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{{Cleanup|date=March 2009}}
'''Small-signal modeling''' is a common analysis technique in [[electrical engineering]] which is used to approximate the behavior of [[nonlinear device]]s with [[linear equations]]. This linearization is formed about the [[Direct current|DC]] [[biasing|bias]] point of the device (that is, the [[voltage]]/[[Electric current|current]] levels present when no signal is applied), and can be accurate for small excursions about this point.
 
==Motivation ==
 
Many electronic circuits, such as [[radio receiver]]s, communications, and [[signal processing]] circuits,  generally carry small time-varying ([[alternating current|AC]]) signals on top of a constant ([[direct current|DC]]) [[bias (electrical engineering)|bias]]. This suggests using a method akin to approximation by [[finite differences|finite difference method]] to analyze relatively small perturbations about the [[bias point]].
 
Any nonlinear device which can be described quantitatively using a formula can then be 'linearized' about a bias point by taking partial derivatives of the formula with respect to all governing variables. These partial derivatives can be associated with physical quantities (such as [[capacitance]], [[electrical resistance|resistance]] and [[inductance]]), and a circuit diagram relating them can be formulated.
Small-signal models exist for [[electron tube]]s, [[diode]]s, [[field-effect transistor]]s (FET) and [[Bipolar junction transistor|bipolar transistors]], notably the [[hybrid-pi model]] and various [[two-port network]].
 
==Variable notation==
 
* Large-signal DC quantities are denoted by uppercase letters with uppercase subscripts. For example, the DC input bias voltage of a transistor would be denoted <math>V_\mathrm{IN}</math>.
 
* Small-signal quantities are denoted using lowercase letters with lowercase subscripts. For example, the input signal of a transistor would be denoted as <math>v_\mathrm{in}</math>.
 
* Total quantities, combining both small-signal and large-signal quantities, are denoted using lower case letters and uppercase subscripts. For example, the total input voltage to the aforementioned transistor would be <math>v_\mathrm{IN}(t)=V_\mathrm{IN}+v_\mathrm{in}(t)</math>.
 
==Example: PN junction diodes==
{{main|Diode modelling#Small-signal modelling}}
 
The (large-signal) Shockley equation for a diode can be linearized about the bias point or quiescent point (sometimes called [[Q-point]]) to find the small-signal [[Electrical conductance|conductance]], capacitance and resistance of the diode. This procedure is described in more detail under [[diode modelling#Small-signal modeling|diode modeling]], which provides an example of the linearization procedure followed in all small-signal models of semiconductor devices.
 
==Differences between small signal and large signal==
 
A large signal is a DC signal (or an AC signal at a point in time) (one or more orders of magnitude larger than the small signal) used to analyse a circuit containing non-linear components and calculate an operating point (bias) of these components.
 
A small signal is an AC signal superimposed on a circuit containing a large signal.
 
In analysis of the small signal's contribution to the circuit, the non-linear components are modeled as linear components.
 
==See also==
*[[Diode modelling]]
*[[Hybrid-pi model]]
*[[Early effect]]
*[[SPICE]] - Simulation Program with Integrated Circuit Emphasis, a general purpose analog electronic circuit simulator capable of solving small signal models.
 
==References==
{{reflist}}
 
[[Category:Electronic device modeling]]

Revision as of 06:59, 13 December 2013

Template:Cleanup Small-signal modeling is a common analysis technique in electrical engineering which is used to approximate the behavior of nonlinear devices with linear equations. This linearization is formed about the DC bias point of the device (that is, the voltage/current levels present when no signal is applied), and can be accurate for small excursions about this point.

Motivation

Many electronic circuits, such as radio receivers, communications, and signal processing circuits, generally carry small time-varying (AC) signals on top of a constant (DC) bias. This suggests using a method akin to approximation by finite difference method to analyze relatively small perturbations about the bias point.

Any nonlinear device which can be described quantitatively using a formula can then be 'linearized' about a bias point by taking partial derivatives of the formula with respect to all governing variables. These partial derivatives can be associated with physical quantities (such as capacitance, resistance and inductance), and a circuit diagram relating them can be formulated. Small-signal models exist for electron tubes, diodes, field-effect transistors (FET) and bipolar transistors, notably the hybrid-pi model and various two-port network.

Variable notation

Example: PN junction diodes

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The (large-signal) Shockley equation for a diode can be linearized about the bias point or quiescent point (sometimes called Q-point) to find the small-signal conductance, capacitance and resistance of the diode. This procedure is described in more detail under diode modeling, which provides an example of the linearization procedure followed in all small-signal models of semiconductor devices.

Differences between small signal and large signal

A large signal is a DC signal (or an AC signal at a point in time) (one or more orders of magnitude larger than the small signal) used to analyse a circuit containing non-linear components and calculate an operating point (bias) of these components.

A small signal is an AC signal superimposed on a circuit containing a large signal.

In analysis of the small signal's contribution to the circuit, the non-linear components are modeled as linear components.

See also

References

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