A thermodynamic system is taken from an original state A to an intermediate state B by a linear process as shown in the figure. It's volume is then reduced to the original value from B to C by an isobaric process. The total work done by the gas from A to B and B to C would be:
The graph plots Pressure (Dyne/cm^2) on the y-axis (with coordinates at 4000 and 8000) versus Volume (m^3) on the x-axis (with marks at 3 and 7). State path goes linearly from A to B, then horizontally from B to C.
The graph plots Pressure (Dyne/cm^2) on the y-axis (with coordinates at 4000 and 8000) versus Volume (m^3) on the x-axis (with marks at 3 and 7). State path goes linearly from A to B, then horizontally from B to C.
A.33800 ~J$33800 \mathrm{~J}$
B.2200 ~J$2200 \mathrm{~J}$
C.600 ~J$600 \mathrm{~J}$
D.1200 ~J$1200 \mathrm{~J}$
Solution & Explanation
Related Formula
Work done (W$W$) in a thermodynamic process corresponds to the area under the curve on a P-V$P-V$ diagram:
W = ∫ P dV$$W = \int P \, dV$$
Core Logic
Let's compute the work done along the distinct steps AB$AB$ and BC$BC$ matching the values shown in the graph:
The graph plots Pressure (Dyne/cm^2) on the y-axis (with coordinates at 4000 and 8000) versus Volume (m^3) on the x-axis (with marks at 3 and 7). State path goes linearly from A to B, then horizontally from B to C.
Step 1: Calculate Work Done in Process AB
Process AB$AB$ is a linear expansion. Fulfilling the area of the trapezoid underneath path AB$AB$:
Since 800 ~J$800 \mathrm{~J}$ is not present in the options, this question was declared a BONUS.
Pattern Recognition
Always be highly vigilant of mixed unit systems in thermodynamic graphics. Here, pressure is in CGS (Dyne/cm²$\text{Dyne/cm}^2$) while volume is in MKS (m³$\text{m}^3$). Converting early keeps you clear of algebraic traps.
More Thermodynamics Previous-Year Questions — Page 2
Q39jee_main_2026_23_january_eveningIsothermal and Adiabatic Processes
One mole of an ideal diatomic gas expands from volume V to 2V isothermally at a temperature27°$27^{\circ}$ C and does W joule of work. If the gas undergoes same magnitude of expansion adiabatically from 27°$27^{\circ}$ C doing the same amount of work W, then its final temperature will be (close to) ____ °${}^{\circ}$ C.
For a diatomic gas, γ = 1.4$\gamma = 1.4$.
Given initial temperature T = 27°C = 300 K$T = 27^{\circ}\mathrm{C} = 300 \, \mathrm{K}$.
Since Wisothermal = Wadiabatic$W_{\text{isothermal}} = W_{\text{adiabatic}}$, we equate the two expressions.
Equating the work of two different processes links the log expansion to the temperature drop. Recognize diatomic gas instantly means γ = 1.4$\gamma = 1.4$, providing the 0.4$0.4$ divisor.
Chapter Mix
Class 11 Physics: Thermodynamics
Q29jee_main_2026_24_january_morningFirst Law of Thermodynamics
Density of water at 4°$4^{\circ}$ C and 20°$20^{\circ}$ C are 1000 kg/m³$1000 \, kg/m^{3}$ and 998 kg/m³$998 \, kg/m^{3}$ respectively. The increase in internal energy of 4 kg water when it is heated from 4°$4^{\circ}$ C to 20°$20^{\circ}$ C is ____J.
(Specific heat capacity of water = 4.2 J/g°C$4.2 \, J/g^{\circ}C$ and 1 atmospheric pressure = 10⁵$10^{5}$ Pa)
Δ U = Q - W$$\Delta U = Q - W$$Δ U = 268800 - 0.8 = 268799.2 J$$\Delta U = 268800 - 0.8 = 268799.2 \text{ J}$$
Pattern Recognition
When heating solids or liquids, the expansion is so small that Δ V$\Delta V$ is negligible, meaning W ≈ 0$W \approx 0$, making Δ U ≈ Δ Q$\Delta U \approx \Delta Q$. Subtracting the exact 0.8J$0.8\text{J}$ provides the highly precise answer required here.
Chapter Mix
Class 11 Physics: Thermodynamics
Class 11 Physics: Thermal Properties of Matter
Q43jee_main_2026_24_january_eveningIsochoric Process and Heat Transfer
10 mole of an ideal gas is undergoing the process shown in the figure. The heat involved in the process from P₁$\mathrm{P}_{1}$ to P₂$\mathrm{P}_{2}$ is α$\alpha$ Joule ( P₁ = 21.7Pa$\mathrm{P}_{1} = 21.7\mathrm{Pa}$ and P₂ = 30Pa$\mathrm{P}_{2} = 30\mathrm{Pa}$ , Cv = 21J / K.mol$\mathrm{C}_{\mathrm{v}} = 21\mathrm{J / K.mol}$ , R = 8.3J / mol.K$R = 8.3\mathrm{J / mol.K}$ ). The value of α$\alpha$ is ____.
A Pressure-Volume graph displaying an isochoric rise from P1 to P2 at constant V=1.
A.24$24$
B.15$15$
C.21$21$
D.28$28$
Solution
Related Formula
Δ Q = n Cv Δ T$$\Delta Q = n C_v \Delta T$$
From Ideal Gas Law for Isochoric Process:
n R Δ T = Δ P · V$$n R \Delta T = \Delta P \cdot V$$
Core Logic
From the P-V graph, the process from P₁$P_1$ to P₂$P_2$ takes place at a constant volume V = 1 m³$V = 1 \text{ m}^3$.
For constant volume processes, Δ Q$\Delta Q$ strictly scales with Δ P$\Delta P$. Re-writing n Δ T$n \Delta T$ as V Δ P / R$V \Delta P / R$ circumvents calculating absolute temperatures entirely.
Chapter Mix
Class 11 Physics: Thermodynamics
Q46jee_main_2026_24_january_eveningSpecific Heat of Gases
When 300 J of heat given to an ideal gas with Cₚ=(7)/(2)R$C_{p}=\frac{7}{2}R$ its temperature raises from 20 °C to 50 °C keeping its volume constant. The mass of the gas is (approximately) ____ g. (R = 8.314 J/mol.K).
Numerical Answer.Answer: 481 to 481
Solution
Related Formula
Cv = CP - R$C_v = C_P - R$
Δ Q = n CV Δ T$$\Delta Q = n C_V \Delta T$$
Core Logic
Cv = (7)/(2)R - R = (5)/(2)R$$C_v = \frac{7}{2}R - R = \frac{5}{2}R$$
For an isochoric process (constant volume), the heat given is strictly equal to internal energy change:
300 = n × (5)/(2) × 8.314 × 30$$300 = n \times \frac{5}{2} \times 8.314 \times 30$$300 = n × 75 × 8.314$$300 = n \times 75 \times 8.314$$n = 0.48 moles$$n = 0.48 \text{ moles}$$(m)/(M) = 0.48$$\frac{m}{M} = 0.48$$
Step 2: Evaluating the output
Our Ans. (Bonus)
We cannot definitively find the mass (m$m$) in grams because the molar mass (M$M$) of the specific ideal gas is not given in the problem statement.
(Note: NTA official answer is 481. This implies assuming M ≈ 1000$M \approx 1000$ or an error in problem specification).
Pattern Recognition
Always extract Cv$C_v$ from Cₚ$C_p$ using Mayer's relation for constant volume heat transfers. If an exam sets a numerical without giving molar mass, it relies on partial contextual hints or is marked as bonus.
Chapter Mix
Class 11 Physics: Thermodynamics
Q37jee_main_2026_28_january_morningWork Done in Thermodynamic Processes
In the following p - V$p - V$ diagram the equation of state along the curved path is given by (V - 2)² = 4ap$(V - 2)^2 = 4ap$ where a$a$ is a constant. The total work done in the closed path is
A p-V graph indicating a cyclic process clockwise with points A at V=1, C at V=3 and a parabolic curve below.
A.-(1)/(a)$-\frac{1}{a}$
B.+(1)/(3a)$+\frac{1}{3a}$
C.(1)/(2a)$\frac{1}{2a}$
D.-(1)/(3a)$-\frac{1}{3a}$
Solution
Related Formula
W = ∫ p dV$$W = \int p \, dV$$
Core Logic
The total work done in a cyclic process is the enclosed area. The cycle is clockwise, but wait—the arrows in the diagram point anti-clockwise (A to B to C and back to A via horizontal top line). Anti-clockwise cycle means negative work. The enclosed area is bounded by a parabola.
Step 1: Identifying the Parabola Parameters
Equation of curve: (V - 2)² = 4ap$(V - 2)^2 = 4ap$
This is an upward-opening parabola with vertex at V = 2$V = 2$, p = 0$p = 0$ (assuming a>0$a>0$).
Let's check points A (V=1$V=1$) and C (V=3$V=3$).
At V=1$V=1$: (1 - 2)² = 4ap ⇒ 1 = 4ap₀ ⇒ p₀ = (1)/(4a)$(1 - 2)^2 = 4ap \Rightarrow 1 = 4ap_0 \Rightarrow p_0 = \frac{1}{4a}$
At V=3$V=3$: (3 - 2)² = 4ap ⇒ 1 = 4ap₀ ⇒ p₀ = (1)/(4a)$(3 - 2)^2 = 4ap \Rightarrow 1 = 4ap_0 \Rightarrow p_0 = \frac{1}{4a}$
So the top horizontal line is at p₀ = (1)/(4a)$p_0 = \frac{1}{4a}$.
Step 2: Area Calculation
The enclosed shape is bounded by the line p = p₀$p = p_0$ and the parabola p = ((V - 2)²)/(4a)$p = \frac{(V - 2)^2}{4a}$.
The area of a parabolic segment (bounded by a chord) is (2)/(3) × Area of enclosing rectangle$\frac{2}{3} \times \text{Area of enclosing rectangle}$.
Rectangle width = Δ V = 3 - 1 = 2$\Delta V = 3 - 1 = 2$.
Rectangle height = p₀ - 0 = p₀$p_0 - 0 = p_0$.
Area = (2)/(3) × (p₀) × (2) = (4p₀)/(3)$\frac{2}{3} \times (p_0) \times (2) = \frac{4p_0}{3}$.
For parabolic curves y = kx²$y = kx^2$, the area inside the 'bowl' up to a chord is 2/3$2/3$ of the bounding rectangle. Direction of arrows dictates the sign: clockwise = positive, anti-clockwise = negative.
Chapter Mix
Class 11 Physics: Thermodynamics
More Thermodynamics Questions — jee_main_2024_29_jan_morning
Practice past-year questions one chapter at a time. Pick an exam → subject → chapter and get every PYQ for that topic — pulled together from all past papers — with the chapter's key formulas alongside.