The force exerted by mercury on the bottom of the tube can be calculated as:
\[ F = P_0A + \rho_m ghA \]
where:
- \( P_0 = 10^5 \, \text{Nm}^{-2} \) (atmospheric pressure),
- \( A = \pi r^2 = \frac{22}{7} \times (2 \times 10^{-2})^2 \) (area of the base),
- \( \rho_m = 1.36 \times 10^4 \, \text{kg m}^{-3} \) (density of mercury),
- \( g = 10 \, \text{ms}^{-2} \),
- \( h = 30 \times 10^{-2} \, \text{m} \) (height of mercury column).
Calculating \( A \):
\[ A = \frac{22}{7} \times (2 \times 10^{-2})^2 \]
Substitute into the force equation:
\[ F = 10^5 \times \frac{22}{7} \times (2 \times 10^{-2})^2 + 1.36 \times 10^4 \times 10 \times (30 \times 10^{-2}) \times \frac{22}{7} \times (2 \times 10^{-2})^2 \]
Solving this:
\[ F = 51.29 + 125.71 = 177 \, \text{N}. \]
A bead of mass \( m \) slides without friction on the wall of a vertical circular hoop of radius \( R \) as shown in figure. The bead moves under the combined action of gravity and a massless spring \( k \) attached to the bottom of the hoop. The equilibrium length of the spring is \( R \). If the bead is released from the top of the hoop with (negligible) zero initial speed, the velocity of the bead, when the length of spring becomes \( R \), would be (spring constant is \( k \), \( g \) is acceleration due to gravity):
Let $ f: \mathbb{R} \to \mathbb{R} $ be a twice differentiable function such that $$ f''(x)\sin\left(\frac{x}{2}\right) + f'(2x - 2y) = (\cos x)\sin(y + 2x) + f(2x - 2y) $$ for all $ x, y \in \mathbb{R} $. If $ f(0) = 1 $, then the value of $ 24f^{(4)}\left(\frac{5\pi}{3}\right) $ is: