Estimating the upper 3dB cutoff in a MOSFET amplifier

AI Thread Summary
The discussion focuses on estimating the upper 3dB cutoff frequency in a MOSFET amplifier using the open circuit time constant method. The user is confused about the transition from one circuit diagram to another, particularly regarding the grounding of the drain of Q2 and the combination of gate-source capacitors. Clarification is sought on the simplification process, specifically when it is permissible to remove connections between nodes that are at the same potential. The conversation also touches on calculating equivalent resistances and time constants, with the user struggling to reconcile their findings with the expected results. Overall, the thread emphasizes the importance of understanding circuit simplification techniques in analyzing MOSFET amplifiers.
Forcefedglas
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Homework Statement
fUH2nU7.png

I've found the gain, but now I need to estimate the upper cutoff frequency with the open circuit time constant method, so the upper 3dB cutoff would roughly be $$\sum_{i = 1}^{n} \frac{1}{\tau_i}$$

The attempt at a solution
I'm currently trying to make sense of the given solutions:
1xSwCpR.png
IDhXnex.png


I got something similar to the first picture after drawing out the small signal equivalent, but I'm completely lost as to how they went from that circuit to the one in the second picture. Why does the drain of Q2 suddenly become grounded, and how did the GS capacitors combine and turn into half of their original value? I've tried searching around but haven't found any explanations of the simplification method used here.

I attempted to use a 1v test voltage at the gate source capacitors (in the first circuit) to find the equivalent resistance seen by them but that yielded a different answer to what I get if I work it out via the second circuit.

Any help/tips would be greatly appreciated, thanks.
 
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It might help to split apart (graphically) some of the ground connection in order to visually isolate in the input and output portions of the circuit. So starting with their first picture and breaking up the ground connections at the drain of Q1 and the gate of Q2:
upload_2016-9-27_7-30-33.png
 
gneill said:
It might help to split apart (graphically) some of the ground connection in order to visually isolate in the input and output portions of the circuit. So starting with their first picture and breaking up the ground connections at the drain of Q1 and the gate of Q2:
View attachment 106562

Ah ok, so the equivalent capacitances (and the voltages across them) combine and since Vgs2=-Vgs1, the current sources are equivalent and one can be removed? So whenever there's a wire connecting two portions of a node like this, can you always just remove it and proceed to simplify the circuit? I guess I'm slightly confused as to what happens to the s1-s2 wire and in what situations I can effectively remove it.

I have one more question, the equivalent resistance seen by 1/2Cgs is Rsig=20k, so the time constant is 20nS. Shouldn't I be able to get the same answer if I insert a test voltage of 1V and sum the equivalent resistances seen by Cgs1 and Cgs2 on the first circuit diagram? When I try to do it however, I get this for the equivalent resistance seen by Cgs1 (other capacitors opened, 1v test voltage where Cgs1 is):
NHFwXKy.png

Which can't be correct as the time constant will already be larger than 20nS from Cgs1 alone. I calculated the equivalent resistance for Cgs2 as 100 ohms, so theoretically Req seen by Cgs1 should be 9.9k, however I've stared at this for hours and couldn't find any errors.
 
Last edited:
Forcefedglas said:
Ah ok, so the equivalent capacitances (and the voltages across them) combine and since Vgs2=-Vgs1, the current sources are equivalent and one can be removed?
More precisely, one is redundant since they are both producing the same current in the same direction.
So whenever there's a wire connecting two portions of a node like this, can you always just remove it and proceed to simplify the circuit?

I guess I'm slightly confused as to what happens to the s1-s2 wire and in what situations I can effectively remove it.

Usually the argument goes that if two nodes are at the same potential then connecting them with a wire will make no change in circuit operation (as no current will flow through that wire and no potentials will change as a result). Here there's an existing wire and the argument is reversed: removing the wire will not change the potentials at the nodes since Vgs1 = Vgs2.

I'll have to think about your test voltage setup.
 
gneill said:
More precisely, one is redundant since they are both producing the same current in the same direction.Usually the argument goes that if two nodes are at the same potential then connecting them with a wire will make no change in circuit operation (as no current will flow through that wire and no potentials will change as a result). Here there's an existing wire and the argument is reversed: removing the wire will not change the potentials at the nodes since Vgs1 = Vgs2.

I'll have to think about your test voltage setup.

Thanks that clears up a lot, strange that I never specifically heard about this in any of my introductory circuit courses but it makes sense now.
 
Forcefedglas said:
Thanks that clears up a lot, strange that I never specifically heard about this in any of my introductory circuit courses but it makes sense now.
You may have seen it used when simplifying highly symmetric resistance or capacitance networks. It's often seen as a simplification "trick" in puzzle or challenge type questions.
 

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