Entropy change in isothermal expansion of ideal gas from \(V\) to \(2V\):
A\(nR\ln 2\)
B0
C\(-nR\ln 2\)
D\(2nR\)
✅ Correct: A
\(\Delta S = Q/T = nRT\ln 2/T = \mathbf{nR\ln 2}\). Entropy increases in irreversible isothermal expansion.
Q14
Zeroth law of thermodynamics defines:
ATemperature
BEntropy
CInternal energy
DHeat capacity
✅ Correct: A
Zeroth law: if A and C are in thermal equilibrium, and B and C are in thermal equilibrium, then A and B are in equilibrium. This defines the concept of temperature as an intrinsic property.
Q15
A real gas obeys \((P + a/V^2)(V-b) = RT\). At very high temperature and large volume, it behaves as:
ASolid
BIdeal gas
CLiquid
DPlasma
✅ Correct: B
At high \(T\) and large \(V\): \(a/V^2 \to 0\) and \(b/V \to 0\). Equation reduces to \(PV = RT\) → behaves as ideal gas.
Q16
Heat required to raise 1 mole monoatomic ideal gas from \(T\) to \(2T\) at constant volume (\(R = 8.3\) J/mol K):
A\(\frac{3}{2}RT\)
B\(\frac{5}{2}RT\)
C\(3RT\)
D\(2RT\)
✅ Correct: A
\(Q = nC_v\Delta T = 1 \times \frac{3}{2}R \times T = \mathbf{\frac{3}{2}RT}\). For monoatomic gas \(C_v = \frac{3}{2}R\).
Q17
In a PV diagram, area enclosed by a closed cycle represents:
AChange in internal energy
BNet heat absorbed
CNet work done
DChange in entropy
✅ Correct: C
Area enclosed in PV diagram = \(\oint P\,dV\) = net work done by gas in one cycle. For clockwise cycle, work is positive (done by gas). For anticlockwise, work is done on gas.
Q18
Temperature at which Celsius and Fahrenheit scales give the same reading: