## 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 426

If we multiply these two results together we get a solution to the wave equation for

this particular value of k and the ... Now if k is also positive, this form represents a

If we multiply these two results together we get a solution to the wave equation for

this particular value of k and the ... Now if k is also positive, this form represents a

**plane wave**traveling in the direction of positive z with speed v =w/ k.Page 438

Consequently, all of our conclusions of the last two sections apply in this case

also; hence we need consider it no further and can continue to use (24-1)

through (24-4) for traveling waves. 24-5

...

Consequently, all of our conclusions of the last two sections apply in this case

also; hence we need consider it no further and can continue to use (24-1)

through (24-4) for traveling waves. 24-5

**Plane Wave**In an Arbitrary Direction For...

Page 473

( sin0,- "1 (2568) where U2 is the normal speed of a wave in this medium. Since 0

, >0,, oz, <02 and this wave travels more slowly than a usual

is not a

( sin0,- "1 (2568) where U2 is the normal speed of a wave in this medium. Since 0

, >0,, oz, <02 and this wave travels more slowly than a usual

**plane wave**; (25-57)is not a

**plane wave**in the sense that its value is not constant on a plane ...### 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