## 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 55

One can quite easily adopt the point of view that this is done merely for

mathematical convenience, if for no other reason than one saves some writing by

not having to carry the symbol q along in all of the equations, but can

first and ...

One can quite easily adopt the point of view that this is done merely for

mathematical convenience, if for no other reason than one saves some writing by

not having to carry the symbol q along in all of the equations, but can

**calculate**Efirst and ...

Page 335

In Section 18-2 we saw that one of the useful applications of the energy

expression was the

other means, we can evaluate (20-83) and by equating it to (18-9), L can be

found from L ...

In Section 18-2 we saw that one of the useful applications of the energy

expression was the

**calculation**of self-inductance. If we have found the fields byother means, we can evaluate (20-83) and by equating it to (18-9), L can be

found from L ...

Page 426

This effect generally goes under the name of radiation pressure and we can

easily

pressure is strongly reminiscent of that of the pressure exerted by a gas on the ...

This effect generally goes under the name of radiation pressure and we can

easily

**calculate**it from results we have already obtained. (This origin of radiationpressure is strongly reminiscent of that of the pressure exerted by a gas on the ...

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### Common terms and phrases

angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitance capacitor cavity charge density charge distribution charge q circuit conductor const constant convenient corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance divergence theorem electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge line integral located Lorentz transformation magnetic magnitude Maxwell's equations obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector potential difference quantities rectangular coordinates region result scalar potential shown in Figure solenoid sphere of radius spherical surface integral tangential components theorem total charge unit vectors vacuum vector potential velocity volume write written xy plane zero