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At 27^(@) a gas is suddenly comperssed s...

At `27^(@)` a gas is suddenly comperssed such that its pressure become `(1)/(8)th` of original pressure. Temperature of the gas will be `(lambda=5//3)`

A

420 k

B

`327^(@)C`

C

300k

D

`-142^(@)`

Text Solution

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The correct Answer is:
To solve the problem, we will use the principles of thermodynamics, particularly focusing on the adiabatic process since the gas is suddenly compressed. ### Step-by-Step Solution: 1. **Understand the Problem**: - Initial temperature \( T_1 = 27^\circ C = 300 \, K \) (converted to Kelvin). - The pressure after compression \( P_2 = \frac{1}{8} P_1 \). - Given \( \gamma = \frac{5}{3} \). 2. **Use the Adiabatic Process Equation**: - For an adiabatic process, the relationship between pressure and temperature can be expressed as: \[ P_1^{\gamma} T_1^{\gamma - 1} = P_2^{\gamma} T_2^{\gamma - 1} \] - Rearranging gives: \[ T_2 = T_1 \left( \frac{P_1}{P_2} \right)^{\frac{\gamma - 1}{\gamma}} \] 3. **Substituting Known Values**: - Substitute \( P_2 = \frac{1}{8} P_1 \): \[ T_2 = T_1 \left( \frac{P_1}{\frac{1}{8} P_1} \right)^{\frac{\gamma - 1}{\gamma}} = T_1 \left( 8 \right)^{\frac{\gamma - 1}{\gamma}} \] 4. **Calculate \( \frac{\gamma - 1}{\gamma} \)**: - Given \( \gamma = \frac{5}{3} \): \[ \frac{\gamma - 1}{\gamma} = \frac{\frac{5}{3} - 1}{\frac{5}{3}} = \frac{\frac{2}{3}}{\frac{5}{3}} = \frac{2}{5} \] 5. **Substituting Back**: - Now substitute back into the equation for \( T_2 \): \[ T_2 = 300 \times 8^{\frac{2}{5}} \] 6. **Calculating \( 8^{\frac{2}{5}} \)**: - Calculate \( 8^{\frac{2}{5}} \): \[ 8 = 2^3 \implies 8^{\frac{2}{5}} = (2^3)^{\frac{2}{5}} = 2^{\frac{6}{5}} = 2^{1.2} \] - Approximate \( 2^{1.2} \approx 2.297 \). 7. **Final Calculation of \( T_2 \)**: - Now calculate \( T_2 \): \[ T_2 \approx 300 \times 2.297 \approx 689.1 \, K \] 8. **Convert \( T_2 \) to Celsius**: - Convert back to Celsius: \[ T_2 = 689.1 - 273 \approx 416.1^\circ C \] ### Final Answer: The final temperature of the gas after compression is approximately \( 416.1^\circ C \).
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