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 for any arbitrary value of the angle 0 , it seems plausible that this can be the case only if each term in the sum is itself zero , that is , if all of the C , are zero . We can easily show that this is the case . In ( 11-103 ) ...
... zero for any arbitrary value of the angle 0 , it seems plausible that this can be the case only if each term in the sum is itself zero , that is , if all of the C , are zero . We can easily show that this is the case . In ( 11-103 ) ...
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 Etang = 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 Etang = 0 just outside of the surface . In other words , E has no tangential component at the ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
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Common terms and phrases
Ampère's law angle assume axes axis bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law current density curve cylinder dielectric dipole direction distance divergence theorem E₁ electric field electromagnetic electrostatic energy equipotential evaluate example expression field point free charge function given induction infinitely long integral integrand Laplace's equation line charge line integral located magnetic magnitude Maxwell's equations obtained origin P₁ perpendicular point charge polarized position vector potential difference quadrupole R₁ region result scalar potential Section shown in Figure sphere of radius spherical surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume wave write written xy plane zero Απερ μο дх