## 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 143

The subscript b appearing in (10-7), (10-8), and (10-10) reflects the fact that these

charge densities arise from the

they are usually referred to as the

The subscript b appearing in (10-7), (10-8), and (10-10) reflects the fact that these

charge densities arise from the

**bound charges**of the dielectric. Consequently,they are usually referred to as the

**bound charge**densities or the polarization ...Page 168

(a) Find the

points on the z axis for which ^z > 0. (c) Verify that your results in (b) satisfy the

boundary condition at z = L. (d) From the result of (b), find E at the origin, (e)

Sketch the ...

(a) Find the

**bound charge**densities ph and ah. (b) Find the ectric field for allpoints on the z axis for which ^z > 0. (c) Verify that your results in (b) satisfy the

boundary condition at z = L. (d) From the result of (b), find E at the origin, (e)

Sketch the ...

Page 206

equal the rate at which the total charge within V is decreasing, since the total

must be constant. ... Now in the process of polarizing a material, the

define a ...

equal the rate at which the total charge within V is decreasing, since the total

must be constant. ... Now in the process of polarizing a material, the

**bound****charges**will generally be moving, as we saw in Section 10-1, so that we candefine a ...

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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