JEE Challenger
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Determination of Volume in Two Stage Reversible Gas Process

One mole of an ideal monoatomic gas undergoes two reversible processes (AB\text{A} \rightarrow \text{B} and BC\text{B} \rightarrow \text{C}) as shown in the given figure:

AB\text{A} \rightarrow \text{B} is an adiabatic process. If the total heat absorbed in the entire process (AB\text{A} \rightarrow \text{B} and BC\text{B} \rightarrow \text{C}) is RT2ln10RT_2 \ln 10, the value of 2logV32 \log V_3 is _____.

[Use, molar heat capacity of the gas at constant pressure, Cp,m=52RC_{p,\text{m}} = \frac{5}{2}R]

Question Diagram 1
Official Numerical Answer7

Step-by-Step Solution

For one mole (n=1n = 1) of an ideal monoatomic gas, the heat capacity at constant volume is: Cv,m=Cp,mR=52RR=32RC_{v,\text{m}} = C_{p,\text{m}} - R = \frac{5}{2}R - R = \frac{3}{2}R

The adiabatic index (Poisson's ratio) γ\gamma is given by: γ=Cp,mCv,m=52R32R=53\gamma = \frac{C_{p,\text{m}}}{C_{v,\text{m}}} = \frac{\frac{5}{2}R}{\frac{3}{2}R} = \frac{5}{3}

Thus, γ1=531=23\gamma - 1 = \frac{5}{3} - 1 = \frac{2}{3}.

Step 1: Process AB\text{A} \rightarrow \text{B} (Reversible Adiabatic Expansion)

From the graph:

  • Temperature at A\text{A}, T1=600 KT_1 = 600\text{ K}
  • Volume at A\text{A}, V1=10 m3V_1 = 10\text{ m}^3
  • Temperature at B\text{B}, T2=60 KT_2 = 60\text{ K}

Since AB\text{A} \rightarrow \text{B} is a reversible adiabatic process: qAB=0q_{\text{A} \rightarrow \text{B}} = 0

Using the relation TVγ1=constantT V^{\gamma - 1} = \text{constant}: T1V1γ1=T2V2γ1T_1 V_1^{\gamma - 1} = T_2 V_2^{\gamma - 1}

Substitute the known values: 600×102/3=60×V22/3600 \times 10^{2/3} = 60 \times V_2^{2/3}

60060=(V210)2/3\frac{600}{60} = \left(\frac{V_2}{10}\right)^{2/3}

10=(V210)2/310 = \left(\frac{V_2}{10}\right)^{2/3}

V2=10×103/2=105/2 m3V_2 = 10 \times 10^{3/2} = 10^{5/2}\text{ m}^3

Step 2: Process BC\text{B} \rightarrow \text{C} (Reversible Isothermal Expansion)

Since the temperature remains constant at T2=60 KT_2 = 60\text{ K} during BC\text{B} \rightarrow \text{C}, the heat absorbed in this reversible isothermal process is: qBC=nRT2ln(V3V2)=RT2ln(V3V2)q_{\text{B} \rightarrow \text{C}} = n R T_2 \ln\left(\frac{V_3}{V_2}\right) = R T_2 \ln\left(\frac{V_3}{V_2}\right)

The total heat absorbed in the entire process ABC\text{A} \rightarrow \text{B} \rightarrow \text{C} is: qtotal=qAB+qBC=0+RT2ln(V3V2)q_{\text{total}} = q_{\text{A} \rightarrow \text{B}} + q_{\text{B} \rightarrow \text{C}} = 0 + R T_2 \ln\left(\frac{V_3}{V_2}\right)

Given that qtotal=RT2ln10q_{\text{total}} = R T_2 \ln 10: RT2ln(V3V2)=RT2ln10R T_2 \ln\left(\frac{V_3}{V_2}\right) = R T_2 \ln 10

ln(V3V2)=ln10    V3=10V2\ln\left(\frac{V_3}{V_2}\right) = \ln 10 \implies V_3 = 10 V_2

Substitute V2=105/2 m3V_2 = 10^{5/2}\text{ m}^3: V3=10×105/2=107/2 m3V_3 = 10 \times 10^{5/2} = 10^{7/2}\text{ m}^3

Step 3: Calculation of 2logV32 \log V_3

Taking the base-10 logarithm of V3V_3: log10V3=log10(107/2)=72\log_{10} V_3 = \log_{10}\left(10^{7/2}\right) = \frac{7}{2}

Therefore: 2logV3=2×72=72 \log V_3 = 2 \times \frac{7}{2} = 7