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The work done, W, during an isothermal p...

The work done, W, during an isothermal process in which the gas expands from an intial volume `V_(1)`, to a final volume `V_(2)` is given by (R : gas constant, T : temperature )

A

`R (V_(2)-V_(1)) log_(e _ ((T_(1))/(T_(2))`

B

`R (T_(2)-T_(1)) log_(e ) ((V_(1))/(V_(2)))`

C

`RT log_(e ) [(V_(2))/(V_(1))]`

D

`2RT log_(e ) [(V_(1))/(V_(2))]`

Text Solution

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The correct Answer is:
To solve the question regarding the work done, W, during an isothermal process where a gas expands from an initial volume \( V_1 \) to a final volume \( V_2 \), we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Work Done in an Isothermal Process**: The work done \( W \) on or by a gas during an isothermal process can be calculated using the formula: \[ W = \int_{V_1}^{V_2} P \, dV \] where \( P \) is the pressure and \( dV \) is the change in volume. 2. **Use the Ideal Gas Law**: According to the ideal gas law, we have: \[ PV = nRT \] For an isothermal process, the temperature \( T \) remains constant. Therefore, we can express pressure \( P \) in terms of volume \( V \): \[ P = \frac{nRT}{V} \] 3. **Substitute Pressure in the Work Done Formula**: Substitute \( P \) into the work done equation: \[ W = \int_{V_1}^{V_2} \frac{nRT}{V} \, dV \] 4. **Factor Out Constants**: Since \( nRT \) is constant during the isothermal process, we can factor it out of the integral: \[ W = nRT \int_{V_1}^{V_2} \frac{1}{V} \, dV \] 5. **Integrate**: The integral of \( \frac{1}{V} \) is: \[ \int \frac{1}{V} \, dV = \ln V \] Therefore, we have: \[ W = nRT \left[ \ln V \right]_{V_1}^{V_2} \] 6. **Evaluate the Integral**: Evaluating the definite integral gives: \[ W = nRT \left( \ln V_2 - \ln V_1 \right) \] 7. **Use Logarithmic Properties**: Using the property of logarithms that states \( \ln a - \ln b = \ln \left( \frac{a}{b} \right) \), we can rewrite the expression: \[ W = nRT \ln \left( \frac{V_2}{V_1} \right) \] ### Final Result: Thus, the work done during the isothermal expansion of the gas is given by: \[ W = nRT \ln \left( \frac{V_2}{V_1} \right) \]
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