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 5
... rectangular coordinates . The product of a scalar s and a vector , which we write as either sA or As , is then ... rectangular coordinate system . They are written ✰ , ŷ , 2 and are defined to be in the directions of the x , y , and z ...
... rectangular coordinates . The product of a scalar s and a vector , which we write as either sA or As , is then ... rectangular coordinate system . They are written ✰ , ŷ , 2 and are defined to be in the directions of the x , y , and z ...
Page 28
... rectangular coordinates , the result is , of course , ( 1-43 ) . 1-16 CYLINDRICAL COORDINATES Up to now , we have used only rectangular coordinates with their constant unit vectors . However , many problems are more conveniently stated ...
... rectangular coordinates , the result is , of course , ( 1-43 ) . 1-16 CYLINDRICAL COORDINATES Up to now , we have used only rectangular coordinates with their constant unit vectors . However , many problems are more conveniently stated ...
Page 31
... rectangular coordinates as given by ( 1-41 ) , ( 1-42 ) , ( 1-43 ) , and ( 1-46 ) by the simple replacement of x , y , z by p , q , z . Similarly , ( 1-44 ) and ( 1-47 ) can only be used for rectangular coordinates ; see ( 1-120 ) for ...
... rectangular coordinates as given by ( 1-41 ) , ( 1-42 ) , ( 1-43 ) , and ( 1-46 ) by the simple replacement of x , y , z by p , q , z . Similarly , ( 1-44 ) and ( 1-47 ) can only be used for rectangular coordinates ; see ( 1-120 ) for ...
Contents
INTRODUCTION | 1 |
ELECTRIC MULTIPOLES | 8 |
Electrostatic Forces | 103 |
Copyright | |
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Ampère's law angle assume axis becomes bound charge boundary conditions calculate capacitance capacitor charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance divergence theorem E₁ electric field electromagnetic electrostatic energy equal equipotential evaluate example expression field point flux force function given induction infinitely long integral integrand line charge located Lorentz transformation magnetic magnitude Maxwell's equations obtained parallel particle perpendicular plane wave plates point charge polarized position vector quantities region result scalar potential Section shown in Figure solenoid sphere of radius spherical surface integral tangential components theorem total charge vacuum vector potential velocity volume write written xy plane zero Απερ μο