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 | |
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