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An ideal gas at 27^(@)C is compressed ad...

An ideal gas at `27^(@)C` is compressed adiabatically to `8//27` of its original volume. If `gamma = 5//3`, then the rise in temperature is

A

`475K`

B

`402K

C

`275K`

D

`375K`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we will follow these steps: ### Step 1: Understand the given data - Initial temperature \( T_1 = 27^\circ C \) - Convert \( T_1 \) to Kelvin: \[ T_1 = 27 + 273 = 300 \, K \] - The volume is compressed to \( \frac{8}{27} \) of its original volume, so: \[ V_2 = \frac{8}{27} V_1 \] - The value of \( \gamma = \frac{5}{3} \). ### Step 2: Use the adiabatic process relation For an adiabatic process, the relation between temperature and volume is given by: \[ T_1 V_1^{\gamma - 1} = T_2 V_2^{\gamma - 1} \] Rearranging this gives: \[ T_2 = T_1 \left( \frac{V_1}{V_2} \right)^{\gamma - 1} \] ### Step 3: Substitute the values into the equation Substituting \( V_2 = \frac{8}{27} V_1 \): \[ T_2 = T_1 \left( \frac{V_1}{\frac{8}{27} V_1} \right)^{\gamma - 1} \] This simplifies to: \[ T_2 = T_1 \left( \frac{27}{8} \right)^{\gamma - 1} \] ### Step 4: Calculate \( \gamma - 1 \) \[ \gamma - 1 = \frac{5}{3} - 1 = \frac{2}{3} \] ### Step 5: Substitute \( T_1 \) and \( \gamma - 1 \) into the equation Now substituting \( T_1 = 300 \, K \): \[ T_2 = 300 \left( \frac{27}{8} \right)^{\frac{2}{3}} \] ### Step 6: Calculate \( \left( \frac{27}{8} \right)^{\frac{2}{3}} \) Calculating \( \left( \frac{27}{8} \right)^{\frac{2}{3}} \): \[ \frac{27}{8} = \left( \frac{3^3}{2^3} \right) = \left( \frac{3}{2} \right)^3 \] Thus, \[ \left( \frac{27}{8} \right)^{\frac{2}{3}} = \left( \frac{3}{2} \right)^2 = \frac{9}{4} \] ### Step 7: Substitute back to find \( T_2 \) Now substituting back: \[ T_2 = 300 \times \frac{9}{4} = 675 \, K \] ### Step 8: Calculate the rise in temperature \( \Delta T \) The rise in temperature is given by: \[ \Delta T = T_2 - T_1 = 675 \, K - 300 \, K = 375 \, K \] ### Final Answer The rise in temperature is \( \Delta T = 375 \, K \). ---
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