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Of¡¡course¡¡the¡¡ether¡¡which¡¡conveys¡¡thermal¡¡and¡¡luminous¡¡undulations¡¡is¡¡not¡¡the¡¡frictionless¡¡fluid¡¡postulated¡¡by¡¡Sir¡¡William¡¡Thomson¡£¡¡The¡¡most¡¡conspicuous¡¡property¡¡of¡¡the¡¡ether¡¡is¡¡its¡¡enormous¡¡elasticity£»¡¡a¡¡property¡¡which¡¡we¡¡should¡¡not¡¡find¡¡in¡¡a¡¡frictionless¡¡fluid¡£¡¡¡¨To¡¡account¡¡for¡¡such¡¡elasticity£»¡¨¡¡says¡¡Professor¡¡Clifford¡¡£¨whose¡¡exposition¡¡of¡¡the¡¡subject¡¡is¡¡still¡¡more¡¡lucid¡¡than¡¡that¡¡of¡¡our¡¡authors£©£»¡¡¡¨it¡¡has¡¡to¡¡be¡¡supposed¡¡that¡¡even¡¡where¡¡there¡¡are¡¡no¡¡material¡¡molecules¡¡the¡¡universal¡¡fluid¡¡is¡¡full¡¡of¡¡vortex¡­motion£»¡¡but¡¡that¡¡the¡¡vortices¡¡are¡¡smaller¡¡and¡¡more¡¡closely¡¡packed¡¡than¡¡those¡¡of¡¡£§ordinary£§¡¡matter£»¡¡forming¡¡altogether¡¡a¡¡more¡¡finely¡¡grained¡¡structure¡£¡¡So¡¡that¡¡the¡¡difference¡¡between¡¡matter¡¡and¡¡ether¡¡is¡¡reduced¡¡to¡¡a¡¡mere¡¡difference¡¡in¡¡the¡¡size¡¡and¡¡arrangement¡¡of¡¡the¡¡component¡¡vortex¡­rings¡£¡¡Now£»¡¡whatever¡¡may¡¡turn¡¡out¡¡to¡¡be¡¡the¡¡ultimate¡¡nature¡¡of¡¡the¡¡ether¡¡and¡¡of¡¡molecules£»¡¡we¡¡know¡¡that¡¡to¡¡some¡¡extent¡¡at¡¡least¡¡they¡¡obey¡¡the¡¡same¡¡dynamic¡¡laws£»¡¡and¡¡that¡¡they¡¡act¡¡upon¡¡one¡¡another¡¡in¡¡accordance¡¡with¡¡these¡¡laws¡£¡¡Until£»¡¡therefore£»¡¡it¡¡is¡¡absolutely¡¡disproved£»¡¡it¡¡must¡¡remain¡¡the¡¡simplest¡¡and¡¡most¡¡probable¡¡assumption¡¡that¡¡they¡¡are¡¡finally¡¡made¡¡of¡¡the¡¡same¡¡stuff£»¡¡that¡¡the¡¡material¡¡molecule¡¡is¡¡some¡¡kind¡¡of¡¡knot¡¡or¡¡coagulation¡¡of¡¡ether¡£¡¨£§5£§

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