Electrical Network Problem: Power Transfer

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Homework Help Overview

The discussion revolves around an electrical network problem focused on power transfer, specifically applying the maximum power transfer theorem and superposition theorem in circuit analysis. Participants are exploring how to relate power results from multiple sources and the implications of source interactions in a circuit.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss the efficiency of power transfer and the conditions under which maximum power is dissipated. There are questions about how to handle multiple power results and the correct application of circuit theorems. Some participants express uncertainty about the setup and the implications of acting sources in the circuit.

Discussion Status

The discussion is active with various interpretations being explored regarding the relationships between power, voltage, and resistance. Some participants have offered guidance on using superposition and considering the effects of source suppression, while others are questioning the assumptions and setup of the problem.

Contextual Notes

Participants are navigating constraints such as unknown values for resistances and voltages, as well as the specific conditions under which sources are acting. There is also mention of potential discrepancies in the signs of voltages affecting the overall power calculations.

cnh1995
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Homework Statement


20180923_123000.jpg


Homework Equations


P=V2/R
For maximum power transfer,
Rload=RThevenin

The Attempt at a Solution


I know the efficiency is 50% during maximum power transfer. So when all the sources are acting simultaneously and ( at the same time) R=Rth, maximum power will be dissipated in R.
I am not sure how to use the given values of power since both R and the source voltages are unknown. Plus, the voltage sources are connected across three different ports. This problem is from Circuit Theorems chapter, so I guess I need to use Maximum power transfer theorem along with Superposition theorem.
Any guidance is appreciated.
 

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cnh1995 said:
For maximum power transfer,
Rload=RThevenin
I don't think this is relevant here. That equation says how to adjust the load to get maximum power transfer into it.
Consider that the direction of current might change between the three given power results.
 
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haruspex said:
Consider that the direction of current might change between the three given power results.
Yes, but I don't know how to relate the three power results. I can't directly add/subtract the power results since I don't know the network inside the box. I think I need to set up an equation using some sort of proportionality (P∝V2 for instance).
The answer given is 450W (max) and 2W (min).
Do I need to use any specific network theorem here?
 
cnh1995 said:
Yes, but I don't know how to relate the three power results. I can't directly add/subtract the power results since I don't know the network inside the box. I think I need to set up an equation using some sort of proportionality (P∝V2 for instance).
The answer given is 450W (max) and 2W (min).
Do I need to use any specific network theorem here?
Plus, when they say 'one source is acting at a time', do I open-circuit the other two sources or short them?
I now doubt if this problem is solvable with the given data.
 
cnh1995 said:
Plus, when they say 'one source is acting at a time', do I open-circuit the other two sources or short them?
Presumably they mean to suppress the sources as is done in superposition analysis. So, short them since they are voltage sources.

Suppose that each individual source produces some potential difference across R. By superposition you know that these potential differences will sum linearly, and the resulting power will go as the square of that sum. But you are given individual power dissipations instead. How might you sum them?
 
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gneill said:
Presumably they mean to suppress the sources as is done in superposition analysis. So, short them since they are voltage sources.

Suppose that each individual source produces some potential difference across R. By superposition you know that these potential differences will sum linearly, and the resulting power will go as the square of that sum. But you are given individual power dissipations instead. How might you sum them?
If E1, E2 and E3 produce voltages V1, V2 and V3 respectively across R individually, then in combined case,
P=V2/R,
where V=aV1+bV2+cV3.
Is that right?
 
cnh1995 said:
If E1, E2 and E3 produce voltages V1, V2 and V3 respectively across R individually, then in combined case,
P=V2/R,
where V=aV1+bV2+cV3.
Is that right?
Yes. You can also say that the individual potential differences expressed across R will be proportional to the square root of the individual powers.
 
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cnh1995 said:
If E1, E2 and E3 produce voltages V1, V2 and V3 respectively across R individually, then in combined case,
P=V2/R,
where V=aV1+bV2+cV3.
Is that right?
That looks reasonable, but there are limits on a, b and c.
 
As per post 7, given the termination has some ## R_o ##, ## P_a=\frac{V_a^2}{R_o} ##, ##P_b=\frac{V_b^2}{R_o} ##, and ## P_c=\frac{V_c^2}{R_o} ##. A little algebra gives ## \sqrt{P_a}+\sqrt{P_b}+\sqrt{P_c}=\frac{V_a+V_b+V_c}{\sqrt{R_o}}=\frac{V_{total}}{\sqrt{R_o}} ##. It is a simple matter to compute ## P_{total} ## by squaring both sides. ## \\ ## Edit: One additional item though: What if the sign of ## V_b ## or ## V_c ## is different from that of ## V_a ##? The above equality doesn't always hold. That's apparently why there is a maximum and a minimum. ## \\ ## Additional edit: And yes, I get the answers of post 3 by selecting the appropriate relative signs for the 3 terms.
 
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  • #10
Sorry for replying so late!

Thanks a lot @gneill, @Charles Link and @haruspex for your clever hints. Turns out what I really need here is only the Superposition theorem. I got the correct answer now.
Thanks again!:smile:
 
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