## 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 26

We have proved this only for a volume bounded by a single surface, but we can

easily extend the proof to a region ... the plane surfaces of intersection shown by

AB and CD; the outward normal to the new part of the

...

We have proved this only for a volume bounded by a single surface, but we can

easily extend the proof to a region ... the plane surfaces of intersection shown by

AB and CD; the outward normal to the new part of the

**bounding surface**is shown...

Page 156

... in the tangential components of F. If we combine these results with those of the

last section, we see that we have obtained a way of finding how the vector F at

the surface of discontinuity changes as we go across the

... in the tangential components of F. If we combine these results with those of the

last section, we see that we have obtained a way of finding how the vector F at

the surface of discontinuity changes as we go across the

**bounding surface**.Page 499

Therefore, if we take any solution of the appropriate two-dimensional electrostatic

potential problem that gives an electric field normal to the perfectly conducting

Therefore, if we take any solution of the appropriate two-dimensional electrostatic

potential problem that gives an electric field normal to the perfectly conducting

**bounding surface**, call this field S , and then find % from (26-67), we can use the ...### What people are saying - Write a review

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angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law cross section current density current element curve cylinder defined dielectric direction displacement distance electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge free currents frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz Lorentz transformation magnitude material Maxwell's equations molecule normal components obtained origin particle perpendicular plane wave point charge polarized position vector potential difference propagation properties quadrupole quantities radiation region relation result satisfy scalar potential shown in Figure situation solenoid spherical substitute surface current surface integral tangential components total charge unit vacuum vector potential velocity volume write written xy plane zero