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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 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 ...
Page 392
Favor ( 12.1 ) с dom - Sver where v , = ( v , ic ) , and Fm , is interpreted as the average field acting on the particle . The left - hand side of ( 12.1 ) is now to be equated to the time rate of change of the momentum and energy of ...
Favor ( 12.1 ) с dom - Sver where v , = ( v , ic ) , and Fm , is interpreted as the average field acting on the particle . The left - hand side of ( 12.1 ) is now to be equated to the time rate of change of the momentum and energy of ...
Page 555
To determine the equation satisfied by the electric multipole function fim ( r ) inside the source , we substitute ( 16.82 ) into the first equation of ( 16.80 ) , take the scalar product of both sides with a typical xim , and integrate ...
To determine the equation satisfied by the electric multipole function fim ( r ) inside the source , we substitute ( 16.82 ) into the first equation of ( 16.80 ) , take the scalar product of both sides with a typical xim , and integrate ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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