The force exerted by mercury on the bottom of the tube is calculated using:
\[ F = P_0A + \rho_m ghA \]
where:
- \( P_0 = 10^5 \, \text{Nm}^{-2} \) (atmospheric pressure),
- \( A = \pi r^2 = \frac{22}{7} \times (2 \times 10^{-2})^2 \) (base area),
- \( \rho_m = 1.36 \times 10^4 \, \text{kg m}^{-3} \) (mercury density),
- \( g = 10 \, \text{ms}^{-2} \),
- \( h = 30 \times 10^{-2} \, \text{m} \) (mercury column height).
The base area \( A \) is calculated as:
\[ A = \frac{22}{7} \times (2 \times 10^{-2})^2 \]
Substituting these values into the force equation yields:
\[ F = 10^5 \times \frac{22}{7} \times (2 \times 10^{-2})^2 + 1.36 \times 10^4 \times 10 \times (30 \times 10^{-2}) \times \frac{22}{7} \times (2 \times 10^{-2})^2 \]
The result of this calculation is:
\[ F = 51.29 + 125.71 = 177 \, \text{N}. \]
Two vessels A and B are of the same size and are at the same temperature. A contains 1 g of hydrogen and B contains 1 g of oxygen. \(P_A\) and \(P_B\) are the pressures of the gases in A and B respectively, then \(\frac{P_A}{P_B}\) is: