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For an isothermal reversible expansion p...

For an isothermal reversible expansion process, the value of q can be calculated by the expressin

A

`q=2.303 n RT log. (V_(2))/(V_(1))`

B

`q=-2.303nRT log.(V_(2))/(V_(1))`

C

`q=-2.303 nRT log. (V_(1))/(V_(2))`

D

`q=-P_("exp")nRT log.(V_(1))/(V_(2))`

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The correct Answer is:
To solve the problem regarding the calculation of \( q \) for an isothermal reversible expansion process, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Isothermal Process**: - An isothermal process is one where the temperature (\( T \)) of the system remains constant throughout the process. Therefore, the change in temperature (\( \Delta T \)) is equal to 0. 2. **Apply the First Law of Thermodynamics**: - The first law of thermodynamics states that: \[ \Delta U = Q + W \] - Where \( \Delta U \) is the change in internal energy, \( Q \) is the heat added to the system, and \( W \) is the work done by the system. 3. **Determine Change in Internal Energy**: - For an ideal gas, the change in internal energy (\( \Delta U \)) can be expressed as: \[ \Delta U = n C_V \Delta T \] - Since \( \Delta T = 0 \) for an isothermal process, it follows that: \[ \Delta U = 0 \] 4. **Relate Heat and Work**: - From the first law of thermodynamics, substituting \( \Delta U = 0 \): \[ 0 = Q + W \implies Q = -W \] 5. **Calculate Work Done (W)**: - The work done during an isothermal expansion of an ideal gas can be calculated using the formula: \[ W = -nRT \ln\left(\frac{V_2}{V_1}\right) \] - Here, \( n \) is the number of moles, \( R \) is the universal gas constant, \( T \) is the absolute temperature, \( V_2 \) is the final volume, and \( V_1 \) is the initial volume. 6. **Substitute Work into the Heat Equation**: - Now substituting the expression for \( W \) into the equation for \( Q \): \[ Q = -(-nRT \ln\left(\frac{V_2}{V_1}\right)) = nRT \ln\left(\frac{V_2}{V_1}\right) \] 7. **Final Expression for Q**: - Thus, we can express \( Q \) as: \[ Q = nRT \ln\left(\frac{V_2}{V_1}\right) \] 8. **Check Options**: - Finally, check the provided options to find the one that matches this derived expression for \( Q \).

To solve the problem regarding the calculation of \( q \) for an isothermal reversible expansion process, we can follow these steps: ### Step-by-Step Solution: 1. **Understand the Isothermal Process**: - An isothermal process is one where the temperature (\( T \)) of the system remains constant throughout the process. Therefore, the change in temperature (\( \Delta T \)) is equal to 0. 2. **Apply the First Law of Thermodynamics**: ...
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For an ideal gas, the work of reversible expansion under isothermal condition can be calculated by using expression = -nRT ln.(V_(f))/(V_(i)) . A sample containing 1.0 mol of an ideal gas is expanded isothermally and reversible to ten times of its original volume, in two separate experiments. The expansion is carried out at 300 K and at 600 K respectively. Choose the correct option

For an isothermal expansion of an ideal gas

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Calculate q,w , and DeltaU for the isothermal reversible expansion of one mole of an ideal gas from an initial pressure of 2.0 bar to a final pressure of 0.2 bar at a constant temperature of 273K .

The pressure-volume of varies thermodynamic process is shown in graphs: Work is the mole of transference of energy. It has been observed that reversible work done by the system is the maximum obtainable work. w_(rev) gt w_(irr) The works of isothermal and adiabatic processes are different from each other. w_("isothermal reversible") = 2.303 nRT log_(10) ((V_(2))/(V_(1))) = 2.303 nRT log_(10)((P_(2))/(P_(1))) w_("adiabatic reversible") = C_(V) (T_(1)-T_(2)) The q value and work done in isothermal reversible expansion of one mole of an ideal gas from initial pressure of 1 bar to final pressure of 0.1 bar at constant temperature 273K are:

For isothermal expansion , which is true?

NCERT FINGERTIPS ENGLISH-THERMODYNAMICS-Assertion And Reason
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