Open-loop gain: Difference between revisions

Revision as of 21:11, 6 December 2015

Revision as of 21:53, 15 February 2016

Line 10:

where <math>V^+-V^-</math> is the input voltage difference that is being amplified. The dependence on frequency is not displayed here.

== Role in non-ideal gain ==

The open-loop gain is a physical attribute of an operation amplifier that is often finite in comparison to the usual gain, denoted <math>G</math>. While open-loop gain is the gain when there is no feedback in a circuit, an operational amplifier will often be configured to use a feedback configuration such that its gain will be controlled by the feedback circuit components.

Take the case of an inverting operational amplifier configuration. If the resistor between the single output node and the inverting input node is <math>R_2</math> and the resistor between a source voltage and the inverting input node is <math>R_1</math>, then the ideal gain for such a circuit at the output terminal is defined, ideally, to be:

<math>G = - \frac{R_2}{R_1}</math>

However, with the use of open-loop gain, the equation becomes:

<math>G = \frac{- \frac{R_2}{R_1}}{1 + \frac{- \frac{R_2}{R_1}}{A}}</math>

Notice that the equation becomes effective the same for the ideal case as <math>A</math> approaches infinity.

In this manner, the open-loop gain is important for computing the actual gain for a given non-ideal operational amplifier network in situations where the ideal model of an operational amplifier begins to become inaccurate.

== See also ==