## 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 3

If we start at some point P, and move in some arbitrary way to another point P2,

we see from Figure 1-1 that the net ... it has a direction; and the addition of two

vectors of the same intrinsic nature follows the basic rule

If we start at some point P, and move in some arbitrary way to another point P2,

we see from Figure 1-1 that the net ... it has a direction; and the addition of two

vectors of the same intrinsic nature follows the basic rule

**illustrated in Figure**1-2.Page 30

An example of such a situation is shown in Figure 1-35. ... bounding curve; this

sense is chosen to keep the area of interest to one's left as one moves along the

curve and is seen to be equivalent to the right-hand rule

An example of such a situation is shown in Figure 1-35. ... bounding curve; this

sense is chosen to keep the area of interest to one's left as one moves along the

curve and is seen to be equivalent to the right-hand rule

**illustrated in Figure**1-24.Page 80

Let us consider the line integral of E between an initial point Pt at r, and a final

point Pj at r2 as

tfr,)] where we have used (5-3) and (1-38). We can write this, using (5-5), ...

Let us consider the line integral of E between an initial point Pt at r, and a final

point Pj at r2 as

**illustrated in Figure**1-22: f2E-ds= f2 -V<Ms= - fd<t>= -(fc-*,)- -[tfrjj-tfr,)] where we have used (5-3) and (1-38). We can write this, using (5-5), ...

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angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law cross section current density current element curve cylinder defined dielectric direction displacement distance electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge free currents frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz Lorentz transformation magnitude material Maxwell's equations molecule normal components obtained origin particle perpendicular plane wave point charge polarized position vector potential difference propagation properties quadrupole quantities radiation region relation result satisfy scalar potential shown in Figure situation solenoid spherical substitute surface current surface integral tangential components total charge unit vacuum vector potential velocity volume write written xy plane zero