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The¡¡question¡¡of¡¡the¡¡nature¡¡and¡¡physical¡¡meaning¡¡of¡¡a¡¡corpuscle¡¡or¡¡electron¡¡remains¡¡for¡¡consideration¡£¡¡¡¡On¡¡the¡¡hypothesis¡¡of¡¡a¡¡universal¡¡luminiferous¡¡aether£»¡¡Larmor¡¡has¡¡suggested¡¡a¡¡centre¡¡of¡¡aethereal¡¡strain¡¡¡¨a¡¡place¡¡where¡¡the¡¡continuity¡¡of¡¡the¡¡medium¡¡has¡¡been¡¡broken¡¡and¡¡cemented¡¡together¡¡again¡¡£¨to¡¡use¡¡a¡¡crude¡¡but¡¡effective¡¡image£©¡¡without¡¡accurately¡¡fitting¡¡the¡¡parts£»¡¡so¡¡that¡¡there¡¡is¡¡a¡¡residual¡¡strain¡¡all¡¡round¡¡the¡¡place¡£¡¨¡¡¡¡£¨Larmor£»¡¡loc¡£¡¡cit¡££©¡¡¡¡Thus¡¡he¡¡explains¡¡in¡¡quasi¡­mechanical¡¡terms¡¡the¡¡properties¡¡of¡¡an¡¡electron¡£¡¡¡¡But¡¡whether¡¡we¡¡remain¡¡content¡¡for¡¡the¡¡time¡¡with¡¡our¡¡identification¡¡of¡¡matter¡¡and¡¡electricity£»¡¡or¡¡attempt¡¡to¡¡express¡¡both¡¡of¡¡them¡¡in¡¡terms¡¡of¡¡hypothetical¡¡aether£»¡¡we¡¡have¡¡made¡¡a¡¡great¡¡step¡¡in¡¡advance¡¡on¡¡the¡¡view¡¡that¡¡matter¡¡is¡¡made¡¡up¡¡of¡¡chemical¡¡atoms¡¡fundamentally¡¡distinct¡¡and¡¡eternally¡¡isolated¡£

Such¡¡was¡¡the¡¡position¡¡when¡¡the¡¡phenomena¡¡of¡¡radio¡­activity¡¡threw¡¡a¡¡new¡¡light¡¡on¡¡the¡¡problem£»¡¡and£»¡¡for¡¡the¡¡first¡¡time¡¡in¡¡the¡¡history¡¡of¡¡science£»¡¡gave¡¡definite¡¡experimental¡¡evidence¡¡of¡¡the¡¡transmutation¡¡of¡¡matter¡¡from¡¡one¡¡chemical¡¡element¡¡to¡¡another¡£

In¡¡1896¡¡H¡£¡¡Becquerel¡¡discovered¡¡that¡¡compounds¡¡of¡¡the¡¡metal¡¡uranium¡¡continually¡¡emitted¡¡rays¡¡capable¡¡of¡¡penetrating¡¡opaque¡¡screens¡¡and¡¡affecting¡¡photographic¡¡plates¡£¡¡¡¡Like¡¡cathode¡¡and¡¡Rontgen¡¡rays£»¡¡the¡¡rays¡¡from¡¡uranium¡¡make¡¡the¡¡air¡¡through¡¡which¡¡they¡¡pass¡¡a¡¡conductor¡¡of¡¡electricity£»¡¡and¡¡this¡¡property¡¡gives¡¡the¡¡most¡¡convenient¡¡method¡¡of¡¡detecting¡¡the¡¡rays¡¡and¡¡of¡¡measuring¡¡their¡¡intensity¡£¡¡¡¡An¡¡electroscope¡¡may¡¡be¡¡made¡¡of¡¡a¡¡strip¡¡of¡¡gold¡­leaf¡¡attached¡¡to¡¡an¡¡insulated¡¡brass¡¡plate¡¡and¡¡confined¡¡in¡¡a¡¡brass¡¡vessel¡¡with¡¡glass¡¡windows¡£¡¡¡¡When¡¡the¡¡gold¡­leaf¡¡is¡¡electrified£»¡¡it¡¡is¡¡repelled¡¡from¡¡the¡¡similarly¡¡electrified¡¡brass¡¡plate£»¡¡and¡¡the¡¡angle¡¡at¡¡which¡¡it¡¡stands¡¡out¡¡measures¡¡the¡¡electrification¡£¡¡¡¡Such¡¡a¡¡system£»¡¡if¡¡well¡¡insulated£»¡¡holds¡¡its¡¡charge¡¡for¡¡hours£»¡¡the¡¡leakage¡¡of¡¡electricity¡¡through¡¡the¡¡air¡¡being¡¡very¡¡slow¡£¡¡¡¡But£»¡¡if¡¡radio¡­active¡¡radiation¡¡reach¡¡the¡¡air¡¡within£»¡¡the¡¡gold¡­leaf¡¡falls£»¡¡and¡¡the¡¡rate¡¡of¡¡its¡¡fall£»¡¡as¡¡watched¡¡through¡¡a¡¡microscope¡¡with¡¡a¡¡scale¡¡in¡¡the¡¡eye¡­piece£»¡¡measures¡¡the¡¡intensity¡¡of¡¡the¡¡radiation¡£¡¡¡¡With¡¡some¡¡form¡¡of¡¡this¡¡simple¡¡instrument£»¡¡or¡¡with¡¡the¡¡more¡¡complicated¡¡quadrant¡¡electrometer£»¡¡most¡¡radio¡­¡¡active¡¡measurements¡¡have¡¡been¡¡made¡£

It¡¡was¡¡soon¡¡discovered¡¡that¡¡the¡¡activity¡¡of¡¡uranium¡¡compounds¡¡was¡¡proportional¡¡to¡¡the¡¡amount¡¡of¡¡uranium¡¡present¡¡in¡¡them¡£¡¡¡¡Thus¡¡radio¡­activity¡¡is¡¡an¡¡atomic¡¡property¡¡dependent¡¡on¡¡the¡¡amount¡¡of¡¡an¡¡element¡¡and¡¡independent¡¡of¡¡its¡¡state¡¡of¡¡chemical¡¡combination¡£

In¡¡a¡¡search¡¡for¡¡radio¡­activity¡¡in¡¡different¡¡minerals£»¡¡M¡£¡¡and¡¡Mme¡¡Curie¡¡found¡¡a¡¡greater¡¡effect¡¡in¡¡pitch¡­blende¡¡than¡¡its¡¡contents¡¡of¡¡uranium¡¡warranted£»¡¡and£»¡¡led¡¡by¡¡the¡¡radio¡­active¡¡property¡¡alone£»¡¡they¡¡succeeded£»¡¡by¡¡a¡¡long¡¡series¡¡of¡¡chemical¡¡separations£»¡¡in¡¡isolating¡¡compounds¡¡of¡¡a¡¡new¡¡and¡¡intensely¡¡radio¡­active¡¡substance¡¡which¡¡they¡¡named¡¡radium¡£

Radium¡¡resembles¡¡barium¡¡in¡¡its¡¡chemical¡¡properties£»¡¡and¡¡is¡¡precipitated¡¡with¡¡barium¡¡in¡¡the¡¡ordinary¡¡course¡¡of¡¡chemical¡¡analysis¡£¡¡¡¡It¡¡is¡¡separated¡¡by¡¡a¡¡prolonged¡¡course¡¡of¡¡successive¡¡crystallisation£»¡¡the¡¡chloride¡¡of¡¡radium¡¡being¡¡less¡¡soluble¡¡than¡¡that¡¡of¡¡barium£»¡¡and¡¡therefore¡¡sooner¡¡separated¡¡from¡¡an¡¡evaporating¡¡solution¡£¡¡¡¡When¡¡isolated£»¡¡radium¡¡chloride¡¡has¡¡a¡¡composition£»¡¡which£»¡¡on¡¡the¡¡assumption¡¡that¡¡one¡¡atom¡¡of¡¡metal¡¡combines¡¡with¡¡two¡¡of¡¡chlorine¡¡as¡¡in¡¡barium¡¡chloride£»¡¡indicates¡¡that¡¡the¡¡relative¡¡weight¡¡of¡¡the¡¡atom¡¡of¡¡radium¡¡is¡¡about¡¡225¡£¡¡¡¡As¡¡thus¡¡prepared£»¡¡radium¡¡is¡¡a¡¡well¡­marked¡¡chemical¡¡element£»¡¡forming¡¡a¡¡series¡¡of¡¡compounds¡¡analogous¡¡to¡¡those¡¡of¡¡barium¡¡and¡¡showing¡¡a¡¡characteristic¡¡line¡¡spectrum¡£¡¡¡¡But£»¡¡unlike¡¡most¡¡other¡¡chemical¡¡elements£»¡¡it¡¡is¡¡intensely¡¡radio¡­active£»¡¡and¡¡produces¡¡effects¡¡some¡¡two¡¡million¡¡times¡¡greater¡¡than¡¡those¡¡of¡¡uranium¡£

In¡¡1899¡¡E¡£¡¡Rutherford£»¡¡then¡¡of¡¡Montreal£»¡¡discovered¡¡that¡¡the¡¡radiation¡¡from¡¡uranium£»¡¡thorium¡¡and¡¡radium¡¡was¡¡complex¡£¡¡¡¡£¨Rutherford£»¡¡¡¨Radio¡­activity¡¨¡¡£¨2nd¡¡edition£©£»¡¡Cambridge£»¡¡1905¡££©¡¡¡¡Three¡¡types¡¡of¡¡rays¡¡were¡¡soon¡¡distinguished¡£¡¡¡¡The¡¡first£»¡¡named¡¡by¡¡Rutherford¡¡alpha¡­rays£»¡¡are¡¡absorbed¡¡by¡¡thin¡¡metal¡¡foil¡¡or¡¡a¡¡few¡¡centimetres¡¡of¡¡air¡£¡¡¡¡When¡¡examined¡¡by¡¡measurements¡¡of¡¡the¡¡deflections¡¡caused¡¡by¡¡magnetic¡¡and¡¡electric¡¡fields£»¡¡the¡¡alpha¡­rays¡¡are¡¡found¡¡to¡¡behave¡¡as¡¡would¡¡positively¡¡electrified¡¡particles¡¡of¡¡the¡¡magnitude¡¡of¡¡helium¡¡atoms¡¡possessing¡¡a¡¡double¡¡ionic¡¡charge¡¡and¡¡travelling¡¡with¡¡a¡¡velocity¡¡about¡¡one¡­tenth¡¡that¡¡of¡¡light¡£¡¡¡¡The¡¡second¡¡or¡¡beta¡¡type¡¡of¡¡radiation¡¡is¡¡much¡¡more¡¡penetrating¡£¡¡¡¡It¡¡will¡¡pass¡¡through¡¡a¡¡considerable¡¡thickness¡¡of¡¡metallic¡¡foil£»¡¡or¡¡many¡¡centimetres¡¡of¡¡air£»¡¡and¡¡still¡¡affect¡¡photographic¡¡plates¡¡or¡¡discharge¡¡electroscopes¡£¡¡¡¡Magnetic¡¡and¡¡electric¡¡forces¡¡deflect¡¡beta¡­rays¡¡much¡¡more¡¡than¡¡alpha¡­rays£»¡¡indicating¡¡that£»¡¡although¡¡the¡¡speed¡¡is¡¡greater£»¡¡approaching¡¡in¡¡some¡¡cases¡¡within¡¡five¡¡per¡¡cent¡£¡¡that¡¡of¡¡light£»¡¡the¡¡mass¡¡is¡¡very¡¡much¡¡less¡£¡¡¡¡The¡¡beta¡­rays¡¡must¡¡be¡¡streams¡¡of¡¡particles£»¡¡identical¡¡with¡¡those¡¡of¡¡cathode¡¡rays£»¡¡possessing¡¡the¡¡minute¡¡mass¡¡of¡¡J¡£J¡£¡¡Thomson's¡¡corpuscle£»¡¡some¡¡eight¡­hundredth¡¡part¡¡of¡¡that¡¡of¡¡a¡¡hydrogen¡¡atom¡£¡¡¡¡A¡¡third¡¡or¡¡gamma¡¡type¡¡of¡¡radiation¡¡was¡¡also¡¡detected¡£¡¡¡¡More¡¡penetrating¡¡even¡¡than¡¡beta¡­rays£»¡¡the¡¡gamma¡­rays¡¡have¡¡never¡¡been¡¡deflected¡¡by¡¡any¡¡magnetic¡¡or¡¡electric¡¡force¡¡yet¡¡applied¡£¡¡¡¡Like¡¡Rontgen¡¡rays£»¡¡it¡¡is¡¡probable¡¡that¡¡gamma¡­rays¡¡are¡¡wave¡­pulses¡¡in¡¡the¡¡luminiferous¡¡aether£»¡¡though¡¡the¡¡possibility¡¡of¡¡explaining¡¡them¡¡as¡¡flights¡¡of¡¡non¡­¡¡electrified¡¡particles¡¡is¡¡before¡¡the¡¡minds¡¡of¡¡some¡¡physicists¡£

Still¡¡another¡¡kind¡¡of¡¡radiation¡¡has¡¡been¡¡discovered¡¡more¡¡recently¡¡by¡¡Thomson£»¡¡who¡¡has¡¡found¡¡that¡¡in¡¡high¡¡vacua£»¡¡rays¡¡become¡¡apparent¡¡which¡¡are¡¡absorbed¡¡at¡¡once¡¡by¡¡air¡¡at¡¡any¡¡ordinary¡¡pressure¡£

The¡¡emission¡¡of¡¡all¡¡these¡¡different¡¡types¡¡of¡¡radiation¡¡involves¡¡a¡¡continual¡¡drain¡¡of¡¡energy¡¡from¡¡the¡¡radio¡­active¡¡body¡£¡¡¡¡When¡¡M¡£¡¡and¡¡Mme¡¡Curie¡¡had¡¡prepared¡¡as¡¡much¡¡as¡¡a¡¡gramme¡¡of¡¡radium¡¡chloride£»¡¡the¡¡energy¡¡of¡¡the¡¡radiation¡¡became¡¡apparent¡¡as¡¡an¡¡evolution¡¡of¡¡heat¡£¡¡¡¡The¡¡radium¡¡salt¡¡itself£»¡¡and¡¡the¡¡case¡¡containing¡¡it£»¡¡absorbed¡¡the¡¡major¡¡part¡¡of¡¡the¡¡radiation£»¡¡and¡¡were¡¡thus¡¡maintained¡¡at¡¡a¡¡temperature¡¡measurably¡¡higher¡¡than¡¡that¡¡of¡¡the¡¡surroundings¡£¡¡¡¡The¡¡rate¡¡of¡¡thermal¡¡evolution¡¡was¡¡such¡¡that¡¡it¡¡appeared¡¡that¡¡one¡¡gramme¡¡of¡¡pure¡¡radium¡¡must¡¡emit¡¡about¡¡100¡¡gramme¡­calories¡¡of¡¡heat¡¡in¡¡an¡¡hour¡£¡¡¡¡This¡¡observation£»¡¡naturally¡¡as¡¡it¡¡follows¡¡from¡¡the¡¡phenomena¡¡previously¡¡discovered£»¡¡first¡¡called¡¡attention¡¡to¡¡the¡¡question¡¡of¡¡the¡¡source¡¡of¡¡the¡¡energy¡¡which¡¡maintains¡¡indefinitely¡¡and¡¡without¡¡apparent¡¡diminution¡¡the¡¡wonderful¡¡stream¡¡of¡¡radiation¡¡proceeding¡¡from¡¡a¡¡radio¡­active¡¡substance¡£¡¡¡¡In¡¡the¡¡solution¡¡of¡¡this¡¡problem¡¡lies¡¡the¡¡point¡¡of¡¡the¡¡present¡¡essay¡£

In¡¡order¡¡to¡¡appreciate¡¡the¡¡evidence¡¡which¡¡bears¡¡on¡¡the¡¡question¡¡we¡¡must¡¡now¡¡describe¡¡two¡¡other¡¡series¡¡of¡¡phenomena¡£

It¡¡is¡¡a¡¡remarkable¡¡fact¡¡that¡¡the¡¡intensity¡¡of¡¡the¡¡radiation¡¡from¡¡a¡¡radio¡­¡¡active¡¡body¡¡is¡¡independent¡¡of¡¡the¡¡external¡¡conditions¡¡of¡¡temperature£»¡¡pressure£»¡¡etc¡£¡¡which¡¡modify¡¡so¡¡profoundly¡¡almost¡¡all¡¡other¡¡physical¡¡and¡¡chemical¡¡processes¡£¡¡¡¡Exposure¡¡to¡¡the¡¡extreme¡¡cold¡¡of¡¡liquid¡¡air£»¡¡or¡¡to¡¡the¡¡great¡¡heat¡¡of¡¡a¡¡furnace£»¡¡leaves¡¡the¡¡radio¡­activity¡¡of¡¡a¡¡substance¡¡unchanged£»¡¡apparent¡¡exceptions¡¡to¡¡this¡¡statement¡¡having¡¡been¡¡traced¡¡to¡¡secondary¡¡causes¡£

Then£»¡¡it¡¡is¡¡found¡¡that¡¡radio¡­activity¡¡is¡¡always¡¡accompanied¡¡by¡¡some¡¡chemical¡¡change£»¡¡a¡¡new¡¡substance¡¡always¡¡appears¡¡as¡¡the¡¡parent¡¡substance¡¡emits¡¡these¡¡radiations¡£¡¡¡¡Thus¡¡by¡¡chemical¡¡reactions¡¡it¡¡is¡¡possible¡¡to¡¡separate¡¡from¡¡uranium¡¡and¡¡thorium¡¡minute¡¡quantities¡¡of¡¡radio¡­active¡¡materials¡¡to¡¡which¡¡the¡¡names¡¡of¡¡uranium¡­X¡¡and¡¡thorium¡­X¡¡have¡¡been¡¡given¡£¡¡¡¡These¡¡bodies¡¡behave¡¡differently¡¡from¡¡t
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