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Pulse electrolysis, when lumped parameters L, C, and R cannot be used in principle. We will show that σ can be calculated using the Maxwell phenomenological macroscopic electromagnetic equations and the electric-charge conservation law accounting for the special features of the interface between the adjacent media. Separate consideration will be given to ion conductors. In constructing a E H are not independent physicomathematical model, we take into account that and functions; therefore, the wave equation for E or H is more preferable than the system of equations (see Equations 6 and 7).
Vesec, I. , 2001; Broe, I. , 1997). , σ(E(∂E/∂t, H(∂H/∂t))); therefore, the surface impedances (Wei Hu & Hong Guo, 2002; Danae, D. , 2002; Larruquert, J. , 2001; Koludzija, B. , 1999; Ehlers, R. A. & Metaxas, A. , 2003) are true for the conditions under which they are determined. These impedances cannot be used in experiments conducted under other experimental conditions. , pulse electrolysis, when lumped parameters L, C, and R cannot be used in principle. We will show that σ can be calculated using the Maxwell phenomenological macroscopic electromagnetic equations and the electric-charge conservation law accounting for the special features of the interface between the adjacent media.
An optical knife, or in diffraction of the electromagnetic wave on a system of parallel lobes, when the gap between the lobes is in the region of microns, and the electromagnetic field is strongly “cut” throughout the space with a step much than the wavelength. A) Optical Knife Figure 7 shows the field of an electromagnetic wave in its diffraction on the optical knife. The parameters of the wave at entry and at exit are Ex=104sin(1010t), Ey=104cos (1010t). 774·107 S/m; the ambient medium is air.