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Physics · Ch 11 — Thermodynamics

Summary

Summary

  • Zeroth Law: If AA and BB are each in thermal equilibrium with CC, then AA and BB are in thermal equilibrium with each other. This defines temperature as a measurable property.

  • Heat and Work — Sign Convention: If Q>0Q>0, heat is added to the system. If Q<0Q<0, heat is removed from the system. If W>0W>0, work is done by the system. If W<0W<0, work is done on the system.

  • First Law: Energy is conserved. ΔU=Q−W\Delta U = Q - W, where ΔU\Delta U is the change in internal energy, QQ is heat added to the system, and WW is work done by the system.

  • Second Law (Kelvin-Planck): No cyclic process can convert heat completely into work without other effects. (Clausius): No cyclic process can transfer heat from a colder to a hotter body without external work.

  • Reversible vs Irreversible: Reversible processes occur through infinitesimal steps with no dissipation; irreversible processes involve friction, unrestrained expansion, or finite temperature differences.

  • Calorie: 1 calorie is the amount of heat required to raise the temperature of 1 g of water from 14.5°C to 15.5°C. 1 cal = 4.186 J.

  • Heat Capacity: C=QΔTC = \frac{Q}{\Delta T}. For ideal gases: CP−CV=nRC_P - C_V = nR (Mayer's relation). γ=CPCV\gamma = \frac{C_P}{C_V}.

  • Molar Specific Heat of Solids (Equipartition): Modelling a solid as NN atoms, each a 3-D oscillator, the equipartition theorem gives a molar specific heat C=3RC = 3R, which generally agrees with experiment at ordinary temperatures (the Law of Dulong and Petit).

  • Adiabatic Process: Q=0Q = 0. For an ideal gas: PVγ=constantPV^\gamma = \text{constant}, TVγ−1=constantTV^{\gamma-1} = \text{constant}, TγP1−γ=constantT^\gamma P^{1-\gamma} = \text{constant}.

  • Isothermal Process: ΔT=0\Delta T = 0, ΔU=0\Delta U = 0, so Q=W=nRTln⁡(VfVi)Q = W = nRT \ln\left(\frac{V_f}{V_i}\right).

  • Carnot Engine: Most efficient reversible engine operating between T1T_1 (source) and T2T_2 (sink). Efficiency η=1−T2T1\eta = 1 - \frac{T_2}{T_1}.

  • Key Formulas:

    • Work in isobaric process: W=PΔVW = P\Delta V
    • Efficiency of any heat engine: η=1−Q2Q1\eta = 1 - \frac{Q_2}{Q_1}

Quantities used in this chapter

| Quantity | Symbol | Dimensions | Unit | Remark |

|---|---|---|---|---| …