## 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 154

}_ij1_},(hb)= }|i§_1})(hV "F) (9-7) Since this difference may be different from zero,

we have the possibility of a discontinuity in the

. 9-3 The Curl and the Tangential Components Stokes' theorem (1-67) ...

}_ij1_},(hb)= }|i§_1})(hV "F) (9-7) Since this difference may be different from zero,

we have the possibility of a discontinuity in the

**normal components**of the vector F. 9-3 The Curl and the Tangential Components Stokes' theorem (1-67) ...

Page 364

The boundary conditions satisfied by the

easily obtained from the fact that the

and when we substitute (20-28) into (16-4) we find that fl-(H2—H|)= -—fl-(M2—M

|) ...

The boundary conditions satisfied by the

**normal components**of H can be mosteasily obtained from the fact that the

**normal components**of B are continuous,and when we substitute (20-28) into (16-4) we find that fl-(H2—H|)= -—fl-(M2—M

|) ...

Page 487

Since the tangential

), we see that E,,ns=0 just outside of the surface. In other words, E has no

tangential

Since the tangential

**components**of E are always continuous, according to (21-26), we see that E,,ns=0 just outside of the surface. In other words, E has no

tangential

**component**at the surface of a perfect conductor so that E must be**normal**to ...### What people are saying - Write a review

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