A highly rigid cubical block \hat{A} of small mass M and side l is fixed rigidly onto another cubical block \(\beta\) of the same dimensions and of low modulus of rigidity "" such that the lower face of \Delta completely covers the upper face of \(\beta\) . The lower face of \(\beta\) is rigidly held on a horizontal surface. A small force \mathfrak{F} is applied perpendicular to one of the side faces of \hat{A} . After the force is withdrawn block A. executes small oscillations. The time period of which is given by
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By substituting the dimensions of mass [M], length [L] and coefficient of rigidity \(\left| M L^{-1} T^{-2} \right|\) we ge \(\tau = 2 \tau \sqrt[3]{\frac{1M}{1\mu L}}\) is the right formula for time period of oscillations
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