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The microscopic model is based on the fractal modeling approach, which provides an accurate representation of the BP|DM interfacial contact by suppressing the resolution dependence of the surface profiles in consideration.
A microscopic model is presented which describes the anisotropic shrinkage induced by particle rearrangement during sintering.
A microscopic model is also introduced for the volume fraction of the interphase as a function of filler concentration as well as filler filler overlapping.
The microscopic model is often enabling to simulate the real structure with complex geometry, so, a homogenisation technique has been developed.
For the first time, the notion of 'rotary' polaron in such structures is introduced and microscopic model is created, which explains band structure transformation.
The microscopic model is written in terms of the phase formulation, i.e. the liquid saturation phase and the gas pressure phase are primary unknowns.
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To clarify the mechanism of the spin alignment, a microscopic model was designed for a π-electron system interacting with two stable radical groups.
If unable to do so, she made use of the conceptual reasoning scaffolds to take note of which area of the microscopic model was to be viewed more carefully.
For anomalous diffusion, a microscopic model was proposed by the continuous-time random walk with the mean square displacement (langle u^{2}(t)rangle ) growing as (t^{sigma }), where (u(t)), (t> 0) is the probability density function and σ is a positive constant.
A key step in the transition toward a true microscopic model was the realization that n in eq 75 should be set to zero.
Next, a central limit theorem for the martingale part of the microscopic models is presented in Sect.
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