## 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 559

1 The quantity m introduced in this way is then called the mass of the

because of the analogy with (28-98). If this procedure is followed, (28-106)

provides the basis for the common statement that the mass of a

longer a ...

1 The quantity m introduced in this way is then called the mass of the

**particle**because of the analogy with (28-98). If this procedure is followed, (28-106)

provides the basis for the common statement that the mass of a

**particle**is nolonger a ...

Page 15

We require that the

be done with an induction normal to the plane of the orbit and with a value BR;

this is known as the “guiding field.” The required value of BR can be obtained ...

We require that the

**particle**be constrained to move in a circle of fixed R. This canbe done with an induction normal to the plane of the orbit and with a value BR;

this is known as the “guiding field.” The required value of BR can be obtained ...

Page 16

A-4 A charged

region of uniform B directed vertically downward. Find the deflection d from its

original direction of travel when the projection of its position on its original

direction is ...

A-4 A charged

**particle**is traveling horizontally with speed 00 when it enters aregion of uniform B directed vertically downward. Find the deflection d from its

original direction of travel when the projection of its position on its original

direction is ...

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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