- 1(current)
Q. No.A gas undergoes an isothermal process. The specific heat capacity of the gas in the process is:
| 1. | infinity | 2. | \(0.5\) |
| 3. | zero | 4. | \(1\) |
Subtopic: Â Molar Specific Heat |
 72%
Level 2: 60%+
NEET - 2022
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One mole of an ideal monatomic gas undergoes a process described by the equation \(PV^3=\text{constant}.\) The heat capacity of the gas during this process is:
| 1. | \(\dfrac{3}{2}R\) | 2. | \(\dfrac{5}{2}R\) |
| 3. | \(2R\) | 4. | \(R\) |
Subtopic: Â Molar Specific Heat |
Level 3: 35%-60%
NEET - 2016
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The volume \((V)\) of a monatomic gas varies with its temperature \((T),\) as shown in the graph. The ratio of work done by the gas to the heat absorbed by it when it undergoes a change from state \(A\) to state \(B\) will be:
| 1. | \(\dfrac{2}{5}\) | 2. | \(\dfrac{2}{3}\) |
| 3. | \(\dfrac{1}{3}\) | 4. | \(\dfrac{2}{7}\) |
Subtopic: Â Molar Specific Heat |
 68%
Level 2: 60%+
NEET - 2018
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The molar specific heats of an ideal gas at constant pressure and volume are denoted by \(C_P\) and \(C_V,\) respectively. If \(\gamma =\frac{C_P}{C_V}\) and \(R\) is the universal gas constant, then \(C_V\) is equal to:
| 1. | \(\dfrac{R}{\gamma -1}\) | 2. | \(\dfrac{\gamma -1}{R}\) |
| 3. | \(\gamma R \) | 4. | \(\dfrac{\left ( \gamma -1 \right )R}{\left ( \gamma +1 \right )}\) |
Subtopic: Â Molar Specific Heat |
 89%
Level 1: 80%+
AIPMT - 2013
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- 1(current)
Q. No.
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