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Page 237
First we assume that just outside the conductor there exists only a normal electric
field E, and a tangential magnetic field Ho, as for a perfect conductor. The values
of these fields are assumed to have been obtained from the solution of an ...
First we assume that just outside the conductor there exists only a normal electric
field E, and a tangential magnetic field Ho, as for a perfect conductor. The values
of these fields are assumed to have been obtained from the solution of an ...
Page 241
John David Jackson. adequately by the methods of Section 8.1. A cylindrical
surface S of general cross-sectional contour is shown in Fig. 8.3. For simplicity,
the cross-sectional size and shape are assumed constant along the cylinder axis.
John David Jackson. adequately by the methods of Section 8.1. A cylindrical
surface S of general cross-sectional contour is shown in Fig. 8.3. For simplicity,
the cross-sectional size and shape are assumed constant along the cylinder axis.
Page 297
The dimensions of the hole are assumed to be very small compared to a
wavelength of the electromagnetic fields which are assumed to exist on one side
of the sheet. The problem is to calculate the diffracted fields on the other side of
the ...
The dimensions of the hole are assumed to be very small compared to a
wavelength of the electromagnetic fields which are assumed to exist on one side
of the sheet. The problem is to calculate the diffracted fields on the other side of
the ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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