## 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 305

If we label these

_ _ Q1. . 5 -gSC13 115- fsat da+gSC(v><B)ds (17-26) which can be written with

the use of (1-67) as fVX(E'—v><B)-da= -faa_'?-116 (17-27) s s so that ...

If we label these

**quantities**with a prime, and use (1-23) again, we find that »_ 1._ _ Q1. . 5 -gSC13 115- fsat da+gSC(v><B)ds (17-26) which can be written with

the use of (1-67) as fVX(E'—v><B)-da= -faa_'?-116 (17-27) s s so that ...

Page 451

+ io,)E0'e""" (24-132) For simplicity, let us assume that E0' is real; then the

physical

aid of (24-22), they are found to be Em|=E0'coswt (24_l33) J ma, = (0,, cos wt + 0,

sin ...

+ io,)E0'e""" (24-132) For simplicity, let us assume that E0' is real; then the

physical

**quantities**of interest are given by the real parts of (24-132) and, with theaid of (24-22), they are found to be Em|=E0'coswt (24_l33) J ma, = (0,, cos wt + 0,

sin ...

Page 549

... £2 _ dt = ( dz _ E dx d1' d'r d'r Y d'r c dr Using (28-52), (28-34), and comparing (

28-53) with (28-28), we see that the four

dr [1_(o2/cz)]l/2 d d (28-54) z _ 0, t _ 1 d'r_ [l_(v2/c2)]1/1 d'r_ [l_(o2/62)]!

... £2 _ dt = ( dz _ E dx d1' d'r d'r Y d'r c dr Using (28-52), (28-34), and comparing (

28-53) with (28-28), we see that the four

**quantities**dx = vx W = 0)' d'r [l_(v2/c2)]l/1dr [1_(o2/cz)]l/2 d d (28-54) z _ 0, t _ 1 d'r_ [l_(v2/c2)]1/1 d'r_ [l_(o2/62)]!

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