Rheological implications of completely monotone fading memory

dc.contributor.authorAnderssen, R. S.
dc.contributor.authorLoy, R. J.
dc.date.accessioned2015-10-19T04:15:33Z
dc.date.available2015-10-19T04:15:33Z
dc.date.issued2002-11
dc.date.updated2015-12-12T09:28:35Z
dc.description.abstractIn the constitutive equation modeling of a (linear) viscoelastic material, the “fading memory” of the relaxation modulusG(t) is a fundamental concept that dates back to Boltzmann [Ann. Phys. Chem. 7, 624 (1876)]. There have been various proposals that range from the experimental and pragmatic to the theoretical about how fading memory should be defined. However, if, as is common in the rheological literature, one assumes that G(t) has the following relaxation spectrum representation: G(t)=∫₀∞ exp(−t/τ)[H(τ)/τ]dτ, t > 0, then it follows automatically that G(t) is a completely monotone function. Such functions have quite deep mathematical properties, that, in a rheological context, spawn interesting and novel implications. For example, because the set of completely monotone functions is closed under positive linear combinations and products, it follows that the dynamics of a linear viscoelastic material, under appropriate stress–strain stimuli, will involve a simultaneous mixture of different molecular interactions. In fact, it has been established experimentally, for both binary and polydisperse polymeric systems, that the dynamics can simultaneously involve a number of different molecular interactions such as the Rouse, double reptation and/or diffusion, [W. Thimm et al., J. Rheol., 44, 429 (2000); F. Léonardi et al., J. Rheol. 44, 675 (2000)]. The properties of completely monotone functions either yield new insight into modeling of the dynamics of real polymers, or they call into question some of the key assumptions on which the current modeling is based, such as the linearity of the Boltzmann model of viscoelasticity and/or the relaxation spectrum representation for the relaxation modulusG(t). If the validity of the relaxation spectrum representation is accepted, the resulting mathematical properties that follow from the complete monotonicity of G(t) allows one to place the classical relaxation model of Doi and Edwards [M. Doi and S. F. Edwards, J. Chem. Soc., Faraday Trans. 2 74, 1789 (1978)], as a linear combination of exp(−t/τ*) relaxation processes, each with a characteristic relaxation time τ*, on a more general and rigorous footing.
dc.identifier.issn0148-6055en_AU
dc.identifier.urihttp://hdl.handle.net/1885/15968
dc.publisherAmerican Institute of Physics (AIP)
dc.rightshttp://www.sherpa.ac.uk/romeo/issn/0148-6055..."Publishers version/PDF may be used on author's personal website, institutional website or institutional repository" from SHERPA/RoMEO site (as at 19/10/15). Copyright © 2002 by The Society of Rheology, Inc. This article may be downloaded for personal use only. Any other use requires prior permission of the author and the American Institute of Physics. The following article appeared in Journal of Rheology and may be found at https://doi.org/10.1122/1.1514203
dc.sourceJournal of Rheology
dc.subjectKeywords: Polymers; Relaxation processes; Strain; Stress analysis; Viscoelasticity; Fading memory; Rheology
dc.titleRheological implications of completely monotone fading memory
dc.typeJournal article
local.bibliographicCitation.issue6en_AU
local.bibliographicCitation.lastpage1472en_AU
local.bibliographicCitation.startpage1459en_AU
local.contributor.affiliationAnderssen, Robert S, CSIRO Mathematical and Information Sciences, Australiaen_AU
local.contributor.affiliationLoy, Richard, College of Physical and Mathematical Sciences, CPMS Mathematical Sciences Institute, Department of Mathematics, The Australian National Universityen_AU
local.contributor.authoremailRick.Loy@anu.edu.auen_AU
local.contributor.authoruidu7000666en_AU
local.description.notesImported from ARIESen_AU
local.description.refereedYes
local.identifier.absfor010399en_AU
local.identifier.ariespublicationMigratedxPub23969en_AU
local.identifier.citationvolume46en_AU
local.identifier.doi10.1122/1.1514203en_AU
local.identifier.scopusID2-s2.0-0036870531
local.identifier.uidSubmittedByu3488905en_AU
local.publisher.urlhttps://www.aip.org/en_AU
local.type.statusPublished Versionen_AU

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