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dc.contributor.advisorRobert C. Armstrong and Robert A. Brown.en_US
dc.contributor.authorNayak, Radha, 1969-en_US
dc.date.accessioned2005-08-19T18:54:06Z
dc.date.available2005-08-19T18:54:06Z
dc.date.copyright1998en_US
dc.date.issued1998en_US
dc.identifier.urihttp://hdl.handle.net/1721.1/9609
dc.descriptionThesis (Ph.D.)--Massachusetts Institute of Technology, Dept. of Chemical Engineering, 1998.en_US
dc.descriptionIncludes bibliographical references (v. 2, leaves 358-374).en_US
dc.description.abstractThe focus of this thesis was twofold. First, efficient numerical methods were developed for the modeling of the molecular orientation distribution function, f, of rigid rod polymers in flow. These methods were used to investigate the liquid crystal polymer (LCP) system. Second, the distribution function calculations were incorporated into a discontinuous Galerkin finite element framework for the modeling of complex LCP flows. Due to the localized nature of f under flow, the Daubechies D6 wavelets were used as basis functions for the approximation of f, and resulted in an efficient numerical technique to model LCPs. Bifurcation analysis of the Doi LCP model in shear flow showed that steady state solutions are lost due to the formation of a limit point in the plot of structure parameter S vs. concentration parameter N, beyond which time-periodic solutions are the only stable solutions. At low De, the time-periodic solutions onset as tumbling states at a global bifurcation. At high De, they onset as wagging states at a Hopf bifurcation, with a subsequent second transition to tumbling as N is increased. The period of oscillation of all tumbling states follows the experimentally observed scaling with strain. However, the wagging states do not follow this scaling, indicating that tumbling and wagging states belong to different solution. families. Computation of f in pressure-driven channel flow of LCPs using the wavelet­finite element method showed that the range of tumbling periods, combined with the existence of an infinite period tumbling streamline at the centerline, provides a mechanism for texture generation and refinement. The analysis also demonstrated the possibility of predicting biphasic solutions to LCP problems. Simulations of LCP flow in a tapering contraction geometry showed that the Doi model predicts inter­mediate concentrations to be most effective in producing flow-alignment of molecular distributions. At higher concentrations, tumbling is found to be widespread in the tapering section despite the presence of an elongational component in the strain rate. Taken together, these calculations demonstrate the feasibility of performing complex flow calculations with molecular models, which will lead to a better physical under­standing of the effect of molecular configuration in polymer flows.en_US
dc.description.statementofresponsibilityby Radha Nayak.en_US
dc.format.extent2 v. (374 leaves)en_US
dc.format.extent28679727 bytes
dc.format.extent28679486 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypeapplication/pdf
dc.language.isoengen_US
dc.publisherMassachusetts Institute of Technologyen_US
dc.rightsM.I.T. theses are protected by copyright. They may be viewed from this source for any purpose, but reproduction or distribution in any format is prohibited without written permission. See provided URL for inquiries about permission.en_US
dc.rights.urihttp://dspace.mit.edu/handle/1721.1/7582
dc.subjectChemical Engineeringen_US
dc.titleMolecular simulation of liquid crystal polymer flow : a wavelet-finite element analysisen_US
dc.title.alternativeWavelet-finite element analysisen_US
dc.typeThesisen_US
dc.description.degreePh.D.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Chemical Engineeringen_US
dc.identifier.oclc42249612en_US


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