1. | same as the \(1^{\text{st}}\) case. |
2. | always greater than the \(1^{\text{st}}\) case. |
3. | always less than the \(1^{\text{st}}\) case. |
4. | may increase or decrease with respect to the \(1^{\text{st}}\) case. |
1. | \(Q_1=Q_2\) | 2. | \(5Q_1=3Q_2\) |
3. | \(Q_1=2Q_2\) | 4. | \(Q_2=2Q_1\) |
1. | \(R\) | 2. | \(2R\) |
3. | \(3R\) | 4. | \(4R\) |
1. | \(\dfrac{M v^2}{7 R} \) | 2. | \(\dfrac{M v^2}{5 R} \) |
3. | \(\dfrac{2M v^2}{7 R} \) | 4. | \(\dfrac{7M v^2}{5 R} \) |
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. |
1. | \(\Delta Q=\Delta U+\Delta W\) |
2. | \(\Delta U=\Delta Q+\Delta W\) |
3. | \(\Delta U=\Delta Q-\Delta W\) |
4. | \(\Delta U+\Delta Q+\Delta W=0\) |
1. | \(a\)–isothermal, \(b\)–monatomic adiabatic, \(c\)–diatomic adiabatic |
2. | \(a\)–monatomic adiabatic, \(b\)–diatomic adiabatic, \(c\)–isothermal |
3. | \(a\)–diatomic adiabatic, \(b\)–monatomic adiabatic, \(c\)–isothermal |
4. | \(a\)–isothermal, \(b\)–diatomic adiabatic, \(c\)–monatomic adiabatic |
1. | the pressure is halved |
2. | \(2\sqrt 2\) | the pressure decreases by a factor of
3. | the temperature is halved |
4. | the temperature decreases by a factor of \(2 \sqrt 2\) |