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(a) The brass scale of a barometer gives...

(a) The brass scale of a barometer gives correct reading at `0^(@)C` . Coefficient of linear expansion of brass is `2.0xx10^(-5)//^(@)C` . The barometer reads `75cm` at `27^(@)C` . What is the atmospheric pressure at `27^(@)C` ?
(b) A barometer reads `75.0cm` on a steel scale. The room temperature is `30^(@)C` . The scale is correctly graduated for `0^(@)C ` . The coefficient of linear expansion of steel is `alpha=1.2xx10^(-5)//^(@)C` and the coefficient of volume expansion of mercury is `gamma=1.8xx10^(-4)//^(@)C` . Find the correct atmospheric pressure.

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To solve the problem step by step, we will break it down into two parts as given in the question. ### Part (a) 1. **Identify the given values**: - Coefficient of linear expansion of brass, \( \alpha = 2.0 \times 10^{-5} \, ^\circ C^{-1} \) - Initial temperature, \( T_1 = 0^\circ C \) - Final temperature, \( T_2 = 27^\circ C \) - Barometer reading at \( T_2 \), \( L + \Delta L = 75 \, cm \) 2. **Calculate the change in temperature**: \[ \Delta T = T_2 - T_1 = 27^\circ C - 0^\circ C = 27^\circ C \] 3. **Calculate the change in length due to thermal expansion**: \[ \Delta L = \alpha L \Delta T \] Since we need to find \( L \), we can express it as: \[ L + \Delta L = 75 \, cm \implies L + \alpha L \Delta T = 75 \, cm \] 4. **Factor out \( L \)**: \[ L(1 + \alpha \Delta T) = 75 \, cm \] 5. **Solve for \( L \)**: \[ L = \frac{75 \, cm}{1 + \alpha \Delta T} \] Substituting the values: \[ L = \frac{75 \, cm}{1 + (2.0 \times 10^{-5}) \times 27} \] \[ L = \frac{75 \, cm}{1 + 0.00054} = \frac{75 \, cm}{1.00054} \approx 74.95 \, cm \] 6. **Convert the length to atmospheric pressure**: Atmospheric pressure \( P \) in atm is given by: \[ P = \frac{L \times 100}{760} \] Thus, \[ P = \frac{74.95 \times 100}{760} \approx 0.9861 \, atm \] ### Part (b) 1. **Identify the given values**: - Coefficient of linear expansion of steel, \( \alpha = 1.2 \times 10^{-5} \, ^\circ C^{-1} \) - Coefficient of volume expansion of mercury, \( \gamma = 1.8 \times 10^{-4} \, ^\circ C^{-1} \) - Initial temperature, \( T_1 = 0^\circ C \) - Final temperature, \( T_2 = 30^\circ C \) - Barometer reading at \( T_2 \), \( L + \Delta L = 75.0 \, cm \) 2. **Calculate the change in temperature**: \[ \Delta T = T_2 - T_1 = 30^\circ C - 0^\circ C = 30^\circ C \] 3. **Calculate the change in length due to thermal expansion**: \[ \Delta L = \alpha L \Delta T \] Again, we express it as: \[ L + \Delta L = 75.0 \, cm \implies L + \alpha L \Delta T = 75.0 \, cm \] 4. **Factor out \( L \)**: \[ L(1 + \alpha \Delta T) = 75.0 \, cm \] 5. **Solve for \( L \)**: \[ L = \frac{75.0 \, cm}{1 + \alpha \Delta T} \] Substituting the values: \[ L = \frac{75.0 \, cm}{1 + (1.2 \times 10^{-5}) \times 30} \] \[ L = \frac{75.0 \, cm}{1 + 0.00036} = \frac{75.0 \, cm}{1.00036} \approx 74.973 \, cm \] 6. **Calculate the change in volume of mercury**: The change in height of mercury due to volume expansion is given by: \[ L_1 + \Delta L_1 = L + \Delta L_1 \] Where \( \Delta L_1 = \frac{\gamma}{3} L_1 \Delta T \). 7. **Express the equation**: \[ L_1(1 + \frac{\gamma}{3} \Delta T) = 74.973 \, cm \] 8. **Solve for \( L_1 \)**: \[ L_1 = \frac{74.973 \, cm}{1 + \frac{1.8 \times 10^{-4}}{3} \times 30} \] \[ L_1 = \frac{74.973 \, cm}{1 + 0.0018} = \frac{74.973 \, cm}{1.0018} \approx 74.838 \, cm \] 9. **Convert the length to atmospheric pressure**: \[ P = \frac{L_1 \times 100}{760} \] Thus, \[ P = \frac{74.838 \times 100}{760} \approx 0.98478 \, atm \]

To solve the problem step by step, we will break it down into two parts as given in the question. ### Part (a) 1. **Identify the given values**: - Coefficient of linear expansion of brass, \( \alpha = 2.0 \times 10^{-5} \, ^\circ C^{-1} \) - Initial temperature, \( T_1 = 0^\circ C \) - Final temperature, \( T_2 = 27^\circ C \) ...
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