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Question #43496

Difficulty: 8/10 | 🟢 Free

The Question

A non-uniform heavy rope of length LL hangs vertically from a rigid support. The linear mass density (mass per unit length) of the rope varies as μ(x)=cx2\mu(x) = c x^2, where xx is the distance measured from its lower free end and cc is a positive constant. A small transverse wave pulse is generated at the lower end (x=0x=0). Find the time taken by the pulse to reach the rigid support at x=Lx=L. Assume the acceleration due to gravity is gg and the rope is perfectly flexible.

Options

  • A.

    23Lg2\sqrt{\frac{3L}{g}}

  • B.

    2Lg2\sqrt{\frac{L}{g}}

  • C.

    22Lg2\sqrt{\frac{2L}{g}}

  • D.

    3Lg\sqrt{\frac{3L}{g}}

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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

Tension in Massless vs Massive Strings|String Tension and Wave Speed|Integration

Why This Question Is Tricky

Common Mistakes

This question tests the student's ability to model wave propagation in a medium with continuously varying properties.

A common trap is assuming the wave speed formula v=T/μv = \sqrt{T/\mu} implies a constant speed or incorrectly using the total mass to find an 'average' tension or density.

Students often mistakenly apply the uniform rope result (t=2L/gt = 2\sqrt{L/g}) or fail to recognize that both tension and linear mass density are local functions of xx.

By setting μ(x)∝x2\mu(x) \propto x^2, the problem forces the explicit integration of the weight to find T(x)T(x) and subsequently integrating dt=dx/v(x)dt = dx/v(x), rigorously testing the application of calculus in Newtonian mechanics and wave dynamics.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterLaws of Motion - Class 11 Part 1
ConceptTension in Massless vs Massive Strings
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree