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 337
... region of the solenoid of length - z and volume ( z ) S as obtained from ( 20-84 ) is umo = on212 . Similarly , the ... region as the product of the energy density within that region and the outward normal to the region . In this case ...
... region of the solenoid of length - z and volume ( z ) S as obtained from ( 20-84 ) is umo = on212 . Similarly , the ... region as the product of the energy density within that region and the outward normal to the region . In this case ...
Page 351
... regions shown in Figure 21-3 . Region 1 is the volume between the capacitor plates , and 2 is the remainder of that enclosed by the two parallel planes which coincide in part with the plates . Regions 3 and 4 are the rest of space ; I ...
... regions shown in Figure 21-3 . Region 1 is the volume between the capacitor plates , and 2 is the remainder of that enclosed by the two parallel planes which coincide in part with the plates . Regions 3 and 4 are the rest of space ; I ...
Page 430
... region as well as being solutions of Maxwell's equations . As soon as we start thinking about bounded regions , it is evident that there can be many possibilities , both in the shape of the region and in the materials comprising the ...
... region as well as being solutions of Maxwell's equations . As soon as we start thinking about bounded regions , it is evident that there can be many possibilities , both in the shape of the region and in the materials comprising the ...
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 current density curve cylinder dielectric dipole direction distance divergence theorem E₁ electric field electromagnetic electrostatic energy equipotential 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 density surface integral tangential components theorem total charge vacuum vector potential velocity volume wave write written xy plane zero Απερ μο дх