## 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

•'all all space When we obtained this expression, we calculated it as the amount

of reversible work required to assemble a given configuration of

did not make any distinction between

•'all 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 wedid not make any distinction between

**free**and bound**charges**, nor was it ...### 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