Category: Part 2: Thermodynamics

  • Problem 2.119 — Maxwell Thermodynamic Relations

    Problem Statement Solve the thermodynamics problem: Solve the thermodynamics problem: Derive the four Maxwell relations from the thermodynamic potentials. Starting from the fundamental relations: $dU = TdS – pdV$ → $\left(\frac{\partial T}{\partial V}\right)_S = -\left(\frac{\partial p}{\partial S}\right)_V$ $dH = TdS + Vdp$ → $\left(\frac{\partial T Given Information See problem statement for all given quantities. Physical…

  • Problem 2.120 — Joule-Thomson Coefficient from Maxwell Relations

    Problem Statement Express the Joule-Thomson coefficient $\mu_{JT} = (\partial T/\partial p)_H$ in terms of measurable quantities using a Maxwell relation. Given Information See problem statement for all given quantities. Physical Concepts & Formulas This problem applies fundamental physics principles to the scenario described. The solution requires identifying the relevant conservation laws and equations of motion,…

  • Problem 2.117 — Helmholtz Free Energy

    Problem Statement Solve the work-energy problem: Solve the work-energy problem: Define the Helmholtz free energy $F = U – TS$. Show that at constant $T$ and $V$, equilibrium corresponds to minimum $F$. For a system at constant temperature (in contact with a heat reservoir) and constant volume: $$dU = dQ – dW = TdS_{env} –…

  • Problem 2.118 — Gibbs Free Energy and Chemical Equilibrium

    Problem Statement Solve the work-energy problem: Solve the work-energy problem: Define the Gibbs free energy $G = H – TS$ and show it is minimized at equilibrium at constant $T$ and $p$. At constant $T$ and $p$: $dG = dH – TdS = dU + p\,dV – TdS$. From the first law: $dU = dQ…

  • Problem 2.115 — Entropy of an Ideal Gas: Absolute Expression

    Problem Statement Solve the thermodynamics problem: Solve the thermodynamics problem: Derive the molar entropy of an ideal gas as a function of $T$ and $V$ (Sackur-Tetrode-like for classical ideal gas). From thermodynamics: $dS = C_v dT/T + R dV/V$ (from $dU = TdS – pdV$ for ideal gas). Integrating (for 1 mol): $$S(T,V) = C_v\ln…

  • Problem 2.116 — Efficiency of a Real Engine

    Problem Statement An engine absorbs $Q_1=10\ \text{kJ}$ from a source at $T_1=500\ \text{K}$ and rejects $Q_2=7\ \text{kJ}$ to a sink at $T_2=300\ \text{K}$. Is this engine reversible, irreversible-allowed, or violating the second law? Given Information See problem statement for all given quantities. Physical Concepts & Formulas This problem applies fundamental physics principles to the scenario…

  • Problem 2.113 — Boltzmann Distribution: Population Ratio

    Problem Statement Two energy states are separated by $\Delta E = 0.020\ \text{eV}$. Find the ratio of populations $N_2/N_1$ at $T=300\ \text{K}$. Given Information See problem statement for all given quantities. Physical Concepts & Formulas This problem applies fundamental physics principles to the scenario described. The solution requires identifying the relevant conservation laws and equations…

  • Problem 2.114 — Second Law: Perpetual Motion

    Problem Statement Explain why a perpetual motion machine of the second kind is impossible, and state the Kelvin-Planck and Clausius formulations of the second law. Given Information See problem statement for all given quantities. Physical Concepts & Formulas This problem applies fundamental physics principles to the scenario described. The solution requires identifying the relevant conservation…

  • Problem 2.112 — Maxwell-Boltzmann: Fraction with $v > v_{esc}$

    Problem Statement Find the fraction of N₂ molecules at $T=300\ \text{K}$ with speed exceeding Earth’s escape velocity $v_{esc}=11.2\ \text{km/s}$. Given Information See problem statement for all given quantities. Physical Concepts & Formulas The Maxwell-Boltzmann distribution describes the statistical distribution of molecular speeds in an ideal gas at thermal equilibrium. It arises from the maximisation of…

  • Problem 2.110 — Specific Heat Ratio from Speed of Sound

    Problem Statement Solve the thermodynamics problem: Solve the thermodynamics problem: The speed of sound in air at $T=273\ \text{K}$ is measured to be $v_s=331\ \text{m/s}$. Find $\gamma$ for air ($M=29\ \text{g/mol}$). $$v_s = \sqrt{\frac{\gamma RT}{M}} \implies \gamma = \frac{v_s^2 M}{RT}$$ $$\gamma = \frac{(331)^2\times0.029}{8.314\times273} = \fr Given Information See problem statement for all given quantities. Physical…