Skip to content
Home

Third law of thermodynamics

Principle describing the behaviour of entropy as temperature approaches absolute zero and its practical and conceptual consequences in physics and chemistry.

Overview

The third law of thermodynamics describes the behaviour of entropy as a system is cooled toward absolute zero. In standard formulations it states that the entropy S of a perfect crystalline substance approaches a constant value as temperature approaches 0 K (equivalent to −273.15 °C or −459.67 °F). For an ideal, defect‑free crystal this constant is taken to be zero, so that a single unique ground state corresponds to zero entropy.

Image gallery

2 Images

Formulations and interpretation

Several closely related statements exist. Planck's formulation assigns zero entropy to a perfectly ordered crystal at zero kelvin. The Nernst heat theorem describes how entropy changes associated with physical or chemical transformations vanish as temperature approaches absolute zero. A practical corollary, commonly called the unattainability principle, states that no physical process can reduce a system to absolute zero in a finite number of steps.

Microscopic and quantum considerations

From statistical mechanics, entropy measures the number of accessible microscopic states. As thermal energy is removed, fewer microstates are thermally occupied and entropy decreases. Quantum mechanics modifies the classical intuition: even at the lowest energy a system may exhibit zero‑point motion and quantum fluctuations, so the simple idea that atoms literally "stop moving" is misleading. Moreover, if the ground state is degenerate or disordered there can be residual entropy at the lowest temperatures.

Residual entropy and examples

Certain materials show measurable entropy remaining as temperature approaches zero because of multiple equivalent ground configurations. Examples discussed in textbooks and experiments include some molecular crystals, glassy solids and particular magnetic systems such as "spin ices." These cases do not invalidate the third law but illustrate that its simplest statement requires qualification: it applies strictly to perfect, nondegenerate crystalline ground states.

Experimental approach to low temperatures

Experimentally, reaching arbitrarily close to absolute zero is possible in the sense of making the temperature ever smaller, but absolute zero itself remains unattainable by finite operations. Cooling techniques used in cryogenics and low‑temperature physics include evaporative cooling, adiabatic demagnetization, laser cooling and dilution refrigeration. These methods have enabled exploration of phenomena such as superconductivity, superfluidity and Bose–Einstein condensation at millikelvin and lower regimes.

Consequences and practical role

The third law provides a reference for absolute entropy scales used in chemistry and materials science (standard definitions). It explains why heat capacities and other response functions typically vanish as temperature approaches zero and why cooling efficiency declines near 0 K. The law also sets conceptual limits for thermodynamic cycles and information‑theoretic considerations at very low temperatures.

Careful statements and modern perspective

Modern texts present the third law with careful qualifications: it concerns the limit T→0 and the behaviour of entropy differences; it presumes an idealized crystalline ground state unless residual degeneracy is specified. In all accepted forms the law is a robust principle of equilibrium thermodynamics and a useful guide for both theory and experiment.

Related articles

Author

AlegsaOnline.com Third law of thermodynamics

URL: https://en.alegsaonline.com/art/99399

Share