## 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 76

4-1 The rectangular parallelepiped of Figure 1-41 with a>b>c is filled with

of constant

origin. Find the flux fE-dii through the surface of this sphere. What is the flux when

...

4-1 The rectangular parallelepiped of Figure 1-41 with a>b>c is filled with

**charge**of constant

**density**p. A sphere of radius 2a is constructed with its center at theorigin. Find the flux fE-dii through the surface of this sphere. What is the flux when

...

Page 165

Conceptual scheme of replacing a dielectric by equivalent

common practice to omit the prime in (10-7) and simply write p,= -VP (10-10) with

the understanding that the differentiations are made with respect to the source ...

Conceptual scheme of replacing a dielectric by equivalent

**charge densities**. It iscommon practice to omit the prime in (10-7) and simply write p,= -VP (10-10) with

the understanding that the differentiations are made with respect to the source ...

Page 180

If we insert this result into (10-38), we find that the total

dielectric can always be written as = ty Pb_ 1 (10-59) which shows us that the

total

If we insert this result into (10-38), we find that the total

**charge density**in a 1. i. h.dielectric can always be written as = ty Pb_ 1 (10-59) which shows us that the

total

**charge density**is always less than the free**charge density**since *e> 1.### What people are saying - Write a review

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angle assume axis becomes bound charge boundary conditions bounding surface calculate capacitance charge density charge distribution charge q circuit conductor consider const constant corresponding Coulomb's law cross section current density current element curve cylinder defined dielectric direction displacement distance electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge free currents frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz Lorentz transformation magnitude material Maxwell's equations molecule normal components obtained origin particle perpendicular plane wave point charge polarized position vector potential difference propagation properties quadrupole quantities radiation region relation result satisfy scalar potential shown in Figure situation solenoid spherical substitute surface current surface integral tangential components total charge unit vacuum vector potential velocity volume write written xy plane zero