Thermodynamic Processes
PHXI12:THERMODYNAMICS

371612 Find the pressure at which temperature attains its maximum value if the relation between pressure and volume for an ideal is \(P=P_{0}+(1-\alpha) V^{2} ; \alpha>1\)

1 \(\dfrac{P_{0}}{3}\)
2 \(\dfrac{2 P_{0}}{3}\)
3 \(\dfrac{4 P_{0}}{3}\)
4 \(P_{0}\)
PHXI12:THERMODYNAMICS

371613 An ideal gas with adiabatic exponent \((\gamma=1.5)\) undergoes a process in which work done by the gas is same as increase in internal energy of the gas. The molar heat capacity of gas for the process is -

1 \(C = 4\,R\)
2 \(C = 0\)
3 \(C = 2\,R\)
4 \(C = R\)
PHXI12:THERMODYNAMICS

371614 A gas expand with temperature according to the relation \(V=K T^{2 / 3}\). What is the work done when the temperature changes by \(30^\circ C\) ?

1 \(20\,R\)
2 \(10\,R\)
3 \(40\,R\)
4 \(30\,R\)
PHXI12:THERMODYNAMICS

371615 Which of the following processes is reversible?

1 Transfer of heat by radiation
2 Transfer of heat by conduction
3 Electrical heating of a nichrome wire
4 Isothermal compression
NEET Test Series from KOTA - 10 Papers In MS WORD WhatsApp Here
PHXI12:THERMODYNAMICS

371612 Find the pressure at which temperature attains its maximum value if the relation between pressure and volume for an ideal is \(P=P_{0}+(1-\alpha) V^{2} ; \alpha>1\)

1 \(\dfrac{P_{0}}{3}\)
2 \(\dfrac{2 P_{0}}{3}\)
3 \(\dfrac{4 P_{0}}{3}\)
4 \(P_{0}\)
PHXI12:THERMODYNAMICS

371613 An ideal gas with adiabatic exponent \((\gamma=1.5)\) undergoes a process in which work done by the gas is same as increase in internal energy of the gas. The molar heat capacity of gas for the process is -

1 \(C = 4\,R\)
2 \(C = 0\)
3 \(C = 2\,R\)
4 \(C = R\)
PHXI12:THERMODYNAMICS

371614 A gas expand with temperature according to the relation \(V=K T^{2 / 3}\). What is the work done when the temperature changes by \(30^\circ C\) ?

1 \(20\,R\)
2 \(10\,R\)
3 \(40\,R\)
4 \(30\,R\)
PHXI12:THERMODYNAMICS

371615 Which of the following processes is reversible?

1 Transfer of heat by radiation
2 Transfer of heat by conduction
3 Electrical heating of a nichrome wire
4 Isothermal compression
PHXI12:THERMODYNAMICS

371612 Find the pressure at which temperature attains its maximum value if the relation between pressure and volume for an ideal is \(P=P_{0}+(1-\alpha) V^{2} ; \alpha>1\)

1 \(\dfrac{P_{0}}{3}\)
2 \(\dfrac{2 P_{0}}{3}\)
3 \(\dfrac{4 P_{0}}{3}\)
4 \(P_{0}\)
PHXI12:THERMODYNAMICS

371613 An ideal gas with adiabatic exponent \((\gamma=1.5)\) undergoes a process in which work done by the gas is same as increase in internal energy of the gas. The molar heat capacity of gas for the process is -

1 \(C = 4\,R\)
2 \(C = 0\)
3 \(C = 2\,R\)
4 \(C = R\)
PHXI12:THERMODYNAMICS

371614 A gas expand with temperature according to the relation \(V=K T^{2 / 3}\). What is the work done when the temperature changes by \(30^\circ C\) ?

1 \(20\,R\)
2 \(10\,R\)
3 \(40\,R\)
4 \(30\,R\)
PHXI12:THERMODYNAMICS

371615 Which of the following processes is reversible?

1 Transfer of heat by radiation
2 Transfer of heat by conduction
3 Electrical heating of a nichrome wire
4 Isothermal compression
PHXI12:THERMODYNAMICS

371612 Find the pressure at which temperature attains its maximum value if the relation between pressure and volume for an ideal is \(P=P_{0}+(1-\alpha) V^{2} ; \alpha>1\)

1 \(\dfrac{P_{0}}{3}\)
2 \(\dfrac{2 P_{0}}{3}\)
3 \(\dfrac{4 P_{0}}{3}\)
4 \(P_{0}\)
PHXI12:THERMODYNAMICS

371613 An ideal gas with adiabatic exponent \((\gamma=1.5)\) undergoes a process in which work done by the gas is same as increase in internal energy of the gas. The molar heat capacity of gas for the process is -

1 \(C = 4\,R\)
2 \(C = 0\)
3 \(C = 2\,R\)
4 \(C = R\)
PHXI12:THERMODYNAMICS

371614 A gas expand with temperature according to the relation \(V=K T^{2 / 3}\). What is the work done when the temperature changes by \(30^\circ C\) ?

1 \(20\,R\)
2 \(10\,R\)
3 \(40\,R\)
4 \(30\,R\)
PHXI12:THERMODYNAMICS

371615 Which of the following processes is reversible?

1 Transfer of heat by radiation
2 Transfer of heat by conduction
3 Electrical heating of a nichrome wire
4 Isothermal compression