Understanding Thevenin Equivalent: Why Zeq = 0

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Discussion Overview

The discussion revolves around understanding the Thevenin equivalent circuit, specifically addressing why the equivalent impedance (Zeq) is considered to be zero in certain conditions. Participants explore the implications of short-circuiting voltage sources and the behavior of parallel elements in the circuit.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant expresses confusion about why Zeq equals zero, noting the voltage drop across parallel elements and questioning the impact of shutting off a voltage source.
  • Another participant outlines the steps for calculating Thevenin equivalent circuits, emphasizing the need for both voltage and current equations, and mentions the process of short-circuiting voltage sources and open-circuiting current sources.
  • Several participants ask about the representation of a specific circuit element, identified as a current source.
  • A participant suggests that shorting the voltage source effectively shuts off parallel elements, leading to a zero equivalent impedance.
  • Another participant provides a mathematical approach to calculating total resistance in a circuit with multiple elements, concluding that the total resistance is zero due to the presence of a short circuit.
  • One participant questions whether the analysis treats the entire circuit as a voltage source or if it is determining the Thevenin impedance of a voltage source in parallel with a current source.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the concept of equivalent impedance, with some agreeing on the implications of short-circuiting voltage sources while others seek clarification on the overall approach to the circuit analysis. No consensus is reached on the interpretation of the equivalent impedance.

Contextual Notes

Participants discuss the implications of short-circuiting voltage sources and the behavior of parallel elements, but there are unresolved assumptions regarding the specific configurations and definitions of the circuit elements involved.

magnifik
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For the circuit below, can someone please help me understand why Zeq = 0 (in words...not by solving):
jt6jw4.png


I know Vth = 50<0° since this is the voltage drop across the parallel elements. I don't understand why the equivalent impedance would be 0. I know when you shut off a voltage source, elements in parallel with it also go away. does this have anything to do with it?
 
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http://en.wikipedia.org/wiki/Th%C3%A9venin%27s_theorem"

To calculate the equivalent circuit, the resistance and voltage are needed, so two equations are required. These two equations are usually obtained by using the following steps, but any conditions placed on the terminals of the circuit should also work:

1. Calculate the output voltage, VAB, when in open circuit condition (no load resistor—meaning infinite resistance). This is VTh.
2. Calculate the output current, IAB, when the output terminals are short circuited (load resistance is 0). RTh equals VTh divided by this IAB.

The equivalent circuit is a voltage source with voltage VTh in series with a resistance RTh.

Step 2 could also be thought of as:

2a. Replace voltage sources with short circuits, and current sources with open circuits.
2b. Calculate the resistance between terminals A and B. This is RTh.

So you know the Thevenin Voltage already. In step two you can short all voltage sources, open all current sources (as per step 2a.) and then comment on the resistance of the remaining circuit.
 
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What is the element represented by a circle with an arrow in it?
 
What is the element represented by a circle with an arrow in it?
 
NascentOxygen said:
What is the element represented by a circle with an arrow in it?

it's a current source
 
Zryn said:
http://en.wikipedia.org/wiki/Th%C3%A9venin%27s_theorem"



So you know the Thevenin Voltage already. In step two you can short all voltage sources, open all current sources (as per step 2a.) and then comment on the resistance of the remaining circuit.

so is it because when you short the voltage source the elements in parallel are shut off, too?
 
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It's only a matter of calculating the parallel resistance as per normal:

1/R(t) = 1 / R(short) + 1 / R(open) + 1 / R(C) + 1 / R(L) + 1 / R(R)

R(t) = 1 / [1 / 0 + 1 / inf + 1 / -j10 + 1 / j20 + 1 / 30]

R(t) = 1 / [(1 + 0 + 0 + 0 + 0)/0] (put all 5 fractions over a common denominator)

R(t) = 1 / [1 / 0]

R(t) = 1 * [0 / 1]

R(t) = 0

You could have just 'seen' that by knowing that the short circuit from the voltage source will bypass all the other elements in the circuit, since current will follow the path of least resistance and split down parallel paths in inverse proportionality to the magnitude of the resistance of each path. I guess 'shut off' is correct, but you could word it better :smile:.
 
Are we treating this whole 5 element thing as a voltage source? So we seek the equivalent impedance as seen between the top rail and the bottom rail?

Or are we determining the thevenin impedance of a voltage source comprising an ideal voltage source in parallel with a current source?

(Please don't say it doesn't matter. I can see that! I'd still like to know the question before I state the answer. :smile: )
 

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