Classical ElectrodynamicsProblems after each chapter |
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Page 7
However , it is often simpler to deal with scalar rather than vector functions of position , and then to derive the vector quantities at the end if necessary ( see below ) . 1.5 Another Equation of Electrostatics and the Scalar ...
However , it is often simpler to deal with scalar rather than vector functions of position , and then to derive the vector quantities at the end if necessary ( see below ) . 1.5 Another Equation of Electrostatics and the Scalar ...
Page 8
1.3 D ( x ) = 1 In ( 1.15 ) the electric field ( a vector ) is derived from a scalar by the gradient operation . Since one function of position is easier to deal with than three , it is worth while concentrating on the scalar function ...
1.3 D ( x ) = 1 In ( 1.15 ) the electric field ( a vector ) is derived from a scalar by the gradient operation . Since one function of position is easier to deal with than three , it is worth while concentrating on the scalar function ...
Page
16 Multipole Fields In Chapters 3 and 4 on electrostatics the spherical harmonic expansion of the scalar potential was used extensively for problems possessing some symmetry property with respect to an origin of coordinates .
16 Multipole Fields In Chapters 3 and 4 on electrostatics the spherical harmonic expansion of the scalar potential was used extensively for problems possessing some symmetry property with respect to an origin of coordinates .
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Contents
Introduction to Electrostatics | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
11 other sections not shown
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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 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 sphere spherical surface transformation unit vanishes vector velocity volume wave written