Thermodynamics JEE Advanced previous year questions with solutions

5 solved JEE Advanced questions on Thermodynamics, free to read — no sign-in needed. The full chapter has 49 questions; sign in to attempt the remaining 44 in the exam simulator.

  1. Q1JEE Advanced Adv 2023 (Paper 1)
    A closed container contains a homogeneous mixture of two moles of an ideal monatomic gas (γ=53)\left(\gamma =\dfrac{5}{3}\right) and one mole of an ideal diatomic gas (γ=75)\left(\gamma =\dfrac{7}{5}\right). Here, γ\gamma is the ratio of the specific heats at constant pressure and constant volume of an ideal gas. The gas mixture does a work of 6666 Joule when heated at constant pressure. The change in its internal energy is _____ Joule.
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    Answer: 121

    Change in internal energy for the mixture can be written as,U=n1(Cv)1T+n2(Cv)2T∆U={n}_{1}{\left({C}_{v}\right)}_{1}∆T+{n}_{2}{\left({C}_{v}\right)}_{2}∆T =(n1(Cv)1+n2(Cv)2)T...(i)=\left({n}_{1}{\left({C}_{v}\right)}_{1}+{n}_{2}{\left({C}_{v}\right)}_{2}\right)∆T...\left(i\right) For isobaric process, work done =PV=P∆V =(n1+n2)RT...(ii)=\left({n}_{1}+{n}_{2}\right)R∆T...\left(ii\right) Divide (i)\left(i\right) by (ii)\left(ii\right), we get UW=(n1(Cv)1+n2(Cv)2)T(n1+n2)RT\dfrac{∆U}{W}=\dfrac{\left({n}_{1}{\left({C}_{v}\right)}_{1}+{n}_{2}{\left({C}_{v}\right)}_{2}\right)∆T}{\left({n}_{1}+{n}_{2}\right)R∆T} U=WR((n1(Cv)1+n2(Cv)2)n1+n2)\Rightarrow ∆U=\dfrac{W}{R}\left(\dfrac{\left({n}_{1}{\left({C}_{v}\right)}_{1}+{n}_{2}{\left({C}_{v}\right)}_{2}\right)}{{n}_{1}+{n}_{2}}\right) =66R[2×3R2+1×5R2]2+1=\dfrac{66}{R}\dfrac{\left[2\times \dfrac{3R}{2}+1\times \dfrac{5R}{2}\right]}{2+1} =121J=121J
  2. Q2JEE Advanced Adv 2020 (Paper 2)
    A spherical bubble inside water has radius RR. Take the pressure inside the bubble and the water pressure to be p0.{p}_{0}. The bubble now gets compressed radially in an adiabatic manner so that its radius becomes (Ra)(R-a). For aRa≪R the magnitude of the work done in the process is given by (4πP0Ra2)X,\left(4\pi {P}_{0}R{a}^{2}\right)X, where XX is a constant and γ=Cp/CV=41/30\gamma ={C}_{p}/{C}_{V}=41/30. The value of XX is______
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    Answer: 2.05

    W=(ΔP)avg ×4πR2a=dP24πR2a\begin{aligned} &\mathrm{W}=(\Delta \mathrm{P})_{\text {avg }} \times 4 \pi \mathrm{R}^2 \mathrm{a} \\ &=\left|\frac{\mathrm{dP}}{2} \cdot 4 \pi \mathrm{R}^2 \mathrm{a}\right| \end{aligned} (for small change (ΔP)avg <P>(\Delta \mathrm{P})_{\text {avg }}<\mathrm{P}> arithmetic mean) =PV gamma =cdP=γPVdV=γP0 V4πR2a=\mathrm{PV} \text { gamma }=\mathrm{c} \Rightarrow \mathrm{dP}=-\gamma \frac{\mathrm{P}}{\mathrm{V}} \mathrm{dV}=-\frac{\gamma \mathrm{P}_0}{\mathrm{~V}} 4 \pi \mathrm{R}^2 \mathrm{a} =γP02 V×4πR2a×4πR2a=\frac{\gamma \mathrm{P}_0}{2 \mathrm{~V}} \times 4 \pi \mathrm{R}^2 \mathrm{a} \times 4 \pi \mathrm{R}^2 \mathrm{a} =γP02×4πR34πR2a×4πR2a=\frac{\gamma \mathrm{P}_0}{2 \times 4 \pi \mathrm{R}^3} 4 \pi \mathrm{R}^2 \mathrm{a} \times 4 \pi \mathrm{R}^2 \mathrm{a} =(4pRP×a2)3γ2=\left(4 \mathrm{pRP} \times \mathrm{a}^2\right) \frac{3 \gamma}{2} x=2.05\therefore \mathrm{x}=2.05
  3. Q3JEE Advanced Adv 2019 (Paper 2)
    A mixture of ideal gas containing 55 moles of monatomic gas and 11 mole of rigid diatomic gas is initially at pressure P0,{P}_{0}, volume V0{V}_{0} and temperature T0.{T}_{0}. If the gas mixture is adiabatically compressed to a volume V04\dfrac{{V}_{0}}{4}, then the correct statement(s) is/are, (Given 21.2=2.3;23.2=9.2;R{2}^{1.2}=2.3\text{;}{2}^{3.2}=9.2\text{;}R is gas constant)
    1. A.The final pressure of the gas mixture after compression is in between 9P09{P}_{0} and 10P010{P}_{0}.
    2. B.The average kinetic energy of the gas mixture after compression is in between 18RT018R{T}_{0} and 19RT019R{T}_{0}.
    3. C.The work W\left|W\right| done during the process is 13RT013R{T}_{0}.
    4. D.Adiabatic constant of the gas mixture is 1.61.6.
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    Answer: A,C,D

    Here,n1=5,CP1=52R,CV1=32Rn2=1,CP2=72R,CV2=52Rγmix=n1CP1+n2CP2n1CV1+n2CV2=85=1.6\begin{matrix}\text{Here,}{n}_{1}=5, & {C}_{{P}_{1}}=\dfrac{5}{2}R, & {C}_{{V}_{1}}=\dfrac{3}{2}R \\ {n}_{2}=1, & {C}_{{P}_{2}}=\dfrac{7}{2}R, & {C}_{{V}_{2}}=\dfrac{5}{2}R\end{matrix} {\gamma }_{mix}=\dfrac{{n}_{1}{C}_{{P}_{1}}+{n}_{2}{C}_{{P}_{2}}}{{n}_{1}{C}_{{V}_{1}}+{n}_{2}{C}_{{V}_{2}}}=\dfrac{8}{5}=1.6 Work done, W=P1V1P2V2γ1,(Inadiabaticprocess)W=\dfrac{{P}_{1}{V}_{1}-{P}_{2}{V}_{2}}{\gamma -1},\left(Inadiabaticprocess\right) Now, for adiabatic compression P1V1r=P2V2r{P}_{1}{V}_{1}^{r}={P}_{2}{V}_{2}^{r} P0V08/5=P2(V04)8/5\Rightarrow {P}_{0}{V}_{0}^{8/5}={P}_{2}{\left(\dfrac{{V}_{0}}{4}\right)}^{8/5} P2=9.2P0(A)\Rightarrow {P}_{2}=9.2{P}_{0}\Rightarrow \left(A\right) is correct. Now, W=P0V09.2P0V043/5=13RT0(C)W=\dfrac{{P}_{0}{V}_{0}-9.2{P}_{0}\dfrac{{V}_{0}}{4}}{3/5}=-13R{T}_{0}\Rightarrow \left(C\right) is correct W=13RT0∴\left|W\right|=13R{T}_{0} Again T1V1γ1=T2V2γ1{T}_{1}{V}_{1}^{\gamma -1}={T}_{2}{V}_{2}^{\gamma -1} T2=T1(2)6/5=2.3T0{T}_{2}={T}_{1}{\left(2\right)}^{6/5}=2.3{T}_{0} Average kinetic energy of gas mixture =nCVmixT2=n{C}_{{V}_{mix}}{T}_{2} =23RT0(B)=23R{T}_{0}\Rightarrow \left(B\right) is incorrect
  4. Q4JEE Advanced Adv 2018 (Paper 2)
    One mole of an ideal monatomic gas undergoes an adiabatic expansion in which its volume becomes eight times its initial value. If the initial temperature of the gas is 100K100K and the universal gas constant R=8.0Jmol1K1R=8.0Jmo{l}^{-1}{K}^{-1}, then how much is the decrease in its internal energy (in JJ) ?
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    Answer: 900

    Vi=V{V}_{i}=V Vf=8V{V}_{f}=8V For adiabatic process {γ=5/3 for monoatomic gas}\{\gamma =5/3\text{ for monoatomic gas}\} T1V1γ1=T2V2γ1{T}_{1}\cdot {V}_{1}^{\gamma -1}={T}_{2}\cdot {V}_{2}^{\gamma -1} 100(V)23=T2(8V)23100{\left(V\right)}^{\dfrac{2}{3}}={T}_{2}{\left(8V\right)}^{\dfrac{2}{3}} T2=25K{T}_{2}=25K Loss in internal energy U=nCvT=1(fR2)[10025]=12×75=900J∆U=n{C}_{v}∆T=1\left(\dfrac{fR}{2}\right)\left[100-25\right]=12\times 75=900J
  5. Q5JEE Advanced Adv 2012 (Paper 2)
    Two moles of ideal helium gas are in a rubber balloon at 30C30^{\circ} \mathrm{C}. The balloon is fully expandable and can be assumed to require no energy in its expansion. The temperature of the gas in the balloon is slowly changed to 35C35^{\circ} \mathrm{C}. The amount of heat required in raising the temperature is nearly (take R=8.31 J/mol.KR=8.31 \mathrm{~J} / \mathrm{mol} . \mathrm{K} )
    1. A.62 J62 \mathrm{~J}
    2. B.104 J104 \mathrm{~J}
    3. C.124 J124 \mathrm{~J}
    4. D.208 J208 \mathrm{~J}
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    Answer: (D)

    The heat is supplied at constant pressure. i.e., the process is isobaric Q=nCpΔt=2[52R]×Δt=2×52×8.31×5=208 J(Cp=52R for mono-atomic gas )\begin{array}{l} \therefore Q=n C_{p} \Delta t \\ =2\left[\frac{5}{2} R\right] \times \Delta t=2 \times \frac{5}{2} \times 8.31 \times 5=208 \mathrm{~J} \\ \left(\because C_{p}=\frac{5}{2} R \text { for mono-atomic gas }\right) \end{array}

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Thermodynamics in JEE Advanced: previous year question analysis

Thermodynamics has appeared 49 times in JEE Advanced between 2006 and 2026, making it the 10th most-asked of 93 chapters and about 2% of the bank. Over the last 5 years it has averaged 2.8 questions per year.

Total PYQs
49
Years covered
2006–2026
Weightage rank
#10 of 93
Share of bank
2%

How many Thermodynamics questions appeared each year

Thermodynamics JEE Advanced question count by year
YearQuestionsRelative volume
20151
20161
20173
20183
20194
20203
20213
20224
20233
20241
20253
20263

Question formats used in Thermodynamics

  • Single-correct MCQ26
  • Numerical / integer answer12
  • Multiple-correct MCQ11

How Thermodynamics compares with nearby chapters

Counts are computed from AcadXL’s own JEE Advanced question bank, tagged chapter- and sub-topic-wise and checked against official answer keys. Sign in to attempt the 49 Thermodynamics questions with solutions.