Electromagnetic FieldsThis revised edition provides patient guidance in its clear and organized presentation of problems. It is rich in variety, large in number and provides very careful treatment of relativity. One outstanding feature is the inclusion of simple, standard examples demonstrated in different methods that will allow students to enhance and understand their calculating abilities. There are over 145 worked examples; virtually all of the standard problems are included. |
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Page 84
... zero , but , in any event , it is the only component that can be different from zero at the surface . ) Now let us apply Gauss ' law ( 4-1 ) to an arbitrary closed surface that is completely in the interior of a conductor such as S ...
... zero , but , in any event , it is the only component that can be different from zero at the surface . ) Now let us apply Gauss ' law ( 4-1 ) to an arbitrary closed surface that is completely in the interior of a conductor such as S ...
Page 192
... zero , that is , if all of the C , are zero . We can easily show that this is the case . In ( 11-103 ) , we let cos 0 = μ , multiply through by P ( μ ) dμ , integrate over μ from +1 , and use ( 11-102 ) ; in this way we get ∞ 2Cm Σ c ...
... zero , that is , if all of the C , are zero . We can easily show that this is the case . In ( 11-103 ) , we let cos 0 = μ , multiply through by P ( μ ) dμ , integrate over μ from +1 , and use ( 11-102 ) ; in this way we get ∞ 2Cm Σ c ...
Page 431
... zero at any point in a perfect conductor . Since the tangential components of E are always continuous , according to ( 21-26 ) , we see that E , = 0 just outside of the surface . In other words , E has no tangential component at the ...
... zero at any point in a perfect conductor . Since the tangential components of E are always continuous , according to ( 21-26 ) , we see that E , = 0 just outside of the surface . In other words , E has no tangential component at the ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
Electrostatic Forces | 103 |
Copyright | |
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Ampère's law angle assume axis becomes bound charge boundary conditions calculate capacitance capacitor charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance divergence theorem E₁ electric field electromagnetic electrostatic energy equal equipotential evaluate example expression field point flux force function given induction infinitely long integral integrand line charge located Lorentz transformation magnetic magnitude Maxwell's equations obtained parallel particle perpendicular plane wave plates point charge polarized position vector quantities region result scalar potential Section shown in Figure solenoid sphere of radius spherical surface integral tangential components theorem total charge vacuum vector potential velocity volume write written xy plane zero Απερ μο