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Page 273
This vector potential can be written as the sum of two terms , one of which gives a transverse magnetic induction and the other of which gives a dt = In ( yx ) – Ci ( x ( Sect . 9.3 ] 273 Simple Radiating Systems and Diffraction.
This vector potential can be written as the sum of two terms , one of which gives a transverse magnetic induction and the other of which gives a dt = In ( yx ) – Ci ( x ( Sect . 9.3 ] 273 Simple Radiating Systems and Diffraction.
Page 458
Thus the single - scattering distribution gives only a very small tail on the multiple - scattering curve . There are two things which cause departures from the simple behavior shown in Fig . 13.8 . The Gaussian shape is the limiting ...
Thus the single - scattering distribution gives only a very small tail on the multiple - scattering curve . There are two things which cause departures from the simple behavior shown in Fig . 13.8 . The Gaussian shape is the limiting ...
Page 531
The disappearance of the magnetic moment also gives rise to radiation , but with a spectrum of quite different character . The intensity distribution in angle and frequency for a point magnetic moment in motion is given by ( 14.74 ) .
The disappearance of the magnetic moment also gives rise to radiation , but with a spectrum of quite different character . The intensity distribution in angle and frequency for a point magnetic moment in motion is given by ( 14.74 ) .
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
TimeVarying Fields Maxwells Equations Con | 169 |
Copyright | |
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