In column II, R is a nonzero variable finite resistance for each diagram. Some facts are given in column I and corresponding figures are given in column II. Match the two columns :
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Solution
Using KVL in loop CDEFC E−I1R+4−6=0...............(i) and loop AFCBA 4+2(I1+I2)+4I2−6=0.....................(ii) After solving equation (i) and (ii), we have
I1=3E−144+3R;
I2=R+6−E4+3R
(A)I2=0,E=R+6 E>6(R≠0) For current from F to C
(B)I2>0R+6>E E<R+6 Possible for any finite value of E, because R is finite. Ans. (p,q,r,s)
(C) For current in 2Ω from B to C I1+I2=R−8+2E4+3R>0 R−8+2E>0 E>4−R2 E can take any value from zero to infinity
Ans. (p,q,r,s)
(D) Current through R is zero 3E−144+3R=0 E=143 Ans. (s)