Thomson, J. J. (Joseph John), Sir, 1856-1940 · New Haven Yale University Press · leaf 71
d, hence to preserve continuitythese tubes must run round in the shell to join thesphere as in Fig. 14. We thus have in this case two pulses, one aplane pulse propa-gated in the direc-tion in which theparticle was mov-ing before it wasstopped, the other aspherical pulse trav-elling outward in… … Fig. 14. RONTGEN RAYS AND LIGHT Ql reduced to zero is merely dimlnislied by A v, wecan show, as on page 57, that it will give rise toa pulse in which the magnetic force H is given bythe equation „ eAv sin 9 ±L = s , ro and the tangential electric force T by rp_ e.Avsm 6~ ~Vr.S Now the thickness S…
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