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Question #43010

Difficulty: 8/10 | 🟢 Free

The Question

A particle of mass mm and charge +q+q is projected from the origin (0,0,0)(0,0,0) with an initial velocity v⃗=3v0i^+v0j^\vec{v} = \sqrt{3}v_0 \hat{i} + v_0 \hat{j}. A non-uniform magnetic field B⃗=B0xk^\vec{B} = B_0 x \hat{k} exists in the region x≥0x \ge 0, where B0B_0 is a positive constant. Neglecting gravity, the maximum x-coordinate reached by the particle is:

Options

  • A.

    2mv0qB0\sqrt{\frac{2mv_0}{q B_0}}

  • B.

    4mv0qB0\sqrt{\frac{4mv_0}{q B_0}}

  • C.

    6mv0qB0\sqrt{\frac{6mv_0}{q B_0}}

  • D.

    8mv0qB0\sqrt{\frac{8mv_0}{q B_0}}

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Variable_Constraint

Develop pure symbolic logic skills by mastering algebraic constraints without relying on numerical data.

Concepts Behind This Question

Cyclotron Frequency Invariance|Lorentz Force Vector Direction|Moving Charge in Non-Uniform B

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to analyze motion in a non-uniform magnetic field, where standard cyclotron formulas (R=mv/qBR = mv/qB) completely fail.

The primary trap lies in assuming the particle's velocity simply reverses its initial y-component (vy=−v0v_y = -v_0) at maximum displacement, or incorrectly assuming the total speed is just v0v_0.

By introducing a spatial gradient (B∝xB \propto x), students are forced to apply the fundamental Lorentz force integration (mdvy=−qB(x)dxm dv_y = -q B(x) dx).

Furthermore, they must correctly apply the Work-Energy theorem to deduce that the velocity vector rotates continuously until vy=−2v0v_y = -2v_0 at the turning point, accounting for the full initial kinetic energy.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMoving Charges and Magnetism - Class 12
ConceptCyclotron Frequency Invariance
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree