Abundance was determined as the average of 10 fields (volumes filtered generally yielded 30 300 cells per field).
For the sake of simplicity, we consider a 2D diffusive field volume of Λ = [-50,50] × [-50,50]m2.
The normalized MSE and CRLB are obtained by dividing each with the diffusive field volume.
A device configuration parameter, D, is defined that links the field volume to the volume of magnetocaloric material.
In addition, the changes of critical buckling temperature due to the effects of temperature field, volume fraction distributions, and system geometric parameters are studied.
The achieved final magnet designs fulfill the predefined requirements of particular field distribution in the air gap, maximized ratio of high field volume to the permanent magnet volume, best utilization of magnets and magnetocaloric materials and constructional simplicity.
For instance, if the available for the system of atoms and field volume has the value equal to V = 0.001 m3, then g = ρ ex ω res 2 ℏ ε 0 V ≈ 77.8597 π rad/sec.
Numerical examples show that the interfacial shear stress transfer behavior can be described and affected by several parameters such as the temperature field, volume fraction of CNT, and numbers of wall layer and the outermost radius of carbon nanotubes.
Time-harmonic electromagnetic scattering by inhomogeneous, three-dimensional structures within a free space environment can be described by electric- and magnetic field, volume integral equations involving the free space Green function.
Finally, the effects of temperature dependence of material properties, temperature field, volume fraction index, geometrical parameters and the boundary conditions on the thermal buckling characteristic of the FG plates of various shapes are studied.
