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Heat and Thermodynamics question

2019 · Shift 2 · Q54
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Heat and Thermodynamics question

2019 · Shift 2 · Q54

JEE AdvancedPhysicsHeat and ThermodynamicsMCQ+3 / −1
In a thermodynamic process on an ideal monatomic gas, the infinitesimal heat absorbed by the gas is given by T Δ\DeltaΔ X where T is temperature of the system and Δ\DeltaΔ X is the infinitesimal change in a thermodynamic quantity X of the system. For a mole of monatomic ideal gas, X=32R ln⁡(TTA)+R ln⁡(VVA)X = {3 \over 2}R\,\ln \left( {{T \over {{T_A}}}} \right) + R\,\ln \left( {{V \over {{V_A}}}} \right)X=23​Rln(TA​T​)+Rln(VA​V​) Here, R is gas constant, V is volume of gas, TA and VA are constants. The List-I below gives some quantities involved in a process and List-II gives some possible values of these quantities. JEE Advanced 2019 Paper 2 Offline Physics - Heat and Thermodynamics Question 46 English ComprehensionIf the process carried out on one mole of monoatomic ideal gas is as shown in the PV-diagram with p0V0=13RT0{p_0}{V_0} = {1 \over 3}R{T_0}p0​V0​=31​RT0​, the correct match is, JEE Advanced 2019 Paper 2 Offline Physics - Heat and Thermodynamics Question 46 English
  1. A
    I →\to→ S, II →\to→ R, III →\to→ Q, IV →\to→ T
  2. B
    I →\to→ Q, II →\to→ R, III →\to→ P, IV →\to→ U
  3. C
    I →\to→ Q, II →\to→ S, III →\to→ R, IV →\to→ U
  4. D
    I →\to→ Q, II →\to→ R, III →\to→ S, IV →\to→ U
View written solutionFree

Correct answer: D

The user wants me to solve a thermodynamics problem involving matching quantities for a specific process of an ideal monatomic gas.

Step-by-step Solution:

  1. Analyze the System and Given Information

    • System: 1 mole of an ideal monatomic gas (n=1, Cv=32RC_v = \frac{3}{2}RCv​=23​R).
    • Process: A straight line on a P-V diagram from state A (V0,p0)(V_0, p_0)(V0​,p0​) to state B (2V0,p0/2)(2V_0, p_0/2)(2V0​,p0​/2).
    • Given relation: p0V0=13RT0p_0 V_0 = \frac{1}{3} R T_0p0​V0​=31​RT0​.
    • Thermodynamic quantity X is given by X=32Rln⁡(TTA)+Rln⁡(VVA)X = \frac{3}{2}R\ln(\frac{T}{T_A}) + R\ln(\frac{V}{V_A})X=23​Rln(TA​T​)+Rln(VA​V​). The infinitesimal heat is dQ = T dX. This implies dX is the change in entropy dS.
  2. Determine Temperatures at States A and B

    • Using the ideal gas law PV = nRT = RT (since n=1).
    • Temperature at state A: TA=pAVAR=p0V0RT_A = \frac{p_A V_A}{R} = \frac{p_0 V_0}{R}TA​=RpA​VA​​=Rp0​V0​​. Using the given relation, TA=(1/3)RT0R=13T0T_A = \frac{(1/3) R T_0}{R} = \frac{1}{3} T_0TA​=R(1/3)RT0​​=31​T0​.
    • Temperature at state B: TB=pBVBR=(p0/2)(2V0)R=p0V0RT_B = \frac{p_B V_B}{R} = \frac{(p_0/2)(2V_0)}{R} = \frac{p_0 V_0}{R}TB​=RpB​VB​​=R(p0​/2)(2V0​)​=Rp0​V0​​. So, TB=13T0T_B = \frac{1}{3} T_0TB​=31​T0​.
    • Since TA=TBT_A = T_BTA​=TB​, the initial and final temperatures are the same.
  3. Calculate the Quantities in List-I

    • I. Work done by the system (W_AB): The work done is the area under the P-V graph. For a linear process (a trapezoid): WAB=12(pA+pB)(VB−VA)=12(p0+p02)(2V0−V0)=12(3p02)(V0)=34p0V0W_{AB} = \frac{1}{2} (p_A + p_B) (V_B - V_A) = \frac{1}{2} (p_0 + \frac{p_0}{2}) (2V_0 - V_0) = \frac{1}{2} (\frac{3p_0}{2}) (V_0) = \frac{3}{4} p_0 V_0WAB​=21​(pA​+pB​)(VB​−VA​)=21​(p0​+2p0​​)(2V0​−V0​)=21​(23p0​​)(V0​)=43​p0​V0​ Substituting the given relation p0V0=13RT0p_0 V_0 = \frac{1}{3} R T_0p0​V0​=31​RT0​: WAB=34(13RT0)=14RT0W_{AB} = \frac{3}{4} \left( \frac{1}{3} R T_0 \right) = \frac{1}{4} R T_0WAB​=43​(31​RT0​)=41​RT0​ This corresponds to option R in List-II.

    • II. Change in internal energy (ΔU_AB): For an ideal monatomic gas, ΔU=nCvΔT=(1)(32R)(TB−TA)ΔU = n C_v ΔT = (1) (\frac{3}{2}R) (T_B - T_A)ΔU=nCv​ΔT=(1)(23​R)(TB​−TA​). Since TA=TBT_A = T_BTA​=TB​, ΔT = 0. Therefore: ΔUAB=0ΔU_{AB} = 0ΔUAB​=0 This value is not present in List-II.

    • IV. ΔX in the process: ΔX is the change in entropy ΔS. The formula for entropy change is: ΔX=ΔS=32Rln⁡(TBTA)+Rln⁡(VBVA)ΔX = ΔS = \frac{3}{2}R \ln\left(\frac{T_B}{T_A}\right) + R \ln\left(\frac{V_B}{V_A}\right)ΔX=ΔS=23​Rln(TA​TB​​)+Rln(VA​VB​​) Since TA=TBT_A = T_BTA​=TB​, the first term ln⁡(1)\ln(1)ln(1) is zero. ΔX=Rln⁡(2V0V0)=Rln⁡(2)ΔX = R \ln\left(\frac{2V_0}{V_0}\right) = R \ln(2)ΔX=Rln(V0​2V0​​)=Rln(2) This corresponds to option U in List-II.

    • III. Heat absorbed by the system (Q_AB): Using the First Law of Thermodynamics, QAB=ΔUAB+WABQ_{AB} = ΔU_{AB} + W_{AB}QAB​=ΔUAB​+WAB​. QAB=0+14RT0=14RT0Q_{AB} = 0 + \frac{1}{4} R T_0 = \frac{1}{4} R T_0QAB​=0+41​RT0​=41​RT0​ This corresponds to option R in List-II.

  4. Analysis and Conclusion

    • Our calculations based on the problem statement give: I → R, II → 0 (not in list), III → R, IV → U. This set of matches is not among the options provided.

    • Let's check the stored answer D: {I → Q, II → R, III → S, IV → U}. Let's check its consistency with the First Law of Thermodynamics (Q = ΔU + W).

      • Q (III → S): (1/2)RT0(1/2) R T_0(1/2)RT0​
      • ΔU (II → R): (1/4)RT0(1/4) R T_0(1/4)RT0​
      • W (I → Q): (3/4)RT0(3/4) R T_0(3/4)RT0​ Is (1/2)RT0=(1/4)RT0+(3/4)RT0(1/2) R T_0 = (1/4) R T_0 + (3/4) R T_0(1/2)RT0​=(1/4)RT0​+(3/4)RT0​? This simplifies to 1/2 = 1, which is false. The provided answer key (D) is thermodynamically inconsistent.
    • Revisiting under assumption of a typo: The problem is likely flawed. A common typo in such problems is the relation between p0,V0,T0p_0, V_0, T_0p0​,V0​,T0​. If we assume p0V0=RT0p_0 V_0 = R T_0p0​V0​=RT0​ instead of p0V0=(1/3)RT0p_0 V_0 = (1/3) R T_0p0​V0​=(1/3)RT0​:

      • WAB=(3/4)p0V0=(3/4)RT0W_{AB} = (3/4) p_0 V_0 = (3/4) R T_0WAB​=(3/4)p0​V0​=(3/4)RT0​. This matches I → Q.
      • TA=T0T_A = T_0TA​=T0​, TB=T0T_B = T_0TB​=T0​. So ΔUAB=0ΔU_{AB} = 0ΔUAB​=0. This is still not in the options.
      • ΔX=Rln⁡(2)ΔX = R \ln(2)ΔX=Rln(2). This matches IV → U. This suggests that I → Q and IV → U are the intended matches, which are present in options B, C, and D. However, the non-zero value for ΔU in all options contradicts the given process path.
    • Given the inconsistencies, the question is flawed. However, to choose the 'best' option as intended by the exam, we recognize that our calculation for ΔX is robust and matches U. Our calculation for W's dependence on p0V0p_0 V_0p0​V0​ is also robust (W=(3/4)p0V0W=(3/4)p_0 V_0W=(3/4)p0​V0​). The options suggest W=(3/4)RT0W=(3/4)RT_0W=(3/4)RT0​, pointing to a typo in the p0V0p_0 V_0p0​V0​ relation. The non-zero ΔU suggests a typo in the process path as well. Without a clear way to resolve these contradictions, we cannot logically derive the given answer. However, if forced to choose based on common intended parts, we lock in IV → U and I → Q. This leaves options B, C, D. The answer key indicates D. This implies II→R and III→S are the intended (though inconsistent) remaining matches.

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