A highly rigid cubical block A of small mass M and side L is fixed
rigidly on another cubical block
B of same dimensions and of low modulus of rigidly n, such that the lower face of A completely
covers the upper face of B. The lower face of B is rigidly held on a horizontal surface. A small force
F is applied perpendicular to one of the side faces of A at the top. The side of B turns by an angle .
Now the whole arrangement is tumed upside down so that lower face of A is rigidly held to the
horizontal surface and we apply a small force F perpendicular to the side face B at the top. The side
of B now tums by an angle of ?
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Answer:
Modulus of rigidity η=
Aθ
F
Here, A=L
2
and θ=
L
x
for small θ
∴ Restoring force =F=−ηAθ
or acceleration, a=
m
F
=
M
ηL
xequation(1)
∵a∝(−x)
∴ Time period, T=2π
∣
∣
∣
∣
∣
∣
a
x
∣
∣
∣
∣
∣
∣
⟹T=2π
ηL
M
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