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E PARALLEL TO PLANE OF INCIDENCE E. ' Дє sin 2i = 2 2 cos i sin r sin ( i + r ) cos ( i – r ) E. μ'ε ' ' sin 2r + и M sin 2i ( 7.60 ) 법 M sin 2i – sin 2r E. " u tan ( i – r ) E. sin 2r + M 브 tan ( i + r ) sin 2i μ ' Again the results ...
E is parallel to the x axis ; B is parallel to the y axis . ( a ) For | E < | B | make the necessary Lorentz transformation described in Section 12.8 to obtain explicitly parametric equations for the particle's trajectory .
it parallel to and perpendicular to the velocity . But we have just seen that for comparable parallel and perpendicular forces the radiation from the parallel component is negligible ( of order 1/72 ) compared to that from the ...
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Introduction to Electrostatics
BoundaryValue Problems in Electrostatics I
TimeVarying Fields Maxwells Equations Con
4 other sections not shown