phase rule | |
—n | |
degree of freedom See also component the principle that in any system in equilibrium the number of degrees of freedom is equal to the number of components less the number of phases plus two |
phase rule A rule used in thermodynamics stating that the number of degrees of freedom in a physical system at equilibrium is equal to the number of chemical components in the system minus the number of phases plus the constant 2. Also called Gibbs phase rule. See also phase transition, state of matter. |
phase rule
law relating variables of a system in thermodynamic equilibrium, deduced by the American physicist J. Willard Gibbs in his papers on thermodynamics (1875-78). Systems in thermodynamic equilibrium are generally considered to be isolated from their environment in some kind of closed container, but many geological systems can be considered to obey the phase rule. The variables are: the number of phases P (forms of matter; i.e., solid, liquid, and gas not necessarily of a single chemical component), the number of chemical components C (pure compounds or elements), and the number of degrees of freedom F of intensive variables, such as temperature, pressure, and percentage composition. The phase rule states that F = C - P + 2. Thus, for a one-component system with one phase, the number of degrees of freedom is two, and any temperature and pressure, within limits, can be attained. With one component and two phases-liquid and vapour, for example-only one degree of freedom exists, and there is one pressure for each temperature. For one component and three phases (e.g., ice floating in water with water vapour above it, in a closed container), there is no degree of freedom, and temperature and pressure are both fixed at what is called the triple point (see phase diagram).
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