Cube of Resistor Problem - Nice one

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The discussion revolves around solving the equivalent resistance of an asymmetrical cube circuit between points A and C'. Participants share their approaches, highlighting the use of Kirchhoff's Laws and the complexity involved in deriving equations. A more efficient method is proposed, leveraging symmetry to simplify the analysis by recognizing that nodes of equal voltage can be shorted, reducing the problem to parallel and series combinations of resistors. The final equivalent resistance is expressed as a formula involving the resistors R1, R2, and R3. The conversation also touches on the implications of using resistors of different values, noting that symmetry is lost in such cases.
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Homework Statement


Asymmetrical Cube - Determine the equivalent resistance between points A and C’ of the circuit below.
resistor_cube.png



Homework Equations



U = R.i

The Attempt at a Solution



This problem was my professor that created. I know how to solve it, but I would like to know if other people have a better idea how to solve it. I tried to use Kirchhoff's Laws and I found 6 equations and was a bit complicate to find the final answer. I think it's a good challenge.
The answer is:

$$\frac{1}{4} \left(R_1+R_2+R_3+\frac{1}{R_1^{-1}+R_2^{-1}+R_3^{-1}} \right)$$
 
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3 equations are sufficient, as the cube still has a symmetry. If you add the potential of opposite points in the cube, you always get the same value.

I like the result.
 
The easy way is to recognize that, by symmetry, the voltage at the three corners connecting A by one resistor each is the same. Similarly, the voltage at the three corners connecting C' by one resistor each is the same.

Nodes of equal voltage can be shorted together without affecting the circuit. This degenerates the cube into three parallel sections connected in series:
Requiv = R1||R2||R3 + R1||R1||R2||R2||R3||R3 + R1||R2||R3.
No KCL or KVL equations needed!
 
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rude man said:
The easy way is to recognize that, by symmetry, the voltage at the three corners connecting A by one resistor each is the same. Similarly, the voltage at the three corners connecting C' by one resistor each is the same.

Nodes of equal voltage can be shorted together without affecting the circuit. This degenerates the cube into three parallel sections connected in series:
Requiv = R1||R2||R3 + R1||R1||R2||R2||R3||R3 + R1||R2||R3.
No KCL or KVL equations needed!
That symmetry does not exist with different resistors.
 
mfb said:
That symmetry does not exist with different resistors.

Yes, I hadn't noticed the resistors could be of different values. Such an old problem, never seen it with differing values before.
 
Borek said:
Makes me think of http://xkcd.com/356/

OK, but I resent a physicist being worth only 2/3 of a mathematician ... I suppose only 1 point per EE, or less even? :-)
 
My solution:

http://www.luiseduardo.com.br/electricity/electrodynamics/cubeofresistors.htm
 
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