Twelve wires of equal length and same cross-section are connected in the from of a cube. If the resistance of each of the wires is R, then the effective resistance between the two diagonal ends would be then
Sol. Let us number the corners as 1,2,3,… and so on as shown
a(1−8−7−6),b(1−2−7−6),c(1−8−5−6),d(1−2
−3−6),e(1−4−5−6),f(1−4−3−6)
Now for each of these paths, we have identical resistances.
Let the current entering at point A be I. The current will be
distributed equally among all the three parts. Therefore, we can
say that the current is
I12=I14=I18=I/3
Now look at all paths from 2 to 6 . We have the following paths
g(2−7−6) and h(2−3−6) .
since they also have the same resistances, we can assume that
current in 2−3 and current in 2−7 must be same. Therefore,
I27=I23=12(I3)=I6
we can say that I43=I45=I85=I87=I/6
Therefore, to calculate the potential difference across 1−6
(see Fig. 5.34 ) the path A12%, we have
V1−I3R−I6R−I3R=V6⇒V1−V6=I[R3+R6+R3]=56IR
Hence, (V1−V6)I=56R
Therefore, the equivalent resistance is going to be 56R .