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dc.contributor.authorNarasimha, Roddam
dc.date.accessioned2017-02-21T07:03:34Z-
dc.date.available2017-02-21T07:03:34Z-
dc.date.issued2014
dc.identifier.citationNarasimha, R, The contribution of the Bhatnagar-Gross-Krook model to the development of rarefied gas dynamics in the early years of the space age. International Journal of Modern Physics C 2014, 25 (1), 1340025 http://dx.doi.org/10.1142/S0129183113400251en_US
dc.identifier.citationInternational Journal of Modern Physics Cen_US
dc.identifier.citation25en_US
dc.identifier.citation1en_US
dc.identifier.issn0129-1831
dc.identifier.urihttps://libjncir.jncasr.ac.in/xmlui/10572/2445-
dc.descriptionRestricted Accessen_US
dc.description.abstractThe advent of the space age in 1957 was accompanied by a sudden surge of interest in rarefied gas dynamics (RGD). The well-known difficulties associated with solving the Boltzmann equation that governs RGD made progress slow but the Bhatnagar-Gross-Krook (BGK) model, proposed three years before Sputnik, turned out to have been an uncannily timely, attractive and fruitful option, both for gaining insights into the Boltzmann equation and for estimating various technologically useful flow parameters. This paper gives a view of how BGK contributed to the growth of RGD during the first decade of the space age. Early efforts intended to probe the limits of the BGK model showed that, in and near both the continuum Euler limit and the collisionless Knudsen limit, BGK could provide useful answers. Attempts were therefore made to tackle more ambitious nonlinear nonequilibrium problems. The most challenging of these was the structure of a plane shock wave. The first exact numerical solutions of the BGK equation for the shock appeared during 1962 to 1964, and yielded deep insights into the character of transitional nonequilibrium flows that had resisted all attempts at solution through the Boltzmann equation. In particular, a BGK weak shock was found to be amenable to an asymptotic analysis. The results highlighted the importance of accounting separately for fast-molecule dynamics, most strikingly manifested as tails in the distribution function, both in velocity and in physical space - tails are strange versions or combinations of collisionless and collision-generated flows. However, by the mid-1960s Monte-Carlo methods of solving the full Boltzmann equation were getting to be mature and reliable and interest in the BGK waned in the following years. Interestingly, it has seen a minor revival in recent years as a tool for developing more effective algorithms in continuum computational fluid dynamics, but the insights derived from the BGK for strongly nonequilibrium flows should be of lasting value.en_US
dc.description.uri1793-6586en_US
dc.description.urihttp://dx.doi.org/10.1142/S0129183113400251en_US
dc.language.isoEnglishen_US
dc.publisherWorld Scientific Publ Co Pte Ltden_US
dc.rights@World Scientific Publ Co Pte Ltd, 2014en_US
dc.subjectComputer Science, Interdisciplinary Applicationsen_US
dc.subjectMathematical Physicsen_US
dc.subjectBgk Modelen_US
dc.subjectRarefield Gas Dynamicsen_US
dc.subjectBoltzmann Equationen_US
dc.subjectShock Wavesen_US
dc.subjectCollision Integralsen_US
dc.subjectStructure Of Distribution Functionen_US
dc.subjectHigh Knudsen Numbersen_US
dc.subjectOrifice Flowen_US
dc.subjectShocken_US
dc.titleTHE CONTRIBUTION OF THE BHATNAGAR-GROSS-KROOK MODEL TO THE DEVELOPMENT OF RAREFIED GAS DYNAMICS IN THE EARLY YEARS OF THE SPACE AGEen_US
dc.typeArticleen_US
Appears in Collections:Research Articles (Roddam Narasimha)

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