Output impedance

The output impedance, source impedance, or internal impedance of an electronic device is the opposition exhibited by its output terminals to the flow of an alternating current (AC) of a particular frequency as a result of resistance, inductance and capacitance. It is the Thévenin equivalent impedance looking back into the output terminals.

In the case of a nonlinear device, such as a transistor, the term "output impedance" usually refers to the effect upon a small amplitude signal, and will vary with the bias point of the transistor, that is, with the DC current and voltage applied to the device.

The small-signal impedance at DC (frequency of 0) is the same as the resistive component of the impedance and is termed output resistance.

It is important to realize that no real device (battery, generator, amplifier) is a perfect source; all have an internal impedance, though this may have little practical effect, depending on the circuit and the load.

Depending on perspective, this impedance can be modeled as being in series with a perfect voltage source, or in parallel with a perfect current source (see: Thevenin's theorem, Norton's theorem, Series and parallel circuits). Both models are equivalent, and one may choose whichever model is most convenient for analysis.

For example, a preamplifier with 100Ω output impedance means the output voltage signal appears to be in series with a 100Ω resistor.

Measurement

It can more accurately be described by keeping track of the voltage vs current curves for various loads, and calculating the resistance from Ohm's law. (The internal resistance may not be the same for different types of loading or at different frequencies, especially in devices like chemical batteries.)

The generalized source impedance for a reactive (inductive or capacitive) source device is more complicated to determine, and is usually measured with specialized instruments, rather than taking many measurements by hand.

Audio amplifiers

The real output impedance (Z_source) of a power amplifier is usually less than 0.1Ω, but this is rarely specified. Instead it is "hidden" within the damping factor parameter, which is:

:$DF\; =\; \backslash frac\{Z\_\backslash mathrm\{load\}\}\{Z\_\backslash mathrm\{source\}\}$

Solving for Z_source,

:$Z\_\backslash mathrm\{source\}\; =\; \backslash frac\{Z\_\backslash mathrm\{load\}\}\{DF\}$

gives the small source impedance (output impedance) of the power amplifier. This can be calculated from the Z_load of the loudspeaker (typically 2, 4, or 8 ohms) and the given value of the damping factor.

Generally in audio and hifi, the input impedance of components is several times (technically, more than 10) the output impedance of the device connected to them. This is called impedance bridging or voltage bridging.

In this case, Z_load>> Z_source, DF > 10

In video, RF, and other systems, impedances of inputs and outputs are the same. This is called impedance matching or a matched connection.

In this case, Z_source = Z_load, DF = 1/1 = 1

The actual output impedance for most devices is not the same as the rated output impedance. A power amplifier may have a rated impedance of 8 ohms, but the actual output impedance will vary depending on circuit conditions. The rated output impedance is simply that impedance into which the amplifier can deliver its maximum amount of power without failing.

Batteries

$R\_B=\backslash left(\; \backslash frac\{Vs\}\{I\}\; \backslash right)-R\_L$

or

$R\_B=\backslash left(\; \backslash frac\{V\_S-V\}\{I\}\; \backslash right)$

where

$R\_B$ is the internal resistance of the battery

$V\_S$ is the battery voltage without a load

$V$ is the battery voltage with a load

$R\_L$ is the total resistance of the circuit

$I$ is the total current supplied by the battery

Internal resistance varies with the age of a battery, but for most commercial batteries the internal resistance is on the order of 1 ohm.

When a current is flowing through a cell, the measured e.m.f. is lower than when there is no current delivered by the cell. The reason for this is that part of the available energy of the cell is used up to drive charges through the cell. This energy wasted by the so-called "internal resistance" of that cell. This wasted energy shows up as lost voltage. Internal resistance, r=(E-V)/I

See also

External links

Category:Electronics terms