A MATHEMATICAL DESCRIPTION OF THE CRITICAL POINT IN PHASE TRANSITIONS
dc.contributor.author | Bilge, Ayşe Hümeyra | |
dc.contributor.author | Pekcan, Mehmet Önder | |
dc.date.accessioned | 2021-01-31T20:03:48Z | |
dc.date.available | 2021-01-31T20:03:48Z | |
dc.date.issued | 2013 | |
dc.department | Fakülteler, Mühendislik ve Doğa Bilimleri Fakültesi, Endüstri Mühendisliği Bölümü | en_US |
dc.description.abstract | Let y(x) be a smooth sigmoidal curve, y((n)) be its nth derivative and {x(m,i)} and {x(a,i)}, i = 1, 2, ... , be the set of points where respectively the derivatives of odd and even order reach their extreme values. We argue that if the sigmoidal curve y(x) represents a phase transition, then the sequences {x(m,i)} and {x(a,i)} are both convergent and they have a common limit x(c) that we characterize as the critical point of the phase transition. In this study, we examine the logistic growth curve and the Susceptible-Infected-Removed (SIR) epidemic model as typical examples of symmetrical and asymmetrical transition curves. Numerical computations indicate that the critical point of the logistic growth curve that is symmetrical about the point (x(0), y(0)) is always the point (x(0), y(0)) but the critical point of the asymmetrical SIR model depends on the system parameters. We use the description of the sol-gel phase transition of polyacrylamide-sodium alginate (SA) composite (with low SA concentrations) in terms of the SIR epidemic model, to compare the location of the critical point as described above with the "gel point" determined by independent experiments. We show that the critical point t(c) is located in between the zero of the third derivative t(a) and the inflection point t(m) of the transition curve and as the strength of activation (measured by the parameter k/eta of the SIR model) increases, the phase transition occurs earlier in time and the critical point, t(c), moves toward t(a). | en_US |
dc.description.sponsorship | Tubitak | en_US |
dc.identifier.citation | 10 | |
dc.identifier.doi | 10.1142/S0129183113500654 | en_US |
dc.identifier.issn | 0129-1831 | en_US |
dc.identifier.issn | 0129-1831 | |
dc.identifier.issue | 10 | en_US |
dc.identifier.scopus | 2-s2.0-84882764288 | en_US |
dc.identifier.scopusquality | Q3 | |
dc.identifier.uri | https://hdl.handle.net/20.500.12469/3855 | |
dc.identifier.uri | https://doi.org/10.1142/S0129183113500654 | |
dc.identifier.volume | 24 | en_US |
dc.identifier.wos | WOS:000324541100001 | en_US |
dc.identifier.wosquality | N/A | |
dc.institutionauthor | Bilge, Ayşe Hümeyra | en_US |
dc.institutionauthor | Pekcan, Önder | en_US |
dc.language.iso | en | en_US |
dc.publisher | World Scientific Publ Co Pte Ltd | en_US |
dc.relation.journal | International Journal of Modern Physics C | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.rights | info:eu-repo/semantics/closedAccess | en_US |
dc.subject | Gelation | en_US |
dc.subject | Phase Transition | en_US |
dc.subject | Epidemic Models | en_US |
dc.title | A MATHEMATICAL DESCRIPTION OF THE CRITICAL POINT IN PHASE TRANSITIONS | en_US |
dc.type | Article | en_US |
dspace.entity.type | Publication | |
relation.isAuthorOfPublication | 1b50a6b2-7290-44da-b8d5-f048fea8b315 | |
relation.isAuthorOfPublication | e5459272-ce6e-44cf-a186-293850946f24 | |
relation.isAuthorOfPublication.latestForDiscovery | 1b50a6b2-7290-44da-b8d5-f048fea8b315 |