## 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 96

(a) Capacitors in

this contradiction will be removed for the general field lines shown in Figure 6-10.

Figure 6-13. Exercise 6-11. Assumed electric field for 6-12 A sheet of conductor

of ...

(a) Capacitors in

**parallel**, (b) Capacitors in series. tion. Show qualitatively thatthis contradiction will be removed for the general field lines shown in Figure 6-10.

Figure 6-13. Exercise 6-11. Assumed electric field for 6-12 A sheet of conductor

of ...

Page 224

The sides of the rectangle of length b are

it attractive or repulsive? r, k -« d *□ a Figure 13-5. The circuits of Exercise 13-4.

13-5 An infinite plane current sheet coincides with the xy plane. The surface ...

The sides of the rectangle of length b are

**parallel**to C. Find the total force on C. Isit attractive or repulsive? r, k -« d *□ a Figure 13-5. The circuits of Exercise 13-4.

13-5 An infinite plane current sheet coincides with the xy plane. The surface ...

Page 458

(27-30) We can analyze the

similar way. The voltages Vx and V2 are equal to the same value V by (27-6) so

that the individual currents are /, = Vx/Zx = V/Zx and I2 = V2/Z2 = V/Z2. The total ...

(27-30) We can analyze the

**parallel**combination shown in Figure 21-lb in asimilar way. The voltages Vx and V2 are equal to the same value V by (27-6) so

that the individual currents are /, = Vx/Zx = V/Zx and I2 = V2/Z2 = V/Z2. The total ...

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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