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Question #43408

Difficulty: 8/10 | 🟢 Free

The Question

A rigid square loop of mass M=1.2 kgM = 1.2 \text{ kg} and side length L=0.5 mL = 0.5 \text{ m} lies initially in the horizontal xyxy-plane. One of its edges is hinged along the yy-axis (from y=0y=0 to y=Ly=L) so that the loop can rotate freely. Gravity acts in the −z-z direction (g=10 m/s2g = 10 \text{ m/s}^2). A constant current I=1 AI = 1 \text{ A} is maintained in the loop by an external source, flowing in the +y+y direction along the hinged edge. The system is immersed in a non-uniform, time-independent magnetic field B⃗=B0(1+xL)i^\vec{B} = B_0 \left(1 + \frac{x}{L}\right) \hat{i}, where B0=2 TB_0 = 2 \text{ T}. An ideal string is attached to the center of the outer edge of the loop (at x=L,y=L/2x=L, y=L/2). The string passes vertically upwards (in the +z+z direction) over a small ideal pulley and is connected to a hanging block of mass m=0.2 kgm = 0.2 \text{ kg}. If the system is released from rest, calculate the initial angular acceleration of the loop. (Neglect any self-induction effects).

Options

  • A.

    407 rad/s2\frac{40}{7} \text{ rad/s}^2

  • B.

    507 rad/s2\frac{50}{7} \text{ rad/s}^2

  • C.

    403 rad/s2\frac{40}{3} \text{ rad/s}^2

  • D.

    8 \text{ rad/s}^2

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Correct Answer

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Explanation

How the Examiner Thinks

Multi-Concept_Bridge

Master problems that require linking physics and math concepts to solve complex competitive questions.

Concepts Behind This Question

Torque on Current Loop|Constraint Relations via String Length|Vector Cross-Products

Why This Question Is Tricky

Common Mistakes

This question tests the application of magnetic torque in a non-uniform field coupled with mechanical constraints.

A common lethal trap is blindly applying the magnetic dipole formula τ⃗=μ⃗×B⃗center\vec{\tau} = \vec{\mu} \times \vec{B}_{center} (which yields an incorrect torque of 1.5IL2B01.5 I L^2 B_0 and leads to Option B).

This formula is strictly valid only for uniform magnetic fields.

In a non-uniform field, students must integrate the Lorentz force dF⃗=Idl⃗×B⃗d\vec{F} = I d\vec{l} \times \vec{B} along the specific geometry of the loop to find the true torque (2IL2B02 I L^2 B_0).

Furthermore, it tests the correct sign convention in the string constraint linking rotational and translational acceleration, ensuring students recognize that the downward rotation of the loop forces the hanging mass to accelerate upwards.

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Question Information

SubjectPhysics
ChapterMoving Charges and Magnetism - Class 12
ConceptTorque on Current Loop
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree