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Heat and Thermodynamics question

2024 · 30 Jan · Shift 1 · Q69
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Heat and Thermodynamics question

2024 · 30 Jan · Shift 1 · Q69

JEE MainPhysicsHeat and ThermodynamicsMCQ+4 / −1
Two thermodynamical processes are shown in the figure. The molar heat capacity for process A and B are CA\mathrm{C}_{\mathrm{A}}CA​ and CB\mathrm{C}_{\mathrm{B}}CB​. The molar heat capacity at constant pressure and constant volume are represented by CP\mathrm{C_P}CP​ and CV\mathrm{C_V}CV​, respectively. Choose the correct statement. JEE Main 2024 (Online) 30th January Morning Shift Physics - Heat and Thermodynamics Question 73 English
  1. A
    CP>CB>CA>CV\mathrm{C_P>C_B>C_A>C_V}CP​>CB​>CA​>CV​
  2. B
    CP>CV>CA=CB\mathrm{C}_{\mathrm{P}}\gt \mathrm{C}_{\mathrm{V}}\gt \mathrm{C}_{\mathrm{A}}=\mathrm{C}_{\mathrm{B}}CP​>CV​>CA​=CB​
  3. C
    CA=0\mathrm{C}_{\mathrm{A}}=0CA​=0 and CB=∞\mathrm{C}_{\mathrm{B}}=\inftyCB​=∞
  4. D
    CA=∞,CB=0\mathrm{C_A=\infty, C_B=0}CA​=∞,CB​=0
View written solutionFree

Correct answer: A

  1. Interpret the processes from the usual PPP–VVV diagram

    The two shown thermodynamic paths are understood as:

    • Process A: steeper than an adiabat / lies between isochoric and adiabatic behavior in such a way that its molar heat capacity is between CVC_VCV​ and CPC_PCP​.
    • Process B: another path whose slope places its heat capacity between that of process A and the isobaric value.

    To decide the ordering, use the general expression for molar heat capacity along any quasi-static process.

  2. General formula for molar heat capacity along a process

    For 1 mole of an ideal gas,

     dQ=dU+P dV=CV dT+P dV.\,dQ = dU + P\,dV = C_V\,dT + P\,dV.dQ=dU+PdV=CV​dT+PdV.

    Hence the heat capacity for the process is

    C=dQdT=CV+PdVdT.C = \frac{dQ}{dT} = C_V + P\frac{dV}{dT}.C=dTdQ​=CV​+PdTdV​.

    Also, using PV=RTPV=RTPV=RT,

    P dV+V dP=R dT.P\,dV + V\,dP = R\,dT.PdV+VdP=RdT.

    Depending on the slope of the path on the PPP–VVV diagram, the value of dVdT\dfrac{dV}{dT}dTdV​ changes, and therefore the heat capacity changes.

  3. Reference values

    • At constant volume: dV=0  ⟹  C=CV.dV=0 \implies C=C_V.dV=0⟹C=CV​.
    • At constant pressure: dP=0  ⟹  P dV=R dT  ⟹  C=CV+R=CP.dP=0 \implies P\,dV=R\,dT \implies C=C_V+R=C_P.dP=0⟹PdV=RdT⟹C=CV​+R=CP​.

    Therefore, for any intermediate process between isochoric and isobaric behavior,

    CP>C>CV.C_P > C > C_V.CP​>C>CV​.
  4. Compare process A and process B

    From the figure, process B is closer to the isobaric case than process A, so its heat capacity is larger. Thus,

    CP>CB>CA>CV.C_P > C_B > C_A > C_V.CP​>CB​>CA​>CV​.
  5. Check options

    • Option A: CP>CB>CA>CVC_P > C_B > C_A > C_VCP​>CB​>CA​>CV​ ✅
    • Option B: CP>CV>CA=CBC_P > C_V > C_A = C_BCP​>CV​>CA​=CB​ ❌
    • Option C: CA=0C_A=0CA​=0 and CB=∞C_B=\inftyCB​=∞ ❌
    • Option D: CA=∞, CB=0C_A=\infty,\ C_B=0CA​=∞, CB​=0 ❌
  6. Final answer

    The correct statement is

    CP>CB>CA>CV\boxed{C_P > C_B > C_A > C_V}CP​>CB​>CA​>CV​​

    i.e. Option A.

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