A pendulum bob of mass m is suspended at rest. A constant horizontal force F=mg2 starts acting on it. The maximum angular deflection of the string is
A
90∘
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B
53∘
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C
37∘
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D
60∘
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Solution
The correct option is B53∘
Let angular deflection be θ when velocity is v, then by work energy theorem W=ΔKE 12mv2=−mgh+Flsinθ
12mv2=−mg(l−lcosθ)+Flsinθ(∵h=l−lcosθ)
At maximum angular deflection, v=0 0=−mgl(1−cosθ)+mgl2sinθ⇒2−2cosθ=sinθ⇒4+4cos2θ−8cosθ=sin2θ=1−cos2θ ⇒5cos2θ−8cosθ+3=0⇒5cos2θ−5cosθ−3cosθ+3=0 ⇒5cosθ(cosθ−1)−3(cosθ−1)=0⇒(5cosθ−3)(cosθ−1)=0 ⇒cosθ=35orcosθ=1⇒θ=53∘orθ=0