A simple formula is derived which expresses the Debye temperature of a disordered multicomponent alloy with small atomic radius disparity in terms of the Debye temperatures of the pure components, the mole fractions of the components, and a set of undetermined parameters, each of which can be found from the Debye temperature for one composition of each possible binary allo3; made from the components. The formula is an improvement on a similar formula for the binary case due to Mitra and Chattopadhyay because the physical significance of the undetermined parameters is more readily apparent. The influence of short-range order in the binary case is considered. Application is made to the Ag-Au-Pd, Cr-Fe, and Cu-Ni systems in order to test the formula.Recently Mitra & Chattopadhyay (1972) derived a formula which can be used to interpolate the Debye temperature of a binary alloy from the Debye temperatures of the pure metals. It contains one adjustable parameter which can be determined from a measurement of the Debye temperature at one intermediate composition. For such a formula to be useful as an interpolation formula it is necessary that the adjustable parameter be independent of composition, and that there be a physical basis for this. The purpose of the present paper is to derive a generalization of the formula to n-component alloys, and to choose a set of adjustable parameters, the physical significance and composition independence of which is somewhat more apparent than in the formula of Mitra & Chattopadhyay (1972). The influence of short-range order in the case of binary alloys is also considered. The formula is applied to the Fe-Cr, Cu-Ni, and Ag-Au-Pd systems.The derivation of the formula begins with a result which can be deduced from a recent formal analysis of correlations in disordered binary cubic substitutional alloys [see equation (24) of Shirley (1974)]. It is that, in the classical regime, for alloys with negligible atomic radius disparity, the mean-square displacement of an atom from its lattice site is (u 2 ) = x T Trace G(0) = tc T Trace g(0)/2 U", where G(0) is the static Green's function for the 'average' lattice evaluated at the origin. T is the absolute temperature and K is Boltzmann's constant. The second equality holds if nearest-neighbor (n.n.) interactions only are taken into account, g is a dimensionless Green's function [tabulated for f.c.c, by Flinn & Maradudin (1962)] and U" is given by
U"= m 2 Vl't" + m22 V22 + 2mira2 V12 ,where ml and m2 are the mole fractions of type 1 and type 2 atoms, and where V~,~ is the second derivative of the interatomic potential acting between an atom of type x and one of type y, evaluated at the nearest-neighbor separation of the average lattice. If the atoms are noble or transition metals, then the most important part of the potentials at the n.n. separation is the exchange repulsion between the core electrons. The shapes of the potentials are not likely to vary greatly with composition because the core electronic configurations are generally insensitiv...