Finding Thevenin Equivalent Circuit

Click For Summary

Discussion Overview

The discussion revolves around finding the Thevenin equivalent circuit for a specific circuit problem, focusing on calculating the open-circuit voltage and Thevenin resistance. Participants explore various approaches and reasoning related to circuit analysis, including the application of Kirchhoff's voltage law (KVL) and the behavior of controlled sources.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant outlines the steps to find the open-circuit voltage, suggesting that it can be expressed as \( v_{oc} = (g_mv)R_1 - v_s \).
  • Another participant proposes an alternative expression for \( V_{oc} \) based on the polarity of the controlled current source, indicating \( V_{oc} = V_s - IR \).
  • There is a discussion about the direction of the short circuit current and its impact on the sign of the results, with one participant suggesting a potential error in the defined direction.
  • One participant questions the reasoning behind setting \( v = 0 \) and suggests that it should remain as \( v = -g_mvR_1 \), leading to confusion about the limit as \( v \) approaches zero.
  • Another participant clarifies that the limit of \( R_{Th} \) as \( v \rightarrow 0 \) is necessary for understanding the behavior of the equivalent circuit.
  • One participant concludes that the Thevenin resistance is \( R_{th} = \frac{R_1}{1 + g_mR_1} \) based on their calculations.

Areas of Agreement / Disagreement

Participants express differing views on the calculations and interpretations of the circuit behavior, particularly regarding the open-circuit voltage and the conditions under which certain values are derived. The discussion remains unresolved with multiple competing perspectives on the correct approach.

Contextual Notes

Some participants note potential errors in sign conventions and assumptions about the circuit elements, indicating that the analysis may depend on specific definitions and interpretations of the circuit components.

opticaltempest
Messages
135
Reaction score
0
Hello,

I am working on the following problem:

http://img155.imageshack.us/img155/2478/thevpo9.jpg

I am stuck on this seemingly simple circuit problem. I've worked many Thevenin circuit problems in my introductory circuit analysis. This problem is from a new class and seems different. I realize that I must first find the open-circuit voltage at the terminals. After that I need to the Thevenin equivalent resistance by using

\LARGE R_{Th}=V_{Th}/I_{sc}.

First let me find the open-circuit voltage v_{oc}. Is this correct?

We know the circuit current is g_mv. Thus the open circuit voltage which is the voltage across the voltage-controlled current source is

Using KVL:

\LARGE -v_s+v-v_{oc}=0 \implies v_{oc}=v-v_s

and

\LARGE v=(g_mv)R_1.

So we have

<br /> \LARGE v_{oc} = (g_mv)R_1-v_s \implies<br /> \LARGE v_{oc} = (0.002v)(50k\Omega)-v_s \implies<br /> \LARGE v_{oc} = 100v-v_s<br />

Does this look correct for the open circuit voltage?
 
Last edited by a moderator:
Physics news on Phys.org
V_oc = voltage across controlled current source, and assuming +polarity on the arrow-head end, you then have V_oc = Vs - V = Vs - IR where I is given by -gm V (passive ref scheme)
 
Does this solution look correct? I see where I was wrong while finding the open-circuit voltage.

http://img293.imageshack.us/img293/1340/image0001tv1.jpg

http://img177.imageshack.us/img177/4223/image0002xe6.jpg

http://img210.imageshack.us/img210/9513/image0003zi6.jpg
 
Last edited by a moderator:
judging by the final diagram with + on top and - on bottom at output, your short circuit current may have been defined in the wrong direction, hence leading to an overall -ve sign error.
 
opticaltempest said:
Hello,

I am working on the following problem:

http://img155.imageshack.us/img155/2478/thevpo9.jpg

I am stuck on this seemingly simple circuit problem. I've worked many Thevenin circuit problems in my introductory circuit analysis. This problem is from a new class and seems different. I realize that I must first find the open-circuit voltage at the terminals. After that I need to the Thevenin equivalent resistance by using

\LARGE R_{Th}=V_{Th}/I_{sc}.

First let me find the open-circuit voltage v_{oc}. Is this correct?

We know the circuit current is g_mv. Thus the open circuit voltage which is the voltage across the voltage-controlled current source is

Using KVL:

\LARGE -v_s+v-v_{oc}=0 \implies v_{oc}=v-v_s

and

\LARGE v=(g_mv)R_1.

So we have

<br /> \LARGE v_{oc} = (g_mv)R_1-v_s \implies<br /> \LARGE v_{oc} = (0.002v)(50k\Omega)-v_s \implies<br /> \LARGE v_{oc} = 100v-v_s<br />

Does this look correct for the open circuit voltage?

The current g_mv is entering the minus terminal of v, so you should have v = -g_mvR_1 or v\left[1+g_mR_1]=0 so, v = 0 and v_{oc}=v_s
 
Last edited by a moderator:
CEL said:
or v\left[1+g_mR_1]=0 so, v = 0 and v_{oc}=v_s

How did you get this? Why isn't it

v_{oc}=v_s-v ?

Thanks
 
opticaltempest said:
How did you get this? Why isn't it

v_{oc}=v_s-v ?

Thanks

It is! But since v=0, v_{oc}=v_s-0=v_s.
 
your expression is pretty much correct, all you need is to look at the limit as v->0. basically R_th has to be infinite... such equivalent circuit does not exist in real life, only in the realm of an analysis tool.
 
I'm still confused. Why is v=0 and not left as v=-g_mvR_1?

Why do we need to look at the limit of v as v \rightarrow 0 ?

Correction: limit of R_{Th} as v \rightarrow 0
 
Last edited:
  • #10
opticaltempest said:
I'm still confused. Why is v=0 and not left as v=-g_mvR_1?

Why do we need to look at the limit of v as v \rightarrow 0 ?

Correction: limit of R_{Th} as v \rightarrow 0

You have v in both members of the equation v=-g_mvR_1. So, unless g_mR_1=1, which it is not, you must have v=0.
Short circuiting the output you have i_{sc}=\frac{v_s}{R_1}+g_mv.
Since v=v_s, i_{sc}=\frac{v_s}{R_1}+g_mv_s=v_s\left[\frac{1}{R_1}+g_m\right]
So
R_{th}=\frac{v_{oc}}{i_{sc}}=\frac{1}{\frac{1}{R_1}+g_m}=\frac{R_1}{1+g_mR_1}.
 
  • #11
Thanks CEL and mjsd for all of the help on this problem. It now makes sense. I found out the answer is R=495 ohms and vth=vs. This is definitely the correct answer when I substitute the given values into the problem. Thanks again!
 
  • #12
ok... i shouldn't have said R_th is infinite.. I evaluated the limit incorrectly.. since vs = v,
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 42 ·
2
Replies
42
Views
7K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
0
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
3
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K