## 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 240

By analogy with similar effects involving “friction” in mechanics, we shall try to

describe the overall effect of collisions as their giving rise to a force proportional

to the

§v ...

By analogy with similar effects involving “friction” in mechanics, we shall try to

describe the overall effect of collisions as their giving rise to a force proportional

to the

**velocity**and opposite to it; thus we write the mechanical force as Fq_m= —§v ...

Page 574

Is this result compatible with (28-37)? R-6 Show that the

formulas can be written in vector form as v =[v“' +V+(vl'/ 7)]/[1 +(V -v')/c2] where v"'

is the

Is this result compatible with (28-37)? R-6 Show that the

**velocity**transformationformulas can be written in vector form as v =[v“' +V+(vl'/ 7)]/[1 +(V -v')/c2] where v"'

is the

**velocity**component parallel to the relative**velocity**V of S and S' while v L' ...Page 12

I = U01: “ on (A54) The expressions for v,' and v,' are just those expected for a

speed wc as in Figure A-6. We can find the particle coordinates by integrating (A-

51) ...

I = U01: “ on (A54) The expressions for v,' and v,' are just those expected for a

**velocity**v' of magnitude |v'|= v'=|v,,,,'| rotating in a clockwise sense with angularspeed wc as in Figure A-6. We can find the particle coordinates by integrating (A-

51) ...

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