Отрывок: Here  is a strain parameter that varies during the experiment. The first experiment provides two stress-strain relations 11 11 1111C C     , (7a) 22 11 1122C C     , (7b) while the second experiment gives 12 12122C    . (7c) The stress tensor ij is related to the Cauchy stress tensor k...
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dc.contributor.authorBatanova, A.A.-
dc.contributor.authorDyshlovenko, P.E.-
dc.date.accessioned2017-05-19 15:21:21-
dc.date.available2017-05-19 15:21:21-
dc.date.issued2017-
dc.identifierDspace\SGAU\20170517\63871ru
dc.identifier.citationBatanova A.A. Modeling of elastic properties of charge stabilized colloidal crystals with body-centered cubic lattice / A.A. Batanova, P.E. Dyshlovenko // Сборник трудов III международной конференции и молодежной школы «Информационные технологии и нанотехнологии» (ИТНТ-2017) - Самара: Новая техника, 2017. - С. 1128-1130.ru
dc.identifier.urihttp://repo.ssau.ru/handle/Informacionnye-tehnologii-i-nanotehnologii/Modeling-of-elastic-properties-of-charge-stabilized-colloidal-crystals-with-bodycentered-cubic-lattice-63871-
dc.description.abstractElastic properties of charge stabilized colloidal crystals of charged spherical particles with monatomic body-centered cubic crystal lattice are studied numerically. The model of the crystals is based on the nonlinear differential Poisson-Boltzmann equation. Elastic constants of the crystals are derived from the stress-strain dependencies obtained by means of computer experiment. Stability of the crystals and the presence of many-body effective interactions in them are briefly discussed.ru
dc.language.isoenru
dc.publisherНовая техникаru
dc.subjectcolloidal crystalsru
dc.subjectPoisson-Boltzmann equationru
dc.subjectelastic constantsru
dc.subjectmany-body interactionru
dc.titleModeling of elastic properties of charge stabilized colloidal crystals with body-centered cubic latticeru
dc.typeArticleru
dc.textpartHere  is a strain parameter that varies during the experiment. The first experiment provides two stress-strain relations 11 11 1111C C     , (7a) 22 11 1122C C     , (7b) while the second experiment gives 12 12122C    . (7c) The stress tensor ij is related to the Cauchy stress tensor k...-
Располагается в коллекциях: Информационные технологии и нанотехнологии

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