Mathematical Characterization of Thermo-reversible Phase Transitions of Agarose Gels
dc.authorid | Bilge, Ayse Humeyra/0000-0002-6043-0833 | |
dc.authorid | Ogrenci, Arif Selcuk/0000-0003-0463-3019 | |
dc.authorid | PEKCAN, Onder/0000-0002-0082-8209 | |
dc.authorwosid | Bilge, Ayse Humeyra/I-5901-2012 | |
dc.authorwosid | Ogrenci, Arif Selcuk/W-1372-2017 | |
dc.authorwosid | PEKCAN, Onder/Y-3158-2018 | |
dc.contributor.author | Ogrenci, Arif Selcuk | |
dc.contributor.author | Pekcan, Onder | |
dc.contributor.author | Kara, Selim | |
dc.contributor.author | Bilge, Ayse Humeyra | |
dc.date.accessioned | 2024-06-12T10:50:55Z | |
dc.date.available | 2024-06-12T10:50:55Z | |
dc.date.issued | 2018 | |
dc.department | Trakya Üniversitesi | en_US |
dc.description.abstract | The thermal phase transition temperatures of high (HMP) and low melting point (LMP) agarose gels were investigated by using UV-vis spectroscopy techniques. Transmitted light intensities from the gel samples with different agarose concentrations were monitored during the heating (gel-sol) and cooling (sol-gel) processes. It was observed that the transition temperatures, T-m, defined as the location of the maximum of the first derivative of the sigmoidal transition paths obtained from the UV-vis technique, slightly increased by increasing the agarose concentration in both the HMP and LMP samples. Here, we express the phase transitions of the agar-water system, as a representative of reversible physical gels, in terms of a modified Susceptible-Infected-Susceptible epidemic model whose solutions are the well-known 5-point sigmoidal curves. The gel point is hard to determine experimentally and various computational techniques are used for its characterization. Based on previous work, we locate the gel point, T-0, of sol-gel and gel-sol transitions in terms of the horizontal shift in the sigmoidal transition curve. For the gel-sol transition (heating), T-0 is greater than T-m, i.e. later in time, and the difference between T-0 and T-m is reduced as the agarose content increases. For the sol-gel transition (cooling), T-0 is again greater than T-m, but it is earlier in time for all agarose contents and moves forward in time and gets closer to T-m as the agarose content increases. | en_US |
dc.identifier.doi | 10.1080/00222348.2018.1463052 | |
dc.identifier.endpage | 376 | en_US |
dc.identifier.issn | 0022-2348 | |
dc.identifier.issn | 1525-609X | |
dc.identifier.issue | 5 | en_US |
dc.identifier.scopus | 2-s2.0-85046020088 | en_US |
dc.identifier.scopusquality | Q3 | en_US |
dc.identifier.startpage | 364 | en_US |
dc.identifier.uri | https://doi.org/10.1080/00222348.2018.1463052 | |
dc.identifier.uri | https://hdl.handle.net/20.500.14551/18176 | |
dc.identifier.volume | 57 | en_US |
dc.identifier.wos | WOS:000435693300004 | en_US |
dc.identifier.wosquality | Q3 | en_US |
dc.indekslendigikaynak | Web of Science | en_US |
dc.indekslendigikaynak | Scopus | en_US |
dc.language.iso | en | en_US |
dc.publisher | Taylor & Francis Inc | en_US |
dc.relation.ispartof | Journal Of Macromolecular Science Part B-Physics | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.rights | info:eu-repo/semantics/openAccess | en_US |
dc.subject | Agarose | en_US |
dc.subject | Gel Point | en_US |
dc.subject | Generalized Logistic Curve | en_US |
dc.subject | Sol-Gel And Gel-Sol Transition | en_US |
dc.subject | Kappa-Carrageenan Gels | en_US |
dc.subject | Gelation Mechanism | en_US |
dc.subject | Epidemic Models | en_US |
dc.subject | Helix | en_US |
dc.subject | Fluorescence | en_US |
dc.subject | Networks | en_US |
dc.subject | Systems | en_US |
dc.title | Mathematical Characterization of Thermo-reversible Phase Transitions of Agarose Gels | en_US |
dc.type | Article | en_US |