## 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 208

There will be a surface charge on the cylinder given by (6-4), but, as we can

easily see, the total charge per unit length on the cylinder will still be A (assuming

a surface in the right half of Figure 5-8).

integration ...

There will be a surface charge on the cylinder given by (6-4), but, as we can

easily see, the total charge per unit length on the cylinder will still be A (assuming

a surface in the right half of Figure 5-8).

**Consider**a Gaussian surface ofintegration ...

Page 267

Chapter The Integral Form of Ampére's Law The first differential source equation

that we want to

given by (1-73) suggests that we

closed ...

Chapter The Integral Form of Ampére's Law The first differential source equation

that we want to

**consider**is VXB. The general definition of the curl of a vectorgiven by (1-73) suggests that we

**consider**the line integral of B about someclosed ...

Page 287

[The expression (16-24) is an example of what is known as a gauge

transformation, and we

have completed the development of the general theory. The requirement (16-26),

and ...

[The expression (16-24) is an example of what is known as a gauge

transformation, and we

**consider**them again in more detail in Chapter 22 after wehave completed the development of the general theory. The requirement (16-26),

and ...

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amplitude angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitor charge density charge distribution charge q circuit conductor consider constant coordinates corresponding Coulomb’s law cross section current density current element cylinder defined dielectric displacement distance electric field electromagnetic electrostatic energy equal evaluate example Exercise expression field point Flgure flux force free currents frequency function Galilean transformation given incident induction infinitely long integral integrand length located loop Lorentz Lorentz transformation magnetic dipole magnitude material Maxwell’s equations medium normal components obtained origin parallel particle perpendicular plane wave plates point charge polarized position vector produced quadrupole quantities radiation radius rectangular reﬂected region relation result rotation satisfy scalar potential shown in Figure solenoid sphere substitute surface charge surface current tangential components transformation unit vacuum vector potential velocity volume write written xy plane zero