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Question #42671

Difficulty: 8/10 | 🟢 Free

The Question

A bead of mass mm and charge +q+q is constrained to slide without friction along a vertical non-conducting wire aligned with the yy-axis. Two fixed point charges, each of charge +Q+Q, are located at coordinates (d,0)(d, 0) and (−d,0)(-d, 0) in the xyxy-plane. The bead is released from rest at y=hy = h. A programmable external mechanism applies a vertical force to the bead such that it undergoes exact vertical free fall kinematics, maintaining a constant downward acceleration gg. Simultaneously, a time-varying uniform electric field E⃗(t)=E0tj^\vec{E}(t) = E_0 t \hat{j} is active in the region. What is the total work done by the external mechanism from the moment of release until the bead reaches the origin (y=0y=0)? (Assume k=14πϵ0k = \frac{1}{4\pi\epsilon_0})

Options

  • A.

    2kQq(1d−1d2+h2)+23qE0h2hg2kQq \left( \frac{1}{d} - \frac{1}{\sqrt{d^2+h^2}} \right) + \frac{2}{3} q E_0 h \sqrt{\frac{2h}{g}}

  • B.

    2kQq(1d−1d2+h2)2kQq \left( \frac{1}{d} - \frac{1}{\sqrt{d^2+h^2}} \right)

  • C.

    2kQq(1d−1d2+h2)−23qE0h2hg2kQq \left( \frac{1}{d} - \frac{1}{\sqrt{d^2+h^2}} \right) - \frac{2}{3} q E_0 h \sqrt{\frac{2h}{g}}

  • D.

    2kQq(1d−1d2+h2)+12qE0h2hg2kQq \left( \frac{1}{d} - \frac{1}{\sqrt{d^2+h^2}} \right) + \frac{1}{2} q E_0 h \sqrt{\frac{2h}{g}}

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Explanation

How the Examiner Thinks

Intuition_Breaker

Train your brain to resist "obvious" answers that are designed to deceive your intuition.

Concepts Behind This Question

Superposition of Potentials|Mechanical Energy Conservation|Variable Force Integration|Kinematics of Vertical Free Fall

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to decouple conservative and non-conservative work components in a constrained kinematic system.

The primary trap is blindly applying the Mechanical Energy Conservation theorem while either ignoring the time-varying electric field or incorrectly treating it as a static potential.

Furthermore, students often fail to express the path integral of a time-dependent force (∫F⃗(t)⋅dr⃗\int \vec{F}(t) \cdot d\vec{r}) by parameterizing the displacement dr⃗d\vec{r} in terms of the known velocity profile v⃗(t)dt\vec{v}(t)dt, leading to incorrect spatial averaging (Option D) or sign errors (Option C).

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectrostatic Potential and Capacitance - Class 12
ConceptSuperposition of Potentials
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree