Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 203
... electron of this energy = ~ - 10 1 - B2≈ 0.04 , we get from ( 15 ) N , dv≈ 1 dv 100 v Considering the entire ... electron . However , if the velocity be high enough , the change of velocity may be quite small in the short time the ...
... electron of this energy = ~ - 10 1 - B2≈ 0.04 , we get from ( 15 ) N , dv≈ 1 dv 100 v Considering the entire ... electron . However , if the velocity be high enough , the change of velocity may be quite small in the short time the ...
Page 221
(a Course of Lectures) A. K. Raychaudhuri. 18 Effects due to motion of electrons in material media 1 Cerenkov radiation An electron moving with uniform velocity in a dielectric medium can emit electromagnetic radiation if its velocity ...
(a Course of Lectures) A. K. Raychaudhuri. 18 Effects due to motion of electrons in material media 1 Cerenkov radiation An electron moving with uniform velocity in a dielectric medium can emit electromagnetic radiation if its velocity ...
Page 284
... electron means that if not replenished by external agencies , the accelerated electron would be losing energy . Thus as the electron radiates , it must be experiencing a retarding force which we call the radiation reaction . We would ...
... electron means that if not replenished by external agencies , the accelerated electron would be losing energy . Thus as the electron radiates , it must be experiencing a retarding force which we call the radiation reaction . We would ...
Contents
The empirical basis of electrostatics | 1 |
Direct calculation of fields | 7 |
dipoles9 The Dirac 8function13 | 13 |
Copyright | |
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angle angular axes axis B₁ boundary conditions calculate called charge density charged particle coil components conductor consider coordinates cos² cose dielectric constant dipole dipole moment direction distance E₁ electric field electromagnetic field electromotive force electron electrostatic equation 16 expression field due field point finite fluid formula frame frequency function gives Hence incident interaction Laplace's equation linear Lorentz Lorentz transformation magnetic field magnitude Maxwell's equations momentum motion normal obtain orthogonal P₁ permanent magnets perpendicular photon plane plasma point charge polarization Poynting vector R₁ radiation field radiation reaction radius refracted region scalar sin² solution spherical surface integral symmetry tensor term theorem theory of relativity transformation transverse uniform vanishes vector potential velocity wave length Απ дв дг ді дх