Column I | Column II | ||
A. | \(W_{ab}\) | P. | \(1.5R\) |
B. | \(\Delta U_{ab}\) | Q. | \(\dfrac {3P_0V_0}{2}\) |
C. | molar heat capacity in the given process | R. | \(\dfrac {9P_0V_0}{2}\) |
D. | \(C_{V}\) for the gas | S. | \(2R\) |
1. | A → P, B → Q, C → S, D → R |
2. | A → R, B → Q, C → S, D → P |
3. | A → Q, B → R, C → P, D → S |
4. | A → Q, B → R, C → S, D → P |
Statement-I: | \(\mu\) amount of an ideal gas undergoes adiabatic change from state \(\left(\mathrm{P}_1, \mathrm{~V}_1, \mathrm{~T}_1\right)\) to state \(\left(\mathrm{P}_2, \mathrm{~V}_2, \mathrm{~T}_2 \right)\), the work done is, \(\mathrm{W}=\frac{\mu{R}\left(\mathrm{T}_2-\mathrm{T}_1\right)}{1-\gamma}\), where \(\gamma=\frac{C_P}{C_v}\) 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 true. |
2. | Both statement-I and statement-II are false. |
3. | Statement-I is true but statement-II is false. |
4. | Statement-I is false but statement-II is true. |
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. |
If a gas changes volume from 2 litres to 10 litres at a constant temperature of 300K, then the change in its internal energy will be:
1. | 12 J | 2. | 24 J |
3. | 36 J | 4. | 0 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