4) A body of mabb M is situated in a potar tial field u(x) = Mo (1-Cobelan), where Constants. The time perioud of small obcillations of body will be to and I are
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U =U0(1-cosαx)
F = -dU/dx
F = -d/dx[U0(1-cosαx)] =U0αsinαx
As αx is small,so sin αx∼αx
∴F=−U0α2x ...(i)
F∝x and −ve shows that F is directed towards the mean position, hence the body executes SHM.
For SHM, F=−kx
Comparing (i) and (ii), we get, k=U0α2
Time period of oscillation,
T=2πkm√m/k
= 2π√m/U0α2m
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