Classical Electrodynamics |
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Page 174
For such time-varying fields there are induced electromotive forces which cause
the sources of current to do work. Since the energy in the field is by definition the
total work done to establish it, we must consider these contributions. Suppose for
...
For such time-varying fields there are induced electromotive forces which cause
the sources of current to do work. Since the energy in the field is by definition the
total work done to establish it, we must consider these contributions. Suppose for
...
Page 208
Either o or k can be viewed as the independent variable when one considers
making a linear superposition. ... To allow for the possibility of dispersion we will
consider a as a general function of k: a) = 0(k) (7.25) Since the dispersive
properties ...
Either o or k can be viewed as the independent variable when one considers
making a linear superposition. ... To allow for the possibility of dispersion we will
consider a as a general function of k: a) = 0(k) (7.25) Since the dispersive
properties ...
Page 269
... the electric field is e-ov × B (9.5) Given a current distribution J(x'), the fields can,
in principle at least, be determined by calculating the integral in (9.3). We will
consider one or two examples of direct integration of the source integral in
Section ...
... the electric field is e-ov × B (9.5) Given a current distribution J(x'), the fields can,
in principle at least, be determined by calculating the integral in (9.3). We will
consider one or two examples of direct integration of the source integral in
Section ...
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Contents
Introduction to Electrostatics | 1 |
Nē 3 | 3 |
Greens theorem | 14 |
Copyright | |
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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends 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 limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative result satisfy scalar scattering shows side simple 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 |