Difference between revisions of "Chapter 26 Problem 40"

From 105/106 Lecture Notes by OBM
(Created page with "==Problem== thumb|right|Resistance is futile! Twelve resistors, each of resistance R, are connected as the edges of a cube. Determine the equi...")
 
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Insert a probe battery between points (a) and (b). Let's label the current drawn from this probe battery as I
 
Insert a probe battery between points (a) and (b). Let's label the current drawn from this probe battery as I
  
This setup has a symmetry plane between abed, so the current split at junction a will be  
+
This setup has a symmetry plane between abed, so the current split at junction a will be
 +
 
<math>I=I_1+I_1+I_2</math>
 
<math>I=I_1+I_1+I_2</math>
  
Another symmetry is that the afhe plane is the mirror cdgb (since one has the current I entering, and the other has the current leaving) thus we have the same currents in erverse directions in those planes.  
+
Another symmetry is that the afhe plane is the mirror cdgb (since one has the current I entering, and the other has the current leaving) thus we have the same currents in erverse directions in those planes.
  
 +
*<math>I=2I_1+I_2</math>
 +
*<math>I_3+I_4=I_1</math>
 +
*<math>I_5=2I_4</math>
 +
*<math>0=-2 I_1 R -I_3 R + I_2 R</math>
 +
*<math>0=-2 I_4 R -I_5 R + I_3 R</math>
 +
*<math>0=\mathcal{E}-2 I_2 R </math>
  
 
===(b)===
 
===(b)===

Revision as of 20:02, 30 March 2019

Problem

Resistance is futile!

Twelve resistors, each of resistance R, are connected as the edges of a cube. Determine the equivalent resistance

(a) between points a and b, the ends of a side;

(b) between points a and c, the ends of a face diagonal;

(c) between points a and d, the ends of the volume diagonal.

[Hint: Apply an emf and determine currents; use symmetry at junctions.]

solution

(a)

The symmetry reduced cube

Insert a probe battery between points (a) and (b). Let's label the current drawn from this probe battery as I

This setup has a symmetry plane between abed, so the current split at junction a will be

Another symmetry is that the afhe plane is the mirror cdgb (since one has the current I entering, and the other has the current leaving) thus we have the same currents in erverse directions in those planes.

(b)

The symmetry reduced cube

Insert a probe battery between points (a) and (c). Let's label the current drawn from this probe battery as I

(c)

The symmetry reduced cube

Insert a probe battery between points (a) and (d). Let's label the current drawn from this probe battery as I