Entropy & Second Law — MH-CET Physics MCQs with Solutions
Free MH-CET Physics Entropy & Second Law MCQs with step-by-step solutions (33 questions). Part of Thermodynamics. Practise online on Prepizo — no login needed.
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Questions with solutions
Q1 — Entropy & Second Law · easy · theory
The change in entropy of a system that absorbs heat $Q$ reversibly at constant absolute temperature $T$ is:
A. $Q T^2$
B. $QT$
C. $\dfrac{Q}{T}$ ✓ Correct
D. $\dfrac{T}{Q}$
Solution: By definition $\Delta S = \dfrac{Q_{rev}}{T}$ for an isothermal reversible exchange of heat.
Q2 — Entropy & Second Law · easy · theory
The SI unit of entropy is:
A. $\text{J}/\text{kg}$
B. $\text{J}\cdot\text{K}$
C. $\text{J}/\text{K}$ ✓ Correct
D. $\text{J}$
Solution: From $\Delta S = \dfrac{Q}{T}$, entropy has the units of energy divided by temperature, i.e. $\text{J}/\text{K}$.
Q3 — Entropy & Second Law · easy · theory
For any irreversible process occurring in an isolated system, the total entropy:
A. Remains constant
B. Always increases ✓ Correct
C. Always decreases
D. May increase or decrease
Solution: This is the entropy statement of the second law: natural, spontaneous processes always increase the entropy of the universe.
Q4 — Entropy & Second Law · medium · theory
For a reversible process, the total entropy change of the system together with its surroundings is:
A. Always negative
B. Zero ✓ Correct
C. Infinite
D. Always positive
Solution: A reversible process is the limiting ideal case in which the entropy gained by one part exactly equals that lost by the other, so $\Delta S_{universe} = 0$.
Q5 — Entropy & Second Law · easy · theory
Entropy is best described physically as a measure of the:
A. Disorder or randomness of a system ✓ Correct
B. Temperature of a system
C. Total energy of a system
D. Pressure exerted by a system
Solution: Statistically, entropy counts the number of microscopic arrangements consistent with the macroscopic state; more disorder means more arrangements and higher entropy.
Q6 — Entropy & Second Law · medium · theory
Entropy is:
A. Always equal to the internal energy
B. A state function, independent of the path followed ✓ Correct
C. Defined only for irreversible processes
D. A path function, like work and heat
Solution: The entropy change between two states is the same whatever path connects them, which is why $\Delta S$ can be computed along a convenient reversible path.
Q7 — Entropy & Second Law · hard · numerical
One kilogram of ice melts at $0^\circ\text{C}$. Taking the latent heat of fusion as $3.34 \times 10^5\text{ J/kg}$, the entropy change of the ice is approximately:
A. $+334\text{ J/K}$
B. $+3.34 \times 10^5\text{ J/K}$
C. $+1223\text{ J/K}$ ✓ Correct
D. $-1223\text{ J/K}$
Solution: Melting occurs at the constant temperature $T = 273\text{ K}$, so $\Delta S = \dfrac{Q}{T} = \dfrac{3.34 \times 10^5}{273} \approx 1223\text{ J/K}$, positive because the liquid is more disordered.
Q8 — Entropy & Second Law · medium · numerical
A system absorbs $100\text{ J}$ of heat reversibly at a constant temperature of $400\text{ K}$. Its entropy change is:
A. $2.5\text{ J/K}$
B. $40000\text{ J/K}$
C. $4\text{ J/K}$
D. $0.25\text{ J/K}$ ✓ Correct
Solution: $\Delta S = \dfrac{Q}{T} = \dfrac{100}{400} = 0.25\text{ J/K}$.
Q9 — Entropy & Second Law · medium · theory
In a reversible adiabatic process, the entropy of the system:
A. Decreases steadily
B. Increases steadily
C. Remains constant, so the process is called isentropic ✓ Correct
D. Becomes zero
Solution: With $Q = 0$ and the process reversible, $\Delta S = \dfrac{Q_{rev}}{T} = 0$, so the entropy is unchanged throughout.
Q10 — Entropy & Second Law · hard · theory
The entropy change of $n$ moles of an ideal gas during a reversible isothermal expansion from $V_1$ to $V_2$ is:
A. $nRT\ln\dfrac{V_2}{V_1}$
B. $nR\ln\dfrac{V_2}{V_1}$ ✓ Correct
C. $nC_v\ln\dfrac{V_2}{V_1}$
D. $nR\ln\dfrac{V_1}{V_2}$
Solution: For an isothermal process $Q = W = nRT\ln\dfrac{V_2}{V_1}$, so $\Delta S = \dfrac{Q}{T} = nR\ln\dfrac{V_2}{V_1}$.
Q11 — Entropy & Second Law · hard · theory
The free expansion of a gas into a vacuum is accompanied by:
A. A decrease in internal energy
B. No change in entropy
C. A decrease in entropy
D. An increase in entropy, since the process is irreversible ✓ Correct
Solution: Although $Q = 0$, the process is irreversible. The gas occupies a larger volume with more accessible microstates, so its entropy rises.
Q12 — Entropy & Second Law · medium · theory
Heat flows spontaneously from a hot body to a cold body because this direction of flow:
A. Conserves entropy exactly
B. Increases the total entropy of the universe ✓ Correct
C. Is required by the first law
D. Decreases the total entropy of the universe
Solution: The cold body gains $\dfrac{Q}{T_C}$ while the hot body loses $\dfrac{Q}{T_H}$. Since $T_C < T_H$, the gain exceeds the loss and the net entropy change is positive.
Q13 — Entropy & Second Law · medium · theory
The second law of thermodynamics is needed, over and above the first law, because it:
A. Determines the direction in which a natural process proceeds ✓ Correct
B. Defines the temperature scale
C. Guarantees the conservation of energy
D. Applies only to ideal gases
Solution: Many energy-conserving processes never happen spontaneously. The second law, through entropy, distinguishes the possible direction from the impossible one.
Q14 — Entropy & Second Law · medium · theory
The third law of thermodynamics states that as the absolute temperature approaches zero, the entropy of a perfect crystal:
A. Becomes negative
B. Approaches zero ✓ Correct
C. Approaches infinity
D. Remains constant at a large value
Solution: At $0\text{ K}$ a perfect crystal has only one possible microscopic arrangement, so its disorder — and hence its entropy — tends to zero.
Q15 — Entropy & Second Law · medium · theory
Of the following, the process with the largest increase in entropy is:
A. A gas being compressed isothermally
B. Water freezing into ice at $0^\circ\text{C}$
C. A reversible adiabatic compression
D. Ice melting into water at $0^\circ\text{C}$ ✓ Correct
Solution: Melting converts an ordered crystal into a disordered liquid, so entropy increases. Freezing and isothermal compression both decrease it, and reversible adiabatic change leaves it unaltered.
Q16 — Entropy & Second Law · medium · theory
For a complete cycle of a reversible heat engine, the total entropy change of the working substance is:
A. Positive
B. Equal to $\dfrac{W}{T}$
C. Zero ✓ Correct
D. Negative
Solution: Entropy is a state function, so returning the working substance to its initial state makes its net entropy change zero over the cycle.
Q17 — Entropy & Second Law · easy · numerical
A system absorbs $500\text{ J}$ of heat reversibly at a constant temperature of $250\text{ K}$. Its entropy change is:
A. $2\text{ J/K}$ ✓ Correct
B. $0.5\text{ J/K}$
C. $125000\text{ J/K}$
D. $5\text{ J/K}$
Solution: $\Delta S = \dfrac{Q}{T} = \dfrac{500}{250} = 2\text{ J/K}$.
Q18 — Entropy & Second Law · hard · numerical
Two kilograms of ice melt at $0^\circ\text{C}$. Taking the latent heat of fusion as $3.34 \times 10^5\text{ J/kg}$, the entropy change is approximately:
A. $2447\text{ J/K}$ ✓ Correct
B. $1223\text{ J/K}$
C. $4894\text{ J/K}$
D. $668\text{ J/K}$
Solution: $Q = mL = 2 \times 3.34 \times 10^5 = 6.68 \times 10^5\text{ J}$ at $T = 273\text{ K}$, so $\Delta S = \dfrac{6.68 \times 10^5}{273} \approx 2447\text{ J/K}$.
Q19 — Entropy & Second Law · hard · numerical
Two moles of an ideal gas expand reversibly and isothermally until the volume doubles. The entropy change is ($R = 8.314$, $\ln 2 = 0.693$):
A. $23.1\text{ J/K}$
B. $3458\text{ J/K}$
C. $11.5\text{ J/K}$ ✓ Correct
D. $5.8\text{ J/K}$
Solution: $\Delta S = nR\ln\dfrac{V_2}{V_1} = 2 \times 8.314 \times 0.693 \approx 11.5\text{ J/K}$.
Q20 — Entropy & Second Law · hard · numerical
An amount of heat $1000\text{ J}$ flows from a body at $400\text{ K}$ to one at $300\text{ K}$. The net entropy change of the system is approximately:
A. Zero
B. $+5.83\text{ J/K}$
C. $-0.83\text{ J/K}$
D. $+0.83\text{ J/K}$ ✓ Correct
Solution: The cold body gains $\dfrac{1000}{300} = 3.33\text{ J/K}$ and the hot body loses $\dfrac{1000}{400} = 2.50\text{ J/K}$. The net change is $+0.83\text{ J/K}$, positive as required for an irreversible process.
Q21 — Entropy & Second Law · easy · numerical
A system absorbs $900\text{ J}$ of heat reversibly at $300\text{ K}$. Its entropy change is:
A. $0.33\text{ J/K}$
B. $2\text{ J/K}$
C. $270000\text{ J/K}$
D. $3\text{ J/K}$ ✓ Correct
Solution: $\Delta S = \dfrac{Q}{T} = \dfrac{900}{300} = 3\text{ J/K}$.
Q22 — Entropy & Second Law · easy · numerical
A system absorbs $800\text{ J}$ of heat reversibly at $200\text{ K}$. Its entropy change is:
A. $2\text{ J/K}$
B. $4\text{ J/K}$ ✓ Correct
C. $8\text{ J/K}$
D. $0.25\text{ J/K}$
Solution: $\Delta S = \dfrac{800}{200} = 4\text{ J/K}$.
Q23 — Entropy & Second Law · hard · numerical
Half a kilogram of ice melts at $0^\circ\text{C}$. Taking $L_f = 3.34 \times 10^5\text{ J/kg}$, the entropy change is approximately:
A. $306\text{ J/K}$
B. $2447\text{ J/K}$
C. $612\text{ J/K}$ ✓ Correct
D. $1223\text{ J/K}$
Solution: $Q = 0.5 \times 3.34 \times 10^5 = 1.67 \times 10^5\text{ J}$ at $273\text{ K}$, so $\Delta S = \dfrac{1.67 \times 10^5}{273} \approx 612\text{ J/K}$.
Q24 — Entropy & Second Law · hard · numerical
Three moles of an ideal gas expand reversibly and isothermally until the volume doubles. The entropy change is ($R = 8.314$, $\ln 2 = 0.693$):
A. $34.6\text{ J/K}$
B. $5.8\text{ J/K}$
C. $11.5\text{ J/K}$
D. $17.3\text{ J/K}$ ✓ Correct
Solution: $\Delta S = nR\ln 2 = 3 \times 8.314 \times 0.693 \approx 17.3\text{ J/K}$.
Q25 — Entropy & Second Law · hard · numerical
One mole of an ideal gas expands reversibly and isothermally to four times its volume. The entropy change is ($R = 8.314$, $\ln 4 = 1.386$):
A. $17.3\text{ J/K}$
B. $23.1\text{ J/K}$
C. $5.8\text{ J/K}$
D. $11.5\text{ J/K}$ ✓ Correct
Solution: $\Delta S = nR\ln 4 = 8.314 \times 1.386 \approx 11.5\text{ J/K}$.
Q26 — Entropy & Second Law · hard · numerical
Heat of $600\text{ J}$ flows from a body at $500\text{ K}$ to one at $300\text{ K}$. The net entropy change is:
A. $-0.8\text{ J/K}$
B. $+3.2\text{ J/K}$
C. Zero
D. $+0.8\text{ J/K}$ ✓ Correct
Solution: The cold body gains $\dfrac{600}{300} = 2\text{ J/K}$ and the hot body loses $\dfrac{600}{500} = 1.2\text{ J/K}$, giving a net $+0.8\text{ J/K}$.
Q27 — Entropy & Second Law · hard · numerical
One kilogram of water vaporises at $100^\circ\text{C}$. Taking $L_v = 2.26 \times 10^6\text{ J/kg}$, the entropy change is approximately:
A. $3030\text{ J/K}$
B. $2260\text{ J/K}$
C. $8278\text{ J/K}$
D. $6059\text{ J/K}$ ✓ Correct
Solution: $T = 373\text{ K}$, so $\Delta S = \dfrac{2.26 \times 10^6}{373} \approx 6059\text{ J/K}$.
Q28 — Entropy & Second Law · easy · numerical
A system absorbs $1000\text{ J}$ of heat reversibly at $250\text{ K}$. Its entropy change is:
A. $0.25\text{ J/K}$
B. $2.5\text{ J/K}$
C. $4\text{ J/K}$ ✓ Correct
D. $250\text{ J/K}$
Solution: $\Delta S = \dfrac{1000}{250} = 4\text{ J/K}$.
Q29 — Entropy & Second Law · medium · numerical
Over one complete cycle of a Carnot engine, the entropy change of the working substance is:
A. Zero ✓ Correct
B. Negative
C. Equal to $\dfrac{Q_H}{T_H}$
D. Positive
Solution: Entropy is a state function, so it returns to its initial value over a closed cycle: $\dfrac{Q_H}{T_H} - \dfrac{Q_C}{T_C} = 0$ for a Carnot cycle.
Q30 — Entropy & Second Law · easy · numerical
In a reversible adiabatic (isentropic) process, the entropy change of the system is:
A. Equal to $\dfrac{Q}{T}$ with $Q \neq 0$
B. Zero ✓ Correct
C. Positive
D. Negative
Solution: With $Q = 0$ and the process reversible, $\Delta S = \dfrac{Q_{rev}}{T} = 0$.