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 144
... polarized dielectric . Figure 10-4 . Origin of bound volume charges in a dielectric with nonuniform polarization . n that Pb = 0 in agreement with ( 10-10 ) . However , there will be no such cancellation on the faces and this will ...
... polarized dielectric . Figure 10-4 . Origin of bound volume charges in a dielectric with nonuniform polarization . n that Pb = 0 in agreement with ( 10-10 ) . However , there will be no such cancellation on the faces and this will ...
Page 168
Roald K. Wangsness. is uniformly polarized in the z direction . Find E at the center of the cube . 10-10 A spherical cavity of radius a is inside a very large dielectric that is uniformly polarized . Find E at the center of the cavity ...
Roald K. Wangsness. is uniformly polarized in the z direction . Find E at the center of the cube . 10-10 A spherical cavity of radius a is inside a very large dielectric that is uniformly polarized . Find E at the center of the cavity ...
Page 428
... polarized , what kind of polariza- tion will the transmitted electric field have in general ? 1 25-6 Evaluate ( S ... polarized such that the components of Eo , perpendicular and parallel to the plane of incidence are equal . Find 0 ...
... polarized , what kind of polariza- tion will the transmitted electric field have in general ? 1 25-6 Evaluate ( S ... polarized such that the components of Eo , perpendicular and parallel to the plane of incidence are equal . Find 0 ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
THE VECTOR POTENTIAL | 16 |
Copyright | |
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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 curve cylinder dielectric dipole direction distance divergence theorem E₁ electric field electromagnetic electrostatic energy equation 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 surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume wave write written xy plane zero Απερ дх