A small ball is attached to one end of a string swings in a vertical plane such that its acceleration at extreme point is equal tovthe aceleration at mean position the angle theta is
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v^2/l=gsinα (1)
wehre α is the maximum deflection angle
From Newton's law in projection form: Ft=mwt
−mgsinθ=mvdv/ldθ
or, −glsinθdθ=vdv
On integrating both the sides within their limits.
−gl∫α0sinθdθ=∫0vvdv
or, v2=2gl(1−cosα) (2)
Note: Eq. (2) can easily be obtained by the conservation of mechanical energy of the ball in the uniform field of gravity.
From Eqs. (1) and (2) with θ=α
2gl(1−cosα)=lgcosα
or cosα=23 so, α=53∘
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