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 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 ...
Page 185
... RECTANGULAR COORDINATES When ( 11-3 ) is expressed in rectangular coordinates with the use of ( 1-46 ) , it becomes 226 226 226 + + = 0 2х2 ay 2 Əz2 ( 11-55 ) We will try to solve this by assuming a solution in the form of a product of ...
... RECTANGULAR COORDINATES When ( 11-3 ) is expressed in rectangular coordinates with the use of ( 1-46 ) , it becomes 226 226 226 + + = 0 2х2 ay 2 Əz2 ( 11-55 ) We will try to solve this by assuming a solution in the form of a product of ...
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