A particle of mass ‘m′ oscillates along the horizontal diameter AB inside a smooth spherical shell of radius R. At any instant K.E. of the particle is K. Then force applied by particle on the shell at this instant is:
A
K2R
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B
3KR
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C
2KR
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D
KR
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Solution
The correct option is B3KR Energy conservation at B and particle position, mgRsinθ=12mv2=K…(i) mgsinθ=KR
From the FBD of the particle, N=mgsinθ+mv2R
Using (i), N=3mgsinθ =3KR