## 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 49

As we will see later, this is not the case if the point of interest is

sphere. Actually, our result is even more general than it first appears. The

location of q was taken to be along the z axis for convenience in evaluating the

integral ...

As we will see later, this is not the case if the point of interest is

**located**inside thesphere. Actually, our result is even more general than it first appears. The

location of q was taken to be along the z axis for convenience in evaluating the

integral ...

Page 131

pole moment will vanish, where should this origin be

charge distribution of Figure 8- 5 fe leads to (8-40) and thus evaluate Q" for this

case. 8-7 A line charge of constant charge density \ and of length L lies in the first

...

pole moment will vanish, where should this origin be

**located**? 8-6 Show that thecharge distribution of Figure 8- 5 fe leads to (8-40) and thus evaluate Q" for this

case. 8-7 A line charge of constant charge density \ and of length L lies in the first

...

Page 226

Although (14-3) was written in terms of the total force on the complete circuit C, it

is natural to interpret the integrand as giving the force dV on the current element

Ids

Although (14-3) was written in terms of the total force on the complete circuit C, it

is natural to interpret the integrand as giving the force dV on the current element

Ids

**located**at r: dF = IdsX B(r) (14-5) This force is perpendicular to both the ...### What people are saying - Write a review

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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