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E PARALLEL TO PLANE OF INCIDENCE E. ' = 2 ( 7.60 ) иє sin 2i 2 cos i sin r EO Nu'e ' sin 2r + sin ( i + r ) cos ( i - r ) u sin 2i u ' M sin 2i sin 2r E. " tan ( i E. sin 2r + и tan ( i + r ) M sin 2i μ ' Again the results on the right ...
E is parallel to the x axis ; B is parallel to the y axis . ( a ) For El < B make the necessary Lorentz transformation described in Section 12.8 to obtain explicitly parametric equations for the particle's trajectory .
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
References and suggested reading
Multipoles Electrostatics of Macroscopic Media
6 other sections not shown