## 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

It is L q, = Gtoui = Q (8-15) where Q is the net

monopole term has the form <U0 - -p— (8-i6) Since this is the dominant term in

the potential, when we are very far away, we see that the whole

act as ...

It is L q, = Gtoui = Q (8-15) where Q is the net

**charge**of the system. Thus, themonopole term has the form <U0 - -p— (8-i6) Since this is the dominant term in

the potential, when we are very far away, we see that the whole

**distribution**willact as ...

Page 131

8-6 Show that the

evaluate Q" for this case. 8-7 A line charge of constant charge density X 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 8-5ft leads to (8-40) and thusevaluate Q" for this case. 8-7 A line charge of constant charge density X 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 capacitor cavity charge density charge distribution charge q circuit conductor const constant convenient corresponding Coulomb's law current density curve cylinder defined dielectric dipole direction displacement distance divergence theorem electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux force free charge frequency function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge line integral located Lorentz transformation magnetic magnitude Maxwell's equations obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector potential difference quantities rectangular coordinates region result scalar potential shown in Figure solenoid sphere of radius spherical surface integral tangential components theorem total charge unit vectors vacuum vector potential velocity volume write written xy plane zero