Classical Electrodynamics |
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Page 13
Equations (1.13) and (1.16) can be combined into one partial differential
equation for the single function p(x): V*q = —4mp (1.28) This equation is called
Poisson's equation. In regions of space where there is no charge density, the
scalar ...
Equations (1.13) and (1.16) can be combined into one partial differential
equation for the single function p(x): V*q = —4mp (1.28) This equation is called
Poisson's equation. In regions of space where there is no charge density, the
scalar ...
Page 337
an independent equation, but may be derived by combining the last two
equations in (10.91). Since the force equation in (10.91) is independent of
magnetic field, we suspect that there exist solutions of a purely electrostatic
nature, with B = 0.
an independent equation, but may be derived by combining the last two
equations in (10.91). Since the force equation in (10.91) is independent of
magnetic field, we suspect that there exist solutions of a purely electrostatic
nature, with B = 0.
Page
Then we find the parallel velocity at any position along the z axis given by 2 B(2)
Bo Equation (12.128) for the velocity of the particle in the z direction is equivalent
to the first integral of Newton's equation of motion for a particle in a ...
Then we find the parallel velocity at any position along the z axis given by 2 B(2)
Bo Equation (12.128) for the velocity of the particle in the z direction is equivalent
to the first integral of Newton's equation of motion for a particle in a ...
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Contents
Introduction to Electrostatics | 1 |
Nš 3 | 3 |
Greens theorem | 14 |
Copyright | |
30 other sections not shown
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Common terms and phrases
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 |