Electrical circuit Source transformation Question

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Discussion Overview

The discussion revolves around the transformation of an infinite arrangement of electrical circuits, specifically focusing on converting current sources into voltage sources using source transformation techniques. Participants explore theoretical approaches, including Thevenin and Norton equivalents, and the implications of circuit symmetry and node analysis.

Discussion Character

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

Main Points Raised

  • One participant expresses uncertainty about transforming current sources into voltage sources due to the presence of multiple parallel resistors.
  • Another suggests creating a Thevenin/Norton equivalent of a "repeated group" in the circuit before connecting these equivalents in series or parallel.
  • Some participants discuss the difficulty of predicting the behavior of the circuit towards infinity if there are no repeated groups of current sources.
  • There is mention of a closed loop in the circuit, leading to questions about how it differs from an infinite straight network.
  • One participant proposes using Kirchhoff's current law (KCL) to derive equations for the voltages at various nodes in the circuit.
  • Another participant clarifies that while one can find voltages through equations, they may also need to calculate currents using Ohm's law.
  • There is a discussion about whether the voltages derived from KCL can be substituted as voltage sources in place of the current sources.

Areas of Agreement / Disagreement

Participants express differing views on the feasibility of transforming current sources into voltage sources, with some suggesting it is not possible without defining an output. The discussion remains unresolved regarding the best approach to handle the infinite circuit arrangement and the implications of closed loops versus infinite networks.

Contextual Notes

Participants mention the need for defining outputs and the implications of circuit symmetry, but there are unresolved assumptions regarding the nature of the infinite circuit and the specific configurations of current and voltage sources.

Who May Find This Useful

This discussion may be useful for students or practitioners interested in circuit theory, particularly those exploring source transformations and the application of Thevenin and Norton equivalents in complex circuit arrangements.

  • #31
tim9000 said:
So without any 'clever' use of a trick like some sort of symmetry there is not conventional way to replace current sources with voltage sources,
In #6 I wrote: You cannot convert a current source into a voltage source, but you can convert a Norton equivalent into a Thevenin equivalent.

I've read the whole thread:

In #1 the figure shows types of blocks in series: Type 1 - 2 - 3 - 4 then 1 - 3 ? That's not infinite repeated blocks. How to continue?

You admit that, but then suddenly in #5 the circuit becomes a loop.

The discussion continues with Thevenin/Norton equivalents, but since the circuit now has become a (finite) loop, KVL or KCL will be a more simple solution. Now the dicussion concerns whether KCL or KVL is to be used.

The thread is a mess. You must clearify what is meant.

If you want the circuit in #1 to be of infinite lenght, you must use Thevenin/Norton equivalents in series, then make a mathematical series of voltages, currents, whatever.
 
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  • #32
Hesch said:
In #6 I wrote: You cannot convert a current source into a voltage source, but you can convert a Norton equivalent into a Thevenin equivalent.

I've read the whole thread:

In #1 the figure shows types of blocks in series: Type 1 - 2 - 3 - 4 then 1 - 3 ? That's not infinite repeated blocks. How to continue?

You admit that, but then suddenly in #5 the circuit becomes a loop.

The discussion continues with Thevenin/Norton equivalents, but since the circuit now has become a (finite) loop, KVL or KCL will be a more simple solution. Now the dicussion concerns whether KCL or KVL is to be used.

The thread is a mess. You must clearify what is meant.

If you want the circuit in #1 to be of infinite lenght, you must use Thevenin/Norton equivalents in series, then make a mathematical series of voltages, currents, whatever.
In my last post (#30) I suppose I meant like 'having the source like that with those parallel resistors isn't a norton/thevenin equivalent?'

I sort of was concidering infinite length, but then when that was difficult I realized that a finite length network (in post #5) would be better. Sorry for the lack of clarity.
But I thought the electrician showed that even if we use KCL or KVL for the finite series, the solution (unless numerical) is huge...unusable. So I can't figure out how to redraw it with the sources switched.Thanks
 
  • #33
tim9000 said:
if we use KCL or KVL for the finite series, the solution (unless numerical) is huge...unusable.
Of course you must solve the equations numerically. Manually you will solve the equations within a day, included 11 calculation errors. In #29 the Electrician has shown you a setup as for the coefficients ( I have not checked it ). You will have to enter about 40 coefficients different from 0. Write them in a file and let a program read them from the file. In this way a forgotten minus sign is easy to correct/edit.

The program/computer will solve the equations within 5 seconds with no errors. This is not unusable
 
  • #34
Hesch said:
Of course you must solve the equations numerically. Manually you will solve the equations within a day, included 11 calculation errors. In #29 the Electrician has shown you a setup as for the coefficients ( I have not checked it ). You will have to enter about 40 coefficients different from 0. Write them in a file and let a program read them from the file. In this way a forgotten minus sign is easy to correct/edit.

The program/computer will solve the equations within 5 seconds with no errors. This is not unusable
Yes I see, oh well.
What's the theoretical version of a solution, the word for it, like the opposite of a 'numerical' solution, like if I was able to find a solution that was the equivilant without it being set numbers?

Also one other question, I have is, I've seen an ideal inductor modeled as a resistor in series with a leakage inductance, in series with the ideal inductor. Couldn't I model this as the resistor in series with the ideal and leakage inductors in parallel with each other?

Thanks
 
  • #35
tim9000 said:
What's the theoretical version of a solution, the word for it, like the opposite of a 'numerical' solution, like if I was able to find a solution that was the equivilant without it being set numbers?
Well, you are the one to know, it's your language :smile:.
Even in my language (danish), I hate these "words". The important matter is to know, what I'm doing rather than to know the word.
The opposite of a numerical solution could be an algebraic solution, but "building" equations and solve them numerically are somehow mixed disciplines.
tim9000 said:
I've seen an ideal inductor modeled as a resistor in series with a leakage inductance, in series with the ideal inductor. Couldn't I model this as the resistor in series with the ideal and leakage inductors in parallel with each other?
You should start a new thread here.

As for a known voltage/current supplied ( 60Hz, sinusoidal ): Yes. Maybe you could find the impedance = R + sL = 10Ω + j100Ω
But say you lower the frequency to 0Hz, then the impedance in the series connection will be R + sL = 10Ω + j0Ω = 10Ω.
Now say you by 60Hz have found an equivalent in parallel. Then by lowering the frequency to 0Hz, the impedance will be R || j0Ω = 0Ω.
So generally you cannot convert a model in series to a model in parallel when inductors/capacitors are included in the models.
 
  • #36
tim9000 said:
Yes I see, oh well.
What's the theoretical version of a solution, the word for it, like the opposite of a 'numerical' solution, like if I was able to find a solution that was the equivilant without it being set numbers?
Thanks

It would be called a "symbolic" solution, such as the one in post #22.
 
  • #37
Analytic solution
 
  • #38
The Electrician said:
It would be called a "symbolic" solution, such as the one in post #22.

William White said:
Analytic solution

Ah yes, Analytic was the word I was looking for, was on the tip of my tongue.
 
  • #39
Hesch said:
Well, you are the one to know, it's your language :smile:.
Even in my language (danish), I hate these "words". The important matter is to know, what I'm doing rather than to know the word.
The opposite of a numerical solution could be an algebraic solution, but "building" equations and solve them numerically are somehow mixed disciplines.

You should start a new thread here.

As for a known voltage/current supplied ( 60Hz, sinusoidal ): Yes. Maybe you could find the impedance = R + sL = 10Ω + j100Ω
But say you lower the frequency to 0Hz, then the impedance in the series connection will be R + sL = 10Ω + j0Ω = 10Ω.
Now say you by 60Hz have found an equivalent in parallel. Then by lowering the frequency to 0Hz, the impedance will be R || j0Ω = 0Ω.
So generally you cannot convert a model in series to a model in parallel when inductors/capacitors are included in the models.

Ah-ha, yeah 'analystic' was the word.

Yeah that's not what I meant by what was in parallel, I took your advice and started it as a new thread:
https://www.physicsforums.com/threads/modeling-an-inductor.825613/
 

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