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Magnetism question

2022 · Shift 1 · Q51
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Magnetism question

2022 · Shift 1 · Q51

JEE AdvancedPhysicsMagnetismMCQ+3 / −1

A small circular loop of area AAA and resistance RRR is fixed on a horizontal xyx yxy-plane with the center of the loop always on the axis n^\hat{n}n^ of a long solenoid. The solenoid has mmm turns per unit length and carries current III counterclockwise as shown in the figure. The magnetic field due to the solenoid is in n^\hat{n}n^ direction. List-I gives time dependences of n^\hat{n}n^ in terms of a constant angular frequency ω\omegaω. List-II gives the torques experienced by the circular loop at time t=π6ωt=\frac{\pi}{6 \omega}t=6ωπ​. Let α=A2μ02m2I2ω2R\alpha=\frac{A^{2} \mu_{0}^{2} m^{2} I^{2} \omega}{2 R}α=2RA2μ02​m2I2ω​.

JEE Advanced 2022 Paper 1 Online Physics - Magnetism Question 12 English

List-I List-II
(I) 12(sin⁡ωtȷ^+cos⁡ωtk^)\frac{1}{\sqrt{2}}(\sin \omega t \hat{\jmath}+\cos \omega t \hat{k})2​1​(sinωt^​+cosωtk^) (P) 0
(II) 12(sin⁡ωtı^+cos⁡ωtȷ^)\frac{1}{\sqrt{2}}(\sin \omega t \hat{\imath}+\cos \omega t \hat{\jmath})2​1​(sinωt^+cosωt^​) (Q) −α4ı^-\frac{\alpha}{4} \hat{\imath}−4α​^
(III) 12(sin⁡ωtı^+cos⁡ωtk^)\frac{1}{\sqrt{2}}(\sin \omega t \hat{\imath}+\cos \omega t \hat{k})2​1​(sinωt^+cosωtk^) (R) 3α4ı^\frac{3 \alpha}{4} \hat{\imath}43α​^
(IV) 12(cos⁡ωtȷ^+sin⁡ωtk^)\frac{1}{\sqrt{2}}(\cos \omega t \hat{\jmath}+\sin \omega t \hat{k})2​1​(cosωt^​+sinωtk^) (S) α4ȷ^\frac{\alpha}{4} \hat{\jmath}4α​^​
(T) −3α4ı^-\frac{3 \alpha}{4} \hat{\imath}−43α​^

Which one of the following options is correct?

  1. A
    I →\rightarrow→ Q, II →\rightarrow→ P, III →\rightarrow→ S, IV →\rightarrow→ T
  2. B
    I→S,II→T\mathrm{I} \rightarrow \mathrm{S}, \mathrm{II} \rightarrow \mathrm{T}I→S,II→T, III →Q\rightarrow \mathrm{Q}→Q, IV →P\rightarrow \mathrm{P}→P
  3. C
    I→Q,II→P\mathrm{I} \rightarrow \mathrm{Q}, \mathrm{II} \rightarrow \mathrm{P}I→Q,II→P, III →S\rightarrow \mathrm{S}→S, IV →R\rightarrow \mathrm{R}→R
  4. D
    I→T\mathrm{I} \rightarrow \mathrm{T}I→T, II →Q\rightarrow \mathrm{Q}→Q, III →P\rightarrow \mathrm{P}→P, IV →R\rightarrow \mathrm{R}→R
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