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 389
... wave . The other part represents a static field that can be a function of position ; while this is a possibility ... PLANE WAVE IN AN ARBITRARY DIRECTION For simplicity , we have considered only plane waves traveling in a specific ...
... wave . The other part represents a static field that can be a function of position ; while this is a possibility ... PLANE WAVE IN AN ARBITRARY DIRECTION For simplicity , we have considered only plane waves traveling in a specific ...
Page 403
... plane wave travels in the positive z direction in a conductor with real conductivity . ( a ) Find the instantaneous and time average power loss per unit volume due to resistive heating for any z . ( b ) Find the total power loss per ...
... plane wave travels in the positive z direction in a conductor with real conductivity . ( a ) Find the instantaneous and time average power loss per unit volume due to resistive heating for any z . ( b ) Find the total power loss per ...
Page 419
... wave travels more slowly than a usual plane wave ; ( 25-57 ) is not a plane wave in the sense that its value is not constant on a plane perpendicular to the direction of propagation . Furthermore , the wave speed v2 , is not a constant ...
... wave travels more slowly than a usual plane wave ; ( 25-57 ) is not a plane wave in the sense that its value is not constant on a plane perpendicular to the direction of propagation . Furthermore , the wave speed v2 , is not a constant ...
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