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    Chemical thermodynamics formula - Practice Questions & MCQ

    Edited By admin | Updated on Sep 18, 2023 18:35 AM | #JEE Main

    Quick Facts

    • 1 Questions around this concept.

    Solve by difficulty

    Three moles of a liquid of molar volume 150 mL at 1.5 bar was compressed to 100 bar in an insulated container. The compression resulted in decrease in the volume of the liquid to 125 mL. Which of the following statements are correct regarding the process?

    Concepts Covered - 1

    Smart Tips: Chemical Thermodynamics

    Ideal gas

    Gas equation: $p V=n R T=N k_B T$
    Internal energy. $U=n C_V T$

    Speed of molecule: $v=\sqrt{\frac{3 k T}{m}}$

    Capacities: $C_P=C_V+R$, Ratio: $\gamma=\frac{C_P}{C_V}$

    Degree of Freedom

    Monoatomic: $(\mathrm{f}=3)$

    $
    \begin{aligned}
    & \mathrm{C}_{\mathrm{V}}=\frac{3}{2} \mathrm{R} \\
    & \mathrm{C}_{\mathrm{p}}=\mathrm{R}\left(\frac{3}{2}+1\right)=\frac{5 \mathrm{R}}{2}
    \end{aligned}
    $
     

    Diatomic: $(\mathrm{f}=5)$

    $
    \begin{aligned}
    & \mathrm{C}_{\mathrm{V}}=\frac{5}{2} \mathrm{R} \\
    & \mathrm{C}_{\mathrm{p}}=\mathrm{R}\left(\frac{5}{2}+1\right)=\frac{7 \mathrm{R}}{2}
    \end{aligned}
    $
     

    Polyatomic: $(\mathrm{f}=6)$

    $
    \begin{aligned}
    & \mathrm{C}_{\mathrm{V}}=\frac{6}{2} \mathrm{R} \\
    & \mathrm{C}_{\mathrm{p}}=\mathrm{R}\left(\frac{6}{2}+1\right)=4 \mathrm{R}
    \end{aligned}
    $
     

    Thermodynamic process

    First law: $\Delta U=Q-W$

    Work: $W_{A \rightarrow B}=\int_A^B p d V$

    Entropy: $\Delta S=\int_A^B \frac{d Q}{T}$

    Special processes

    $
    \begin{array}{|c|c|c|c|c|}
    \hline & \text { Isochoric } & \text { Isobaric } & \text { Isothermal } & \text { Adiabatic } \\
    \hline \text { Definition } & \Delta V=0 & \Delta P=0 & \Delta T=0 & Q=0 \\
    \text { Ideal gas } & p V=n R T & p V=n R T & p V=n R T & p V=n R T, p V^\gamma=\text { const } \\
    \text { Work } & W=0 & W=p\left(V_2-V_1\right) & W=n R T \ln \frac{V_2}{V_1} & W=n C_V\left(T_1-T_2\right)=\frac{1}{1-\gamma}\left(p_2 V_2-p_1 V_1\right) \\
    \text { Heat } & Q=n C_V \Delta T & Q=n C_P \Delta T & Q=W & Q=0 \\
    \text { Internal E } & \Delta U=Q & \Delta U=Q-W & \Delta U=0 & \Delta U=-W \\
    \text { Entropy } & \Delta S=n C_V \ln \frac{T_2}{T_1} & \Delta S=n C_P \ln \frac{T_2}{T_1} & \Delta S=n R \ln \frac{V_2}{V_1} & \Delta S=0 \\
    \hline
    \end{array}
    $

    Constants

    Gas: $R=8.31 \mathrm{~J} / \mathrm{K} . \mathrm{mol}$
    Boltzmann: $k_B=1.38 \times 10^{-23} \mathrm{~J} / \mathrm{K}$
    Avogadro: $N_A=6.02 \times 10^{23} / \mathrm{mol}$

    Stefan-Boltzmann: $\sigma=5.67 \times 10^{-8} \mathrm{~W} / \mathrm{m}^2 \cdot \mathrm{~K}^4$

     

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