Equipartition Theorem: Equal Energy Sharing at Thermal Equilibrium

The equipartition theorem is a principle in classical statistical mechanics that states:

At thermal equilibrium, each independent degree of freedom that appears quadratically in the energy contributes, on average, an equal amount of energy—specifically, (1/2) kT per degree of freedom, where k is the Boltzmann constant and T is the temperature in kelvins.

Degrees of freedom refer to the independent ways in which a system can store energy, such as:

  • Translational motion (movement in x, y, z directions),
  • Rotational motion (rotation about axes),
  • Vibrational motion (bond stretching in molecules).

Key Implications:

  • A monatomic ideal gas (with 3 translational degrees) has an average energy of (3/2) kT per atom.
  • A diatomic gas has more degrees of freedom (translational + rotational + vibrational), so its total energy per molecule is higher.
  • The theorem breaks down at very low temperatures or in systems where quantum effects dominate (some degrees of freedom may be “frozen out”).

Examples:

  • Helps predict specific heat capacities of gases and solids.
  • Explains why monatomic gases like helium have lower heat capacities than diatomic gases like oxygen.
  • Used to understand thermal energy distribution in molecules.

The equipartition theorem provides deep insight into how energy is partitioned across the various motions and interactions within a system at thermal equilibrium.

Leave a Reply

Your email address will not be published. Required fields are marked *