The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1904 - English periodicals |
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Page iv
... Corpuscles arranged at equal intervals around the Circumference of a Circle ; with Application of the results to the Theory of Atomic Structure 237 Mr. O. W. Richardson on the Solubility and Diffusion in Solution of Dissociated Gases ...
... Corpuscles arranged at equal intervals around the Circumference of a Circle ; with Application of the results to the Theory of Atomic Structure 237 Mr. O. W. Richardson on the Solubility and Diffusion in Solution of Dissociated Gases ...
Page 237
... Corpuscles arranged at equal intervals around the Circumference of a Circle ; with Application of the results to the Theory of Atomic Structure . By J. J. THOMSON , F.R.S. , Cavendish Professor of Experimental Physics , Cambridge ...
... Corpuscles arranged at equal intervals around the Circumference of a Circle ; with Application of the results to the Theory of Atomic Structure . By J. J. THOMSON , F.R.S. , Cavendish Professor of Experimental Physics , Cambridge ...
Page 238
... corpuscles are at rest this must be equal to the radial attraction . Hence , if π = cosec + cosec - n νέα e2 2π ( n ... corpuscles , we get by ( 1 ) the following values for a / b : - n . a 223 .5 5773 4 ⚫6208 5 • 6505 6 .6726 If the ...
... corpuscles are at rest this must be equal to the radial attraction . Hence , if π = cosec + cosec - n νέα e2 2π ( n ... corpuscles , we get by ( 1 ) the following values for a / b : - n . a 223 .5 5773 4 ⚫6208 5 • 6505 6 .6726 If the ...
Page 239
... corpuscle by all the other corpuscles , is equal to where € 2 4a2 ¿ S —¡¿A ' — Σpp + sAp.p + s — aΣ ¢ p + sВp . 1 - + p.p + 8 , 1 ( n − 1 ) π ; 1 S = π + 2π sin sin sin n n n e2 13 1 1 1 A ' = 4a 2 + + π 2π sin ( n - 1 ) π sin sin n ...
... corpuscle by all the other corpuscles , is equal to where € 2 4a2 ¿ S —¡¿A ' — Σpp + sAp.p + s — aΣ ¢ p + sВp . 1 - + p.p + 8 , 1 ( n − 1 ) π ; 1 S = π + 2π sin sin sin n n n e2 13 1 1 1 A ' = 4a 2 + + π 2π sin ( n - 1 ) π sin sin n ...
Page 240
... , is given by the equation where e2 D = Saï ( Zp = 2pD - Σ = p + sDs , 1 + 1 1 - ( - ) sin3 π n 3 2π sin3 sin ( n - 1 ) π n n and D1 = Sa 1 ST sin n The equations of motion of the pth corpuscle are -rp 240 Prof. J. J. Thomson on the.
... , is given by the equation where e2 D = Saï ( Zp = 2pD - Σ = p + sDs , 1 + 1 1 - ( - ) sin3 π n 3 2π sin3 sin ( n - 1 ) π n n and D1 = Sa 1 ST sin n The equations of motion of the pth corpuscle are -rp 240 Prof. J. J. Thomson on the.
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Common terms and phrases
absorption æther aggregate Aleph alternating current ampere angle anode antenna apparatus arrangement atom basalt calculated canal rays cardinal number cathode rays cell cent charge colours conductivity connexion constant corpuscles corresponding curve cylinder Dattenberg deflexion density diameter direct current direction distance doublet electric electrodes electrometer emanation emission energy equal equation excited activity experiments galvanometer gases given glass heating effect hydrogen increase ionization ions isostacy J. J. Thomson length light liquid magnetic maximum means measured mercury mercury vapour metal method molecules negative number of corpuscles observed obtained ordinal oscillations paper particles Phil plane plate platinum polarization position potential pressure produced Prof radiation radioactivity radium radium bromide reflecting-power resistance ring rotation selenide selenium shown surface temperature theory thickness tube velocity vibration volts wave-length waves wire