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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

2075 J

B

207.5 J

C

207.5 erg

D

201.1 erg

Text Solution

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The correct Answer is:
To solve the problem of finding the work done on a diatomic gas during an adiabatic compression, we can follow these steps: ### Step 1: Understand the Process Since the gas is compressed adiabatically, there is no heat exchange with the surroundings. Therefore, the heat added to the system \( Q = 0 \). ### Step 2: Use the First Law of Thermodynamics According to the first law of thermodynamics: \[ \Delta U = Q - W \] For an adiabatic process, \( Q = 0 \), so: \[ \Delta U = -W \] This means the work done on the gas \( W \) is equal to the negative change in internal energy \( \Delta U \). ### Step 3: Calculate the Change in Internal Energy The change in internal energy for an ideal gas can be calculated using the formula: \[ \Delta U = n C_V \Delta T \] Where: - \( n \) = number of moles (1 gm mol = 1 mol) - \( C_V \) = molar specific heat at constant volume - \( \Delta T \) = change in temperature in Kelvin For a diatomic gas, the degrees of freedom \( F \) is given by: \[ \gamma = \frac{C_P}{C_V} \quad \text{and} \quad C_P = C_V + R \] Given \( \gamma = 1.4 \), we can find \( C_V \): \[ \gamma = \frac{5}{3} \Rightarrow C_V = \frac{R}{\gamma - 1} = \frac{R}{0.4} = 2.5R \] Thus, \( C_V = \frac{5}{2} R \). ### Step 4: Calculate the Change in Temperature Convert the temperatures from Celsius to Kelvin: \[ T_1 = 27^\circ C = 300 K \] \[ T_2 = 127^\circ C = 400 K \] So, the change in temperature \( \Delta T \) is: \[ \Delta T = T_2 - T_1 = 400 K - 300 K = 100 K \] ### Step 5: Substitute Values into the Change in Internal Energy Formula Now we can calculate \( \Delta U \): \[ \Delta U = n C_V \Delta T = 1 \cdot \left(\frac{5}{2} R\right) \cdot 100 \] Using \( R = 8.31 \, J/(mol \cdot K) \): \[ \Delta U = \frac{5}{2} \cdot 8.31 \cdot 100 = 2077.5 \, J \] ### Step 6: Calculate the Work Done Since \( W = -\Delta U \): \[ W = -2077.5 \, J \] This indicates that the work is done on the gas. ### Final Answer The work done on the gas is: \[ W = -2077.5 \, J \]

To solve the problem of finding the work done on a diatomic gas during an adiabatic compression, we can follow these steps: ### Step 1: Understand the Process Since the gas is compressed adiabatically, there is no heat exchange with the surroundings. Therefore, the heat added to the system \( Q = 0 \). ### Step 2: Use the First Law of Thermodynamics According to the first law of thermodynamics: \[ ...
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