## 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 196

Sometimes the boundary involved is very far away, that is, at infinity. We let ¢,(r)

be a solution of (ll-3) that satisfies the given

assume that there is another distinct solution ¢2(r) satisfying these same

boundary ...

Sometimes the boundary involved is very far away, that is, at infinity. We let ¢,(r)

be a solution of (ll-3) that satisfies the given

**boundary conditions**. We alsoassume that there is another distinct solution ¢2(r) satisfying these same

boundary ...

Page 457

We will find that we can solve this problem by using the

the field vectors have to satisfy at a surface of discontinuity in properties, and we

recall that these

We will find that we can solve this problem by using the

**boundary conditions**thatthe field vectors have to satisfy at a surface of discontinuity in properties, and we

recall that these

**boundary conditions**were obtained directly from Maxwell's ...Page 486

In such situations, it is fairly clear that the solutions cannot generally be plane

waves with definite values of the fields over an infinite plane since the fields will

have to satisfy

In such situations, it is fairly clear that the solutions cannot generally be plane

waves with definite values of the fields over an infinite plane since the fields will

have to satisfy

**boundary conditions**at the limits of the region as well as being ...### What people are saying - Write a review

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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