Electricity and magnetism for advanced students (1920)
Starling, Sydney George, 1873- · London Longmans, Green · leaf 442
urves for R and y8 are drawn in Fig. 372 for the instant XlV, REFLECTION OF l^LANE WAVES 431 when t = , , and the wave is completely represented by the motion 1 of the curves A and C from right to left with velocity v = —r7~ ■ If then YOZ be a perfectly conducting plane, the electric intensityin… … tX Fig. 372. differing from zero. The electric intensity at the plane is obtained by putting a; = 0 in the equation for R, whence R = Rq sin 277?^, and this opposite intensity created in the conducting plane is therefore R = — Rq sin 27r™. A harmonic disturbance such as this gives rise to two sets…
Electricity · Magnetism
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