Teleki Electronics
Op Amp circuits

Transfer function derivation of some circuits.

Writing down the nodal equations of various Operational amplifier circuits, and then deriving the output, seems to be a bit quicker than fumbling around with currents . Did all these in part of one morning. The 'output current being independant of load' proof, for some reason wasn't able to do whilst at University (Keele, UK: Electronics, no longer a mainstream subject here, think !). Also have had to leave the calculations in their original form, as it really is too much trouble to try to convert it all into HTML Some of these you will find in textbooks, with the author completely omitting how the calculation is done. One current textbook, specifically for Op-Amps, was found to be riddled with stupid mistakes. It won't be mentioned, to save further embarrassing the Authors, who should have done a better job of proof-reading their work. In most feedback configurations, both inputs will be driven to the same potential (Virtual Earth). Va is the reference voltage used in most of these examples. Its elegant, the way various terms cancel out, (especially the 1st and 2nd order Group Delay equalisers), to leave a fairly simple equation.

The first two are the standard inverting and non-inverting configurations.
Inverting Configuration

Inverting Op Amp
Inverting Proof

Non-Inverting Configuration

Non Inverting Op Amp
Non Inverting Proof

Differential Amp

Differential Op Amp
Differential Op Amp Proof

Proof that IL is independant of load Z. Question of class test in part of Electronics Degree.

IL independant of Z
IL independant of Z Proof

Transfer function of First Order Group Delay Equaliser.
This and the next, use complex s frequency operator. This particular one is a complete proof, with rationalising and taking the modulus of the complex number terms.

1st order Delay Equaliser
1st order Delay Equaliser proof

Transfer function of Second Order Group Delay Equaliser.

Second order Delay Equaliser
Second order Delay Equaliser Proof
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To do this analysis, assume that there is zero voltage difference between the two inputs, and that the inputs take in no current.

Most Op-Amps can nowadays be assumed to have this ideal behaviour, up to a certain frequency.