A solid spherical cork of radius $R$ and specific gravity $0.5$ floats on water. The cork is pushed down so that its centre of mass is at a distance $h$ (where $0 < h < R$) below the surface of water, and then released. The volume of the part of the cork above water level is $\pi R^3 \left(\frac{2}{3} - \cos\theta_0 + \frac{1}{3}\cos^3\theta_0\right)$, where $\theta_0$ is the angle as shown in the figure. At the moment of release, the dependence of the upward force on the cork on $h$ is
To determine the dependence of the upward force on the cork on \( h \), we can analyze the buoyant force acting on the cork.
The cork has a specific gravity of \( 0.5 \), meaning it is half as dense as water. Therefore, it floats with half of its volume submerged when in equilibrium. The volume submerged when the cork is pushed down is more than half, and it is given by the volume of a segment of a sphere.
The upward buoyant force \( F_b \) is equal to the weight of the displaced water.
The displaced volume of water when the center is at \( h \) is:
\[V = \frac{4}{3} \pi R^3 - \pi R^3 \left(\frac{2}{3} - \cos\theta_0 + \frac{1}{3}\cos^3\theta_0\right)\]The net upward force is the additional buoyant force minus the weight of the submerged cork:
\[F = \rho g \left( V_{submerged} - \frac{1}{2} V_{total} \right)\]The change in submerged volume due to the depression by \( h \) is about the cap-shaped volume:
\[V_{cap} = \pi R^2 \left( R - h \right) - \pi R^2 \cos\theta_0 (R - \frac{1}{3} R \cos^2\theta_0 )\]The restoring force can now be determined approximately, since:
\[F \approx \rho g \cdot \pi R^2 \left( h - \frac{1}{3} \frac{h^3}{R^2} \right)\]Therefore, the dependence of the upward force on \( h \) when expanded is:
\[\frac{h}{R} - \frac{1}{3}\left(\frac{h}{R}\right)^3\]This matches the correct answer option provided.
Illustration showing the floating cork and angles involved.
Which one of the following pairs of international organizations and their headquarters is incorrect?
The low lying energy levels due to the vibrational excitations of an even-even nucleus are shown in the figure below.
The spin-parity $J^p$ of the level $E_1$ is