## 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 224

The two currents of Exercise 13-3. distance p from it, crosses the x

0, and makes the angle a with the xy plane as shown. Show that the force on / of

C due to /' of C is - ^0//'cotai. 13-4 Consider the two circuits shown in Figure 13-5.

The two currents of Exercise 13-3. distance p from it, crosses the x

**axis**at y = z =0, and makes the angle a with the xy plane as shown. Show that the force on / of

C due to /' of C is - ^0//'cotai. 13-4 Consider the two circuits shown in Figure 13-5.

Page 261

Show that these same results follow if one assumes distributed steady currents.

16-2 Apply (16-5) to a small cylinder in the interior of an infinitely long ideal

solenoid. Assume the

thus ...

Show that these same results follow if one assumes distributed steady currents.

16-2 Apply (16-5) to a small cylinder in the interior of an infinitely long ideal

solenoid. Assume the

**axis**of the cylinder to coincide with the solenoid**axis**, andthus ...

Page 282

17-4 An infinitely long straight wire carrying a constant current / coincides with the

z

x

17-4 An infinitely long straight wire carrying a constant current / coincides with the

z

**axis**. A circular loop of radius a lies in the xz plane with its center on the positivex

**axis**at a distance b from the origin. Find the flux through the loop. If the loop ...### 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