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Thermodynamics

The Third Law and Low Temperatures

Physics II 330 words Free to read

The Unreachable Floor

The third law comes in two related statements. Nernst: as T0T \to 0, the entropy change of any isothermal process tends to zero. Planck, stronger: the entropy of a perfect crystal tends to zero itself,

limT0S=0\lim_{T\to 0} S = 0

The statistical reading makes this natural. With S=kBlnWS = k_B\ln W, a perfect crystal at zero temperature has exactly one accessible arrangement, so W=1W = 1 and S=0S = 0. Unlike energy, entropy therefore has a genuine absolute zero, which is why tables list absolute SS^\circ rather than differences.

Real systems can retain residual entropy if they freeze into a disordered state. Carbon monoxide, whose CO and OC orientations differ by very little energy, keeps roughly kBln2k_B\ln 2 per molecule, the crystal is not perfect, so Planck's statement does not apply to it.

A striking consequence: heat capacities must vanish as T0T \to 0. Since S(T)=0T(C/T)dTS(T) = \int_0^T (C/T)\,dT' must converge, CC has to fall faster than TT. Experiment agrees, metals show C=γT+AT3C = \gamma T + AT^3, the linear term from electrons and the cubic from phonons.

The third law also implies the unattainability of absolute zero. Cooling methods remove entropy in finite steps, and as S0S \to 0 for every accessible state, each step removes less. Reaching exactly zero would take infinitely many steps. Absolute zero is a limit, not a destination.

Practical cooling uses staged techniques: liquid nitrogen to 77 K, liquid helium to 4.2 K, pumped helium-3 to about 0.3 K, dilution refrigeration to a few millikelvin, and adiabatic demagnetisation below that, magnetise a paramagnetic salt isothermally to order the spins, then demagnetise it adiabatically so the spins re-disorder at the expense of the lattice's thermal energy.

Common pitfall: reading unattainability as a practical difficulty to be engineered around. It is a statement about the structure of thermodynamics: each cooling step removes a smaller entropy increment than the last, so no finite sequence of steps reaches zero however good the apparatus.
Each cooling step halves the gap to zero, and never closes it

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Thermodynamics