## 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 24

Again, for convenience, we have written the

sign although in reality it is a triple integral. Since S is a closed surface, the unit

normal fl used for dais the outward normal according to our convention of ...

Again, for convenience, we have written the

**volume**integral with a single integralsign although in reality it is a triple integral. Since S is a closed surface, the unit

normal fl used for dais the outward normal according to our convention of ...

Page 26

We have proved this only for a

easily extend the proof to a region bounded by several surfaces, such as a

hollow ball. Figure l-32 shows a

two ...

We have proved this only for a

**volume**bounded by a single surface, but we caneasily extend the proof to a region bounded by several surfaces, such as a

hollow ball. Figure l-32 shows a

**volume**V surrounded by two surfaces S, and S2;two ...

Page 51

If the charges are distributed throughout a

charge density p, which is defined as the charge per unit

be measured in cou1ombs/ (meter)? (We will write this charge density as pd, in

the ...

If the charges are distributed throughout a

**volume**, we can introduce a**volume**charge density p, which is defined as the charge per unit

**volume**and hence willbe measured in cou1ombs/ (meter)? (We will write this charge density as pd, in

the ...

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amplitude angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitor charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb’s law cross section current density current element cylinder defined dielectric displacement distance electric field electromagnetic electrostatic energy equal evaluate example Exercise expression field point Flgure flux force free currents frequency function Galilean transformation given incident induction infinitely long integral integrand length located loop Lorentz Lorentz transformation magnetic dipole magnitude material Maxwell’s equations medium normal components obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector produced quadrupole quantities radiation radius rectangular reﬂected region relation result rotation satisfy scalar potential shown in Figure solenoid sphere substitute surface charge surface current tangential components transformation unit vacuum vector potential velocity volume write written xy plane zero