Skip to content
dronacharya.ai
← JEE Advanced 2022 · Paper 1
PhysicsList match+3 / -1Question 33 of 54

JEE Advanced 2022 · Paper 1, Physics question 15

A small circular loop of area AA and resistance RR is fixed on a horizontal xyxy-plane with the center of the loop always on the axis n^\hat n of a long solenoid. The solenoid has mm turns per unit length and carries current II counterclockwise as shown in the figure. The magnetic field due to the solenoid is in n^\hat n direction. List-I gives time dependences of n^\hat n in terms of a constant angular frequency ω\omega. List-II gives the torques experienced by the circular loop at time t=π6ωt = \dfrac{\pi}{6\omega}. Let α=A2μ02m2I2ω2R\alpha = \dfrac{A^2\mu_0^2m^2I^2\omega}{2R}.

Which one of the following options is correct?

A long solenoid with its axis along a unit vector n̂ tilted from the vertical z-axis; the current I circulates counterclockwise about n̂. A small horizontal circular loop sits on the solenoid axis inside it. Axes x, y, z shown.

List-I

  • I
    12(sin⁡ωt j^+cos⁡ωt k^)\frac1{\sqrt2}(\sin\omega t\,\hat j + \cos\omega t\,\hat k)
  • II
    12(sin⁡ωt i^+cos⁡ωt j^)\frac1{\sqrt2}(\sin\omega t\,\hat i + \cos\omega t\,\hat j)
  • III
    12(sin⁡ωt i^+cos⁡ωt k^)\frac1{\sqrt2}(\sin\omega t\,\hat i + \cos\omega t\,\hat k)
  • IV
    12(cos⁡ωt j^+sin⁡ωt k^)\frac1{\sqrt2}(\cos\omega t\,\hat j + \sin\omega t\,\hat k)

List-II

  • P
    00
  • Q
    −α4 i^-\frac\alpha4\,\hat i
  • R
    3α4 i^\frac{3\alpha}4\,\hat i
  • S
    α4 j^\frac\alpha4\,\hat j
  • T
    −3α4 i^-\frac{3\alpha}4\,\hat i
Choose one option
Answer and worked solution

Official answer: Dropped: full marks to everyone

This question was dropped (marks to all) in the official key. Below is the standard working. The organisers did not publish a reason.

Flux and current. The solenoid's field is B⃗=μ0mI n^\vec B=\mu_0mI\,\hat n, and the loop's normal is k^\hat k. Let β=μ0mIA\beta=\mu_0mIA.

  • Flux: Φ=β nz\Phi=\beta\,n_z.
  • Current: i=−βn˙zRi=-\frac{\beta\dot n_z}{R}.
  • Moment μ⃗=iAk^\vec\mu=iA\hat k, so the torque is
    τ⃗=μ⃗×B⃗=−β2Rn˙z (k^×n^)=−2αωn˙z (k^×n^).\vec\tau=\vec\mu\times\vec B=-\frac{\beta^2}{R}\dot n_z\,(\hat k\times\hat n)=-\frac{2\alpha}{\omega}\dot n_z\,(\hat k\times\hat n).

At ωt=π6\omega t=\frac\pi6.

Case nzn_z Torque Match
(I) cos⁡ωt2\frac{\cos\omega t}{\sqrt2} −αsin⁡2ωt i^=−α4i^-\alpha\sin^2\omega t\,\hat i=-\frac\alpha4\hat i Q
(II) 0 0 P
(III) cos⁡ωt2\frac{\cos\omega t}{\sqrt2} αsin⁡2ωt j^=α4j^\alpha\sin^2\omega t\,\hat j=\frac\alpha4\hat j S
(IV) sin⁡ωt2\frac{\sin\omega t}{\sqrt2} αcos⁡2ωt i^=3α4i^\alpha\cos^2\omega t\,\hat i=\frac{3\alpha}4\hat i R

This is option (C). Option (A) differs only in (IV), which suggests the expected sign was disputed.