Q.

A small circular loop of area A and resistance R is fixed on a horizontal xy-plane with the center of the loop always on the axis n^ of a long solenoid. The solenoid has m turns per unit length and carries current I counterclockwise as shown in the figure. The magnetic field due to the solenoid is in n^ direction. List-I gives time dependences of n^ in terms of a constant angular frequency ω. List-II gives the torques experienced by the circular loop at time t=π6ω. Let α=A2μ02m2I2ω2R.             [2022]

  List-I   List-II
(I) 12(sinωtj^+cosωtk^) (P) 0
(II) 12(sinωti^+cosωtj^) (Q) -α4i^
(III) 12(sinωti^+cosωtk^) (R) 3α4i^
(IV) 12(cosωtj^+sinωtk^) (S) α4j^
    (T) -3α4i^

Which one of the following options is correct

1 (I) → (Q); (II) → (P); (III) → (S); (IV) → (T)  
2 (I) → (S); (II) → (T); (III) → (Q); (IV) → (P)  
3 (I) → (Q); (II) → (P); (III) → (S); (IV) → (R)  
4 (I) → (T); (II) → (Q); (III) → (P); (IV) → (R)  

Ans.

(3)

(I)   B→=μ0mI2(sinωtj^+cosωtk^)

ϕ=B→·A→=μ0mI2cos(ωt)A

ε=-dϕdt=μ0mI ωA2sin(ωt)

i=εR=μ0mI ωA2Rsin(ωt)

So, M→=iA→=μ0mI ωA22Rsin(ωt)k^

τ→=M→×B→=μ0 2m2I2ωA22Rsin2(ωt) (-i^)

For t=π6ω

τ→=μ0 2m2I2ωA22R×14(-i^)

=A2μ0 2m2I2ω2R×14(-i^)=α4(-i^).  So, (I)→Q

(II) Solving as (I), ϕ=0, ε=0, i=0, M→=0. So, (II)→P

Similarly, (III)→S

                  (IV)→R