Chaos analysis of viscoelastic chaotic flows of polymeric fluids in a micro-channel

Many fluids, including biological fluids such as mucus and blood, are viscoelastic. Through the introduction of chaotic flows in a micro-channel and the construction of maps of characteristic chaos parameters, differences in viscoelastic properties of these fluids can be measured. This is demonstrat...

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Main Authors: C. P. Lim, J. Han, Y. C. Lam
Format: Article
Language:English
Published: AIP Publishing LLC 2015-07-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.4927474
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spelling doaj-b75beb0d7e3e4e06b249e70a998b20852020-11-24T21:12:54ZengAIP Publishing LLCAIP Advances2158-32262015-07-0157077150077150-810.1063/1.4927474051507ADVChaos analysis of viscoelastic chaotic flows of polymeric fluids in a micro-channelC. P. Lim0J. Han1Y. C. Lam2School of Mechanical and Aerospace Engineering, Nanyang Technological University, 639798, SingaporeBioSystems and Micromechanics (BioSyM) IRG, Singapore-MIT Alliance for Research and Technology (SMART) Centre, 138602, SingaporeSchool of Mechanical and Aerospace Engineering, Nanyang Technological University, 639798, SingaporeMany fluids, including biological fluids such as mucus and blood, are viscoelastic. Through the introduction of chaotic flows in a micro-channel and the construction of maps of characteristic chaos parameters, differences in viscoelastic properties of these fluids can be measured. This is demonstrated by creating viscoelastic chaotic flows induced in an H-shaped micro-channel through the steady infusion of a polymeric fluid of polyethylene oxide (PEO) and another immiscible fluid (silicone oil). A protocol for chaos analysis was established and demonstrated for the analysis of the chaotic flows generated by two polymeric fluids of different molecular weight but with similar relaxation times. The flows were shown to be chaotic through the computation of their correlation dimension (D2) and the largest Lyapunov exponent (λ1), with D2 being fractional and λ1 being positive. Contour maps of D2 and λ1 of the respective fluids in the operating space, which is defined by the combination of polymeric fluids and silicone oil flow rates, were constructed to represent the characteristic of the chaotic flows generated. It was observed that, albeit being similar, the fluids have generally distinct characteristic maps with some similar trends. The differences in the D2 and λ1 maps are indicative of the difference in the molecular weight of the polymers in the fluids because the driving force of the viscoelastic chaotic flows is of molecular origin. This approach in constructing the characteristic maps of chaos parameters can be employed as a diagnostic tool for biological fluids and, more generally, chaotic signals.http://dx.doi.org/10.1063/1.4927474
collection DOAJ
language English
format Article
sources DOAJ
author C. P. Lim
J. Han
Y. C. Lam
spellingShingle C. P. Lim
J. Han
Y. C. Lam
Chaos analysis of viscoelastic chaotic flows of polymeric fluids in a micro-channel
AIP Advances
author_facet C. P. Lim
J. Han
Y. C. Lam
author_sort C. P. Lim
title Chaos analysis of viscoelastic chaotic flows of polymeric fluids in a micro-channel
title_short Chaos analysis of viscoelastic chaotic flows of polymeric fluids in a micro-channel
title_full Chaos analysis of viscoelastic chaotic flows of polymeric fluids in a micro-channel
title_fullStr Chaos analysis of viscoelastic chaotic flows of polymeric fluids in a micro-channel
title_full_unstemmed Chaos analysis of viscoelastic chaotic flows of polymeric fluids in a micro-channel
title_sort chaos analysis of viscoelastic chaotic flows of polymeric fluids in a micro-channel
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2015-07-01
description Many fluids, including biological fluids such as mucus and blood, are viscoelastic. Through the introduction of chaotic flows in a micro-channel and the construction of maps of characteristic chaos parameters, differences in viscoelastic properties of these fluids can be measured. This is demonstrated by creating viscoelastic chaotic flows induced in an H-shaped micro-channel through the steady infusion of a polymeric fluid of polyethylene oxide (PEO) and another immiscible fluid (silicone oil). A protocol for chaos analysis was established and demonstrated for the analysis of the chaotic flows generated by two polymeric fluids of different molecular weight but with similar relaxation times. The flows were shown to be chaotic through the computation of their correlation dimension (D2) and the largest Lyapunov exponent (λ1), with D2 being fractional and λ1 being positive. Contour maps of D2 and λ1 of the respective fluids in the operating space, which is defined by the combination of polymeric fluids and silicone oil flow rates, were constructed to represent the characteristic of the chaotic flows generated. It was observed that, albeit being similar, the fluids have generally distinct characteristic maps with some similar trends. The differences in the D2 and λ1 maps are indicative of the difference in the molecular weight of the polymers in the fluids because the driving force of the viscoelastic chaotic flows is of molecular origin. This approach in constructing the characteristic maps of chaos parameters can be employed as a diagnostic tool for biological fluids and, more generally, chaotic signals.
url http://dx.doi.org/10.1063/1.4927474
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