Deformation during interdiffusion

Abstract A general theory of stress and deformation during interdiffusion is presented which spans the gap between the Darken analysis of the Kirkendall effect and the recent treatment by Larche and Cahn of the interaction between stress and diffusion. Special consideration is given to the generation of internal stress and vacancy chemical potential, to the contribution of these potentials to the diffusion potentials, to the relaxation of these potentials via plastic deformation and vacancy creation/annihilation, and to convective transport due to deformation induced by diffusion. When the mobilities or the partial molal volumes of the components differ, the coupling of the relaxation equations for plastic strain and vacancy creation to the diffusion equations for the component densities can lead to a change in the rate-limiting step for interdiffusion as a function of the distance scale of the composition and stress profiles. The characteristic lengths at which these changes occur are determined by relations between the mobilities, the viscosity, and the rate constant for vacancy creation. When a relaxation process is rate-limiting, composition penetration profiles have an exponential (rather than error-function) form, and the integrated amount of material transported increases linearly with time (rather than as t 1 2 ).

[1]  A. R. Cooper Electric field buildup and relaxation for chemical diffusion , 1974 .

[2]  John W. Cahn,et al.  On Spinodal Decomposition , 1961 .

[3]  George W. Housner,et al.  The Analysis Of Stress And Deformation , 1966 .

[4]  J. Ross,et al.  A derivation and comparison of two equations (Landau–Ginzburg and Cahn) for the kinetics of phase transitions , 1976 .

[5]  G. Yurek,et al.  Deviations from Local Thermodynamic Equilibrium During Interdiffusion of CoOMgO and CoONiO , 1975 .

[6]  John W. Cahn,et al.  Overview no. 41 The interactions of composition and stress in crystalline solids , 1985 .

[7]  John Crank,et al.  The Mathematics Of Diffusion , 1956 .

[8]  G. H. Frischat Ionic diffusion in oxide glasses , 1975 .

[9]  Conyers Herring,et al.  Diffusional Viscosity of a Polycrystalline Solid , 1950 .

[10]  M. Planck,et al.  Ueber die Erregung von Electricität und Wärme in Electrolyten , 1890 .

[11]  J. R. Manning,et al.  Diffusion Kinetics for Atoms in Crystals , 1968 .

[12]  R. A. Oriani,et al.  The Thermodynamics of Stressed Solids , 1966 .

[13]  Noreen L. Thomas,et al.  A theory of case II diffusion , 1982 .

[14]  J. Langer,et al.  New computational method in the theory of spinodal decomposition , 1975 .

[15]  G. Stephenson Spinodal decomposition in amorphous systems , 1984 .

[16]  A. R. Cooper,et al.  Stress Buildup and Relaxation During Ion Exchange Strengthening of Glass , 1987 .

[17]  J. Cahn,et al.  A linear theory of thermochemical equilibrium of solids under stress , 1973 .

[18]  F. C. Larcht'e,et al.  The effect of self-stress on diffusion in solids , 1982 .

[19]  A. R. Cooper,et al.  Atomic mobilities and multicomponent diffusion , 1965 .

[20]  G. Stephenson Plastic strain and stress during interdiffusion , 1986 .

[21]  Samuel Glasstone,et al.  The Theory Of Rate Processes , 1941 .

[22]  J. Langer Statistical methods in the theory of spinodal decomposition , 1973 .

[23]  R. Doremus Exchange and Diffusion of Ions in Glass , 1964 .