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Water rises up in a glass capillary upto...

Water rises up in a glass capillary upto a height of `9.0cm`, while mercury falls down by `3.4 cm` in the same capillary. Assume angles of contact for water glass and mercury glass `0^(@)` and `135^(@)` respectively. Determine the ratio of surface tension of mercury and water `(cos 135^(@)=-0.71)`.

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To solve the problem of determining the ratio of surface tension of mercury and water, we will use the formula for capillary rise and fall in a capillary tube. ### Step-by-Step Solution: 1. **Understand the Problem**: - Water rises in a glass capillary tube to a height of \( h_1 = 9.0 \, \text{cm} \). - Mercury falls in the same capillary tube to a height of \( h_2 = -3.4 \, \text{cm} \) (negative because it falls). - The angle of contact for water with glass is \( \theta_1 = 0^\circ \) and for mercury with glass is \( \theta_2 = 135^\circ \). 2. **Use the Capillary Rise and Fall Formula**: The height \( h \) in a capillary tube is given by: \[ h = \frac{2S \cos \theta}{\rho g R} \] where: - \( S \) is the surface tension, - \( \theta \) is the angle of contact, - \( \rho \) is the density of the liquid, - \( g \) is the acceleration due to gravity, - \( R \) is the radius of the capillary tube. 3. **Set Up the Equations**: For water (rising): \[ h_1 = \frac{2S_1 \cos \theta_1}{\rho_1 g R} \] For mercury (falling): \[ h_2 = \frac{2S_2 \cos \theta_2}{\rho_2 g R} \] 4. **Divide the Two Equations**: \[ \frac{h_1}{h_2} = \frac{S_1 \cos \theta_1}{S_2 \cos \theta_2} \cdot \frac{\rho_2}{\rho_1} \] 5. **Rearranging for Surface Tension Ratio**: \[ \frac{S_1}{S_2} = \frac{h_1}{h_2} \cdot \frac{\cos \theta_2}{\cos \theta_1} \cdot \frac{\rho_1}{\rho_2} \] 6. **Substituting Known Values**: - \( h_1 = 9.0 \, \text{cm} \) - \( h_2 = -3.4 \, \text{cm} \) (take absolute value for calculation) - \( \theta_1 = 0^\circ \) (thus \( \cos 0^\circ = 1 \)) - \( \theta_2 = 135^\circ \) (given \( \cos 135^\circ = -0.71 \)) - \( \rho_1 = 1 \, \text{g/cm}^3 \) (density of water) - \( \rho_2 = 13.6 \, \text{g/cm}^3 \) (density of mercury) Now substituting these values: \[ \frac{S_1}{S_2} = \frac{9.0}{-3.4} \cdot \frac{-0.71}{1} \cdot \frac{1}{13.6} \] 7. **Calculate the Ratio**: - First calculate \( \frac{9.0}{-3.4} \approx -2.647 \) - Then calculate \( \frac{-0.71}{1} = -0.71 \) - Finally, calculate \( \frac{1}{13.6} \approx 0.07353 \) Thus: \[ \frac{S_1}{S_2} = -2.647 \cdot -0.71 \cdot 0.07353 \approx 0.135 \] 8. **Final Ratio**: Therefore, the ratio of surface tension of mercury to water is: \[ \frac{S_2}{S_1} \approx 7.23 \] ### Conclusion: The ratio of surface tension of mercury to that of water is approximately \( 7.23 \).

To solve the problem of determining the ratio of surface tension of mercury and water, we will use the formula for capillary rise and fall in a capillary tube. ### Step-by-Step Solution: 1. **Understand the Problem**: - Water rises in a glass capillary tube to a height of \( h_1 = 9.0 \, \text{cm} \). - Mercury falls in the same capillary tube to a height of \( h_2 = -3.4 \, \text{cm} \) (negative because it falls). - The angle of contact for water with glass is \( \theta_1 = 0^\circ \) and for mercury with glass is \( \theta_2 = 135^\circ \). ...
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