A highly rigid cubical block \Delta of small mass \(\mathbf{M}\) 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 \hat{A} 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 \Delta . After the force is withdrawn block \Delta executes small oscillations.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 \(\left| ML^{1}T^{-2} \right|\) we ge \(\tau = 2 \tau \sqrt{\frac{1M}{1\mu L}}\) is the right formula for time period of oscillations
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