Figure 2 Simulated maximum electric field values for different doping concentrations (10 15 -10 19 cm -2 ) of n -type 4H-SiC and Si. Figure 3 Variations in AFM-LO oxide height with different loading forces and applied voltages.
As evident from Figure 7, the maximum E field values increase with respect to the case in the absence of metallic walls; this increase reaches 15 dB for the 120 cm plane in several points depending on the relative position of the cell phones with respect to the metallic walls.
These values are compared to theoretical values of the maximum field strength E m for avalanche breakdown, which can be calculated after [21, 23] by (2).
Finally, we compare the coil dimensions, overall conductor length as well as coil critical current and maximum field in the winding if the value of required central field changes between 1 and 3 T.
The calculations are for four values of the maximum field strength B 0 within the solenoid.
For each study form, we developed a data dictionary that contained several elements, including the name, description, type, allowable values (range), and maximum field width for each variable.
Remanent polarization [Pr], maximum polarization [Pmax], coercive field [Ec], maximum field [Emax], and loop squareness [Rsq] values were evaluated from the loops.
The increase in average and maximum SAR values is directly proportional to the initial power (P) and the electric field value (E) for each subgroup (Fig. 1).
With maximum field current and thus maximum magnetic flux, the generated voltage will equal the supply voltage at a minimum value of no-load speed.
Although concentrations vary with temperature and reservoir depth for any given petroleum field, maximum values are generally present in Cenozoic-age reservoir rocks in the temperature range 80 to 120°C (Hanor,[111] Kharaka et al.,[79] Lundegard and Kharaka[78]).
