vanishes for one microstate and is positive for more
ProvedThirdLawThermo.boltzmannEntropy_one_eq_zero_and_posLet be the Boltzmann constant and let be the Boltzmann entropy of a macrostate with accessible microstates.
Theorem.
- If only one microstate is accessible, the entropy vanishes: .
- If the number of accessible microstates is greater than one, the entropy is positive:
This is the statistical-mechanics reading of the third law used throughout the source: a system at absolute zero with a single accessible configuration has zero entropy, while at positive temperature several microstates are accessible and the entropy is positive.
import Definitions.Def_ThirdLawThermo_Defs import Mathlib open Filter Topology
namespace ThirdLawThermo
theorem boltzmannEntropy_one_eq_zero_and_pos (kB : ℝ) (hkB : 0 < kB) :
boltzmannEntropy kB 1 = 0 ∧ ∀ W : ℕ, 1 < W → 0 < boltzmannEntropy kB W := by sorry
end ThirdLawThermoRead-back
What the Lean code literally says, in plain math · Aristotle (Harmonic), the drafting agent itself; non-blind read-back
Disclosure: this read-back is NOT blind. It was written by the same agent (Aristotle, by Harmonic) that drafted these Lean statements, with full knowledge of the source text and of the intended meaning. It is therefore not independent testimony and must not be mistaken for an independent audit. Reviewers should check the Lean code against the source themselves.
Let be a real number with . The statement is the conjunction of two claims about (with viewed as a real number):
- ;
- for every natural number with (i.e. ), .
The cases and are excluded from the second claim.