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 353
... MAXWELL'S EQUATIONS IN GENERAL FORM At this point , finally , our present knowledge of macroscopic descriptive electromag- netism is complete and can be ... MAXWELL'S EQUATIONS IN GENERAL FORM 353 Maxwell's Equations in General Form.
... MAXWELL'S EQUATIONS IN GENERAL FORM At this point , finally , our present knowledge of macroscopic descriptive electromag- netism is complete and can be ... MAXWELL'S EQUATIONS IN GENERAL FORM 353 Maxwell's Equations in General Form.
Page 355
... equations in terms of the pairs ( E , H ) , ( D , B ) , and ( D , H ) if it is desirable and the terms that arise can be interpreted in the same way . The so - called integral ... Maxwell's Equations for Linear Isotropic Homogeneous Media.
... equations in terms of the pairs ( E , H ) , ( D , B ) , and ( D , H ) if it is desirable and the terms that arise can be interpreted in the same way . The so - called integral ... Maxwell's Equations for Linear Isotropic Homogeneous Media.
Page 362
... the relation we found after ( 16-40 ) compatible with these re- sults ? This property is often called the duality property of the electromagnetic field . EXERCISES 22-1 Show that ( 22-8 ) and ( 22-9 362 MAXWELL'S EQUATIONS.
... the relation we found after ( 16-40 ) compatible with these re- sults ? This property is often called the duality property of the electromagnetic field . EXERCISES 22-1 Show that ( 22-8 ) and ( 22-9 362 MAXWELL'S EQUATIONS.
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