We show that for finite anchoring energy, the saturation transition is possible, and find the correlation between the saturation fields, the anchoring strength, the material and cell parameters.
Since the nuclear energy possesses saturation property, therefore, it is possible for the mass difference between two neighboring nuclides of (Z0N0) and (Z N), namely M(Z N −M Z0N0), to be expanded as power series in terms of ΔZ= Z−Z0 and ΔN= N−N0.
Furthermore, we found that at a constant input voltage the saturation energy density and output energy density, Eout, regardless of the type of N2-lasers and their operational conditions, are linearly correlated.
Figure 4 Plot of the dependency of the thermal energy on the saturation magnetization M s(T) together with the thermal deviation ΔM s(T) due to the saturation magnetization.
Moreover, area of hysteresis loop (magnetization energy density) and saturation magnetic moment/coercive field ratio can also be derived.
Previous literature demonstrated that there are two factors determine the heterogeneous nucleation energy: the gas saturation concentration and the curvature of the surface [43].
However, SONOS-type Flash memories have several drawbacks such as shallow trap energy level, erase saturation, and vertical stored charge migration [74].
According to (25) and (27), the saturation energy threshold (E_{mathrm{S}}) is expressed by: Ln E_{mathrm{S}} equiv left( { - frac{d}{{p_2 }}} right).
However, paraffin/expanded graphite composites provide thermal management only for a certain period of time i.e. until the attainment of saturation energy storage limit.
The striking similarities between changes in the lattice volume, bandgap energy, morphology and saturation magnetization indicated a strong correlation among these properties.
