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In general, the Kapitza resistance may be computed using NEMD simulations by measuring the temperature jump across the considered interface.
Whatever the considered interface, the contact radius is found very small compared to the electron mean free path of materials (reported in Table 2).
We propose a special discretization at and near the points on the interface, which combines the approximation of the governing equations and the considered interface conditions.
The method aims at solving the electromagnetic equations in the stack with weak inhomogeneity hypotheses: where Rq is the quadratic roughness of the considered interface in the case of surface scattering, and p the relative permittivity heterogeneity in the case of bulk scattering (full theory developments are presented in [ 19]).
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The capacities and availabilities of the considered interfaces are also expressed in AUs.
However, the fact that the considered interfaces are brittle triggers some reported numerical difficulties.
In the numerical results, we only compare the energy consumed on the two considered interfaces.
Pipe design to accommodate the thermal contraction considering interface with adjacent components and detailed design of support structure are presented.
It is also revealed that the optimal design considering interface behavior may exhibit tension/compression non-symmetric topology, in which material interfaces mainly undergo compression.
The condition of the dislocation stability and the critical radius of the inclusion are revised for considering interface stresses.
We consider the MAC layer will be responsible for managing collisions in both the considered radio interfaces.
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