Column I | Column II | ||
\(\mathrm{(A)}\) | Work done in the process \(ab\) \((W_{ab})\) | \(\mathrm{(P)}\) | \(1.5R\) |
\(\mathrm{(B)}\) | Change in internal energy in the process \(ab\) \((\Delta U_{ab})\) | \(\mathrm{(Q)}\) | \(\dfrac {3P_0V_0}{2}\) |
\(\mathrm{(C)}\) | Molar heat capacity in the given process | \(\mathrm{(R)}\) | \(\dfrac {9P_0V_0}{2}\) |
\(\mathrm{(D)}\) | Molar heat capacity at constant volume \((C_{V})\) for the gas | \(\mathrm{(S)}\) | \(2R\) |
1. | \(\mathrm{A\text-P,B\text-Q,C\text-S,D\text-R}\) |
2. | \(\mathrm{A\text-R,B\text-Q,C\text-S,D\text-P}\) |
3. | \(\mathrm{A\text-Q,B\text-R,C\text-P,D\text-S}\) |
4. | \(\mathrm{A\text- Q,B\text-R,C\text-S,D\text-P}\) |
Statement I: | \(\mu\) amount of an ideal gas undergoes adiabatic change from state \(\left({P}_1, {V}_1, {T}_1\right)\) to state \(\left({P}_2, {V}_2, {T}_2\right)\), the work done is \({W}=\dfrac{\mu{R}\left({T}_2-{T}_1\right)}{1-\gamma}\), where \(\gamma=\dfrac{C_P}{C_V}\) and \(R=\) universal gas constant, |
When
Statement II: | In the above case, when work is done on the gas, the temperature of the gas would rise. |
1. | Both Statement I and Statement II are correct. |
2. | Both Statement I and Statement II are incorrect. |
3. | Statement I is correct, but statement II is incorrect. |
4. | Statement I is incorrect, but statement II is correct. |
Assertion (A): | Reversible systems are difficult to find in the real world. |
Reason (R): | Most processes are dissipative in nature. |
1. | Both (A) and (R) are true and (R) is the correct explanation of (A). |
2. | Both (A) and (R) are true but (R) is not the correct explanation of (A). |
3. | (A) is true but (R) is false. |
4. | Both (A) and (R) are false. |
Assertion (A): | It is possible that the temperature of a gas may fall even as it is being heated. |
Reason (R): | The specific heat capacity of a gas changes from process to process. |
1. | Both (A) and (R) are True and (R) is the correct explanation of (A). |
2. | Both (A) and (R) are True but (R) is not the correct explanation of (A). |
3. | (A) is True but (R) is False. |
4. | Both (A) and (R) are False. |
Statement I: | \(100\%\) if friction and all dissipative processes are reduced. | The efficiency of any thermodynamic engine can approach
Statement II: | The first law of thermodynamics is applicable only to non-living systems. |
1. | Statement I is incorrect and Statement II is correct. |
2. | Both Statement I and Statement II are correct. |
3. | Both Statement I and Statement II are incorrect. |
4. | Statement I is correct and Statement II is incorrect. |
Assertion (A): | In an isothermal process, whole of the heat energy supplied to the body is converted into internal energy. |
Reason (R): | \(\Delta Q = \Delta U + \Delta W \). | According to the first law of thermodynamics,
1. | Both (A) and (R) are True and (R) is the correct explanation of (A). |
2. | Both (A) and (R) are True but (R) is not the correct explanation of (A). |
3. | (A) is True but (R) is False. |
4. | (A) is False but (R) is True. |
1. | \(\Delta {U}=-{W}\) in an isothermal process. |
2. | \(\Delta {U}={W}\) in an isothermal process. |
3. | \(\Delta {U}=-{W}\) in an adiabatic process. |
4. | \(\Delta {U}={W}\) in an adiabatic process. |
1. | \(12~\text{J}\) | 2. | \(24~\text{J}\) |
3. | \(36~\text{J}\) | 4. | \(0~\text{J}\) |
An ideal gas heat engine operates in a Carnot cycle between 227ºC and 127ºC. It absorbs 6 × 104 cals of heat at higher temperatures.
The amount of heat converted to work will be?
1. 4.8 × 104 cals
2. 2.4 × 104 cals
3. 1.2 × 104 cals
4. 6 × 104 cals