## 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 3

In the study of electricity and magnetism, we are constantly dealing with

quantities that need to be described in terms of their directions as well as their

properties in ...

In the study of electricity and magnetism, we are constantly dealing with

quantities that need to be described in terms of their directions as well as their

**magnitudes**. Such quantities are called vectors and it is well to consider theirproperties in ...

Page 9

We see from Figure 1-13 that we can get a simple interpretation of the scalar

product: (Bcos^)A = component of B along the direction of A times the

of A = (A cos ty)B = component of A along B times the

from ...

We see from Figure 1-13 that we can get a simple interpretation of the scalar

product: (Bcos^)A = component of B along the direction of A times the

**magnitude**of A = (A cos ty)B = component of A along B times the

**magnitude**of B. It is clearfrom ...

Page 525

The fields of a uniformly moving point charge. the charge but that, at a given

distance, its

Coulomb field. In order to illustrate the dependence of the

direction, ...

The fields of a uniformly moving point charge. the charge but that, at a given

distance, its

**magnitude**depends strongly on direction, in contrast to the simpleCoulomb field. In order to illustrate the dependence of the

**magnitude**upondirection, ...

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### Common terms and phrases

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