Classical Electrodynamics |
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Page 12
This can be seen by letting the observation point come infinitesimally close to the
double layer . The double layer is now imagined to consist of two parts , one
being a small disc directly under the observation point . The disc is sufficiently
small ...
This can be seen by letting the observation point come infinitesimally close to the
double layer . The double layer is now imagined to consist of two parts , one
being a small disc directly under the observation point . The disc is sufficiently
small ...
Page 292
Historically , diffraction patterns were classed as Fresnel diffraction and
Fraunhofer diffraction , depending on the distance of the observation point from
the diffracting system . Generally the diffracting system ( e . g . , an aperture in an
opaque ...
Historically , diffraction patterns were classed as Fresnel diffraction and
Fraunhofer diffraction , depending on the distance of the observation point from
the diffracting system . Generally the diffracting system ( e . g . , an aperture in an
opaque ...
Page 531
81 ) where is the angle between u and the observation direction n . In a
semiclassical sense the electronic magnetic moment can be thought of as having
a magnitude u = V 3 ( eħ / 2mc ) , but being observed only through its projection
pz = E ...
81 ) where is the angle between u and the observation direction n . In a
semiclassical sense the electronic magnetic moment can be thought of as having
a magnitude u = V 3 ( eħ / 2mc ) , but being observed only through its projection
pz = E ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |