## 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 225

For historical reasons, the field that we will use for this purpose is called the "

vector field that we define later when we include the effects of matter. 14-1

DEFINITION ...

For historical reasons, the field that we will use for this purpose is called the "

**magnetic**induction"; the term "**magnetic**field" is generally used for a differentvector field that we define later when we include the effects of matter. 14-1

DEFINITION ...

Page 343

In the electrical circuit, the moving charges comprising the current do not leave

the conductor, while in a general

of B to be out in the space surrounding the material. This flux "leakage" can result

...

In the electrical circuit, the moving charges comprising the current do not leave

the conductor, while in a general

**magnetic**circuit, it is quite possible for the linesof B to be out in the space surrounding the material. This flux "leakage" can result

...

Page 583

... 365, 519 Lorentz force, 233, 354 in Gaussian system, 370 Lorentz gauge, 366

Lorentz' lemma, 404 Lorentz transformation, 502, 509 Lorenz-Lorentz law, 565

Lumped parameters, 449 M

, ...

... 365, 519 Lorentz force, 233, 354 in Gaussian system, 370 Lorentz gauge, 366

Lorentz' lemma, 404 Lorentz transformation, 502, 509 Lorenz-Lorentz law, 565

Lumped parameters, 449 M

**Magnet**, 313,328, 343 fields of, 344**Magnetic**charge, ...

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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