Zeroth law of thermodynamics

Thermal equilibrium is transitive, enabling temperature to be defined as a state variable.
Zeroth law of thermodynamics

The zeroth law formalizes the idea that “being in thermal equilibrium” is a consistent notion across many systems, and it provides the conceptual foundation for defining .

Definition (transitivity of thermal equilibrium). If system AA is in with system BB, and BB is in thermal equilibrium with system CC, then AA is in thermal equilibrium with CC.

This is often summarized as: thermal equilibrium is transitive.

Physical interpretation. The zeroth law justifies thermometry: if a thermometer (system BB) reaches thermal equilibrium with a system of interest (AA), and the same thermometer reading is obtained when it equilibrates with another system (CC), then AA and CC are mutually in thermal equilibrium. Operationally, this means a single scalar label—temperature—can characterize the “thermal state” shared by systems in mutual thermal equilibrium.

Equivalence-class viewpoint. Define a relation “\sim” on equilibrium states by declaring ABA\sim B if they are in thermal equilibrium. The zeroth law asserts that, on equilibrium states, this relation behaves like an (in particular, it is transitive). The corresponding classes are sometimes emphasized explicitly as .

Consequences in thermodynamics.

  • Temperature as a state variable. The zeroth law supports the existence of a state variable TT that is equal for systems in mutual thermal equilibrium, fitting into the general framework of descriptions.
  • Thermal contact and walls. Whether two systems can approach thermal equilibrium depends on the : a permits energy exchange as heat, while an blocks it.
  • Reservoir idealization. A is an ideal system whose temperature is effectively unchanged by exchanges, making the zeroth-law notion of “same TT” especially operational.

To turn “equal temperature” into a specific numerical scale requires additional structure; see .