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One gm mol of a diatomic gas (gamma=1.4)...

One gm mol of a diatomic gas `(gamma=1.4)` is compressed adiabatically so that its temperature rises from `27^(@)C` to `127^(@)C` . The work done will be

A

`2077.5` joules

B

`207.5` joules

C

`207.5` ergs

D

`205.5` joules

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The correct Answer is:
To solve the problem of calculating the work done during the adiabatic compression of a diatomic gas, we can follow these steps: ### Step 1: Identify the parameters We have: - Number of moles, \( n = 1 \) gm mol = 1 mol - Initial temperature, \( T_1 = 27^\circ C = 300 \, K \) (convert to Kelvin by adding 273) - Final temperature, \( T_2 = 127^\circ C = 400 \, K \) (convert to Kelvin by adding 273) - Heat capacity at constant volume for a diatomic gas, \( C_v = \frac{R}{\gamma - 1} \) - Given \( \gamma = 1.4 \) ### Step 2: Calculate \( C_v \) Using the ideal gas constant \( R = 8.314 \, J/(mol \cdot K) \): \[ C_v = \frac{R}{\gamma - 1} = \frac{8.314}{1.4 - 1} = \frac{8.314}{0.4} = 20.785 \, J/(mol \cdot K) \] ### Step 3: Calculate the change in temperature \( \Delta T \) \[ \Delta T = T_2 - T_1 = 400 \, K - 300 \, K = 100 \, K \] ### Step 4: Calculate the change in internal energy \( \Delta U \) Using the formula for change in internal energy: \[ \Delta U = n C_v \Delta T = 1 \, mol \times 20.785 \, J/(mol \cdot K) \times 100 \, K = 2078.5 \, J \] ### Step 5: Calculate the work done \( W \) Since the process is adiabatic, the work done on the system is equal to the negative change in internal energy: \[ W = -\Delta U = -2078.5 \, J \] ### Step 6: State the magnitude of work done The magnitude of work done is: \[ |W| = 2078.5 \, J \] ### Final Answer The work done during the adiabatic compression is \( -2078.5 \, J \) (indicating work is done on the gas). ---

To solve the problem of calculating the work done during the adiabatic compression of a diatomic gas, we can follow these steps: ### Step 1: Identify the parameters We have: - Number of moles, \( n = 1 \) gm mol = 1 mol - Initial temperature, \( T_1 = 27^\circ C = 300 \, K \) (convert to Kelvin by adding 273) - Final temperature, \( T_2 = 127^\circ C = 400 \, K \) (convert to Kelvin by adding 273) - Heat capacity at constant volume for a diatomic gas, \( C_v = \frac{R}{\gamma - 1} \) ...
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