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JEE Advanced 2026Paper 2
Exam
JEE Advanced
Year
2026
Paper
Paper 2
Subject
Physics
Chapter
Thermodynamics

JEE Advanced 2026 · Paper 2 · Physics · Thermodynamics

Ten moles of an ideal monoatomic gas, initially in state a at...

Ten moles of an ideal monoatomic gas, initially in state a\boldsymbol{a} at atmospheric pressure and temperature Ta=27∘T_a = 27^\circC, is enclosed in a metal cylinder of volume V0V_0 fitted with a frictionless piston. The gas is suddenly compressed to state b\boldsymbol{b} with volume V0/3V_0/3. Now, keeping the piston stationary, the cylinder is submerged in a water bath of temperature 11∘11^\circC until the gas reaches the temperature of the water bath, which is denoted as state c\boldsymbol{c}. Finally, while still in the water bath, the piston is brought slowly to its initial position, which is denoted as state f\boldsymbol{f}. If RR is universal gas constant, then the correct option(s) is/are:
[Given: 91/3=2.089^{1/3} = 2.08]Ten moles of an ideal monoatomic gas, initially in state a at atmospheric pressure and temperature T_a = 27^ C, is

Options

  1. AThe schematic P-V diagram of the processes described above is: The value of _ x arrow 0 (1)/(x^3) ∫_0^x (t (1+t))/(t^4+4) d t is
  2. BThe change in internal energy in going from state a\boldsymbol{a} to b\boldsymbol{b} is 4860R4860R.
  3. CThe net change in the internal energy in the whole process is −240R-240R.
  4. DThe pressure and temperature of the state b\boldsymbol{b} are 2.082.08 times the atmospheric pressure and 624624 K, respectively.

Correct answer

A. The schematic P-V diagram of the processes described above is: The value of _ x arrow 0 (1)/(x^3) ∫_0^x (t (1+t))/(t^4+4) d t is

Step-by-step solution

For state aa: n=10n = 10, Ta=27∘C=300 KT_a = 27^{\circ}\text{C} = 300\text{ K}, Pa=1 atmP_a = 1\text{ atm}, Va=V0V_a = V_0.
For a monoatomic gas, Cv=32RC_v = \dfrac{3}{2}R and γ=53\gamma = \dfrac{5}{3}.

Process a→ba \rightarrow b is a sudden compression, which is an adiabatic process.
Vb=V03V_b = \dfrac{V_0}{3}
Using TaVaγ−1=TbVbγ−1T_a V_a^{\gamma-1} = T_b V_b^{\gamma-1}:
Tb=Ta(VaVb)γ−1=300×(3)5/3−1=300×32/3=300×(9)1/3T_b = T_a \left(\dfrac{V_a}{V_b}\right)^{\gamma-1} = 300 \times (3)^{5/3 - 1} = 300 \times 3^{2/3} = 300 \times (9)^{1/3}
Given 91/3=2.089^{1/3} = 2.08, we get Tb=300×2.08=624 KT_b = 300 \times 2.08 = 624\text{ K}.
Using PaVaγ=PbVbγP_a V_a^\gamma = P_b V_b^\gamma:
Pb=Pa(VaVb)γ=1×(3)5/3=3×32/3=3×2.08=6.24 atmP_b = P_a \left(\dfrac{V_a}{V_b}\right)^\gamma = 1 \times (3)^{5/3} = 3 \times 3^{2/3} = 3 \times 2.08 = 6.24\text{ atm}.
Thus, the pressure at state bb is 6.246.24 times the atmospheric pressure. Option (D) is incorrect.

The change in internal energy for process a→ba \rightarrow b is:
ΔUab=nCv(Tb−Ta)=10×32R×(624−300)=15R×324=4860R\Delta U_{ab} = n C_v (T_b - T_a) = 10 \times \dfrac{3}{2}R \times (624 - 300) = 15R \times 324 = 4860R.
Option (B) is correct.

Process b→cb \rightarrow c is isochoric (stationary piston), so Vc=V03V_c = \dfrac{V_0}{3}.
The gas cools to the water bath temperature, Tc=11∘C=284 KT_c = 11^{\circ}\text{C} = 284\text{ K}.

Process c→fc \rightarrow f is isothermal (slow expansion in water bath), so Tf=Tc=284 KT_f = T_c = 284\text{ K} and Vf=V0V_f = V_0.
The net change in internal energy for the entire process a→fa \rightarrow f depends only on the initial and final temperatures:
ΔUnet=nCv(Tf−Ta)=10×32R×(284−300)=15R×(−16)=−240R\Delta U_{net} = n C_v (T_f - T_a) = 10 \times \dfrac{3}{2}R \times (284 - 300) = 15R \times (-16) = -240R.
Option (C) is correct.

For the P-V diagram:
Process a→ba \rightarrow b is an adiabatic compression (curve upwards and to the left).
Process b→cb \rightarrow c is an isochoric cooling (vertical line downwards).
Process c→fc \rightarrow f is an isothermal expansion (curve downwards and to the right).
Comparing pressures at volume V0V_0:
Pa=nR(300)V0P_a = \dfrac{nR(300)}{V_0} and Pf=nR(284)V0P_f = \dfrac{nR(284)}{V_0}
Since Pa>PfP_a > P_f, point aa lies above point ff. The given schematic diagram correctly represents all these features. Option (A) is correct.

Answer: The schematic P-V diagram of the processes described above is: Ten moles of an ideal monoatomic gas, initially in state a at atmospheric pressure and temperature T_a = 27^ C, is; The change in internal energy in going from state a\boldsymbol{a} to b\boldsymbol{b} is 4860R4860R.; The net change in the internal energy in the whole process is −240R-240R.
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