The interfaces between different materials can be coherent (heteroepitaxial), semi-coherent or incoherent.
Differences in strain-rate dependence of mechanical properties between both materials can be explained qualitatively based on the fcc (AISI 316L) and bcc (Fe99.7) lattice structure.
The interface between two materials can be either perfectly bonded, namely type A, so that the continuity of electric displacements holds, or a thin electrode, namely type B, so that the electric potential is grounded.
Reviewing concepts presented earlier, the process of transferring ions between two materials can be broken down into Equations (37),, – (40): (37) (38) (39) (40) in which is the ionic charge.
Furthermore, the thermodynamics of processes of ions crossing boundaries between dissimilar materials can be described in terms of inherent thermodynamic functions, whereas intrinsic thermodynamic functions cannot be used to describe the thermodynamics of ions crossing these boundaries.
Hence, the large variation of Bs observed between the three materials can be attributed to the difference in the paramagnetic PARA.
The shear bond properties between the two materials can be determined by this model in the form of the bond stress-versus-slip relation.
Here the intermediate surfaces between two constituent materials can be directly extracted without building the volumetric mesh, and the manifold topology is preserved on each surface patch.
That is to say that the type of building material and locations, as well as the connections between the building materials can be visualized through the reconstructed 3D model.
Within the IDIS model, a notable perturbation of the molecular DOS is assumed when a molecule approaches a surface, even if the interaction between the two materials can be regarded as weak.
