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A gas for which gamma=1.5 is suddenly co...

`A` gas for which `gamma=1.5` is suddenly compressed to `1//4` th of the initial volume. Then the ratio of the final to initial pressure is

A

`1:16`

B

`1:8`

C

`1:4`

D

`8:1`

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The correct Answer is:
To solve the problem, we need to find the ratio of the final pressure to the initial pressure (P2/P1) after the gas is suddenly compressed to 1/4th of its initial volume (V1). We will use the adiabatic process relation for this calculation. ### Step-by-Step Solution: 1. **Identify Given Values**: - The ratio of specific heats, \( \gamma = 1.5 \). - The final volume \( V_2 = \frac{1}{4} V_1 \). 2. **Use the Adiabatic Relation**: The adiabatic process is described by the equation: \[ P_1 V_1^\gamma = P_2 V_2^\gamma \] Rearranging this gives us: \[ \frac{P_2}{P_1} = \frac{V_1^\gamma}{V_2^\gamma} \] 3. **Substitute the Volume Relationship**: Since \( V_2 = \frac{1}{4} V_1 \), we can substitute this into the equation: \[ \frac{P_2}{P_1} = \frac{V_1^\gamma}{\left(\frac{1}{4} V_1\right)^\gamma} \] 4. **Simplify the Equation**: This simplifies to: \[ \frac{P_2}{P_1} = \frac{V_1^\gamma}{\left(\frac{1}{4^\gamma} V_1^\gamma\right)} = \frac{V_1^\gamma}{\frac{1}{4^\gamma} V_1^\gamma} \] The \( V_1^\gamma \) terms cancel out: \[ \frac{P_2}{P_1} = 4^\gamma \] 5. **Calculate \( 4^\gamma \)**: Now we substitute \( \gamma = 1.5 \): \[ \frac{P_2}{P_1} = 4^{1.5} = (4^1) \cdot (4^{0.5}) = 4 \cdot 2 = 8 \] 6. **Final Result**: Therefore, the ratio of the final pressure to the initial pressure is: \[ \frac{P_2}{P_1} = 8 \] ### Final Answer: The ratio of the final pressure to the initial pressure is \( 8 \). ---

To solve the problem, we need to find the ratio of the final pressure to the initial pressure (P2/P1) after the gas is suddenly compressed to 1/4th of its initial volume (V1). We will use the adiabatic process relation for this calculation. ### Step-by-Step Solution: 1. **Identify Given Values**: - The ratio of specific heats, \( \gamma = 1.5 \). - The final volume \( V_2 = \frac{1}{4} V_1 \). ...
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