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:
\[ F = 51.29 + 125.71 = 177 \, \text{N}. \]
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:
LIST I | LIST II | ||
A | Surface tension | 1 | kgm−1s−1 |
B | Pressure | 2 | kgms−1 |
C | Viscosity | 3 | kgm−1s−2 |
D | Impulse | 4 | kgs−2 |
The portion of the line \( 4x + 5y = 20 \) in the first quadrant is trisected by the lines \( L_1 \) and \( L_2 \) passing through the origin. The tangent of an angle between the lines \( L_1 \) and \( L_2 \) is: