The derivation for the Gibbs phase
rule, provided in physical chemistry
text books, often assumes that all the components are present in all
the phases coexisting at equilibrium. However, very often we have
situations where all the phases at equilibrium do not have all the
components, the binary eutectic system being a classic example. The
melt (miscible solution of A and B) coexists with pure solid A and
pure solid B at the eutectic point. The solid phases are one-component
phases, whereas the system itself is binary. How does the phase rule,
derived under the above-mentioned assumption, apply to the eutectic
point? Using a simple example, we demonstrate that all the components need not be present in all the phases to arrive at the phase
rule.