Finding Transfer Function from Circuit

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Discussion Overview

The discussion revolves around finding the transfer function from a circuit schematic involving resistors and a capacitor. Participants explore the implications of including a DC voltage source (V_DD) in the analysis and how it affects the transfer function, particularly in the context of small signal analysis and superposition.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • One participant presents an initial attempt to derive the transfer function using nodal analysis, leading to a complex equation involving Vout and Vin.
  • Another participant argues that Vout cannot be solely expressed as a function of Vin, suggesting that it also depends on V_DD, and proposes a superposition approach to separate the contributions from Vin and V_DD.
  • A later reply questions how to interpret the transfer function when Vout appears on both sides of the equation, particularly in relation to plotting a Bode plot.
  • One participant suggests that the overall transfer function consists of both DC and AC components, indicating a potential misunderstanding of how to derive the transfer function in this context.
  • Another participant clarifies that in small signal analysis, the DC source V_DD establishes bias points and that the varying part of the response can be isolated for transfer function analysis by setting V_DD to zero.
  • Participants discuss the role of capacitors in blocking DC components and how this affects the analysis of the circuit's response.

Areas of Agreement / Disagreement

Participants express differing views on how to derive the transfer function, particularly regarding the role of Vout and V_DD. There is no consensus on a single method for interpreting the transfer function, and multiple approaches are discussed.

Contextual Notes

Limitations include the dependence on the assumptions made during small signal analysis and the treatment of DC and AC components separately. The discussion does not resolve the mathematical steps necessary to derive the transfer function fully.

Mr.Tibbs
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I need to find the transfer function from the attached circuit schematic.

V_DD = 5V; R1 = 200kΩ; R2 = 300kΩ; and C1 = 900nF

I used nodal analysis to attempt to get Vout over Vin but alas ended up with an equation like this:

\frac{Vout}{Vin} = \frac{-j}{120kΩ*ωC} + \frac{5j}{200kΩ*ω*c*Vout}


I've run into a wall on how to derive the equation with V_DD. Any help would be great.
 

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It's not possible to find a transfer function that depends only on Vin :)

Vout is a function of both Vin and Vout and its equation will therefore look like
Vout = A*Vin + B*Vdd
which can be seen immediately if you consider superposition to solve for Vout

Are you doing a small signal analysis?

EDIT:

By using superposition you can consider the portion of Vout caused by Vdd and Vin separately. Then:

Vout = (Vout/Vin)*Vin + (Vout/Vdd)*Vdd

where

Vout/Vin = transfer function due to Vin with Vdd=0
Vout/Vdd = transfer function due to Vdd with Vin=0
 
Last edited:
Yes, at least that's how the question is set up. So if I can't get rid of Vout on the right hand side of the equation how do I interpret the transfer function?

i.e. plotting a bode plot
 
Ok, I think I have it then. So the overall transfer function of the circuit is the addition of the DC and the AC portions of the circuit correct?

(Wording might be a little off)
 
Ah ok. In small signal analysis, the DC Vdd source is only setting up bias points. Because Vdd = constant, in this equation:

Vout = A*Vin + B*Vdd

The B*Vdd term settles to a constant value some short time after the circuit is switched on. We then only consider the remaining portion:

Vout = A*Vin

which you can write a transfer function for. The total result is understood to be the sum of the steady (dc) value supplied by Vdd and the variable part due to Vin.

By superposition, we find Vout=A*Vin by setting the dc sources to zero (ie set Vdd=0).

===So for ac analysis:

1.

Find the DC portion of the response. This is called the bias point. We only consider steady inputs like your Vdd=5 volts in this part. If Vin had a dc component we would consider that dc part *only* as well. Superposition is going to allow us to find the total response by separating this DC part that doesn't change while the circuit is on from the more interesting part in 2 below.

In your circuit, Vin is applied to a series capacitor. This is often done in audio circuits to block the dc component of Vin. In other words, if Vin has a dc component (and it will), it is blocked by that capacitor and will not affect the steady value of Vout determined by Vdd. This is a means to allow the dc bias point of the circuit generating Vin to be set without considering the following circuit.

2.

Find the part of the response that varies. By superpostion, we can set Vdd (and all other steady sources, including the dc portion of Vin) to zero in this part. This means in your circuit you would ground Vdd. Now you can find your transfer function Vout/Vin.It is understood that the total response will be a steady output voltage plus a varying part (Vout/Vin) added to it. In your bode plot, you are only interested in Vout/Vin. The steady part is what keeps the following transistors properly biased in their active regions.
I explained it differently than is normally done in books so I hope I gave a different angle if you didn't pick up on it the other way :)
 
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that's what I was thinking when you mentioned it in your earlier post! (except you had better words. . . and descriptions. . .) that cleared the entire problem up for me!

Thank you very much! :)
 

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