## 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 39

The theorem deals with the question of what information we need to calculate a

vector field. ... The point r where we evaluate F is called the

point r7 where the sources are evaluated for purposes of integration is called the

...

The theorem deals with the question of what information we need to calculate a

vector field. ... The point r where we evaluate F is called the

**field point**, while thepoint r7 where the sources are evaluated for purposes of integration is called the

...

Page 58

The. Electric. Field. Coulomb's law is an example of what is known as an "action

at a distance" law. It provides us with a ... Equation 3-2 then provides us with a

prescription for calculating E at the location r (the "

The. Electric. Field. Coulomb's law is an example of what is known as an "action

at a distance" law. It provides us with a ... Equation 3-2 then provides us with a

prescription for calculating E at the location r (the "

**field point**") for a given ...Page 149

It makes an angle a with the positive x axis. Find Q, p, and all of the Qjk. Express

the quadrupole term of the potential due to this charge distribution in terms of the

rectangular coordinates of the

It makes an angle a with the positive x axis. Find Q, p, and all of the Qjk. Express

the quadrupole term of the potential due to this charge distribution in terms of the

rectangular coordinates of the

**field point**. 8-8 A sphere of radius a has a surface ...### 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