Classical ElectrodynamicsProblems after each chapter |
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Page 7
... position , and then to derive the vector quantities at the end if necessary ( see below ) . 1.5 Another Equation of Electrostatics and the Scalar Potential The single equation ( 1.13 ) is not enough to specify completely the three ...
... position , and then to derive the vector quantities at the end if necessary ( see below ) . 1.5 Another Equation of Electrostatics and the Scalar Potential The single equation ( 1.13 ) is not enough to specify completely the three ...
Page 124
... position . The initial electrostatic energy is = Wo = 1 1 = √E · Do d3x . Ꭰ ᎴᏆ 8πT € 0 where Do E. Then with the sources fixed in position a dielectric object of volume V1 is introduced into the field , changing the field from Eo to ...
... position . The initial electrostatic energy is = Wo = 1 1 = √E · Do d3x . Ꭰ ᎴᏆ 8πT € 0 where Do E. Then with the sources fixed in position a dielectric object of volume V1 is introduced into the field , changing the field from Eo to ...
Page 150
... position of lowest potential energy . We remark in passing that ( 5.73 ) is not the total energy of the magnetic moment in the external field . In bringing the dipole m into its final position in the field , work must be done to keep ...
... position of lowest potential energy . We remark in passing that ( 5.73 ) is not the total energy of the magnetic moment in the external field . In bringing the dipole m into its final position in the field , work must be done to keep ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ