## 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 239

The path C does not link the circuit C. In this case, the relative orientations are

like those shown in Figure 15-2. Here, if we start at P, then when we come back

to P after completing the loop C, the final solid

had ...

The path C does not link the circuit C. In this case, the relative orientations are

like those shown in Figure 15-2. Here, if we start at P, then when we come back

to P after completing the loop C, the final solid

**angle**has the same value that ithad ...

Page 408

By comparing these different expressions for the components of kr, we see that 6,

= 8, (25-14) so that the

this ancient and well-known law of optics is seen to be a direct consequence of ...

By comparing these different expressions for the components of kr, we see that 6,

= 8, (25-14) so that the

**angle**of reflection equals the**angle**of incidence. Thus,this ancient and well-known law of optics is seen to be a direct consequence of ...

Page 410

The three propagation vectors as related by the laws of reflection and refraction

when n, > n2 and the

7. The three propagation vectors when the

The three propagation vectors as related by the laws of reflection and refraction

when n, > n2 and the

**angle**of incidence is less than the critical**angle**. Figure 25-7. The three propagation vectors when the

**angle**of incidence equals the critical ...### What people are saying - Write a review

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