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The op amp as an amplifier

For the op amp to work as a amplifier the difference between the two input voltages V2 and V1 must be less than 150 m. (More generally it must be less than VS/AoV.) This is achieved in different ways by the non-inverting and the inverting voltage amplifiers.

The inverting voltage amplifier

In this use the input is applied to the inverting input and the non- inverting input is earthed (Figure 1). So that the value of (V2 – V1) is less than 150 mV a resistor R1 is placed in the input circuit. Hence V2 is 0 and V1 is less than 150 μV. A resistor R2 forms a feedback loop and since the inverting input is used the feedback is out of phase with the input and is therefore negative feedback.


The maximum value of V1 at P will be 150 m when the output is VS and so we can consider V1 to be virtually zero. P is said to be a virtual earth.


The potential difference across R1 is therefore virtually V and the potential difference across R2 is virtually Vo (but reversed in sign). Since almost no current flows through the op amp, the current (I) in R2 is equal to that in R1 and so we can write:

I = Vi/R1 = - Vo/R2




The voltage gain of the amplifier (A) is known as the closed loop gain and is given by the formula:


Closed loop gain (A) = Vo/Vi = -R2/R1


Example problem
Calculate the closed loop gain of an inverting voltage amplifier with R1 = 3 kΩ and R2 = 1 kΩ.

Closed loop gain (A) = -3/1 = -3.

Notice that this depends only on the values of the two external resistors.

 
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© Keith Gibbs 2013