It¡¡was¡¡only¡¡through¡¡the¡¡atomic¡¡theory£»¡¡at¡¡first¡¡apparently¡¡diametrically¡¡opposed¡¡to¡¡it£»¡¡that¡¡the¡¡conception¡¡of¡¡evolution¡¡in¡¡the¡¡physical¡¡world¡¡was¡¡to¡¡gain¡¡an¡¡established¡¡place¡£¡¡¡¡For¡¡a¡¡century¡¡the¡¡atomic¡¡theory£»¡¡when¡¡put¡¡into¡¡a¡¡modern¡¡form¡¡by¡¡Dalton£»¡¡led¡¡farther¡¡and¡¡farther¡¡away¡¡from¡¡the¡¡idea¡¡of¡¡change¡¡in¡¡matter¡£¡¡¡¡The¡¡chemical¡¡elements¡¡seemed¡¡quite¡¡unalterable£»¡¡and¡¡the¡¡atoms£»¡¡of¡¡which¡¡each¡¡element¡¡in¡¡modern¡¡view¡¡is¡¡composed£»¡¡bore¡¡to¡¡Clerk¡¡Maxwell£»¡¡writing¡¡about¡¡1870£»¡¡¡¨the¡¡stamp¡¡of¡¡manufactured¡¡articles¡¨¡¡exactly¡¡similar¡¡in¡¡kind£»¡¡unchanging£»¡¡eternal¡£
Nevertheless¡¡throughout¡¡these¡¡years£»¡¡on¡¡the¡¡whole¡¡so¡¡unfavourable¡¡to¡¡its¡¡existence£»¡¡there¡¡persisted¡¡the¡¡idea¡¡of¡¡a¡¡common¡¡origin¡¡of¡¡the¡¡distinct¡¡kinds¡¡of¡¡matter¡¡known¡¡to¡¡chemists¡£¡¡¡¡Indeed£»¡¡this¡¡idea¡¡of¡¡unity¡¡in¡¡substance¡¡in¡¡nature¡¡seems¡¡to¡¡accord¡¡with¡¡some¡¡innate¡¡desire¡¡or¡¡intimate¡¡structure¡¡of¡¡the¡¡human¡¡mind¡£¡¡¡¡As¡¡Mr¡¡Arthur¡¡Balfour¡¡well¡¡puts¡¡it£»¡¡¡¨There¡¡is¡¡no¡¡a¡¡priori¡¡reason¡¡that¡¡I¡¡know¡¡of¡¡for¡¡expecting¡¡that¡¡the¡¡material¡¡world¡¡should¡¡be¡¡a¡¡modification¡¡of¡¡a¡¡single¡¡medium£»¡¡rather¡¡than¡¡a¡¡composite¡¡structure¡¡built¡¡out¡¡of¡¡sixty¡¡or¡¡seventy¡¡elementary¡¡substances£»¡¡eternal¡¡and¡¡eternally¡¡different¡£¡¡¡¡Why¡¡then¡¡should¡¡we¡¡feel¡¡content¡¡with¡¡the¡¡first¡¡hypothesis¡¡and¡¡not¡¡with¡¡the¡¡second£¿¡¡¡¡Yet¡¡so¡¡it¡¡is¡£¡¡¡¡Men¡¡of¡¡science¡¡have¡¡always¡¡been¡¡restive¡¡under¡¡the¡¡multiplication¡¡of¡¡entities¡£¡¡¡¡They¡¡have¡¡eagerly¡¡watched¡¡for¡¡any¡¡sign¡¡that¡¡the¡¡different¡¡chemical¡¡elements¡¡own¡¡a¡¡common¡¡origin£»¡¡and¡¡are¡¡all¡¡compounded¡¡out¡¡of¡¡some¡¡primordial¡¡substance¡£¡¡¡¡Nor£»¡¡for¡¡my¡¡part£»¡¡do¡¡I¡¡think¡¡that¡¡such¡¡instincts¡¡should¡¡be¡¡ignored¡£¡£¡£that¡¡they¡¡exist¡¡is¡¡certain£»¡¡that¡¡they¡¡modify¡¡the¡¡indifferent¡¡impartiality¡¡of¡¡pure¡¡empiricism¡¡can¡¡hardly¡¡be¡¡denied¡£¡¨¡¡¡¡£¨¡¨Report¡¡of¡¡the¡¡74th¡¡Meeting¡¡of¡¡the¡¡British¡¡Association¡¨¡¡£¨Presidential¡¡Address£»¡¡Cambridge¡¡1904£©£»¡¡page¡¡9£»¡¡London£»¡¡1905¡££©
When¡¡Dalton's¡¡atomic¡¡theory¡¡had¡¡been¡¡in¡¡existence¡¡some¡¡half¡¡century£»¡¡it¡¡was¡¡noted¡¡that¡¡certain¡¡numerical¡¡relations¡¡held¡¡good¡¡between¡¡the¡¡atomic¡¡weights¡¡of¡¡elements¡¡chemically¡¡similar¡¡to¡¡one¡¡another¡£¡¡¡¡Thus¡¡the¡¡weight¡¡£¨88£©¡¡of¡¡an¡¡atom¡¡of¡¡strontium¡¡compared¡¡with¡¡that¡¡of¡¡hydrogen¡¡as¡¡unity£»¡¡is¡¡about¡¡the¡¡mean¡¡of¡¡those¡¡of¡¡calcium¡¡£¨40£©¡¡and¡¡barium¡¡£¨137£©¡£¡¡¡¡Such¡¡relations£»¡¡in¡¡this¡¡and¡¡other¡¡chemical¡¡groups£»¡¡were¡¡illustrated¡¡by¡¡Beguyer¡¡de¡¡Chancourtois¡¡in¡¡1862¡¡by¡¡the¡¡construction¡¡of¡¡a¡¡spiral¡¡diagram¡¡in¡¡which¡¡the¡¡atomic¡¡weights¡¡are¡¡placed¡¡in¡¡order¡¡round¡¡a¡¡cylinder¡¡and¡¡elements¡¡chemically¡¡similar¡¡are¡¡found¡¡to¡¡fall¡¡on¡¡vertical¡¡lines¡£
Newlands¡¡seems¡¡to¡¡have¡¡been¡¡the¡¡first¡¡to¡¡see¡¡the¡¡significance¡¡of¡¡such¡¡a¡¡diagram¡£¡¡¡¡In¡¡his¡¡¡¨law¡¡of¡¡octaves£»¡¨¡¡formulated¡¡in¡¡1864£»¡¡he¡¡advanced¡¡the¡¡hypothesis¡¡that£»¡¡if¡¡arranged¡¡in¡¡order¡¡of¡¡rising¡¡atomic¡¡weight£»¡¡the¡¡elements¡¡fell¡¡into¡¡groups£»¡¡so¡¡that¡¡each¡¡eighth¡¡element¡¡was¡¡chemically¡¡similar¡£¡¡¡¡Stated¡¡thus£»¡¡the¡¡law¡¡was¡¡too¡¡definite£»¡¡no¡¡room¡¡was¡¡left¡¡for¡¡newly¡¡¡discovered¡¡elements£»¡¡and¡¡some¡¡dissimilar¡¡elements¡¡were¡¡perforce¡¡grouped¡¡together¡£
But¡¡in¡¡1869¡¡Mendeleeff¡¡developed¡¡Newland's¡¡hypothesis¡¡in¡¡a¡¡form¡¡that¡¡attracted¡¡at¡¡once¡¡general¡¡attention¡£¡¡¡¡Placing¡¡the¡¡elements¡¡in¡¡order¡¡of¡¡rising¡¡atomic¡¡weight£»¡¡but¡¡leaving¡¡a¡¡gap¡¡where¡¡necessary¡¡to¡¡bring¡¡similar¡¡elements¡¡into¡¡vertical¡¡columns£»¡¡he¡¡obtained¡¡a¡¡periodic¡¡table¡¡with¡¡natural¡¡vacancies¡¡to¡¡be¡¡filled¡¡as¡¡new¡¡elements¡¡were¡¡discovered£»¡¡and¡¡with¡¡a¡¡certain¡¡amount¡¡of¡¡flexibility¡¡at¡¡the¡¡ends¡¡of¡¡the¡¡horizontal¡¡lines¡£¡¡¡¡From¡¡the¡¡position¡¡of¡¡the¡¡vacancies£»¡¡the¡¡general¡¡chemical¡¡and¡¡physical¡¡properties¡¡of¡¡undiscovered¡¡elements¡¡could¡¡be¡¡predicted£»¡¡and¡¡the¡¡success¡¡of¡¡such¡¡predictions¡¡gave¡¡a¡¡striking¡¡proof¡¡of¡¡the¡¡usefulness¡¡of¡¡Mendeleeff's¡¡generalisation¡£
When¡¡the¡¡chemical¡¡and¡¡physical¡¡properties¡¡of¡¡the¡¡elements¡¡were¡¡known¡¡to¡¡be¡¡periodic¡¡functions¡¡of¡¡their¡¡atomic¡¡weights£»¡¡the¡¡idea¡¡of¡¡a¡¡common¡¡origin¡¡and¡¡common¡¡substance¡¡became¡¡much¡¡more¡¡credible¡£¡¡¡¡Differences¡¡in¡¡atomic¡¡weight¡¡and¡¡differences¡¡in¡¡properties¡¡alike¡¡might¡¡reasonably¡¡be¡¡explained¡¡by¡¡the¡¡differences¡¡in¡¡the¡¡amount¡¡of¡¡the¡¡primordial¡¡substance¡¡present¡¡in¡¡the¡¡various¡¡atoms£»¡¡an¡¡atom¡¡of¡¡oxygen¡¡being¡¡supposed¡¡to¡¡be¡¡composed¡¡of¡¡sixteen¡¡times¡¡as¡¡much¡¡stuff¡¡as¡¡the¡¡atom¡¡of¡¡hydrogen£»¡¡but¡¡to¡¡be¡¡made¡¡of¡¡the¡¡same¡¡ultimate¡¡material¡£¡¡¡¡Speculations¡¡about¡¡the¡¡mode¡¡of¡¡origin¡¡of¡¡the¡¡elements¡¡now¡¡began¡¡to¡¡appear£»¡¡and¡¡put¡¡on¡¡a¡¡certain¡¡air¡¡of¡¡reality¡£¡¡¡¡Of¡¡these¡¡speculations¡¡perhaps¡¡the¡¡most¡¡detailed¡¡was¡¡that¡¡of¡¡Crookes£»¡¡who¡¡imagined¡¡an¡¡initial¡¡chaos¡¡of¡¡a¡¡primordial¡¡medium¡¡he¡¡named¡¡protyle£»¡¡and¡¡a¡¡process¡¡of¡¡periodic¡¡change¡¡in¡¡which¡¡the¡¡chemical¡¡elements¡¡successively¡¡were¡¡precipitated¡£
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Then¡¡came¡¡J¡£J¡£¡¡Thomson's¡¡great¡¡discovery¡¡of¡¡minute¡¡particles£»¡¡much¡¡smaller¡¡than¡¡any¡¡chemical¡¡atom£»¡¡forming¡¡a¡¡common¡¡constituent¡¡of¡¡many¡¡different¡¡kinds¡¡of¡¡matter¡£¡¡¡¡£¨Thomson£»¡¡¡¨Conduction¡¡of¡¡Electricity¡¡through¡¡Gases¡¨¡¡£¨2nd¡¡edition£©£»¡¡Cambridge£»¡¡1906¡££©¡¡¡¡If¡¡an¡¡electric¡¡discharge¡¡be¡¡passed¡¡between¡¡metallic¡¡terminals¡¡through¡¡a¡¡glass¡¡vessel¡¡containing¡¡air¡¡at¡¡very¡¡low¡¡pressure£»¡¡it¡¡is¡¡found¡¡that¡¡rectilinear¡¡rays£»¡¡known¡¡as¡¡cathode¡¡rays£»¡¡proceed¡¡from¡¡the¡¡surface¡¡of¡¡the¡¡cathode¡¡or¡¡negative¡¡terminal¡£¡¡¡¡Where¡¡these¡¡rays¡¡strike¡¡solid¡¡objects£»¡¡they¡¡give¡¡rise¡¡to¡¡the¡¡Rontgen¡¡rays¡¡now¡¡so¡¡well¡¡known£»¡¡but¡¡it¡¡is¡¡with¡¡the¡¡cathode¡¡rays¡¡themselves¡¡that¡¡we¡¡are¡¡concerned¡£¡¡¡¡When¡¡they¡¡strike¡¡an¡¡insulated¡¡conductor£»¡¡they¡¡impart¡¡to¡¡it¡¡a¡¡negative¡¡charge£»¡¡and¡¡Thomson¡¡found¡¡that¡¡they¡¡were¡¡deflected¡¡from¡¡their¡¡path¡¡both¡¡by¡¡magnetic¡¡and¡¡electric¡¡forces¡¡in¡¡the¡¡direction¡¡in¡¡which¡¡negatively¡¡electrified¡¡particles¡¡would¡¡be¡¡deflected¡£¡¡¡¡Cathode¡¡rays¡¡then¡¡were¡¡accepted¡¡as¡¡flights¡¡of¡¡negatively¡¡charged¡¡particles£»¡¡moving¡¡with¡¡high¡¡velocities¡£¡¡¡¡The¡¡electric¡¡and¡¡magnetic¡¡deflections¡¡give¡¡two¡¡independent¡¡measurements¡¡which¡¡may¡¡be¡¡made¡¡on¡¡a¡¡cathode¡¡ray£»¡¡and¡¡both¡¡the¡¡deflections¡¡involve¡¡theoretically¡¡three¡¡unknown¡¡quantities£»¡¡the¡¡mass¡¡of¡¡the¡¡particles£»¡¡their¡¡electric¡¡charge¡¡and¡¡their¡¡velocity¡£¡¡¡¡There¡¡is¡¡strong¡¡cumulative¡¡evidence¡¡that¡¡all¡¡such¡¡particles¡¡possess¡¡the¡¡same¡¡charge£»¡¡which¡¡is¡¡identical¡¡with¡¡that¡¡associated¡¡with¡¡a¡¡univalent¡¡atom¡¡in¡¡electrolytic¡¡liquids¡£¡¡¡¡The¡¡number¡¡of¡¡unknown¡¡quantities¡¡was¡¡thus¡¡reduced¡¡to¡¡twothe¡¡mass¡¡and¡¡the¡¡velocity¡£¡¡¡¡The¡¡measurement¡¡of¡¡the¡¡magnetic¡¡and¡¡electric¡¡deflections¡¡gave¡¡two¡¡independent¡¡relations¡¡between¡¡the¡¡unknowns£»¡¡which¡¡could¡¡therefore¡¡be¡¡determined¡£¡¡¡¡The¡¡velocities¡¡of¡¡the¡¡cathode¡¡ray¡¡particles¡¡were¡¡found¡¡to¡¡vary¡¡round¡¡a¡¡value¡¡about¡¡one¡tenth¡¡that¡¡of¡¡light£»¡¡but¡¡the¡¡mass¡¡was¡¡found¡¡always¡¡to¡¡be¡¡the¡¡same¡¡within¡¡the¡¡limits¡¡of¡¡error£»¡¡whatever¡¡the¡¡nature¡¡of¡¡the¡¡terminals£»¡¡of¡¡the¡¡residual¡¡gas¡¡in¡¡the¡¡vessel£»¡¡and¡¡of¡¡the¡¡conditions¡¡of¡¡the¡¡experiment¡£¡¡¡¡The¡¡mass¡¡of¡¡a¡¡cathode¡¡ray¡¡particle£»¡¡or¡¡corpuscle£»¡¡as¡¡Thomson£»¡¡adopting¡¡Newton's¡¡name£»¡¡called¡¡it£»¡¡is¡¡about¡¡the¡¡eight¡hundredth¡¡part¡¡of¡¡the¡¡mass¡¡of¡¡a¡¡hydrogen¡¡atom¡£
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