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Wikipedia / Lattice diffusion coefficient

In condensed matter physics, lattice diffusion (also called bulk or volume diffusion) refers to atomic diffusion within a crystalline lattice, which occurs by either interstitial or substitutional mechanisms. In interstitial lattice diffusion, a diffusant (such as carbon in an iron alloy), will diffuse in between the lattice structure of another crystalline element. In substitutional lattice diffusion (self-diffusion for example), the atom can only move by switching places with another atom. Substitutional lattice diffusion is often contingent upon the availability of point vacancies throughout the crystal lattice. Diffusing particles migrate from point vacancy to point vacancy by the rapid, essentially random jumping about (jump diffusion). Since the prevalence of point vacancies increases in accordance with the Arrhenius equation, the rate of crystal solid state diffusion increases with temperature. For a single atom in a defect-free crystal, the movement can be described by the "random walk" model.

Diffusion Coefficient for Interstitial Diffusion

An atom diffuses in the interstitial mechanism by passing from one interstitial site to one of its nearest neighboring interstitial sites. The movement of atoms can be described as jumps, and the interstitial diffusion coefficient depends on the jump frequency. The jump frequency, is given by:

where

can be expressed as the sum of activation enthalpy and the activation entropy, which gives the diffusion coefficient as:

where

  • is the jump distance.

The diffusion coefficient can be simplified to an Arrhenius equation form:

where

is only dependent on the activation energy barrier to the movement of interstitial atoms from one site to another. The diffusion coefficient increases exponentially.

Diffusion Coefficient for Substitution Diffusion

Self-Diffusion

The rate of self-diffusion can be measured experimentally by introducing radioactive A atoms (A*) into pure A and measuring the rate at which penetration occurs at various temperatures. A* and A atoms have approximately identical jump frequencies since they are chemically identical. The diffusion coefficient of A* and A can be related to the jump frequency and expressed as:

where

  • is the diffusion coefficient of radioactive A atoms in pure A.

  • is the diffusion coefficient of A atoms in pure A.

  • is the jump frequency for both the A* and A atoms.

  • is the jump distance.

An atom can make a successful jump when there are vacancies nearby and when it has enough thermal energy to overcome the energy barrier to migration. The number of successful jumps an atom will make in one second, or the jump frequency, can be expressed as:

where

  • is the number of nearest neighbors.

  • is the frequency of temperature-independent atomic vibration.

  • is the vacancy fraction of the lattice.

  • is the activation energy barrier to atomic migration.

In thermodynamic equilibrium,

is the free energy of vacancy formation for a single vacancy.

, giving:

Substituting ΔG = ΔH – TΔS gives:

The diffusion coefficient can be simplified to an Arrhenius equation form:

where

Compared to that of interstitial diffusion, the activation energy for self-diffusion has an extra term (ΔHv). Since self-diffusion requires the presence of vacancies whose concentration depends on ΔHv.

Vacancy Diffusion

Diffusion of a vacancy can be viewed as the jumping of a vacancy onto an atom site. It is the same process as the jumping of an atom into a vacant site but without the need to consider the probability of vacancy presence, since a vacancy is usually always surrounded by atom sites to which it can jump. A vacancy can have its own diffusion coefficient that is expressed as:

is the jump frequency of a vacancy.

) of a vacancy, which are the same as for the migration of a substitutional atom:

Comparing the diffusion coefficient between self-diffusion and vacancy diffusion gives:

Diffusion in a Binary System

In a system with multiple components (e.g. a binary alloy), the solvent (A) and the solute is defined by the Darken's equation as:

are the amount fractions of species A and B, respectively.

See also

References