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Coagulation equations with gelation

dc.contributor.authorHendriks, E. M.en_US
dc.contributor.authorErnst, M. H.en_US
dc.contributor.authorZiff, Robert M.en_US
dc.date.accessioned2006-09-11T15:43:28Z
dc.date.available2006-09-11T15:43:28Z
dc.date.issued1983-06en_US
dc.identifier.citationHendriks, E. M.; Ernst, M. H.; Ziff, R. M.; (1983). "Coagulation equations with gelation." Journal of Statistical Physics 31(3): 519-563. <http://hdl.handle.net/2027.42/45146>en_US
dc.identifier.issn0022-4715en_US
dc.identifier.issn1572-9613en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/45146
dc.description.abstractSmoluchowski's equation for rapid coagulation is used to describe the kinetics of gelation, in which the coagulation kernel K ij models the bonding mechanism. For different classes of kernels we derive criteria for the occurrence of gelation, and obtain critical exponents in the pre- and postgelation stage in terms of the model parameters; we calculate bounds on the time of gelation t c , and give an exact postgelation solution for the model K ij =( ij ω ) (ω>1/2) and K ij =a i+j ( a >1). For the model K ij = i ω + j ω ( ω <1, without gelation) initial solutions are given. It is argued that the kernel K ij ∼ ij ω with ω≃1−1/d ( d is dimensionality) effectively models the sol-gel transformation in polymerizing systems and approximately accounts for the effects of cross-linking and steric hindrance neglected in the classical theory of Flory and Stockmayer ( Ω =1). For all Ω the exponents, t=Ω +3/2 and σ=Ω −1/2, γ =(3/2− Ω)/(Ω − 1/2) and Β =1, characterize the size distribution, at and slightly below the gel point, under the assumption that scaling is valid.en_US
dc.format.extent2089816 bytes
dc.format.extent3115 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherKluwer Academic Publishers-Plenum Publishers; Plenum Publishing Corporation ; Springer Science+Business Mediaen_US
dc.subject.otherCritical Exponentsen_US
dc.subject.otherSmoluchowski Equationen_US
dc.subject.otherGelationen_US
dc.subject.otherPolymerizationen_US
dc.subject.otherMathematical and Computational Physicsen_US
dc.subject.otherPhysical Chemistryen_US
dc.subject.otherPhysicsen_US
dc.subject.otherQuantum Physicsen_US
dc.subject.otherStatistical Physicsen_US
dc.subject.otherCoagulationen_US
dc.subject.otherSolgel Phase Transitionen_US
dc.subject.otherPercolationen_US
dc.titleCoagulation equations with gelationen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelMathematicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Mechanical Engineering, State University of New York, 11794, Stony Brook, New York; Department of Chemical Engineering, University of Michigan, Dow Building, 48109, Ann Arbor, Michigan, USAen_US
dc.contributor.affiliationotherInstitut voor Theoretische Fysica, Rijksuniversiteit Utrecht, The Netherlandsen_US
dc.contributor.affiliationotherInstitut voor Theoretische Fysica, Rijksuniversiteit Utrecht, The Netherlandsen_US
dc.contributor.affiliationumcampusAnn Arboren_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/45146/1/10955_2005_Article_BF01019497.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1007/BF01019497en_US
dc.identifier.sourceJournal of Statistical Physicsen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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