Thermodynamic Systems & Zeroth Law — MH-CET Physics MCQs with Solutions
Free MH-CET Physics Thermodynamic Systems & Zeroth Law MCQs with step-by-step solutions (34 questions). Part of Thermodynamics. Practise online on Prepizo — no login needed.
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Questions with solutions
Q1 — Thermodynamic Systems & Zeroth Law · easy · theory
The zeroth law of thermodynamics states that if two systems are each in thermal equilibrium with a third system, then:
A. They are in thermal equilibrium with each other ✓ Correct
B. They must have equal volumes
C. Heat flows spontaneously between them
D. They must have equal internal energies
Solution: This law establishes temperature as a valid physical property: bodies in mutual thermal equilibrium share a common temperature, which is what a thermometer measures.
Q2 — Thermodynamic Systems & Zeroth Law · medium · theory
Which of the following is NOT a thermodynamic state variable?
A. Internal energy
B. Work done ✓ Correct
C. Pressure
D. Temperature
Solution: Pressure, volume, temperature and internal energy depend only on the current state of the system. Work and heat depend on the path taken, so they are path functions, not state variables.
Q3 — Thermodynamic Systems & Zeroth Law · easy · theory
The work done by a gas expanding at constant pressure $P$ from volume $V_1$ to $V_2$ is:
A. $P(V_2 - V_1)$ ✓ Correct
B. $\dfrac{1}{2}P(V_2 - V_1)$
C. $\dfrac{P}{V_2 - V_1}$
D. $P V_1 V_2$
Solution: For an isobaric process $W = \int P\,dV = P\int dV = P\,\Delta V = P(V_2 - V_1)$.
Q4 — Thermodynamic Systems & Zeroth Law · medium · numerical
During an isobaric expansion of $2\text{ moles}$ of an ideal gas, the temperature rises by $50\text{ K}$. The work done by the gas is ($R = 8.314\text{ J}\cdot\text{mol}^{-1}\cdot\text{K}^{-1}$):
A. $1662.8\text{ J}$
B. $415.7\text{ J}$
C. $831.4\text{ J}$ ✓ Correct
D. $1247\text{ J}$
Solution: At constant pressure $W = P\,\Delta V = nR\,\Delta T = 2 \times 8.314 \times 50 = 831.4\text{ J}$.
Q5 — Thermodynamic Systems & Zeroth Law · easy · theory
On a $P$-$V$ indicator diagram, the work done by a gas during a process is represented by:
A. The intercept on the pressure axis
B. The area under the curve ✓ Correct
C. The length of the curve
D. The slope of the curve
Solution: Since $W = \int P\,dV$, the work is the area between the process curve and the volume axis.
Q6 — Thermodynamic Systems & Zeroth Law · easy · theory
For a gas taken around a complete cyclic process, the change in internal energy is:
A. Equal to the heat absorbed
B. Always positive
C. Equal to the work done
D. Zero ✓ Correct
Solution: Internal energy is a state function, so returning to the initial state means $\Delta U = 0$, whatever path the cycle follows.
Q7 — Thermodynamic Systems & Zeroth Law · easy · theory
In a cyclic process, the net heat absorbed by the system is equal to:
A. Zero
B. The change in temperature
C. The net work done by the system ✓ Correct
D. The change in internal energy
Solution: The first law gives $Q = \Delta U + W$, and with $\Delta U = 0$ over a cycle, $Q = W$.
Q8 — Thermodynamic Systems & Zeroth Law · medium · theory
The net work done by a gas during a cyclic process on a $P$-$V$ diagram is equal to:
A. Zero in all cases
B. The area enclosed by the closed loop ✓ Correct
C. The area under the upper curve only
D. The perimeter of the loop
Solution: Expansion contributes positive area and compression negative area, so the net work is the area enclosed by the cycle.
Q9 — Thermodynamic Systems & Zeroth Law · medium · theory
A cyclic process traced in the clockwise sense on a $P$-$V$ diagram represents a process in which:
A. No net work is done
B. Net work is done by the gas and heat is converted into work ✓ Correct
C. Net work is done on the gas
D. The internal energy increases each cycle
Solution: A clockwise loop expands at high pressure and compresses at low pressure, so the positive area dominates. This is the cycle of a heat engine.
Q10 — Thermodynamic Systems & Zeroth Law · easy · theory
In an isochoric (constant volume) process, the work done by the gas is:
A. Equal to $nR\Delta T$
B. Equal to $P\Delta V$
C. Zero ✓ Correct
D. Equal to the heat supplied
Solution: With $\Delta V = 0$, $W = P\,\Delta V = 0$. All the heat supplied therefore goes into raising the internal energy.
Q11 — Thermodynamic Systems & Zeroth Law · medium · theory
A quasi-static thermodynamic process is one that is carried out:
A. Without any exchange of heat
B. As rapidly as possible
C. At constant pressure only
D. So slowly that the system remains in equilibrium at every stage ✓ Correct
Solution: Only if the process is infinitesimally slow can the pressure and temperature be well defined throughout, which is what allows the state to be plotted as a curve.
Q12 — Thermodynamic Systems & Zeroth Law · medium · theory
Which of the following pairs correctly classifies the quantities as intensive and extensive respectively?
A. Mass and volume
B. Volume and temperature
C. Temperature and volume ✓ Correct
D. Temperature and pressure
Solution: Intensive properties (temperature, pressure, density) do not depend on the amount of matter; extensive properties (volume, mass, internal energy) scale with it.
Q13 — Thermodynamic Systems & Zeroth Law · medium · theory
Internal energy is a state function whereas heat and work are:
A. Path functions, depending on how the change is brought about ✓ Correct
B. Also state functions
C. Always equal to each other
D. Always zero
Solution: Two different paths between the same pair of states give the same $\Delta U$ but generally different $Q$ and $W$.
Q14 — Thermodynamic Systems & Zeroth Law · easy · theory
Two bodies are said to be in thermal equilibrium when:
A. They have equal heat capacities
B. There is no net flow of heat between them ✓ Correct
C. They have equal masses
D. They have equal internal energies
Solution: Thermal equilibrium means both are at the same temperature, so heat flows equally in both directions and there is no net transfer.
Q15 — Thermodynamic Systems & Zeroth Law · easy · theory
A wall that permits no exchange of heat between a system and its surroundings is called:
A. A diathermic wall
B. An isothermal wall
C. A conducting wall
D. An adiabatic wall ✓ Correct
Solution: An adiabatic (perfectly insulating) wall blocks heat flow, whereas a diathermic wall conducts heat freely and allows the two sides to reach a common temperature.
Q16 — Thermodynamic Systems & Zeroth Law · easy · theory
By the usual sign convention in thermodynamics, work done by the system and heat absorbed by the system are taken respectively as:
A. Negative and positive
B. Positive and positive ✓ Correct
C. Positive and negative
D. Negative and negative
Solution: Heat added to the system and work done by the system are both counted positive, which is why the first law is written $Q = \Delta U + W$.
Q17 — Thermodynamic Systems & Zeroth Law · easy · numerical
A gas expands by $0.01\text{ m}^3$ against a constant external pressure of $2 \times 10^5\text{ Pa}$. The work done by the gas is:
A. $20000\text{ J}$
B. $200\text{ J}$
C. $2000\text{ J}$ ✓ Correct
D. $2 \times 10^7\text{ J}$
Solution: $W = P\Delta V = 2 \times 10^5 \times 0.01 = 2000\text{ J}$.
Q18 — Thermodynamic Systems & Zeroth Law · medium · numerical
Three moles of an ideal gas are heated at constant pressure so that the temperature rises by $40\text{ K}$. The work done by the gas is ($R = 8.314$):
A. $333\text{ J}$
B. $998\text{ J}$ ✓ Correct
C. $2494\text{ J}$
D. $1663\text{ J}$
Solution: $W = nR\Delta T = 3 \times 8.314 \times 40 \approx 998\text{ J}$.
Q19 — Thermodynamic Systems & Zeroth Law · easy · numerical
A gas at a constant pressure of $10^5\text{ Pa}$ expands from $0.02\text{ m}^3$ to $0.05\text{ m}^3$. The work done is:
A. $5000\text{ J}$
B. $3000\text{ J}$ ✓ Correct
C. $7000\text{ J}$
D. $2000\text{ J}$
Solution: $W = P(V_2 - V_1) = 10^5 \times (0.05 - 0.02) = 10^5 \times 0.03 = 3000\text{ J}$.
Q20 — Thermodynamic Systems & Zeroth Law · medium · numerical
A gas is carried around a clockwise cycle enclosing an area of $500\text{ J}$ on a $P$-$V$ diagram. The net heat absorbed per cycle is:
A. $-500\text{ J}$
B. $500\text{ J}$ ✓ Correct
C. $1000\text{ J}$
D. Zero
Solution: Over a cycle $\Delta U = 0$, so $Q = W$. The clockwise area gives $W = +500\text{ J}$, hence $Q = 500\text{ J}$.
Q21 — Thermodynamic Systems & Zeroth Law · easy · numerical
A gas in a rigid closed vessel is supplied with $300\text{ J}$ of heat. The increase in its internal energy is:
A. $150\text{ J}$
B. Zero
C. $600\text{ J}$
D. $300\text{ J}$ ✓ Correct
Solution: A rigid vessel means $\Delta V = 0$, so $W = 0$ and the first law gives $\Delta U = Q = 300\text{ J}$.
Q22 — Thermodynamic Systems & Zeroth Law · easy · numerical
A gas expands by $0.04\text{ m}^3$ against a constant pressure of $5 \times 10^4\text{ Pa}$. The work done by the gas is:
A. $2000\text{ J}$ ✓ Correct
B. $20000\text{ J}$
C. $1250\text{ J}$
D. $200\text{ J}$
Solution: $W = P\Delta V = 5 \times 10^4 \times 0.04 = 2000\text{ J}$.
Q23 — Thermodynamic Systems & Zeroth Law · medium · numerical
Four moles of an ideal gas are heated at constant pressure through $25\text{ K}$. The work done by the gas is ($R = 8.314$):
A. $831\text{ J}$ ✓ Correct
B. $1663\text{ J}$
C. $208\text{ J}$
D. $2494\text{ J}$
Solution: $W = nR\Delta T = 4 \times 8.314 \times 25 \approx 831\text{ J}$.
Q24 — Thermodynamic Systems & Zeroth Law · easy · numerical
A gas at a constant pressure of $2 \times 10^5\text{ Pa}$ expands from $0.01\text{ m}^3$ to $0.04\text{ m}^3$. The work done is:
A. $3000\text{ J}$
B. $2000\text{ J}$
C. $8000\text{ J}$
D. $6000\text{ J}$ ✓ Correct
Solution: $W = P(V_2 - V_1) = 2 \times 10^5 \times 0.03 = 6000\text{ J}$.
Q25 — Thermodynamic Systems & Zeroth Law · medium · numerical
A gas is taken clockwise around a cycle enclosing an area of $800\text{ J}$ on a $P$-$V$ diagram. The net work done by the gas per cycle is:
A. $800\text{ J}$ ✓ Correct
B. Zero
C. $-800\text{ J}$
D. $1600\text{ J}$
Solution: The enclosed area is the net work, and a clockwise sense means the gas does positive work on the surroundings.
Q26 — Thermodynamic Systems & Zeroth Law · easy · numerical
A gas in a rigid sealed container absorbs $450\text{ J}$ of heat. The increase in its internal energy is:
A. $900\text{ J}$
B. $225\text{ J}$
C. $450\text{ J}$ ✓ Correct
D. Zero
Solution: A rigid container gives $\Delta V = 0$, so $W = 0$ and $\Delta U = Q = 450\text{ J}$.
Q27 — Thermodynamic Systems & Zeroth Law · medium · numerical
A gas is compressed at a constant pressure of $10^5\text{ Pa}$ from $0.05\text{ m}^3$ to $0.02\text{ m}^3$. The work done on the gas is:
A. $3000\text{ J}$ ✓ Correct
B. $5000\text{ J}$
C. $7000\text{ J}$
D. $2000\text{ J}$
Solution: $|W| = P|\Delta V| = 10^5 \times 0.03 = 3000\text{ J}$, done on the gas since the volume decreases.
Q28 — Thermodynamic Systems & Zeroth Law · medium · numerical
Three moles of an ideal gas are heated at constant pressure through $100\text{ K}$. The work done by the gas is ($R = 8.314$):
A. $1247\text{ J}$
B. $3741\text{ J}$
C. $831\text{ J}$
D. $2494\text{ J}$ ✓ Correct
Solution: $W = nR\Delta T = 3 \times 8.314 \times 100 \approx 2494\text{ J}$.
Q29 — Thermodynamic Systems & Zeroth Law · hard · numerical
A gas is taken anticlockwise around a cycle enclosing an area of $600\text{ J}$ on a $P$-$V$ diagram. The net work done by the gas is:
A. $-1200\text{ J}$
B. $-600\text{ J}$ ✓ Correct
C. Zero
D. $+600\text{ J}$
Solution: An anticlockwise cycle means net work is done on the gas, so the work done by the gas is negative. This is the cycle of a refrigerator.
Q30 — Thermodynamic Systems & Zeroth Law · easy · numerical
A gas is heated at constant volume and its internal energy rises by $500\text{ J}$. The heat supplied is:
A. $1000\text{ J}$
B. Zero
C. $250\text{ J}$
D. $500\text{ J}$ ✓ Correct
Solution: With $W = 0$ at constant volume, the first law gives $Q = \Delta U = 500\text{ J}$.