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 66
... charge density given by p = Ar2 Ar2 where A = const . Another sphere of radius 2a is concentric with the first . Find the flux E da through the surface of the larger sphere . • 4-3 The infinite line charge of Figure 4-3 is surrounded by ...
... charge density given by p = Ar2 Ar2 where A = const . Another sphere of radius 2a is concentric with the first . Find the flux E da through the surface of the larger sphere . • 4-3 The infinite line charge of Figure 4-3 is surrounded by ...
Page 143
... charge density p , distributed throughout the volume and a surface charge density σ , on the bounding surface where Рь b = -- = -V ' . P P.n = Pn ( 10-7 ) ( 10-8 ) for then we would have 1 $ ( r ) = Απεργι S Podr ' 1 + R $ 0 da ' ( 10-9 ) ...
... charge density p , distributed throughout the volume and a surface charge density σ , on the bounding surface where Рь b = -- = -V ' . P P.n = Pn ( 10-7 ) ( 10-8 ) for then we would have 1 $ ( r ) = Απεργι S Podr ' 1 + R $ 0 da ' ( 10-9 ) ...
Page 157
... charge density in a l.i.h. dielectric can always be written as ρ = Pf Ke = Ke Pb 1 - = = 0 , then Pь Pf ( 10-59 ) which shows us that the total charge density is always less than the free charge density since Ke > 1. As a special case ...
... charge density in a l.i.h. dielectric can always be written as ρ = Pf Ke = Ke Pb 1 - = = 0 , then Pь Pf ( 10-59 ) which shows us that the total charge density is always less than the free charge density since Ke > 1. As a special case ...
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