Thermodynamics – Temperature, Zeroth Law & Thermal Expansion

Overview of Thermodynamics

  • Thermodynamics = study of energy flow in the universe as it relates to work, heat, entropy, and other energy forms.
    • Classical (macroscopic) thermodynamics: only observable/ measurable variables (temperature, pressure, volume, work).
    • Statistical model of entropy (microscopic, probabilistic) briefly mentioned to clarify “disorder” concept, but MCAT focuses on macroscopic definition.
  • Chapter map
    • Review of Zeroth, First, Second Laws (Third Law only briefly).
    • Zeroth Law → temperature scales.
    • Thermal expansion illustrates relation between thermal energy and physical properties (length, volume, conductivity).
    • Thermodynamic terminology/functions intersect with Ch. 7 of MCAT General Chemistry Review.
    • First Law (conservation of energy): relationship among internal energy, heat, work; specific heat; heat of transformation.
    • Processes moving a system from one equilibrium state to another; link heat with work (ties to Ch. 2 of MCAT Physics & Math Review).
    • Second Law: entropy & its measurement.

Laws of Thermodynamics (Exam-Relevant Emphasis)

  • Zeroth Law
    • Observation: If A is in thermal equilibrium with B, and B with C, then A is in thermal equilibrium with C.
    • Consequence: When brought into thermal contact, no net heat flows between objects already in equilibrium.
    • “Thermal contact” can occur without physical contact (across space).
  • First Law (preview; detailed later in book)
    • Energy conservation: change in internal energy = heat added − work done by system.
  • Second Law (preview)
    • Entropy and directionality of heat flow.
  • Third Law (mentioned only)
    • Entropy of a perfectly organized crystal at absolute zero is 00.

Temperature & Heat

  • Temperature
    • Everyday sense = “hot/cold”; precise thermodynamic sense = proportional to average kinetic energy of particles.
    • Temperature difference determines direction of spontaneous heat flow.
  • Heat
    • Transfer of thermal energy from higher-T object to lower-T object.
    • If no net heat flows → equal temperatures → thermal equilibrium.

Temperature Scales

  • Three common scales: Fahrenheit (°F), Celsius (°C), Kelvin (K).
    • Fahrenheit & Celsius devised using water phase changes (freezing/boiling), convenient for everyday use.
    • Kelvin = SI base unit; zero point is absolute zero (no thermal energy); water freezes at 273.15 K273.15\text{ K}.
    • No negative temperatures on Kelvin scale.
  • Unit sizes
    • 1°C=1 K1\,\text{°C} = 1\text{ K} (same magnitude).
    • Fahrenheit degree is smaller (180° between phase changes vs. 100 on °C/K).
  • Conversion formulas
    • F=95C+32F = \frac{9}{5} C + 32
    • K=C+273K = C + 273
  • Example conversion
    • High of 86°F86\,\text{°F}
    • C=59(F32)=59(8632)=30°CC = \frac{5}{9}(F-32) = \frac{5}{9}(86-32) = 30\,\text{°C}
    • K=30+273=303KK = 30 + 273 = 303\,\text{K}

Thermal Expansion

  • General observation: physical properties (length, volume, solubility, conductivity) vary with temperature.
    • Historical role in thermometer design (Fahrenheit mercury thermometer): mercury height correlated with reference temperatures (ice–salt bath, ice–water, body temperature).
  • Linear Expansion (solids)
    • Rising T → length increases; falling T → length decreases.
    • Equation: ΔL=αLΔT\Delta L = \alpha L \Delta T
    • ΔL\Delta L = change in length.
    • α\alpha (alpha) = coefficient of linear expansion (units K1\text{K}^{-1} or °C1\text{°C}^{-1}).
    • LL = original length.
    • ΔT\Delta T = change in temperature.
  • Example (linear expansion)
    • Metal rod: L=2mL=2\,\text{m}, α=1.0×106K1\alpha = 1.0 \times 10^{-6}\,\text{K}^{-1}.
    • Cooled: T<em>i=1080°CT<em>i = 1080\,°CT</em>f=80°CT</em>f = 80\,°C.
    • ΔL=αLΔT=(1.0×106)(2)(801080)\Delta L = \alpha L \Delta T = (1.0\times10^{-6})(2)(80-1080)
    • ΔL=2×103m\Delta L = -2\times10^{-3}\,\text{m} (length decreases).
    • Final length =2.000m0.002m=1.998m= 2.000\,\text{m} - 0.002\,\text{m} = 1.998\,\text{m}.
  • Volumetric Expansion (liquids & solids)
    • Equation: ΔV=βVΔT\Delta V = \beta V \Delta T
    • β\beta = coefficient of volumetric expansion.
    • β=3α\beta = 3\alpha for isotropic solids.
  • Example (volumetric expansion)
    • Mercury thermometer, V=1mLV=1\,\text{mL}.
    • T<em>i=25°CT<em>i=-25\,°C, T</em>f=275°CT</em>f=275\,°CΔT=300°C\Delta T = 300\,°C.
    • β=1.8×104K1\beta = 1.8\times10^{-4}\,\text{K}^{-1}.
    • ΔV=(1.8×104)(1)(300)=5.40×102mL=0.054mL\Delta V = (1.8\times10^{-4})(1)(300) = 5.40\times10^{-2}\,\text{mL} = 0.054\,\text{mL}.

Conceptual & Real-World Connections

  • Thermometers: rely on predictable thermal expansion; calibration grounded in Zeroth Law (equilibrium between thermometer & object).
  • Engineering implications
    • Construction joints, bridges, piping require allowances for ΔL\Delta L and ΔV\Delta V to prevent structural failure.
  • Cross-disciplinary links
    • Coefficient of expansion appears in materials science, civil engineering, geophysics (thermal stress in rocks), electronics (thermal management).
  • Ethical / practical relevance
    • Accurate temperature measurement critical in medicine, climate science, and industrial safety.
    • Misunderstanding unit conversion (°F ↔ °C) can cause dosing or operational errors.

Key Equations Cheat-Sheet

  • Temperature conversions
    • F=95C+32F = \frac{9}{5}C + 32
    • K=C+273K = C + 273
  • Linear expansion
    • ΔL=αLΔT\Delta L = \alpha L \Delta T
  • Volumetric expansion
    • ΔV=βVΔT\Delta V = \beta V \Delta T with β=3α\beta = 3\alpha.
  • Third Law statement (entropy reference)
    • Scrystal(0K)=0S_{\text{crystal}}(0\,\text{K}) = 0