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⚡️College Physics III – Thermodynamics, Electricity, and Magnetism Unit 3 Review

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3.5 Heat Capacities of an Ideal Gas

⚡️College Physics III – Thermodynamics, Electricity, and Magnetism
Unit 3 Review

3.5 Heat Capacities of an Ideal Gas

Written by the Fiveable Content Team • Last updated September 2025
Written by the Fiveable Content Team • Last updated September 2025
⚡️College Physics III – Thermodynamics, Electricity, and Magnetism
Unit & Topic Study Guides

Heat capacity in ideal gases is a crucial concept in thermodynamics. It measures how much heat energy is needed to raise a substance's temperature by one degree. Understanding this helps us grasp how gases behave under different conditions and how energy flows in thermal systems.

The relationship between heat capacity at constant pressure and constant volume is key for ideal gases. It's linked to the gas's molecular structure and degrees of freedom. This connection helps us predict how gases will respond to heating in various situations, from engine cylinders to atmospheric processes.

Heat Capacities of Ideal Gases

Heat capacity in ideal gases

  • Quantifies heat required to change temperature of a substance by 1°C or 1K
    • Isobaric process occurs at constant pressure
      • Molar heat capacity at constant pressure denoted as $C_p$
      • Defined as $C_p = (\frac{\partial H}{\partial T})_p$ where $H$ represents enthalpy
    • Isochoric process occurs at constant volume
      • Molar heat capacity at constant volume denoted as $C_V$
      • Defined as $C_V = (\frac{\partial U}{\partial T})_V$ where $U$ represents internal energy

Specific heat calculations

  • Specific heat is heat capacity per unit mass
    • At constant pressure, specific heat $c_p = \frac{C_p}{m}$ where $m$ is mass
    • At constant volume, specific heat $c_V = \frac{C_V}{m}$
  • For an ideal gas:
    • $C_p = C_V + R$ where $R$ is universal gas constant
    • $C_p = \frac{f+2}{2}R$ where $f$ is degrees of freedom (translational, rotational, vibrational)
    • $C_V = \frac{f}{2}R$
    • Ratio of specific heats $\gamma = \frac{C_p}{C_V} = \frac{f+2}{f}$ (5/3 for monatomic, 7/5 for diatomic)
    • These relationships are derived from the equipartition theorem

Ideal vs real gas heat capacities

  • Ideal gas heat capacities are:
    • Independent of temperature and pressure
    • Dependent only on degrees of freedom (monatomic, diatomic, polyatomic)
  • Real gas heat capacities:
    • Vary with temperature and pressure changes
    • Deviate from ideal behavior at low temperatures and high pressures
    • Affected by intermolecular forces (van der Waals) and finite molecular size

Temperature effects on gas specific heat

  • In ideal gases, specific heat remains constant with temperature changes
  • For real gases:
    • Specific heat increases at higher temperatures
      • More energy required to excite vibrational and rotational modes (bending, stretching)
    • At high temperatures, specific heat approaches ideal gas value
      • Kinetic energy dominates over intermolecular forces
    • $c_p$ always greater than $c_V$
      • Additional work done by gas during expansion at constant pressure (piston, cylinder)

Thermodynamic Processes and Heat Capacity

  • Adiabatic process: No heat exchange with surroundings, important for understanding heat capacity's role in temperature changes
  • Various thermodynamic processes affect how heat capacity influences system behavior
  • Internal energy and enthalpy are state functions crucial for describing heat capacity in different processes