

Electronics 4RSP.PNG (a)
Electronics 7RSP.PNG (b)
Electronics R cube.PNG (c)

Figure 3: Combined parallel and series circuits

In Figure 3 (a), if the three resistors in the outer loop of the circuit are R1, R2 and R3 and the other resistor is R4. It is simpler to see what is going on if we combine R2 and R3 into their series equivalent resistance

R23{displaystyle R_{2}3}

. It is clear now that the equivalent resistance is R1 in series with the parallel combination of

R23{displaystyle R_{2}3}

and R4. If we want to calculate the voltage across the parallel combination of R4 and

R23{displaystyle R_{23}}

then we just use voltage divider.

If we want to calculate the current through R2 and R3 then we can use the voltage across

R4||(R2+R3){displaystyle R_{4}||(R_{2}+R_{3})}

and Ohm’s law.

Or we could calculate the current in the main circuit and then use current divider rule to get the current.

In Figure 3 (b) we take the same approach simplifying parallel combinations and series combinations of resistors until we get the equivalent resistance.

In Figure 3 (c) this process doesn’t work then because there are resistors connected in a delta this means that there is no way to simplify this beyond transforming them to a star or wye connection.

Note: To calculate the current draw from the source the equivalent resistance always must be calculated. But if we just need the voltage across a series resistor this may be necessary. If we want to calculate the current in parallel combination then we must use either current divider rule or calculate the voltage across the resistor and then use Ohm’s law to get the current. The second method will often require less work since the current flowing from the source is required for the use of current divider rule. The use of current divider rule is much simpler in the case when the source is a current source because the value of the current is set by the current source.

Star Network

The above image shows three points 1, 2, and 3 connected with resistors R1, R2, and R3 with a common point.
Such a configuration is called a star network or a Y-connection.

Delta Network

The above image shows three points 1, 2, and 3 connected with resistor R12, R23, and R31.
The configuration is called a delta network or delta connection.

We have seen that the series and parallel networks can be reduced by the use of simple equations.
Now we will derive similar relations to convert a star network to delta and vice versa.
Consider the points 1 and 2.
The resistance between them in the star case is simply

R1 + R2

For the delta case, we have

R12 || (R31 + R23)

We have similar relations for the points 2, 3 and 3, 1.
Making the substitution r1= R23 etc., we have, simplifying,

R1=r2r3r1+r2+r3{displaystyle R_{1}={frac {r_{2}r_{3}}{r_{1}+r_{2}+r_{3}}}}

r1=R1R2+R2R3+R3R1R1{displaystyle r_{1}={frac {R_{1}R_{2}+R_{2}R_{3}+R_{3}R_{1}}{R_{1}}}}

in the most general case.
If all the resistances are equal, then R = r/3.


Ammeters are devices that measure current. Current in electronics is usually measured in mA which are called milliamperes, which are 1/1000s of an ampere.
….. Basically an ammeter consists of a coil that can rotate inside a magnet, but a spring is trying to push the coil back to zero. The larger the current that flows through the coil, the larger the angle of rotation, the torque (= a rotary force) created by the current being counteracted by the return torque of the spring.
….. Usually ammeters are connected in parallel with various switched resistors that can extend the range of currents that can be measured. Assume, for example, that the basic ammeter is “1000 ohms per volt”, which means that to get the full-scale deflection of the pointer a current of 1 mA is needed (1 volt divided by 1000 ohms is 1 mA – see “Ohm’s Law”).
….. To use that ammeter to read 10 mA full-scale it is shunted with another resistance, so that when 10 mA flows, 9 mA will flow through the shunt, and only 1 mA will flow through the meter. Similarly, to extend the range of the ammeter to 100 mA the shunt will carry 99 mA, and the meter only 1 mA.


Ohmmeters are basically ammeters that are connected to an internal battery, with a suitable resistance in series. Assume that the basic ammeter is “1000 ohms per volt”, meaning that 1 mA is needed for full-scale deflection. When the external resistance that is connected to its terminals is zero (the leads are connected together at first for calibration), then the internal, variable, resistor in series with the ammeter is adjusted so that 1 mA will flow; that will depend on the voltage of the battery, and as the battery runs down that setting will change. The full scale point is marked as zero resistance. If an external resistance is then connected to the terminals that causes only half of the current to flow (0.5 mA in this example), then the external resistance will equal the internal resistance, and the scale is marked accordingly. When no current flows, the scale will read infinity resistance. The scale of an ohmmeter is NOT linear.Ohmmeters are usually useful in checking the short circuit and open circuit in boards.


Multimeters contain Ohmeters, Voltmeters, Ammeters and a variety of capabilities to measure other quantities. AC and DC voltages are most often measurable. Frequency of AC voltages. Multimeters also feature a continuity detector, basically an Ohmmeter with a beeper if the multimeter sees less than 100 Ω then it beeps otherwise it is silent. This is very useful for finding whether components are connected when debugging or testing circuits. Multimeters are also often able to measure capacitance and inductance. This may be achieved using a Wien bridge. A diode tester is also generally onboard, this allows one to determine the anode and cathode of an unknown diode. A LCD display is also provided for easily reading of results.



The instrument is used to view AC waveforms. For better explanation of the oscilloscope.

Spectrum Analyzer[edit]


Signal Generator[edit]

This instrument is used to generate low voltage AC signals. Most common signal generators can create sinusoidal(sine), triangular and square waves of various frequencies. They are used in conjunction with the oscilloscope to test analogue circuits.


Logic Probe[edit]

This instrument generates high and low logic states to test digital circuits. If a logic probe is not available a square wave through a signal generator can be used. Square waves can also be used to test the response time of a digital circuits.

Wikipedia:Logic Probe
Electrical Noise
any unwanted form of energy tending to interfere with the proper and easy reception and reproduction of wanted signals.


Based on Origin[edit]

  1. External noise
    1. Atmospheric
    2. Extraterrestrial
      1. solar
      2. Cosmic
    3. Industrial
  2. Internal noise
    1. Thermal Agitation Noise
    2. Shot Noise
    3. Transit Time Noise
    4. Flicker Noise
    5. Miscellaneous Sources

Thermal noise[edit]

Thermal Agitation Noise
Also known as Johnson noise or White noise.

where k = Boltzmann’s constant = 1.38×10-23J/K

T = absolute temperature, K = 273 + °C
δ f = bandwidth of interest
Pn = maximum noise power output of a resistor

Shot Noise[edit]

where in = r.m.s. shot-noise current

e = charge of an electron = 1.6×10-19C
ip = direct diode current
δ f = bandwidth of system

Noise Calculations[edit]

Addition due to several sources[edit]

noise voltages:

where Rtot = R1+R2+…

Addition due to Cascaded Amplifier stages[edit]

Req = R1+R’2

Analog Noise Models[edit]



Noise in digital circuits:[edit]

Methods of reducing noise[edit]

Differential signaling[edit]

Differential signaling is a method of transmitting information electrically by means of two complementary signals sent on two separate wires. The technique can be used for both analogue signaling, as in some audio systems, and digital signaling, as in RS-422, RS-485, PCI Express and USB.

Good grounding[edit]

An ideal signal ground maintains zero voltage regardless of how much electrical current flows into ground or out of ground.

When low-level signals travel near high currents, their return currents shouldn’t be allowed to flow in the same conductor. Otherwise, noise such as AC ripple on the high current will modulate the low-level signal.


Kennedy, George ‘Electronic Communication Systems’ , 3rd Ed. ISBN 0-07-034054-4

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Relationship between Voltage and Current[edit]


In a resistor, the current is in phase with the voltage always. This means that the peaks and valleys of the two waveforms occur at the same times. Resistors can simply be defined as devices that perform the sole function of inhibiting the flow of current through an electrical circuit. Resistors are commercially available having various standard values, nevertheless variable resistors are also made called potentiometers, or pots for short. In theory electricity is a method used to harness myriad numbers including symbols to give the notion on how circuits function on a schematic drawing


The capacitor is different from the resistor in several ways. First, it consumes no real power. It does however, supply reactive power to the circuit. In a capacitor, as voltage is increasing the capacitor is charging. Thus a large initial current. As the voltage peaks the capacitor is saturated and the current falls to zero. Following the peak the circuit reverses and the charge leaves the capacitor. The next half of the cycle the circuit runs mirroring the first half.

The relationship between voltage and current in a capacitor is:

i(t)=Cd(v(t))dt{displaystyle i(t)=C{d(v(t)) over dt}}

. This is valid not only in AC but for any function v(t). As a direct consequence we can state that in the real world, the voltage across a capacitor is always a continuous function of the time.

If we apply the above formula to a AC voltage (i.e.

v(t)=Vsin(ωt+Φ){displaystyle v(t)=Vcdot sin(omega t+Phi )}

), we get for the current a 90° phase shift:

i(t)=Vωcos(ωt+Φ){displaystyle i(t)=Vcdot omega cdot cos(omega t+Phi )}


In an AC circuit, current leads voltage by a quarter phase or 90 degrees. Note that while in DC circuits after the initial charge or discharge no current can flow, in AC circuits a current flows all the time into and out of the capacitor, depending on the impedance in the circuit. This is similar to the resistance in DC circuits, except that the impedance has 2 parts; the resistance included in the circuit, and also the reactance of the capacitor, which depends not only on the size of the capacitor, but also on the frequency of the applied voltage. In a circuit that has DC applied plus a signal, a capacitor can be used to block the DC, while letting the signal continue.


In inductors, current is the negative derivative of voltage, meaning that however the voltage changes the current tries to oppose that change. When the voltage is not changing there is no current and no magnetic field.

In an AC Circuit, voltage leads current by a quarter phase or 90 degrees.

Voltage Defined as the derivative of the flux linkage:

V(t)=d(Ni(t))dt{displaystyle V(t)={d(Ni(t)) over dt}}


A circuit containing resistors, capacitors, and inductors is said to be in resonance when the reactance of the inductor cancels that of the capacitor to leave the resulting total resistance of the circuit to be equal to the value of the component resistor. The resonance state is achieved by fine tuning the frequency of the circuit to a value where the resulting impedance of the capacitor cancels that of the inductor, resulting in a circuit that appears entirely resistive.

See also[edit]

AC Voltage:

When the polarity of the Voltage between two points is changing continuously with time then the voltage is called AC Voltage.
For AC Voltages there will be no constant value so we define it by the average value called RMS value RMS means Root Means Square. In retrospect on AC the power that is used to theoretically determine by an unkown which we assume to be a steady flow, this is also what technicians label the fluctuation of current that determines how electricity moves in a diagram.

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Figure One: Rectangular Notation

Figure Two: Polar Notation

Phasors provide a simple means of analyzing linear circuits. At the heart of phasor analysis lies Euler’s formula:

A complex exponential can also be expressed as

A~=Aejθ{displaystyle {tilde {A}}=Ae^{jtheta }}

is called a phasor. It contains information about the magnitude and phase of a sinusoidal signal, but not the frequency or time. This simplifies use in circuit analysis, since most of the time, all quantities in the circuit will have the same frequency. (For circuits with sources at different frequencies, the principle of superposition must be used.)

A shorthand phasor notation is:

A~=Aθ{displaystyle {tilde {A}}=Aangle theta }

Note that this is simply a polar form, and can be converted to rectangular notation by (see figure one):

and back again by (see figure two):

Sinusoidal Signals[edit]

To begin, we must first understand what sinusoidal signals are. Sinusoidal signals can be represented as

where A is the amplitude,

ω{displaystyle omega }

is the frequency in radians per second, and

θ{displaystyle theta }

is the phase angle in degrees(phase shift).
We can return to the sinusoidal signal by taking the real part of Euler’s formula:

For the moment, consider single-frequency circuits. Every steady state current and voltage will have the same basic form:


We have three sinusoidal signals with the same frequency added together:

In phasor notation, this is:

We can combine these terms to get one phasor notation. This is done first by separating the real and imaginary components:

The phasor notation can be written as:

Back to the time domain, we get the answer:

    • j is the Imaginary unit (
    • In electrical engineering, the imaginary unit is symbolized by j rather than the symbol i because i is used to denote current in electrical engineering.
    • The frequency of the wave, in Hz, is given by

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Z~{displaystyle {tilde {Z}}}

, is the quantity that relates voltage and current in the frequency domain. (The tilde indicates a phasor. An overscore or arrow may also be used.)

In rectangular form,

where R is the resistance and X is the reactance. Impedance is generally a function of frequency, i.e.

NOTE: ω = 2 π f

where f is the frequency in cycles per second (f=50 or 60 Hertz usually, depending on the country concerned. Aircraft systems often use 400 Hertz.)


Reactance (symbol

X{displaystyle X}

) is the resistance to current flow of a circuit element that can store energy (i.e. a capacitor or an inductor), and is measured in ohms.

The reactance of an inductor of inductance

L{displaystyle L}

(in Henries), through which an alternating current of angular frequency

w{displaystyle w}

flows is given by:

The reactance of a capacitor of capacitance

C{displaystyle C}

(in Farads) is given similarly:

The two formulae for inductive reactance and capacitive reactance create interesting counterpoints. Notice that for inductive reactance, as the frequency of the AC increases, so does the reactance. Hence, higher frequencies result in lower current. The opposite is true of capacitive reactance: The higher the frequency of AC, the less reactance a capacitor will present.

Similarly, a more inductive inductor will present more reactance, while a capacitor with more capacitance will yield less reactance.


Resistors have zero reactance, since they do not store energy, so their impedance is simply


Capacitors have zero resistance, but do have reactance. it is stored in the power of a circuit or it can be also stored in a motor running off a AC current. Their impedance is

where C is the capacitance in farads. The reactance of one microfarad at 50 Hz is -3183 ohms, and at 60 Hz it is -2653 ohms. In much more basic terms storing energy would be equivalent to a battery the power source is active and stays in this manner without any loss of power, this is what is regarded as a means for reversing electricity in the process of keeping that current.



Like capacitors, inductors have zero resistance, but have reactance. Their impedance is

where L is the inductance in henries. The reactance of one henry at 50 Hz is 314 ohms, and at 60 Hz it is 377 ohms.

Circuit Analysis Using Impedance[edit]

Analysis in the frequency domain proceeds exactly like DC analysis, but all currents and voltages are now phasors (and so have an angle). Impedance is treated exactly like a resistance, but is also a phasor (has an imaginary component/angle depending on the representation.)

(In the case that a circuit contains sources with different frequencies, the principle of superposition must be applied.)

Note that this analysis only applies to the steady state response of circuits. For circuits with transient characteristics, circuits must be analyzed in the Laplace domain, also known as s-domain analysis.

Steady State[edit]

That can be said to be the condition of “rest”, after all the changes/alterations were made. This may imply, for examples, that nothing at all happens, or that a “steady” current flows, or that a circuit has “settled down” to final values – that is until the next disturbance occurs.

If the input signal is not time invariant, say if is a sinosoid, the steady state will not be invariant either. The response of a systematic convergence can be considered to be composed of a transient response: the response to a disturbance, and the steady state response, in the absence of disturbance.

The transient part of the response tends to zero as time since a disturbance tends to infinity, so the steady state can be considered to be the response remaining as T -> infinity.. In this case we make an assumption for error we can determine by calculation the extent of statistics how much power there is according to the formulae. Deducing the theory of certain parts of a sinuous making plausible solution in understanding the intricate mechanism of a steady state solution.

RL Series Open-Closed.svg

The following is a description of the events that take place when a DC voltage is applied to an inductor. We need to consider that fact that the inductor has a parasitic resistance caused by the fact the wire it is made from is not superconducting. If we do not consider this, then we have a circuit with no way to dissipate energy – an ideal inductor is just a short circuit to DC once the magnetic field has been set up. So, we consider an ideal inductor in series with an ideal resistor as shown to the right.

  • Before the switch is closed, there is no voltage or current across either the resistor or the inductor.
  • When the switch is first closed, the current through the inductor is zero, because it cannot change instantaneously.
  • This means that the inductor acts like an open circuit, so all the voltage is across the inductor.
  • As the current ramps up from zero, the magnetic field builds in strength.
  • The changing magnetic field creates a back emf which acts to oppose the current in the inductor. This back emf will not stop the current completely, but it will slow it down.
  • Eventually, the current in the inductor reaches full strength (as governed by the resistor and the voltage by Ohm’s Law).
  • When this happens, the current is no longer changing, so the voltage across the inductor is zero. The magnetic field is still present, but it is static, so there is no back emf.
  • All the voltage is now across the resistor, and the inductor acts as a short circuit.

The circuit will remain like this, with a certain current, all the voltage across the resistors and none over the inductor. There is a constant magnetic field in the inductor, and no back emf. However, when the switch is opened again,

  • The current drops to zero very rapidly.
  • The magnetic field collapses rapidly.
  • The hanging magnetic field induces a back emf in the inductor. As the magnetic field changes so rapidly, the back emf is very large (infinite if the switch was perfect).
  • This large voltage is across the switch.
  • It is likely that a spark will jump the gap, possibly damaging the switch. If a transistor is used, it should be protected with diodes.
  • After the back emf has settled, the circuit has no current and no voltage in it – we are where we started.

As you can see, inductors don’t really add much to a DC circuit, except when energized and de-energized. However, in AC circuits, inductors can be used for many things.

For a series RC consist of one resistor connected with one capacitor in a closed loop.

Circuit Impedance[edit]

In Polar Form Z/_θ

In Complex Form Z(jω)

T = RC

Differential Equation of circuit at equilibrium[edit]

Time Constant[edit]

T = R C
t V(t) % Vo
0 A = eC = Vo 100%
1/RC .63 Vo 60% Vo
2/RC Vo
3/RC Vo
4/RC Vo
5/RC .01 Vo 10% Vo
Capacitor Charge-Discarge.svg

Angle Difference Between Voltage and Current[edit]

Current leads Voltage on an angle; Does this mean in measuring a angle of DC current causes a decrease in current? Let us take some time to understand the previous math in determing a factor of sinuous solution.

Change the value of R and C will change the value of Angle Difference, Angular Frequency, Frequency and Time



RC switch.PNG

When the switch is open, the initial voltage across the capacitor is zero. When the switch closes (which we will refer to as time zero) the capacitor charges via the resistor to

V0{displaystyle V_{0}}


When the switch is closed, the circuit must follow the relationship:

which is derived by analysing the circuit using Kirchoff’s Voltage Law.

By letting

τ=RC{displaystyle tau =RC}

and rearranging the equation:

This is a first order linear differential equation with integrating factor:

Multiplying both sides by the integrating factor:

Note that:

Substituting and integrating both sides:

where K is the integration constant.

When t=0


When t>0 this gives:

when t<0:

Rc circuit plot.png
RL Series Open-Closed.svg

For a series RL of one resistor connected with one inductor in a closed loop

Circuit Impedance[edit]

In Polar Form Z/_θ

Z = |Z|/_θ =

In Complex Form Z(jω)

Differential Equation of circuit at equilibrium[edit]

Time Constant[edit]

t I(t) % Io
0 A = eC = Io 100%
R/L .63 Io 60% Io
2 R/L Io
3 R/L Io
4 R/L Io
5 R/L .01 Io 10% Io

Angle Difference between Voltage and Current[edit]

Voltage leads Current at an angle ? When a determining process is necessary many problems arise in a diagram. We need to expend on one process for the determing factor in this type of formulae

Tan? =

Change the value of R and L will change the value Angle Difference, Angular Frquency, Frequency, Time

For a series LC consists of one capacitor connected with one coil in series in a closed loop

Circuit Impedance[edit]

In Polar Form

In Compled Form

Circuit at equilibrium[edit]

Time Constant[edit]

T = -1/LC

Phase Difference[edit]

Phase: A particular appearnce or state in a regulalry recurring cycle of changes.
A phase should be used as a problem yet to be discoverd. With a tool measuring the distance BC we can for example discover that a certain peculiarity a difference in single circuits theory causes the diagram to carry out its function. Such is the case with AB the same process may take place except a difference in diagram causes a difference in phasing. MAGNETIC coils as mentioned in singularity gives an engineer the means to figure how or where the short might be located. Of course on the basis of general phase the assumed starting point of electricity is found within an oscillation, a point of contact this contact appears different depending on the schematic drawing. In a mathematical notation you can determine using calculus how much power there is in a closed loop. The only problem is to figure a way when the loop is open in what other method can you use to make that solution possible?

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RLC Series[edit]

An RLC series circuit consists of a resistor, inductor, and capacitor connected in series:

RLC series circuit v1.svg

By Kirchhoff’s voltage law the differential equation for the circuit is:


Leading to:


There are three cases to consider, each giving different circuit behavior,

α2=β2,α2>β2,orα2<β2{displaystyle alpha ^{2}=beta ^{2},alpha ^{2}>beta ^{2},oralpha ^{2}


Equation above has only one real root

s = -α =

Equation above has only two complex roots

Circuit Analysis[edit]

R = 0[edit]

If R = 0 then the RLC circuit will reduce to LC series circuit . LC circuit will generate a standing wave when it operates in resonance; At Resonance the conditions rapidly convey in a steady functional method.

R = 0 ZL = ZC[edit]

If R = 0 and circuit above operates in resonance then the total impedance of the circuit is Z = R and the current is V / R

At Resonance

At Frequency

I = 0 . Capacitor opens circuit . I = 0
I = 0 Inductor opens circuit . I = 0

Plot the three value of I at three I above we have a graph I – 0 At Resonance frequency

ω=1LC{displaystyle omega ={sqrt {frac {1}{LC}}}}

the value of current is at its maximum

I=VR{displaystyle I={frac {V}{R}}}

. If the value of current is half then circuit has a stable current

I=V2R{displaystyle I={frac {V}{2R}}}

does not change with frequency over a Bandwidth of frequencies É1 – É2 . When increase current above

I=V2R{displaystyle I={frac {V}{2R}}}

circuit has stable current over a Narrow Bandwidth . When decrease current below

I=V2R{displaystyle I={frac {V}{2R}}}

circuit has stable current over a Wide Bandwidth

Thus the circuit has the capability to select bandwidth that the circuit has a stable current when circuit operates in resonance therefore the circuit can be used as a Resonance Tuned Selected Bandwidth Filter

Further Reading[edit]

  1. RCL circuit analysed in the time domain
  2. RCL circuit analysed in the frequency domain

As explained later, digital signals can only take one of two values at any one point.
Analog signals, however, can take any value within a range.
In modern electronics, many traditionally analog circuits are being replaced with digital ICs for various reasons:

  • Reduced cost:
    • Digital ICs can be programmed, meaning many different analog circuits can each be replaced with the same IC, reducing cost. For example, the same DSP chip might replace many different analog filters.
    • Digital ICs can be easily expanded to put multiple functions on the same chip. For example, a DSP chip replacing multiple analog filters at the same time.
    • Digital ICs can be reprogrammed without modifying the circuit, simplifying prototyping and field upgrades.
  • Increased versatility:
    • A digital IC can have its settings changed arbitrarily while it is being operated, these settings can even be changed by software. The equivalent in an analog circuit might require expensive and complicated switching techniques.
  • Numeric precision: once a signal is converted to digital data, distortion and circuit noise are no longer a significant issue. A cheap modern watch driven by a digital circuit (such as a quartz oscillator and a counter) is more precise than any analog or mechanical clock.
  • Ease of storage: digital data, once recorded, does not degrade as easily as analog data.

Digital circuits are also becoming more prevalent where there are no analog analogues, such as computers. Although analogue computers exist, their utility is severely limited by comparison.

Analog circuits are still more suitable for many functions.
One important category is interfaces.
Digital circuits are usually inferior to analog circuits for receiving and transmitting signals.

  • A common digital interface, the differential line, needs an analog circuit to function well. The receiver must filter out common mode interference by computing the analog difference between the two lines. Most digital interfaces are designed as analog, only a few legacy interfaces (which have poor performance) use entirely digital circuits.
  • Many radio signals are simply too high frequency to work with existing digital circuits. Radio modulators, demodulators, mixers, transmitters, and receivers are still analog. Some signals are even too high frequency for transistor circuits of any kind to amplify efficiently, such as microwave signals, which are still transmitted using vacuum tubes.
  • Signals must be conditioned before conversion to digital to avoid aliasing: analog filters remove unwanted parts of signals.
  • Many devices, such as monitors, require analog control. Even LCD monitors require analog circuits, although they need not be as sophisticated as CRT analog circuits.
  • Audio equipment requires analog circuits. Speakers must be driven by analog signals, microphones produce analog signals. Signal of a microphone must be conditioned before conversion to digital, this usually entails sophisticated analog circuits such as preamplifers, compressors, and filters.

Semiconductors typically use silicon as a base material. Silicon has 14 electrons in three shells. The inner two shells are full with 2 and 8 electrons each. The outermost shell has spots for 8 electrons, but only 4 are present.

With four electrons and four holes, multiple silicon atoms can form a stable configuration, each sharing electrons with neighboring atoms to fill their electron shells.

In a pure crystal of silicon, all atoms share electrons perfectly with all their neighboring atoms. However, other elements can be introduced to the crystal via semiconductor doping to produce extra electrons or extra holes (unfilled spots for an electron). These types of crystals are called n-doped semiconductors (for having a net negative charge due to extra electrons) and p-doped semiconductors (for having a net positive charge due to having a deficit of electrons).

It doesn’t take many impurity atoms to create a semiconductor; one impurity atom per half-million silicon atoms will make a reasonable semiconductor.[1] The most common elements used in semiconductor doping are ones with only one extra electron or hole relative to silicon: boron, phosphorous, gallium, and arsenic are all common dopants.

Electrical current flows in a material by causing a cascading jumping of electrons/holes. An electron will enter one side of the material and knock another electron free from its shell, taking its place. That electron will continue in a similar direct and do the same. Eventually, an electron will come out the other end of the material.


The first vacuum tube diodes were created by Thomas Edison in 1904. These initial tubes could only be used for rectification. The triode, which allowed for voltage and power amplification, was invented 3 years later in 1907 by Lee De Forest.

Vacuum tubes are also referred to as thermionic tubes, thermionic valves, electron tubes, valves and just plain tubes.

While, for most electronics, vacuum tubes have been replaced by transistors, there are still some uses for which vacuum tubes are desired. Vacuum tubes are frequently used in high end Hi Fi amplifiers and are generally desirable over transistors for their “warmer” tone. They are also generally preferred in guitar amplifiers both for their smoother clipping in overdrive and the warmer tone.

Finally, vacuum tubes are used in high frequency communications (at frequencies that would destroy solid state components) as well as satellite and military communications due to their durability (they stand up to solar radiation better than solid state and are immune to electromagnetic pulse).

Passive Versus Active Components[edit]

Passive components have no gain and are not valves

  • Voltage Regulator: an active component which accepts a range of voltages and outputs one constant voltage.

Vacuum Tube Basics[edit]

A Vacuum Tube is a container (usually of glass) from which the air is removed. Inside the tube are two or more “Elements”.

– Cathode: (electron emitter) has an electrically heated filament (which you can usually see glow red ) which spits out electrons that travel through the vacuum to the Anode (electron acceptor).

– Anode (a.k.a. Plate): Is a conductive (usually metal) plate that is connected to a positive voltage. The negative electrons flow from the Cathode to the Anode.

A vacuum tube with just Cathode and Anode elements is a DIODE. Current will flow only when the Anode has a positive voltage relative to the Cathode.

– Grid(s): metal gratings or grids are placed between the Cathode and Anode to produce devices that can amplify signals.

NOTE: A tube with 3 elements (one grid) is a TRIODE, with 2 grids a TETRODE, with 3 grids a PENTODE.

A Grid between the cathode and anode controls the flow of electrons. By applying a negative voltage to the grid it is possible to control the flow of electrons. This is the basis of the Vacuum Tube amplifier.

Vacuum tubes contain heater filaments. These are similar to the filaments one would find in a standard light bulb. The filaments usually run at low voltages (6V and 12V are common, though tubes can be found with a variety of filament voltages). The filament is surrounded by a cathode. The filaments are constructed of heat the cathode to about 800 degree Celsius, at which point the cathode begins to emit electrons. The electrons normally float on the surface of the cathode and this is called a space charge. The anode is generally kept more positive than the cathode and so it draws the electrons off of the cathode.

The voltage difference in the direction from the cathode to the anode is known as the forward bias and is the normal operating mode. If the voltage applied to the Anode becomes negative relative to the Cathode, no electrons will flow. In electronics vacuum electron tube or valve is a device that controls current. Through a vacuum in sealed container. Vacuum tubes rely on thermionic emission of electrons from hot filament.

Tube Characteristics[edit]

Below is an explanation of various tube parameters:

Name Description
Va (or Vp) Anode(Plate) voltage (more accurately, Vak or Vpk, as it is the voltage relative to the cathode)
Ia (or Ip) Anode current
Ra (or Rp) Anode load resistor
ra (or rp) Anode resistance (internal. Separate from and not to be confused with Ra/Rp)
Vg Control grid voltage (more accurately Vgk, as it is also relative to the cathode)
Vk Cathode voltage
Ik Cathode current
Vg2 Screen grid voltages
Ig2 Screen grid current

Diode vacuum tube construction

The symbol for an indirect heated vacuum-tube diode. From top to bottom, the components are the anode, the cathode, and the heater filament.

Vacuum tube diodes contain only two electrodes (besides the heater): A cathode and an anode. The filament heats up the cathode, producing a space charge. A relatively positive voltage on the anode then draws electrons from the cathode to the anode, producing the one way current of a diode. Current will not flow from anode to cathode.

As with silicon diodes, vacuum tube diodes can be used for various functions. They can be used in voltage multipliers, envelope detectors, and rectifiers, for example.

Common rectifier tubes are: 5AR4/GZ-34, 5V4-GA, GZ37, 5U4-G/GA/GB, 5Y3-G/GA, 5R4GYB, and 5R4-G/GY/GYA. Different rectifier tubes have different maximum voltages, current ratings and forward voltage drops. Some have 5V filaments and others 6.3V. And some draw more filament current than others.

Some rectifiers are half-wave (single diode) and some are full-wave, containing a single cathode, but two anodes, one for each half of the wave, as shown in the Full-wave rectifier image to the right.

Full-wave rectifier, with vacuum tube having two anodes.

Rectifier Tube Chart[edit]

Tube Type Max ACV PIV Max DCV Max DC mA Vf Fil. V Fil. mA
5AR4-G/GY/GYA 750 3100 358 250 67 5 2000
5AR4-GYB 900 3100 362 250 63 5 2000
5Y3-G/GA 350 1400 365 125 60 5 2000
5U4-GB 450 1550 375 275 50 5 3000
5U4-G 450 1550 381 225 44 5 3000
5U4-GA 450 1550 381 250 44 5 3000
GZ37 450 1000 388 350 37 5 2800
5V4-GA 375 1400 400 175 25 5 2000
5AR4/GZ-34 425 1500 415 250 10 5 1900
6CA4/EZ81 450 1300 500 150 20 6.3 1000


A klystron is a vacuum tube used for production of microwave energy. This device is related to but not the same as a magnetron. The klystron was invented after the magnetron.

Klystrons work using a principle known as velocity modulation.

The klystron is a long narrow vacuum tube. There is an electron gun (heater, cathode, beam former) at one end and an anode at the other. In between is a series of donut shaped resonant cavity structures positioned so that the electron beam passes through the hole.

The first and last of the resonant cavities are electrically wired together.

At the cathode the electron beam is relatively smooth. There are natural slight increases and decreases in the electron density of the beam. As the beam passes through the holes of the resonant cavities, any changes in the electron beam cause some changes in the resting electro magnetic (EM) field of the cavities. The EM fields of the cavities begin to oscillate. The oscillating EM field of the cavities then has an effect on the electrons passing through, either slowing down or speeding up their passage.

As electrons are affected by the EM field of the first cavity they change their speed. This change in speed is called velocity modulation. By the time the electrons arrive at the last cavity there are definite groups in the beam. The groups interact strongly with the last cavity causing it to oscillate in a more pronounced way. Some of the last cavity’s energy is tapped off and fed back to the first cavity to increase its oscillations. The stronger first cavity oscillations produce even stronger grouping of the electrons in the beam causing stronger oscillations in that last cavity and so on. This is positive feedback.

The output microwave energy is tapped of for use in high power microwave devices such as long range primary RADAR systems.

The klystron is a coherent microwave source in that it is possible to produce an output with a constant phase. This is a useful attribute when combined with signal processing to measure RADAR target attributes like Doppler shift.

Related microwave vacuum tubes are the Travelling Wave Tube (TWT) and the Travelling Wave Amplifier (TWA). A Hybrid device, which combines some aspects of these devices and the klystron, is a device called a Twicetron.


Magnetrons are used to produce microwaves.

This is the original device used for production of microwaves and was invented during the Second World War for use in RADAR equipment.

Magnetrons work using a principle known as velocity modulation.

A circular chamber, containing the cathode, is surrounded by and connected to a number of resonant cavities. The walls of the chamber are the anode. The cavity dimensions determine the frequency of the output signal. A strong magnetic field is passed through the chamber, produced by a powerful magnet.
The cathode is similar to most thermionic valves, except heavy, rigid construction is necessary for power levels used in most Magnetrons.
Early, experimental designs used directly heated cathodes. Modern, high powered designs use a rigid, tubular cathode enclosing a heater element.

Naturally excited electrons on the surface of the cathode are drawn off, into the chamber, toward the outer walls or anode. As the electrons move out, they pass through a magnetic field that produces a force perpendicular to the direction of motion and direction of the magnetic field. The faster the electrons move, the more sideways force is produced. The result is that the electrons rotate around the central cathode as they move toward the outside of the chamber.

As electrons move past the entrances to the resonant cavities a disturbance is made to the electro magnetic (EM) field that is at rest in the cavities. The cavity begins to oscillate. When another electron moves past the cavities, it also interacts with the internal EM field. The motion of the electron can be slowed or sped up by the cavity field. As more electrons interact with the cavity EM fields, the internal cavity oscillations increase and the effect on the passing electrons is more pronounced.

Eventually, bands of electrons rotating together develop within the central chamber. Any electrons that fall behind a band are given a kick by the resonant cavity fields. Any electrons going too fast have their excess energy absorbed by the cavities. This is the velocity modulation effect. The frequency of the resonance and electron interaction is in the order of GHz. (10^9 cycles per second)

In order to have a signal output from the magnetron, one of the cavities is taped with a slot or a probe to direct energy out into a waveguide for distribution.

Magnetrons for RADARs are pulsed with short duration and high current. Magnetrons for microwave ovens are driven with a continuous lower current.

The magnetrons for WWII bombers, operated by the RAF, were sometimes taped into a shielded box so that the aircrew could heat their in-flight meals, hence the first microwave ovens.

Cathode Ray Tube[edit]

A cathode ray tube or CRT is a specialized vacuum tube in which images are produced when an electron beam strikes a phosphorescent surface. Television sets, computers, automated teller machines, video game machines, video cameras, monitors, oscilloscopes and radar displays all contain cathode-ray tubes. Phosphor screens using multiple beams of electrons have allowed CRTs to display millions of colors.

The first cathode ray tube scanning device was invented by the German scientist Karl Ferdinand Braun in 1897. Braun introduced a CRT with a fluorescent screen, known as the cathode ray oscilloscope. The screen would emit a visible light when struck by a beam of electrons.

TV Tubes[edit]

TV tubes are basically cathode ray tubes. An electron beam is produced by an electrically-heated filament, and that beam is guided by two magnetic fields to a particular spot on the screen. The beam is moved so very quickly, that the eye can see not just one particular spot, but all the spots on the screen at once, forming a variable picture.

Colours are produced by having 3 or more differently coloured screen spots activated at once to a variable degree.

The 2 magnetic fields are one for the vertical deflection, one for the horizontal deflection, and they are provided to the beam by external coils.

Oscilloscope Tubes[edit]

Oscilloscope tubes are basically the same as TV tubes, but the beam is guided by two electrostatic fields provided by internal pieces of metal. It is a necessity because an oscilloscope uses a very large range of synchronisation frequencies for the deflection, when a TV set uses fixed frequencies, and it would be too difficult to drive large coils on a so large band of frequency.
They are much deeper for the same screen size as a TV tube because the deflection angle is little. A TV tube has a deflection angle of 90° for the be

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Theoretically, a diode allows current flow in only one direction. An ideal diode acts as a perfect insulator for currents flowing in one direction and as a perfect conductor for currents flowing through it in the other direction. The direction in which the diode allows current to flow is called the forward bias direction and that in which current is resisted is called reverse bias direction. Diode has a symbol as shown

Diode symbol.svg


The modern semiconductor diode consists of two regions of semiconductor each having impurities of different types such that one side has excess holes (p-region) and the other has excess electrons (n-region). Such a junction of p and n regions is called a pn junction diode. The p-region has about twice as much area as the n-region to compensate for the lesser mobility of holes compared to electrons.

+ o– [P | N]–o – .Theoretically, a diode allows current flow in only one direction the most common type today is a crystalline piece of material with a p junction connected to two electrical terminals.


I V Curve[edit]

Rectifier vi curve.GIF

As seen in the graph above the diode actually works in both the forward region and the backward region. In the forward region the value of I and V are positive and in the backward region I and V are negative.

Forward Region[edit]

Current and Voltage are positive
When V < Vd . I = 0 . Diode does not conduct
Khi V = Vd . I = 1mA . Diode starts to conduct . Vd = 0.3v|Ge , 0.6v|Si
Vd is called Forward Break Over Voltage
Khi V > Vd . Diode conducts current . Current is calculated by

Backward Region[edit]

Current and Voltage are Negative
When the value of voltage is more negative than the Peak Inverse Voltage (PIV) Voltage the Diode will be destroyed

Ideal Diode[edit]

The real diode approaches the ideal diode in the sense that the reverse current is extremely small (less than 1fA) at least for a significant part of the characteristic, and the forward current is very high (on the order of 1mA). Although a real diode does not have the characteristics as the ideal diode, in theory it is possible to make an ideal diode if the concentrations of dopants in both the regions are infinite. However, there is no way of actually doing this and experiments do not agree.

The Shockley equation[edit]

The diode reverse (saturation) current is governed by the doping concentration. The current flowing through the device varies as the voltage applied across it changes as given by the Shockley diode equation (not to be confused with Schottky):

ID=IS[exp(VD/nVT)1]{displaystyle I_{D}=I_{S}[exp(V_{D}/nV_{T})-1]}

In the equation above

VT{displaystyle V_{T}}

is defined as

VT=kT/q{displaystyle V_{T}=kT/q}

, where

k{displaystyle k}

is Boltzmann’s constant,

T{displaystyle T}

is the temperature in Kelvin, and

q{displaystyle q}

is the magnitude of the charge on an electron.

In the forward bias direction, current flows with low voltage. If one draws a characteristic for this equation, a sharp increase in current can be seen at a particular voltage called the cut-in voltage or the on-voltage.

In the reverse bias mode, the diode current is approximately

IS{displaystyle -I_{S}}

. This is called the reverse saturation current because it looks like the diode is saturated with charge and cannot allow more current in the reverse bias direction than this.

It initially appears that as the temperature

T{displaystyle T}

increases, the total diode current would decrease. However, the saturation current

IS{displaystyle I_{S}}

increases with temperature faster than the

VT{displaystyle V_{T}}

term decreases the current. This leads to a negative temperature coefficient for the entire device: as the diode heats up, it will pass more current.


However, a break from the above equation takes place at a point called break-down voltage. One could think of it as the point where the Shockley equation breaks down and is no longer valid. There are two reasons for breakdown to occur.

Avalanche Breakdown

This occurs as a result of excess minority carriers in a region. Minority carriers are those carriers that are in the wrong region. For example, electrons will be minority carriers in the p-region.

Zener Breakdown

This is basically due to a size difference or dopant concentration difference. One of the regions has a greater region of depletion (Reverse bias voltage induces a depletion region, which is sparse in a densely doped region and dense in a sparsely doped region. )

See also Zener diodes


So basically, there are three modes in which a diode operates:


No current flows until a small forward voltage is reached called cut-in voltage.


The diode prevents current from flowing in the opposite direction. Current is small, and voltage can be large (but not exceeding the Zener voltage.)


Once the diode voltage is more negative than the Zener voltage, the diode allows current to flow in the reverse direction.

When there is no voltage applied, the excess electrons of the N type semiconductor flow into the holes of the P type semiconductor. This creates a depletion region that acts as a voltage.

Diode Variations[edit]

Bridge Rectifier:

A diode circuit that ‘rectifies’ alternating current (AC) into direct current (DC). The bridge rectifier is a full-wave rectifier, meaning that both the positive and negative portions of the wave become positive. (In a half-wave rectifier, positive stays positive, and negative becomes zero.) The bridge rectifier has advantages over other full-wave rectifier designs, because it reduces peak-inverse voltage (PIV), the largest negative voltage across a single junction diode. By reducing the PIV, it becomes possible to use diodes with lower breakdown (Zener) voltages. This allows the use of cheaper diodes to perform the same function.

A bridge rectifier shown as 4 discrete diodes.

LED (Light Emitting Diode)

A diode that emits light!
LED symbol.svg


A diode made from a metal-semiconductor junction, rather than an p-type/n-type silicon junction. These diodes typically have a much lower forward voltage drop than standard diodes (around 0.2V versus 0.6V).
Schottky diode symbol.svg


A diode that is meant to be operated in the breakdown region. These diodes have lower Zener (breakdown) voltages, so that they can achieve the breakdown mode without melting. Unlike other diodes, these have very specific breakdown voltages, typically between 2 and 200 volts. See also Zener diodes
Zener diode symbol.svg


A diode that is build to use the capacity in dependance of the cross voltage. Although they rectify, they will be used in tuning circuits as a replacement of manual operated variable capacitors. They permit the use of electronic equipment to be controlled, this permits a phase-locked loop and other circuits which needs stability and electronic control. Semiconductor diodes begin conducting electricity under certain conditions.

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A transistor is a solid state device made by joining three positive-type and negative-type semiconductors together. In general, all transistors have three pins: base, collector, and emitter. Transistor is a bi-polar device that is a transistor with two junctions namely BE and CE DE EE FE. In theory we take a specified formulae incorporate this with using any type of meter in figuring the mathematical solution.

Electronic component transistors.jpg


A lightly doped region called base is sandwiched between two regions called the emitter and collector respectively. The collector handles large quantities of current, hence its dopant concentration is the highest. The emitter’s dopant concentration is slightly lesser, but its area is larger to provide for more current than the collector. The collector region should be heavily doped because electron-hole pairs recombine in that region, while the emitter is not such a region. We can have two varieties in this kind of transistor.

NPN Transistor[edit]

An NPN transistor is made by joining one positive-type semiconductor in between two negative-type semiconductors. Here a lightly doped p-type semiconductor (semiconductor with more holes than electrons) is sandwiched between two well-doped n-type regions. It is like two pn-junctions facing away. An IEEE symbol for the NPN transistor is shown here. The arrow between the base and emitter is in the same direction as current flowing between the base-emitter junction. Power dissipated in the transistor is


BJT symbol NPN.svg

PNP Transistor[edit]

A PNP transistor is made by sandwiching a negative-type semiconductor in between two positive-type semiconductors.


BJT symbol PNP.svg

Transistor Operation[edit]


A transistor conducts current when the base voltage is greater than BE junction’s voltage. Current is non zero.


A transistor conducts current when the base voltage is greater than BE junction’s voltage. Current is non zero. This corresponds to a closed switch. A transistor does not conduct current when the base voltage is less than BE junction’s voltage. Current is zero. This correspond to an open switch.

External links[edit]

Field Effect Transistor[edit]

The most common transistors today are FETs (Field Effect Transistor). These transistors are characterized as having a conductance between source and drain dependent on the voltage applied between the gate and the source terminals. The dependence is linear if the gate to drain voltage is also high along with the gate to source voltage. It turns into a square-law relationship if the gate to drain voltage is not enough.

Current Voltage Characteristics[edit]


One of the issues that comes up in circuit design is that as chips get smaller the insulator gets thinner and it starts to look like Swiss cheese. As a result the insulator starts acting like a conductor. This is known as leakage current. One solution is to replace the insulator by a material with a higher dielectric coefficient.

Two types: enhancement and depletion. Enhancement is the standard MOSFET, in which a channel must be induced by applying voltage. Depletion MOSFETs have the channel implanted, and applying voltage causes the channel to cease being conductive.

FET transistors respond to the difference in voltage bias between the gate and the source.

MOSFET (Metal-Oxide-Semiconductor FET): standard FET

JFET (Junction Fet): When voltage is applied between the source and drain current flows. Current only stops flowing when a voltage is applied to the gate.

MESFET (MEtal-Semiconductor FET): p-n junction is replaced with Scottky junction. Not made with Silicon.

HEMT (High Electron Mobility Transfer): A MESFET

PHEMT (Pseudomorphic HEMT):

Complementary Metal Oxide Semiconductor[edit]

CMOS , Complementary Metal Oxide Semiconductor is not a type of transistor. It is a logic family, based on MOS transistors.

Construction & Operation[edit]

CMOS is made of two FETs blocking the positive and negative voltages. Since only one FET can be on at a time, CMOS consumes negligible power during any of the logic states. But when a transition between states occurs, power is consumed by the device. This power consumed is of two types.

Short-circuit power

For a very short duration, both transistors are on and a very huge current flows through the device for that duration. This current accounts for about 10% of the total power consumed by the CMOS.

Dynamic power

This is due to charge stored on the parasitic capacitance of the output node of the device. This parasitic capacitance depends on the wire’s area, and closeness to other layers of metal in the IC, besides the relative permittivity of the quartz layer separating consecutive metal layers. It also depends (to a much smaller extent) upon the input capacitance of the next logic gate. This capacitance delays the rise in the output voltage and hence the rise or fall in the output of a gate is more like a that in a resistor-capacitor (RC) network. Thus the dynamic power consumed due to switching action in one gate is given by:

Pd=CVd2f{displaystyle P_{d}=CV_{d}^{2}f}

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Circuit Models for Amplifiers[edit]

Amplifier are generally put in four categories

  1. voltage amplifier,
  2. current amplifier,
  3. transresistance amplifier and
  4. transconductance amplifier.

These models apply irrespective of the complexity of the internal circuit of the amplifier. The values of the model parameters can be found either by analyzing the amplifier circuit or by performing measurements at the amplifier temlinals.

The model for a voltage amplifier is shown in figure 1. Real amplifiers have input and output resistance. This is reflected in the model.

Amplifier model.svg

Figure 1: A Voltage Amplifier.

Gain is the increase in the strength of a signal and is often expressed in decibels (dB). An increase of 3 dB is about equal to doubling in a linear scale. A gain of more than 1 is called amplification, while a gain of less than 1 is called Attenuation.

Gain is given different symbols depending of the type. For No load gains

Voltage gain is Avo,
Current gain Aio,
Transconductance Gm
Transresistance Rm.

Using the model, the gain with a load can be calculated.

Transistor amplifiers[edit]

Common Emitter[edit]

Common emitter amplifier.svg


  • Current Gain: ….. HIGH
  • Voltage Gain: ….. HIGH
  • Power Gain: ….. HIGH
  • Input Impedance: … AVERAGE
  • Output Impedance:… AVERAGE

Input Resistance(base): Zb=β×re'
-> β: Current Gain (Ic/Ib), where 'Ic' is Colector DC current and 'Ib' is DC Base current;
-> re': Base-Emitter dynamic resistor (Ut/Ie), where Ut is thermal voltage(≈25mV at 25°C) and
'Ie' is DC emitter current;

Input Resistance(general): Zg= Zb || R1 || R2, where R1 and R2 are the same as the picture above.

Common Collector[edit]

Common collector amplifier.svg


Current Gain: ..... HIGH
Voltage Gain: ..... ≈1
Power Gain:   ..... LOW
Input Resistance: ... HIGH
Output Resistance:... LOW

Common Base[edit]

Common base amplifier.svg


Current Gain: ..... ≈1
Voltage Gain: ..... HIGH
Power Gain:   ..... AVERAGE
Input Resistance: ... LOW
Output Resistance:... HIGH

FET Configurations[edit]

As with BJT configurations, there are three FET configurations, each one corresponding to one of the terminals of the transistor.

Common Source[edit]

Common source.png

Common Drain[edit]

Common drain.png

Common Gate[edit]

Common gate.png

Biased Voltage Class[edit]

Transistors may be biased in a variety of classes. A trade off of linearity and power consumption is usually made where a Class A

Class A[edit]

The transistor is “on” all the time. We say 360 degrees of conduction, representing an entire period of the sine waveform. Ideally, this class produces very little distortion, however consumes a lot of power and is also least preferred.

This is the most linear of the classes, meaning the output signal is a truer representation of what was imputed. Here are the characteristics of the class:
1. The output device (transistor) conducts electricity for the entire cycle of input signal. In other words, they reproduce the entire waveform in its entirety.
2. These amps run hot, as the transistors in the power amp are on and running at full power all the time.
3. There is no condition where the transistor(s) is/are turned off. That doesn’t mean that the amplifier is never or can never be turned off; it means the transistors doing the work inside the amplifier have a constant flow of electricity through them. This constant signal is called “bias”.
4. Class A is the most inefficient of all power amplifier designs, averaging only around 20%.

Because of the way they are usually designed, Class A amplifiers are very inefficient. They do not need to be built in this way, but for every watt of output power, they can typically waste 4-5 watts as heat. They are usually very large, heavy and because of the 4-5 watts of heat energy released per watt of output, they run very hot, needing lots of ventilation (not at all ideal for a car, and rarely acceptable in a home). This is not due to the amplifier type, but the fact that even many design engineers do not fully understand how they work and often copy their designs from previous ones. The upside is that these amps are the most enjoyed of all amplifiers. When properly designed, the Class A amp gives the best representation of musical detail, with no clipping of the waveform. As a result the sound is cleaner and more linear; that is, it contains much lower levels of distortion.

They are the most accurate of all amps available, but at greater cost to manufacture, calling for tight tolerances and additional components for cooling and heat regulation.

Class AB[edit]

The transistor is “on” for slightly more than half the cycle (>180 degrees) of a sine wave and is the most common configuration used in push-pull audio power amplifiers. In push-pull amplifiers, Class AB produces mostly odd order distortion, however it is far more power efficient than Class A. Odd order distortion is not considered pleasing to hear in audio power amplifiers. This distortion can easily be removed with the addition of a simple negative feedback loop into the system as shown by the diagram below:

Class AB Amp

This type of amplifier is extremely easy to build and is the industry standard for audio amplifiers.

Issues with this type of amplifier include poor efficiency, size and cost. A typical class ab amplifier will have a power efficiency of 40-80%. Because of this they require large heat sinks to cool the transistors, this also increases the cost of the amplifier due to the extra material to create these heat sinks.

This is the compromise of the bunch. Class AB operation has some of the best advantages of both Class A and Class B built-in. Its main benefits are sound quality comparable to that of Class A and efficiency similar to that of Class B. Most modern amp designs employ this topology.

Its main characteristics are:
In fact, many Class AB amps operate in Class A at lower output levels, again giving the best of both worlds
The output bias is set so that current flows in a specific output device for more than a half the signal cycle but less than the entire cycle.
There is enough current flowing through each device to keep it operating so they respond instantly to input voltage demands.
In the push-pull output stage, there is some overlap as each output device assists the other during the short transition, or crossover period from the positive to the negative half of the signal.

There are many implementations of the Class AB design. A benefit is that the inherent non-linearity of Class B designs is almost totally eliminated, while avoiding the heat-generating and wasteful inefficiencies of the Class A design. And as stated before, at some output levels, Class AB amps operate in Class A. It is this combination of good efficiency (around 50) with excellent linearity that makes class AB the most popular audio amplifier design.

There are quite a few excellent Class AB amps available. This is the design I recommended for most general-use applications in home and car. Usually, parts choice rivals that of Class A amps, and dollar for dollar these are some of the best values in stereo amplification. There can be some variation in design principle, but generally these are well-designed amps since their function is very well-understood by audio designers.

Class B[edit]

The transistor is “on” for only half the cycle (exactly 180 degrees) of a sine wave and is also very typically used in push-pull amplifier circuits. Ideally this class produces mostly odd order distortion. In audio applications it is believed that odd order distortion is not pleasing to hear. It is difficult to build a low distortion Class B amplifier and hence Class AB is almost universal.

In this amp, the positive and negative halves of the signal are dealt with by different parts of the circuit. The output devices continually switch on and off. Class B operation has the following characteristics:
The input signal has to be a lot larger in order to drive the transistor appropriately.
This is almost the opposite of Class A operation
There have to be at least two output devices with this type of amp. This output stage employs two output devices so that each side amplifies each half of the waveform. [li Either both output devices are never allowed to be on at the same time, or the bias (remember, that trickle of electricity?) for each device is set so that current flow in one output device is zero when not presented with an input signal.
Each output device is on for exactly one half of a complete signal cycle.

These amps run cooler than Class A amps, but the sound quality is not as pure, as there is a lot of “crossover” distortion, as one output device turns off and the other turns on over each signal cycle.

This type of amplifier design, or topology, gives us the term “push-pull,” as this describes the tandem of output devices that deliver the audio signal to your speakers: one device pushes the signal, the other pulls the signal. They can be less expensive, because one can use two cheap output devices instead of one high-quality one in the design.

As I mentioned before, the input signal has to be lot larger, meaning that from the amplifier input, it needs to be “stepped up” in a gain stage, so that the signal will allow the output transistors to operate more efficiently within their designed specifications. This means more circuitry in the path of your signal, degrading sound even before it gets to the output stage

Class C[edit]

The transistor is “on” less than half the cycle of a sine wave. We say <180 of conduction. This class produces both even and odd order distortion, however is very efficient.

Class D[edit]

The class D amp has been developed after the short-comings of past generations, including classes A, B, AB, and C. Many people mistake the D as standing for digital. Although it is a “switching” amp, meaning it turns “on” and “off” at a specific frequency, it is a wrong assumption. D was simply the next letter in the alphabet. Consuming the least power out of its previous generations, the class D amps are generally smaller, making them ideal for mobile devices. It is because of their power efficiency, small size, and cheaper costs that the class D amps are quickly becoming the new industry standard for audio electronic. Companies such as Advanced Analog, Texas Instruments as well as other companies have released 50W stereo class d amplifiers that are the size of a penny and did not require any sort of heat sinking, something that was not possible with other types of amplifiers.

class d amplifier

The basic design includes two MOSFET transistors in series, one pFET and one nFET being driven by a pulse width modulated (PWM) signal. Because of the properties of MOSFET transistors they are either fully on or fully off. When the transistor is off and the current is zero (so the amount of power wasted heating up the transistor is zero), or the transistor is fully on and the voltage across it is very close to zero (so the amount of power wasted heating up the transistor is again, very close to zero).

Because an analog signal needs to be transformed into a PWM signal a certain amount of distortion can occur, but the amount of distortion can be minimized. Because a PWM signal is very much like a digital signal, the sampling theorem states that if the sampling frequency is more than half the maximum frequency of the source it can be reproduced exactly. For audio signals the maximum frequency heard by humans is roughly 20kHz, so a PWM generator would only need to provide a minimum switching frequency of 40kHz. Because of the availability of faster components many class d amplifier designers will use switching frequencies closer to 400kHz to further reduce the distortion.

Issues of concern with a class d amplifier include electromagnetic emissions. Due to the presence of a medium frequency signal in the circuit, steps must be taken to reduce the emission of these signals that could interfere with other electronic devices.

==== Class E ==== (oops, class D again?)
Switching amplifier
These amplifiers are erroneously called “digital” amplifiers by the press and many audio “experts.” Here’s the skinny on Class D:
While some Class D amps do run in true digital mode, using coherent binary data, most do not.
They are better termed “switching” amplifiers, because here the output devices are rapidly switched on and off at least twice for each cycle.
Depending on their switching frequency, they may be “switched on” or “off” millions of times a second.
Class D operation is theoretically 100% efficient, but in practice, they are closer to 80-90% efficiency.
This efficiency gain is at the cost of high-fidelity.

Think of Class D amps as being similar to a switchable power supply, but with audio signals controlling, or modulating, the switching action. To do this, you use a technology called Pulse Width Modulation (or PWM, a technology found in many CD players).

According to experts, audio signals can be used to modulate a PWM system to create a high power audio amplifier at fairly low voltages using very small components. Class D audio uses a fixed, high frequency signal having pulses that vary in width based on input signal amplitude. So, for example, a deep bass note creates a large pulse in the carrier signal. This can be translated into a musical signal by the on/off nature of the output devices.

Class D amplifiers are generally used for non-high-fidelity, or subwoofer applications.

There is a fifth (and, nominally, a sixth) class of amplifier, but they are rarely seen in practice in the consumer market. One is the Class G and the other Class H. These are similar in design to Class AB topologies, but both feature two power supplies that switch on or off, depending on the musical signal imputed. Using two power supplies improves efficiency enough to allow significantly more power for a given size and weight. Class G is becoming common for pro audio designs. Class H amps are designed to use the same topology as Class G, but it provides just enough voltage for optimum operation of the output devices. Again, its an attempt to increase efficiency, but at the expense of fidelity ultimately.

Class F[edit]

Class S[edit]


Electronic amplifier.svg

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Op-Amp (operational amplifier)[edit]

Op-amp stands for operational amplifier. It is available in IC (Integrated Circuit) chip. It is an electronic components already connected and packaged inside a chip of many pins for external connection. Originally, op-amps were so named because they were used to model the basic mathematical operations of addition, subtraction, integration, differentiation, etc. in electronic analog computers. In this sense a true operational amplifier is an ideal circuit element.

741 Op-amp[edit]


The 741 op-amp has a symbol as shown.


Its terminals are:

  • V+: noninverting input
  • V: inverting input
  • Vout: output
  • VS+: positive power supply
  • VS−: negative power supply


The 741 op-amp can be thought as Universal Voltage Difference Amplifier. The main function of the 741 op-amp is to amplify the difference of two input voltages which can be expressed mathematically like below


It can be shown that an op-amp can function as a noninverting voltage amplifier or inverting voltage amplifier.

Also, it can be shown that an op-amp can function as a voltage comparator

Vo = VS+ .