## 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 516

customary then to regard the total energy of the

two parts — an intrinsic part due to its rest mass (the rest energy) and the

additional part, which appears when the

the kinetic ...

customary then to regard the total energy of the

**particle**as being composed oftwo parts — an intrinsic part due to its rest mass (the rest energy) and the

additional part, which appears when the

**particle**is moving. Thus, if we let T bethe kinetic ...

Page 536

qBR/m0, so that the final kinetic energy of a

q2B2R2 ^max = ~">0Vą mJ = ~Z (A"3°) which is proportional to B2 and to R2.

When the

105) ...

qBR/m0, so that the final kinetic energy of a

**particle**in the emerging beam is 1q2B2R2 ^max = ~">0Vą mJ = ~Z (A"3°) which is proportional to B2 and to R2.

When the

**particle**speed gets very large, the relativistic equation of motion (29-105) ...

Page 544

dt (A-65) (A-66) We require that the

fixed R. This can 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

...

dt (A-65) (A-66) We require that the

**particle**be constrained to move in a circle offixed R. This can 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

...

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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