## 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 110

If we are near such a volume, we can expect that the values of the potential at

different points can be quite sensitive to the details of the

However, as we get farther and farther away, it seems clear that the finer details

of the ...

If we are near such a volume, we can expect that the values of the potential at

different points can be quite sensitive to the details of the

**charge distribution**.However, as we get farther and farther away, it seems clear that the finer details

of the ...

Page 113

l where Q is the net

47Te0r Since this is the dominant term in the potential, when we are very far

away, we see that the whole

...

l where Q is the net

**charge**of the system. Thus, the monopole term has the form47Te0r Since this is the dominant term in the potential, when we are very far

away, we see that the whole

**distribution**will act as if it were a point**charge**as we...

Page 131

8-6 Show that the

evaluate Q" for this case. 8-7 A line charge of constant charge density \ and of

length L lies in the first quadrant of the xy plane with one end at the origin. It

makes an ...

8-6 Show that the

**charge distribution**of Figure 8- 5 fe leads to (8-40) and thusevaluate Q" for this case. 8-7 A line charge of constant charge density \ and of

length L lies in the first quadrant of the xy plane with one end at the origin. It

makes an ...

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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