Solveeit Logo

Question

Question: Find the change in entropy (in cal/k) of \({\text{1}}\) mole of \({{\text{O}}_{\text{2}}}\) gas \(\l...

Find the change in entropy (in cal/k) of 1{\text{1}} mole of O2{{\text{O}}_{\text{2}}} gas (Cv=52R)\left( {{{\text{C}}_{\text{v}}} = \dfrac{5}{2}{\text{R}}} \right), when it is
i.Heated from 300K{\text{300K}} to 400K{\text{400K}} isobarically
ii.Heated from 300K{\text{300K}} to 400K{\text{400K}} isochorically (Given ln3=11,ln2=07\ln 3 = 1 \cdot 1,\ln 2 = 0 \cdot 7)

Explanation

Solution

Entropy can be defined as the measure of randomness of the system. Entropy change is an extensive property. The isobaric process can be defined as a process during which the pressure of the system remains constant while the isochoric process is a process during which the volume of the system remains constant.

Complete step by step answer:

  1. First of all we will learn to calculate the change in entropy in the isobaric process by using the formula given below:
    ΔS=nCpln(T2T1)\Delta {\text{S}} = {\text{n}}{{\text{C}}_{\text{p}}}{\text{ln}}\left( {\dfrac{{{{\text{T}}_{\text{2}}}}}{{{{\text{T}}_{\text{1}}}}}} \right) ......(1)......\left( 1 \right)
    Where,
    T1{{\text{T}}_1} = Initial temperature i.e. 300 K
    T2{{\text{T}}_{\text{2}}} = Final temperature i.e. 400 K
    n = 1 mole
  2. The value of Cp{{\text{C}}_{\text{p}}} can be calculated from the given value of Cv{{\text{C}}_v} as:
    CpCv=nR{{\text{C}}_{\text{p}}} - {{\text{C}}_{\text{v}}} = {\text{nR}}
    Now, lets put the value of Cv{{\text{C}}_v} in the above formula we get,
    Cp52R=1×R{{\text{C}}_{\text{p}}} - \dfrac{5}{2}{\text{R}} = 1 \times {\text{R}}
    By taking the Cp{{\text{C}}_{\text{p}}} value on one side we get,
    Cp=R+52R{{\text{C}}_{\text{p}}} = {\text{R}} + \dfrac{{\text{5}}}{{\text{2}}}{\text{R}}
    By doing the addition part in the above equation we get,
    CP=72R{C_P} = \dfrac{7}{2}{\text{R}}
  3. Now, let's substitute this value of Cp{{\text{C}}_{\text{p}}} in equation (1), we get
    ΔS=1×72R×ln(400300)\Delta {\text{S}} = {\text{1}} \times \dfrac{7}{2}{\text{R}} \times {\text{ln}}\left( {\dfrac{{{\text{400}}}}{{{\text{300}}}}} \right)
    By putting the values of R and logarithm we get,
    ΔS=1×72×8314×ln(133)\Delta {\text{S}} = {\text{1}} \times \dfrac{7}{2} \times 8 \cdot 314 \times {\text{ln}}\left( {1 \cdot 33} \right)
    By putting the values of logarithm we get,
    ΔS=1×72×8314×02851\Delta {\text{S}} = {\text{1}} \times \dfrac{7}{2} \times 8 \cdot 314 \times 0 \cdot 2851
    By doing the above calculation we get,
    ΔS=21  calT1\Delta S = 2 \cdot 1\;{\text{cal}}{{\text{T}}^{ - 1}}
  4. Now the change in entropy in isochoric process can be calculated using the formula given below:
    ΔS=nCvln(T2T1)\Delta {\text{S}} = {\text{n}}{{\text{C}}_{\text{v}}}{\text{ln}}\left( {\dfrac{{{{\text{T}}_{\text{2}}}}}{{{{\text{T}}_{\text{1}}}}}} \right) ......(2)......\left( 2 \right)
    Where,
    T1{{\text{T}}_1} = Initial temperature i.e. 300 K
    T2{{\text{T}}_{\text{2}}} = Final temperature i.e. 400 K
    n = 1 mole
    Cv=52R{{\text{C}}_{\text{v}}} = \dfrac{5}{2}{\text{R}}
    Now, let us substitute the value in equation (2), we get
    ΔS=1×52R×ln(400300)\Delta {\text{S}} = {\text{1}} \times \dfrac{5}{2}{\text{R}} \times {\text{ln}}\left( {\dfrac{{{\text{400}}}}{{{\text{300}}}}} \right)
    By putting the values of R and logarithm we get,
    ΔS=1×52×8314×ln(133)\Delta {\text{S}} = {\text{1}} \times \dfrac{5}{2} \times 8 \cdot 314 \times {\text{ln}}\left( {1 \cdot 33} \right)
    By putting the values of logarithm we get,
    ΔS=1×52×8314×02851\Delta {\text{S}} = {\text{1}} \times \dfrac{5}{2} \times 8 \cdot 314 \times 0 \cdot 2851
    By doing the above calculation we get,
    ΔS=15  calT1\Delta S = 1 \cdot 5\;{\text{cal}}{{\text{T}}^{ - 1}}
  5. Therefore we got the answers as,
    i) ΔS=21  calT1\Delta S = 2 \cdot 1\;{\text{cal}}{{\text{T}}^{ - 1}}
    ii) ΔS=15  calT1\Delta S = 1 \cdot 5\;{\text{cal}}{{\text{T}}^{ - 1}}

Note:
Entropy (S) is a state function that does not depend on the path followed. Therefore, entropy change depends on the initial and the final states only. Entropy change is an extensive property which means the entropy is dependent on the mass.