## 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 151

In Section 10-2, we encountered a particular class of charge — the bound charge

whose density is given by (10-10) as pb = - V . P. It is conventional and

convenient to divide charge into the two broad classes of bound charge and

In Section 10-2, we encountered a particular class of charge — the bound charge

whose density is given by (10-10) as pb = - V . P. It is conventional and

convenient to divide charge into the two broad classes of bound charge and

**free****charge**...Page 152

We can think of (10-41) as an expression of Coulomb's law for the force between

point

discontinuous only if there is a

...

We can think of (10-41) as an expression of Coulomb's law for the force between

point

**charges**plus the electrical ... Thus, the normal component of D will bediscontinuous only if there is a

**free**surface**charge**density; this is in contrast to E...

Page 161

p<jj> dr (10-78) all space When we obtained this expression, we calculated it as

the amount of reversible work required to assemble a given configuration of

nor ...

p<jj> dr (10-78) all space When we obtained this expression, we calculated it as

the amount of reversible work required to assemble a given configuration of

**charges**, and we did not make any distinction between**free**and bound**charges**,nor ...

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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