## 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 13

Comparing this with (1-15), we see that Vu and dsx are

us consider displacements of constant magnitude ds0 from a given point but of ...

Comparing this with (1-15), we see that Vu and dsx are

**perpendicular**; thus V u is**perpendicular**to a surface of constant u, as is also shown in Figure 1-18. Now letus consider displacements of constant magnitude ds0 from a given point but of ...

Page 28

mutually

components of V X A in each of these directions and thus obtain the whole vector

V X A. When this procedure is carried out for rectangular coordinates, the result is

, ...

mutually

**perpendicular**directions (such as x, y, and z), we will get thecomponents of V X A in each of these directions and thus obtain the whole vector

V X A. When this procedure is carried out for rectangular coordinates, the result is

, ...

Page 410

The shaded plane is

also

can be written as the vector sum E; = E. , +E„ (25-22) where ElX is the component

...

The shaded plane is

**perpendicular**to k, and therefore contains E,; this plane isalso

**perpendicular**to the plane of incidence defined by k, and fi. We see that E,can be written as the vector sum E; = E. , +E„ (25-22) where ElX is the component

...

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