Which is the correct statement ?
(1) For an isothermal change PV = constant
(2) In an isothermal process the change in internal energy must be equal to the work done
(3) For an adiabatic change , where γ is the ratio of specific heats
(4) In an adiabatic process work done must be equal to the heat entering the system
1. | Isothermal curve slope = adiabatic curve slope |
2. | Isothermal curve slope = \(\gamma \times\) adiabatic curve slope |
3. | Adiabatic curve slope = \(\gamma \times\) isothermal curve slope |
4. | Adiabatic curve slope = \(\frac{1}{2}\times\) isothermal curve slope |
During the adiabatic expansion of 2 moles of a gas, the internal energy of the gas is found to decrease by 2 joules, the work done during the process by the gas will be equal to -
(1) 1 J
(2) –1 J
(3) 2 J
(4) – 2 J
If denotes the ratio of two specific heats of a gas, the ratio of slopes of adiabatic and isothermal PV curves at their point of intersection is
(1)
(2)
(3)
(4)
Air in a cylinder is suddenly compressed by a piston, which is then maintained at the same position. With the passage of time
1. | The pressure decreases |
2. | The pressure increases |
3. | The pressure remains the same |
4. | The pressure may increase or decrease depending upon the nature of the gas |
The adiabatic Bulk modulus of a perfect gas at pressure P is given by
(1) P
(2) 2P
(3) P/2
(4) γ P
An adiabatic process occurs at constant
(1) Temperature
(2) Pressure
(3) Heat
(4) Temperature and pressure
For adiabatic processes
(1) = constant
(2) = constant
(3) = constant
(4) = constant
An ideal gas is expanded adiabatically at an initial temperature of \(300~\text{K}\) so that its volume is doubled. The final temperature of the hydrogen gas is: \((\gamma = 1.40)~\left[2^{0.4}= 1.3\right]\)
1. \(230.76~\text{K}\)
2. \(500.30~\text{K}\)
3. \(454.76~\text{K}\)
4. \(-47~^{\circ}\text{C}\)
In an adiabatic expansion of a gas, if the initial and final temperatures are \(T_1\) and \(T_2\), respectively, then the change in internal energy of the gas is:
1. \(\frac{nR}{\gamma-1}(T_2-T_1)\)
2. \(\frac{nR}{\gamma-1}(T_1-T_2)\)
3. \(nR ~(T_1-T_2)\)
4. Zero