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Question #42751

Difficulty: 8/10 | 🟢 Free

The Question

A thin rod of length LL is placed along the x-axis with its ends at x=0x = 0 and x=Lx = L. The rod has a non-uniform linear mass density given by λ(x)=αx\lambda(x) = \alpha x, where α\alpha is a positive constant with units of kg/m2\text{kg/m}^2. What is the gravitational potential VV at a point PP located on the x-axis at x=−Lx = -L? (Let GG be the universal gravitational constant).

Options

  • A.

    −GαL(1−ln⁡2)-G \alpha L (1 - \ln 2)

  • B.

    −310GαL-\frac{3}{10} G \alpha L

  • C.

    −12GαLln⁡2-\frac{1}{2} G \alpha L \ln 2

  • D.

    −GαLln⁡2-G \alpha L \ln 2

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Correct Answer

Step-by-Step Solution

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

Superposition of Potentials|Potential vs Field Relationship|Integration

Why This Question Is Tricky

Common Mistakes

This question tests the student's understanding of the superposition principle for scalar fields in continuous, non-uniform mass distributions.

A common, fatal heuristic is treating an extended body as a point mass located at its center of mass (xcm=2L/3x_{cm} = 2L/3), which incorrectly yields V=−GM/rcm=−3GαL/10V = -GM/r_{cm} = -3G\alpha L/10.

While the center of mass approximation is valid for calculating the external gravitational field of spherically symmetric bodies, it strictly fails for rods and non-symmetric distributions.

Students must recognize that potential requires the direct integration of dV=−Gdm/rdV = -G dm/r, forcing them to account for the spatially varying density λ(x)\lambda(x) and the non-linear dependence of potential on distance.

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