Equation 9–3, along with the boundary conditions and loads, governs the
      diffusion process in a homogeneous domain. In an inhomogeneous domain, different materials
      have different saturated concentrations. This difference in the saturation levels is
      responsible for the discontinuity in the concentration across the material interface. To be
      able to use Equation 9–3 in a finite element analysis, a continuous
      variable, normalized concentration , is introduced [401]. 
| (9–5) | 
where  is the saturated concentration of the material (input as CSAT on
        MP command). 
Substituting the concentration  from Equation 9–5 into Equation 9–3
      produces a governing equation for the diffusion analysis in terms of normalized concentration 
:
| (9–6) | 
When  is not specified, it defaults to 1.0 and Equation 9–6
      becomes Equation 9–3.
       can be temperature-dependent for the coupled-field elements
        PLANE222, PLANE223,
        SOLID225, SOLID226, and
        SOLID227 only with thermal and diffusion DOFs. In this case,
      applying the chain rule of differentiation with respect to temperature T to Equation 9–6 without the transport term produces:
| (9–7) | 
For more information, see Thermal-Diffusion Coupling.