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 91
... equal and opposite to the charge on the other . - Accordingly , we take for our general definition of a capacitor the following : any two conductors with equal and opposite charges Q and Q. Even so , it is not immediately evident that ...
... equal and opposite to the charge on the other . - Accordingly , we take for our general definition of a capacitor the following : any two conductors with equal and opposite charges Q and Q. Even so , it is not immediately evident that ...
Page 283
... equal to b and the radius of its circular cross section is a . Show that its self- inductance is N2 [ b ( b2 - a2 ) 1 / 2 ] . - 17-21 A toroidal coil of N turns has a central radius b and a square cross section of side a . Find its self ...
... equal to b and the radius of its circular cross section is a . Show that its self- inductance is N2 [ b ( b2 - a2 ) 1 / 2 ] . - 17-21 A toroidal coil of N turns has a central radius b and a square cross section of side a . Find its self ...
Page 359
... equal to the rate at which energy is being dissipated into heat within the volume . This is exactly what is required ... equal and opposite , that is , they are in agreement with Newton's third law . On the other hand , we found in ( 13 ...
... equal to the rate at which energy is being dissipated into heat within the volume . This is exactly what is required ... equal and opposite , that is , they are in agreement with Newton's third law . On the other hand , we found in ( 13 ...
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