## 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 Px 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 Px 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 17

In Figure 1-23 we show an infinitesimal element of area da that has some

particular orientation with respect to the ... This right-hand rule is

the ...

In Figure 1-23 we show an infinitesimal element of area da that has some

particular orientation with respect to the ... This right-hand rule is

**illustrated in****Figure**1-24; note how the direction of h would be reversed if C were traversed inthe ...

Page 409

We find from (25-18) that sin#, = (nl/n2)sit\8l. If n, < n2, then sin 8, < sin 8i <, 1 and

cos2 8, = 1 - sin2 8, > 0; thus 8, is a real angle and 8, < 6,. This case is

We find from (25-18) that sin#, = (nl/n2)sit\8l. If n, < n2, then sin 8, < sin 8i <, 1 and

cos2 8, = 1 - sin2 8, > 0; thus 8, is a real angle and 8, < 6,. This case is

**illustrated****in Figure**25-5; note that k2/kl = n2/nl > 1. If nx > n2, then we still have sinfl, ...### What people are saying - Write a review

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angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitance cavity charge density charge distribution charge q circuit conducting conductor const constant corresponding Coulomb's law current density curve cylinder dielectric dipole direction displacement distance divergence theorem electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux free charge function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz transformation magnetic magnitude Maxwell's equations normal component obtained origin parallel plate capacitor particle perpendicular point charge polarized position vector potential difference quadrupole quantities rectangular coordinates region result satisfy scalar potential shown in Figure situation solenoid solution sphere of radius spherical surface charge surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume write written xy plane zero