## 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 197

The significance of this result (11-9) from a practical point of view is that, once we

find a solution of Laplace's equation, by any means whatsoever, which

given boundary conditions, we know that it is the only solution and we do not ...

The significance of this result (11-9) from a practical point of view is that, once we

find a solution of Laplace's equation, by any means whatsoever, which

**satisfies**given boundary conditions, we know that it is the only solution and we do not ...

Page 287

choice of x- We can see what this will be by substituting (16-24) into (16-26) and

using (16-17) and (1-45): V-Af = 0 = V • A + V • Vx = V2x, and therefore, V2X=0 ...

**satisfy**(16-17): V-A^O (16-26) This will clearly lead to some restriction on ourchoice of x- We can see what this will be by substituting (16-24) into (16-26) and

using (16-17) and (1-45): V-Af = 0 = V • A + V • Vx = V2x, and therefore, V2X=0 ...

Page 551

It is also evident that these ajk cannot all be independent because the

transformation equations (28-60) have not yet been made to

fundamental physical requirement that the axes are related by a rotation, that is,

that r2 be an ...

It is also evident that these ajk cannot all be independent because the

transformation equations (28-60) have not yet been made to

**satisfy**thefundamental physical requirement that the axes are related by a rotation, that is,

that r2 be an ...

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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