Please use this identifier to cite or link to this item: http://nopr.niscpr.res.in/handle/123456789/16783
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dc.contributor.authorWisniak, Jaime-
dc.date.accessioned2013-04-03T12:45:16Z-
dc.date.available2013-04-03T12:45:16Z-
dc.date.issued2004-03-
dc.identifier.issn0975-0991 (Online); 0971-457X (Print)-
dc.identifier.urihttp://hdl.handle.net/123456789/16783-
dc.description275-285en_US
dc.description.abstractJohn Herapath (1790-1868), a self-taught scientist, was the first to present a comprehensive description of the structure of a gas, in which the molecules moved and collided with each other, instead of vibrating in a fixed lattice. His model made the wrong assumption that the momentum of the molecules, instead of their kinetic energy measured the temperature. He used his model to calculate for the first time the velocity of a molecule, the velocity of sound and to describe effusion phenomena through small pores, and adiabatic compression. His speculative approach put him at odds with the empirical approach of the British scientific establishment of his time.en_US
dc.language.isoen_USen_US
dc.publisherNISCAIR-CSIR, Indiaen_US
dc.rights CC Attribution-Noncommercial-No Derivative Works 2.5 Indiaen_US
dc.sourceIJCT Vol.11(2) [March 2004]en_US
dc.subjectKinetic theory of gasesen_US
dc.titleJohn Herapath-The beginning of the kinetic theory of gasesen_US
dc.typeArticleen_US
Appears in Collections:IJCT Vol.11(2) [March 2004]

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