← 2014 Paper 1

UPSC 2014 Maths Optional Paper 1 Q7b — Step-by-Step Solution

15 marks · Section B

Constrained motion · Dynamics & Statics · asked 7× in 13 yrs · Read the full method →

Question

A particle of mass mm, hanging vertically from a fixed point by a light inextensible cord of length ll, is struck by a horizontal blow which imparts to it a velocity 2gl2\sqrt{gl}. Find the velocity and height of the particle from the level of its initial position when the cord becomes slack.

Technique

Energy conservation + centripetal force balance + slack condition T=0T=0.

Solution

Setup. Particle hangs at the lowest point of a cord (length ll, fixed top). Horizontal blow gives initial speed u=2glu=2\sqrt{gl}. Let θ\theta denote angle of cord from downward vertical. Particle rises along a circle of radius ll until the cord goes slack.

Step 1 — Energy conservation

Height above initial position: h(θ)=l(1cosθ)h(\theta)=l(1-\cos\theta).

12mv2+mgl(1cosθ)=12mu2    v2=u22gl(1cosθ).\tfrac{1}{2}mv^{2}+mg\,l(1-\cos\theta)=\tfrac{1}{2}mu^{2}\;\Longrightarrow\;v^{2}=u^{2}-2gl(1-\cos\theta).

With u2=4glu^{2}=4gl:

v2=4gl2gl+2glcosθ=2gl(1+cosθ).v^{2}=4gl-2gl+2gl\cos\theta=2gl(1+\cos\theta).

Step 2 — Centripetal equation; tension

At angle θ\theta, the centripetal direction is toward the fixed point. Tension TT pulls along the cord in this direction. Gravity component in the centripetal direction: mgcosθ-mg\cos\theta (negative for θ<π/2\theta<\pi/2, i.e., gravity pulls away from centre; positive for θ>π/2\theta>\pi/2, gravity pulls toward centre when particle is above horizontal).

Newton’s second law (centripetal):

Tmgcosθ=mv2l    T=mv2l+mgcosθ.T-mg\cos\theta=\dfrac{mv^{2}}{l}\;\Longrightarrow\;T=\dfrac{mv^{2}}{l}+mg\cos\theta.

Step 3 — Cord becomes slack: T=0T=0

mv2l+mgcosθ=0    v2=glcosθ.\dfrac{mv^{2}}{l}+mg\cos\theta=0\;\Longrightarrow\;v^{2}=-gl\cos\theta.

For v2>0v^{2}>0, need cosθ<0\cos\theta<0, i.e., θ>π/2\theta>\pi/2 — particle is above the horizontal through the anchor when the cord goes slack.

Step 4 — Solve for θ\theta

Equating the two expressions for v2v^{2}:

2gl(1+cosθ)=glcosθ    2+2cosθ=cosθ    3cosθ=2    cosθ=23.2gl(1+\cos\theta)=-gl\cos\theta\;\Longrightarrow\;2+2\cos\theta=-\cos\theta\;\Longrightarrow\;3\cos\theta=-2\;\Longrightarrow\;\cos\theta=-\dfrac{2}{3}.

Step 5 — Velocity and height at slack

Velocity: v2=gl(2/3)=2gl3v^{2}=-gl(-2/3)=\dfrac{2gl}{3}, so

v=2gl3.v=\sqrt{\dfrac{2gl}{3}}.

Height above initial position: h=l(1cosθ)=l(1+23)=5l3h=l(1-\cos\theta)=l(1+\tfrac{2}{3})=\dfrac{5l}{3}.

Answer

  v=2gl3   and   h=5l3.  \boxed{\;v=\sqrt{\dfrac{2gl}{3}}\;\text{ and }\;h=\dfrac{5l}{3}.\;}
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