The internal energy of a gas is given by U=2pV.U=2pV. The gas expands from 100100 cc to 200200 cc against a constant pressure of 105105 Pa. The heat absorbed by the gas is:
1. 1010 J
2. 2020 J
3. 3030 J
4. 4040 J
The ratio CP/CV=1.5CP/CV=1.5 for a certain ideal gas. The gas is taken at an initial pressure of 22 kPa and compressed suddenly to 1414 of its initial volume. The final pressure is:
1. 1212 kPa
2. 44 kPa
3. 88 kPa
4. 1616 kPa
An ideal gas is enclosed in a volume by means of a piston-cylinder arrangement as shown in the adjacent diagram. The piston as well as the walls of the cylinder are non-conducting. The cross-sectional area of the piston is A.A. Gravity gg is acting downward. A small block of mass mm is placed on top of the piston. There is no atmospheric pressure outside. An amount of thermal energy ΔQΔQ is slowly supplied to the gas, and its temperature rises. Then, the gas:
1. | expands continuously, making the volume infinite. |
2. | first expands and then contracts slightly. |
3. | expands and then reaches a steady-state. |
4. | expands and then contracts to return to its initial volume. |
In a reversible process, the change in internal energy UU of an ideal gas (CP/CV=γ)(CP/CV=γ) is zero, while the volume increases from VV to 2V2V. If the initial pressure is PP, the final pressure will be:
1. | 2P2P | 2. | P2P2 |
3. | PP | 4. | P2γP2γ |
The quantity of heat required to take a system from AA to CC through the process ABCABC is 2020 cal. The quantity of heat required to go from AA to CC directly is:
1. | 300300 K | 2. | 30025/330025/3 K |
3. | 30022/330022/3 K | 4. | 600600 K |
1. | U0ln(2)U0ln(2) | 2. | 12U0 ln(2)12U0 ln(2) |
3. | 13U0 ln(2)13U0 ln(2) | 4. | 23U0 ln(2) |
1. | VT = constant | 2. | V2T = constant |
3. | T2V = constant | 4. | TV2 = constant |
1. | 1.5% | increases by
2. | 1.5% | decreases by
3. | 13% | increases by
4. | 23% | increases by
1. | zero |
2. | negative |
3. | positive |
4. | non-negative(positive or zero) |