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 21
... plane , and it is clear that this expression is somehow related to one of the components of da . In order to find this relationship , let us consider Figure 1-26 , which shows a rectangular area ... xy and yz planes VECTOR ELEMENT OF AREA 21.
... plane , and it is clear that this expression is somehow related to one of the components of da . In order to find this relationship , let us consider Figure 1-26 , which shows a rectangular area ... xy and yz planes VECTOR ELEMENT OF AREA 21.
Page 64
... xy plane . For what points , if any , will E1 = 0 ? 3-2 Four point charges are located at the corners of a square in the xy plane . Their values and locations are as follows : q , ( 0,0 ) ; 2q , ( 0 , a ) ; 3q , ( a , 0 ) ; −4q , ( a ...
... xy plane . For what points , if any , will E1 = 0 ? 3-2 Four point charges are located at the corners of a square in the xy plane . Their values and locations are as follows : q , ( 0,0 ) ; 2q , ( 0 , a ) ; 3q , ( a , 0 ) ; −4q , ( a ...
Page 265
... xy plane at the point ( x1 , y1 ) ; the other , with current 12 , intersects the xy plane at ( x2 , y2 ) . Find the resultant B produced by them at any field point ( x , y , z ) . 14-4 A square of edge a lies in the xy plane with the ...
... xy plane at the point ( x1 , y1 ) ; the other , with current 12 , intersects the xy plane at ( x2 , y2 ) . Find the resultant B produced by them at any field point ( x , y , z ) . 14-4 A square of edge a lies in the xy plane with the ...
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Common terms and phrases
Ampère's law angle assume axis bound charge boundary conditions bounding surface calculate capacitance cavity charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb's law current density cylinder defined dielectric dipole direction displacement distance E₁ electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge function given incident induction infinitely long integral integrand k₁ Laplace's equation located Lorentz transformation magnetic magnitude material Maxwell's equations medium molecule n₂ normal components obtained origin parallel plate capacitor particle perpendicular plane wave point charge polarized position vector potential difference quantities radiation rectangular refraction region result satisfy scalar scalar potential shown in Figure solenoid spherical surface charge density tangential components total charge vacuum vector potential velocity volume write written xy plane Z₂ zero Απερ дх