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dc.title | Note on the relation betweeen the parameters of the Mark-Houwink-Kuhn-Sakurada equation | en |
dc.contributor.author | Halabalová, Věra | |
dc.contributor.author | Šimek, Lubomír | |
dc.contributor.author | Dostál, Jiří | |
dc.contributor.author | Bohdanecký, Miloslav | |
dc.relation.ispartof | International Journal of Polymer Analysis and Characterization | |
dc.identifier.issn | 1023-666X Scopus Sources, Sherpa/RoMEO, JCR | |
dc.date.issued | 2004 | |
utb.relation.volume | 9 | |
utb.relation.issue | 1-3 | |
dc.citation.spage | 65 | |
dc.citation.epage | 75 | |
dc.type | article | |
dc.language.iso | en | |
dc.publisher | Taylor and Francis | en |
dc.identifier.doi | 10.1080/10236660490890484 | |
dc.relation.uri | http://www.tandfonline.com/doi/abs/10.1080/10236660490890484 | |
dc.subject | equation [eta] = KMa | en |
dc.subject | parameters K and A | en |
dc.subject | interpretation | en |
dc.description.abstract | The relation between the parameters K and a of the equation [eta] = Km(a). which has been empirically established by several authors,, is discussed. Equations describing this relation are derived based on the two-parameter theory of the intrinsic viscosity for flexible, chain polymers (where a < 0.8) and on the worm-like cylinder model for stiff chains (a > 0.8). The correspondence of calculated and empirical results is good. | en |
utb.faculty | Faculty of Technology | |
dc.identifier.uri | http://hdl.handle.net/10563/1002052 | |
utb.identifier.scopus | 2-s2.0-12444307414 | |
utb.identifier.wok | 000226382700006 | |
utb.source | j-wok | |
dc.date.accessioned | 2011-08-16T15:06:17Z | |
dc.date.available | 2011-08-16T15:06:17Z | |
utb.contributor.internalauthor | Halabalová, Věra | |
utb.contributor.internalauthor | Šimek, Lubomír | |
utb.contributor.internalauthor | Dostál, Jiří |