DOCSLIB.ORG

Liquid Crystalline Polymers 1990017655-002

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Liquid Crystalline Polymers 1990017655-002 1990017655 NAEI CNINASIIOMI _,_• " TF!,.-'-,-E_r _t,US"-,-,_v (_) AD-A223 253 Liquid Crystalline Polymers 1990017655-002 NATIONAL RESEARCH COUNCIL COMMISSION ON ENGINEERING AND TECHNICAL SYSTEMS NATIONAL MATERIALS ADVISORY BOARD The purpose of the National Materials Advisory Board is the advancement of materials science and engineering in the national interest. CHAIRMAN PAST CHAIRMAN Dr. James C. Wflhams Dr. Bernard H. Kear General Manager Chairman, Department of Materials Technology l,aboratene,, Mechanics and Materials Science Mall Drop #85 Director. Center for Materials General Electric Company Synthesis I Neumann Wa) College of Engineering Cincinnati, OH 45215-6301 Rutgers University P.O. Box 9119 Pi_cataway, NJ 08854 MEMBERS Dr. Norbert S. Baer Dr. Frank F, Jamerson Dr. John P. Riggs Hagop Kevorkmn Profes,,or of Manager Vice President. R&D Research Conservation l)_v=sion and Staff Contact,, Division Net, York Umver,qt_ General Motors Re,,earch Managing Director, Mitchell Conservation Center of the Institute Labaratories Technical Center of Fine Art,, 30500 Mound Road Hoechst Celanese Corporation 14 East 78th Street Warlen. MI 48091)-thi5 'I 86 Morris Avenue Ne_ York. NY 10021 Summit. NJ 079t)1 I)r Mel,,m F Kannlnen Mr Robert R Beebe In,41tute Seventh,4 Dr. Maxnne L. Savitz • Semor _ce Ihe,qdent Southwest Re,,carch Inshlule D_rectur Itomeqake Mmmg Company P.(). l)ra'_er 28510 Garrett Ceramic Components 651) ('ahfornm Slreet San Antonio. TX 78284 Divi-,ton San Ft'ant_t,,co. ('A 9410g Allied-Signal Aerospace Co. l)r. Ronald M. Latarnsmn 19800 South Van Ness Avenue Ih' Fl,lnk _, (ro.,snlan Prolc,,sor of Matcrutl,, Soence & Tonance. CA 90509 A,,',tqant l)trecto_ Engineering, and l)_rector. i elecommumcat_tm,,. S)qem', & ()peratlon,, Materials Processing (.enter Dr. Dale F. Stein I.ockheed Missde,, & Space ('o . Inc Room 8.202 President Oig No 19-i'_(I Bldg. 11)2 Massachusetts Instflute of Michigan lechnologlcal Univermty i) O Box i.s04 "1cchnolol:._, Hougltton. MI 49931 Sttnnv_. ale, (A 94(188-'451)4 ('ambrldge. '>IA 021 '49 Dr. F:,rl R. Thompson I)l..lanl¢., |,(onoll]V Dr. Robert A I.an,alp.t2 AsslManl Director of Research for Profe,,,,oi & |lead of Material', I)u,:ctol. Ph._,,lc,ll and Inorgamc Material,, Technology Sclent. c Cheml,4_ .', Re.,e,tt ch I,,iborator_. t ]rated Technologies Re,,earch t niverslt), of llhnor, Roonl IA-2M Center I)epartment of Malell;lls Science & A I&I Bell l,aboiatorles Silver Lane t-ngmeermg Munay Ihll. NJ 07'i74 Ea,,t ttartford, CT 06108 I "t04(;teen Street t'rbana. II. 6181)1 I)t. Wdham I). Nix Mr. James R. Weir, Jr Profes,,or. [)ep;ulmenl of Materials A_socmle Director l)r. James .,'_ I old Sclcno" and Engineering Metals & Ceramics Division ('onsullant Stanford Unt_,erslt_, Oak Ridge National Laboratory 70'4 .hidith I)tl'¢e St,lnford. ('A 9430'_ P.O. I]ox X John,,on ('lix. TN _7604 ()ak Ridge. TN 378311 DI. I),mald R. Paul Mek in H. Gertz Regent,, ('h,ur I)r. Robert M. White I)r Robert I-. (;veen, ,h m ('heroical Engineering Vice President Dilcctor ot'('entcr fo: NI)I-. I)ueutor. t'entet for Polymer MCC th ofessor. Matei lals Science Re,,eal ch '4s00 West Balcones ('enter I)rtve I)epav tment I)epartment of ('heroical Austin, TX 787'19 Johns |lopkms I.rnp,el'sit.,. Engmeenng lialtiniore, MI)21218 t:ni_elsll_ of Texas ,ausmL I'X 78712 NMAB STAFF I)t. John K, Ihdm ('hlefScienll,,t |_lncillu,, I)r .Ioscph I Pcnlecosl K.M. Zwilsky. I)irector Westinghouse Reseaich I)rofe.,sor S M. Itarkln, Assoc l)lreclor l,:iboralol les School fir Malel lals Eng,neerlng Mary Ill Ittaln, Adm. ()filter I_ 10 lleulah Road (icoigi.i In,,lllute of Technolog) 2101 Constitution Ave.. NW Pittsburgh, PA 152_5 Atlant,i. (i,i _1}_2 Washinglon, D(" 211418 3f90 1990017655-003 UNCLASSIFIED _ECumRITYCLASSIFICATIONOF THISPAGE REPORT DOCUMENTATION PAGE _la REPORTSECURITYCLASSIFICATION lb RESTRICTIVMAE RKINGS b_CLASSI_IED NONE 2a. SECURITYCL.ASSIFICATIONAUTHORITY 3 DISTRIBUTION/AVAILABILITYOF REPORT "'_. DECLASSiFN/t_ ICATIO/ DOWNGRADN INGSCHEDULE Approved for Public Release Distribution Unlimited N/_ ,, 4.PERFORMING ORGANIZATIONREPORT NUMBER(S) 5 MONITORING ORGANIZATION REPORT NUMBER(S) NMAB-453 6a NAME OF PERFORMINGORGANIZATION 6b OFFICESYMBOL 7_. NAME OF MONITORINGORGAN;ZATION National Materials Advisory (Ifapplicable) Department of Defense/National Aeronautics Board NMAB & Space Administration 6<.ADDRESS(0;7, State. and ZlPCode) 7b ADDRESS(City, St, re, and ZlPCode) National Academy of Sciences Washington, DC 20418 Washington, DC 20301 h 8a. NAME OFFUNDING/SPONSORING Bb OFFICESYMBOL I 9, PROCUREMENTINSTRUMENTiDENTiFiCATIONNUMBER ORGANIZATION _lf applic_b_) See 7a DOD/NASA MDA903-89-K-0078 8c ADDRESS{C/_, State, and ZIPCo_o) 10 SOURCEO_ FUNDINGN_JMBERS PROGRAM PROJECT TASK WORK UNIT Washington, DC 20301 ELEMENTNO. NO. NO ACCESSIONNO 11. TITLE(Indude SecurrtyCla_fication) LIQUID CRYSTALLINE POL_fMERS I, 12.PERSONALAuTHOR(S) N_IAB Committee on Liouid Crvsta]llnp Polvmer_ . i _3a TYPE OF REPORTOne of a :._bTSMECOVERED I_4.DATE OF REPORT _emr,Month,D_yJ IS.PAGE COUNT series under subi. co_; FROM IO_V TO IQan I 1990 F_hr1,m_-v P_ 117 16 SUPPLEMENTARYNOTATION -' NONE 17 COSATICODES 1B SUBJECTTERMSL(C_-c__tfBlr, j.Bam_mc_l_,t_ bytb/ock-_rd_e&l... FIELD _ROUP SUB-.GRO_uI Liquid crystalline polymers (LCPs); fibers; thermotropic; lyotropic; processing; rheology; nonlinear optical (4_ -._ i properties; blends: comno_, t_-rf_ _-- 19_BS_ RACT(Con_nue on reverse ff _eum'y _nd _.t_y by bloc*number) " ' The remarkable mechanical properties and thermal stability of fibers fabricated from liquid crystalline polymers (LCPs) have led to the use of these materials in structural applications where weight savings are critical. Advances in processing of LCPs could permit the incorporation of these polymers into other than uniaxial designs and extend their utility into new areas such as nonlinear optical devices. However, the unique feature of LCPs--intrinsic orientational order--is itself problematic, and current understanding of processing with control of orientation falls short of allowing manipula- tion of macroscopic orientatioe (except for the case of uniaxial fibers). This report reviews the current and desirable characteristics of LCPs and identifies specific problems and issues t|'at mu_t be addressed so that advances in the use of these unique po]ymers can be expedited. I 20 DISTRIBUTIONIAVAILABILITYOF ABSTRA(.'r 21. ABSTRACTSECURITYCLASSIFICATION I:_71UNCLASSIFIED/UNLIMITEr]D SAMEAS RPT, _ DT:CUSERS UNCLASSIFIED 22a NA_E OF RESPONSIBLEiNDIVIDUAL 22b TELEPHON(Einclude Area Co(_e) 22c.OFFICESYMBOL Jerome Persh. ,.,,, 2021695-0005 OUSDR&E/R&AT/MST DD FORM 1473.84 MArC |_1 APR edition m_lly be used u_tll el_hausted SECURITY CLASSIFICATION OF THIS PAGE All othereditionsarkobsolete UNCLASSIFIED 1990017655-004 Liquid Crystalline Polymers Report of the Committee on Liquid Crystalline Polymers NATIONAL MATERIALS ADVISORY BOARD Commission on Engineering and Technical Systems National Research Council ___es_slon _For NTIS C_RA&I _ -- DTIC T.\B UI_r.:_'_c,,mcod [] Just ±_''_c_tt orL NMAB-453 By Na_,onal Academy Press Dist.r_' _',,,-,_/ 1990 _,w_i_.,, ',_ '_ C_s Dist " I_'_' _: ' _ior-_ 1990017655-005 NOTICE: The project that i3 the subject of this report was approved by the Governing Board of the National Research Council, whose members are drawn from the councils of the National Academy of Sciences, the National Academy of Engineering, aad the Institute of Medicine. The members of the committee responsible for the report were chosen for their special competences arld with regard for appropriate balance. This report has been reviewed by a group other than the authors according to procedures approved by a Report Review Committee consisting of members of the National Academy of Sciences, the National Academy of Engineering, and the Institute of Medicine. The National Academy of Sciences is a private, nonprofit, self-perpetuating society of distinguished scholars engaged in scientific and engineering research, dedicated to the furtherance of science and technology and to their use for the general welfare. Upon the authority of the charter granted to it by the Congress in 1863, the Academy has a mandate that requires it to advise the federal government on scientific and technical matters. Dr. Frank Press is president of the National Academy of Sciences. The National Academy of Engineering was established in 1964, under the charter of the National Academy of Sciences, as a parallel organization of outstanding engineers. It is autonomous in its administration and in the selection of its members, sharing with _he Nationa! Academy of Sciences the responsiblity for advising the federal government. The National Academy of Engineering also sponsors engineering programs aimed at meeting national needs, encourages education and research, apd recognizes the superior achievements of engineers. Dr. Robert M. White is president of the National Academy of Engineering. The Institute of Medicine was established in 1970 by the National Academy of Sciences to secure the services of eminent members of appropriate professions in the examination of policy matters pertaining to the health of the public. The Institute acts under the responsibility given to the National Academy of Sciences by its congressional charter t,J be an adviser to the federal government and, upon its own initiative, to identify issues of medical care, research, and education. Dr. Samuel O. Thier is president of the Institute of Medicine. The National Research Council was organized by the National Academy of Sciences in 1916 to associate the broad community of science and technology with the Academy's purposes of furthering knowledge and advising the federal government. Functioning in accordance with general policies determined by the Academy, the Council has become the principal operating agency of both the National Academy of Sciences and the National Academy of Engineering in providing services to the go-Jernment, the public, and the scientific and engineering communities. The Council is administered jointly by both Academies and the Institute of Medicine.
Load more

Recommended publications
  • Machine Learning for Condensed Matter Physics
    Review Article Machine Learning for Condensed Matter Physics Edwin A. Bedolla-Montiel1, Luis Carlos Padierna1 and Ram´on Casta~neda-Priego1 1 Divisi´onde Ciencias e Ingenier´ıas,Universidad de Guanajuato, Loma del Bosque 103, 37150 Le´on,Mexico E-mail: [email protected] Abstract. Condensed Matter Physics (CMP) seeks to understand the microscopic interactions of matter at the quantum and atomistic levels, and describes how these interactions result in both mesoscopic and macroscopic properties. CMP overlaps with many other important branches of science, such as Chemistry, Materials Science, Statistical Physics, and High-Performance Computing. With the advancements in modern Machine Learning (ML) technology, a keen interest in applying these algorithms to further CMP research has created a compelling new area of research at the intersection of both fields. In this review, we aim to explore the main areas within CMP, which have successfully applied ML techniques to further research, such as the description and use of ML schemes for potential energy surfaces, the characterization of topological phases of matter in lattice systems, the prediction of phase transitions in off-lattice and atomistic simulations, the interpretation of ML theories with physics- inspired frameworks and the enhancement of simulation methods with ML algorithms. We also discuss in detial the main challenges and drawbacks of using ML methods on CMP problems, as well as some perspectives for future developments. Keywords: machine learning, condensed matter physics Submitted
    [Show full text]
  • Calorimetric Study on Kinetics of Mesophase Transition in Thermotropic Copolyesters
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Directory of Open Access Journals IJRRAS 3 (1) ● April 2010 Talukdar & Achary ● Study on Kinetics of Mesophase Transition CALORIMETRIC STUDY ON KINETICS OF MESOPHASE TRANSITION IN THERMOTROPIC COPOLYESTERS Malabika Talukdar & P.Ganga Raju Achary Department Of Chemistry, Institute Of Technical Education and Research (ITER), S ‘O’A University, Bhubaneswar, Orissa, India ABSTRACT Macromolecular crystallization behaviour, especially those of liquid crystalline polymers, has been a subject of great interest. The crystallization process for the polyester samples under discussion are analyzed assuming a nucleation controlled process and by using the Avrami equation. The study mainly deals with the crystallization process from the mesophase of two thermotropic liquid crystalline polyesters exhibiting smectic order in their mesophasic state. In order to analyze crystallization behavior of the polyesters, crystallization rate constant and the Avrami exponent have been estimated. Total heat of crystallization and entropy change during the transition has been calculated for both the polyesters. Keywords: Crystallization; Mesophase; Nucleation; Orthorhombic; Smectic. 1. INTRODUCTION The transition kinetics of liquid crystal polymers appears to be of great interest in order to control the effect of processing conditions on the morphology as well as on the final properties of the materials. These LC polymers show at least three main transitions: a glass transition, a thermotropic transition from the crystal to the mesophase and the transition from the mesophase to the isotropic melt. The kinetics of phase transition in liquid crystals may be analyzed for three different processes, the three dimensional ordering from both the isotropic melt state and the mesophase and the formation of the mesophase from the isotropic melt.
    [Show full text]
  • Soft Matter Theory
    Soft Matter Theory K. Kroy Leipzig, 2016∗ Contents I Interacting Many-Body Systems 3 1 Pair interactions and pair correlations 4 2 Packing structure and material behavior 9 3 Ornstein{Zernike integral equation 14 4 Density functional theory 17 5 Applications: mesophase transitions, freezing, screening 23 II Soft-Matter Paradigms 31 6 Principles of hydrodynamics 32 7 Rheology of simple and complex fluids 41 8 Flexible polymers and renormalization 51 9 Semiflexible polymers and elastic singularities 63 ∗The script is not meant to be a substitute for reading proper textbooks nor for dissemina- tion. (See the notes for the introductory course for background information.) Comments and suggestions are highly welcome. 1 \Soft Matter" is one of the fastest growing fields in physics, as illustrated by the APS Council's official endorsement of the new Soft Matter Topical Group (GSOFT) in 2014 with more than four times the quorum, and by the fact that Isaac Newton's chair is now held by a soft matter theorist. It crosses traditional departmental walls and now provides a common focus and unifying perspective for many activities that formerly would have been separated into a variety of disciplines, such as mathematics, physics, biophysics, chemistry, chemical en- gineering, materials science. It brings together scientists, mathematicians and engineers to study materials such as colloids, micelles, biological, and granular matter, but is much less tied to certain materials, technologies, or applications than to the generic and unifying organizing principles governing them. In the widest sense, the field of soft matter comprises all applications of the principles of statistical mechanics to condensed matter that is not dominated by quantum effects.
    [Show full text]
  • Low Shear Rheological Behaviour of Two-Phase Mesophase Pitch
    Published as: Shatish Ramjee, Brian Rand, Walter W. Focke. Low Shear Rheological Behaviour of Two-Phase Mesophase Pitch. Carbon 82 (2015), pp. 368-380. DOI : 10.1016/j.carbon.2014.10.082 Low Shear Rheological Behaviour of Two-Phase Mesophase Pitch Shatish Ramjee, Brian Rand*, Walter W. Focke SARChI Chair of Carbon Technology and Materials, Department of Chemical Engineering University of Pretoria, Pretoria, South Africa, 0002 Abstract: The low shear rate rheology of two phase mesophase pitches derived from coal tar pitch has been investigated. Particulate quinoline insolubles (QI) stabilised the mesophase spheres against coalescence. Viscosity measurements over the range 10 to 106 Pa.s were made at appropriate temperature ranges. Increasing shear thinning behaviour was evident with increasing mesophase content. At low mesophase contents the dominant effect on the near Newtonian viscosity was temperature but at higher contents it was the shear rate; temperature dependence declined to near zero. The data indicated that agglomeration could be occurring at intermediate mesophase volume fractions, 0.2-0.3. The Krieger-Dougherty function and its emulsion analogue indicated that in this region the mesophase pitch emulsions actually behaved like „hard‟ sphere systems and the effective volume fraction was estimated as a function of shear rate illustrating the change in extent of agglomeration. At the higher volume fractions approaching the maximum packing fraction, which could only be measured at higher temperatures, the shear thinning behaviour
    [Show full text]
  • Exploring Thein Meso Crystallization Mechanism by Characterizing the Lipid Mesophase Microenvironment During the Growth of Singl
    Exploring the in meso crystallization mechanism rsta.royalsocietypublishing.org by characterizing the lipid mesophase microenvironment Research during the growth of single Cite this article: van`tHagLet al.2016 transmembrane α-helical Exploring the in meso crystallization mechanism by characterizing the lipid peptide crystals mesophase microenvironment during the 1,3,4 2,5 growth of single transmembrane α-helical Leonie van `t Hag , Konstantin Knoblich , Shane Phil.Trans.R.Soc.A peptide crystals. 374: A. Seabrook6, Nigel M. Kirby7, Stephen T. Mudie7, 20150125. http://dx.doi.org/10.1098/rsta.2015.0125 Deborah Lau4,XuLi1,3, Sally L. Gras1,3,8,Xavier 4 2,5 2,5 Accepted: 12 February 2016 Mulet , Matthew E. Call , Melissa J. Call , Calum J. Drummond4,9 and Charlotte E. Conn9 One contribution of 15 to a discussion meeting 1 issue ‘Soft interfacial materials: from Department of Chemical and Biomolecular Engineering, and 2 fundamentals to formulation’. Department of Medical Biology, The University of Melbourne, Parkville, Victoria 3052, Australia Subject Areas: 3Bio21 Molecular Science and Biotechnology Institute, physical chemistry, biochemistry The University of Melbourne, 30 Flemington Road, Parkville, Victoria 3052, Australia Keywords: 4 in meso crystallization, cubic mesophase, CSIRO Manufacturing Flagship, Private Bag 10, Clayton, Victoria local lamellar phase, DAP12. 3169, Australia 5Structural Biology Division, The Walter and Eliza Hall Institute of Authors for correspondence: Medical Research, 1G Royal Parade, Parkville, Victoria 3052,
    [Show full text]
  • Nematic Phases Smectic Phases
    Phases of Liquid Crystals http://plc.cwru.edu/tutorial/enhanced/files/lc/phase... Liquid Crystal Phases The liquid crystal state is a distinct phase of matter observed between the crystalline (solid) and isotropic (liquid) states. There are many types of liquid crystal states, depending upon the amount of order in the material. This section will explain the phase behavior of liquid crystal materials. Nematic Phases The nematic liquid crystal phase is characterized by molecules that have no positional order but tend to point in the same direction (along the director). In the following diagram, notice that the molecules point vertically but are arranged with no particular order. Liquid crystals are anisotropic materials, and the physical properties of the system vary with the average alignment with the director. If the alignment is large, the material is very anisotropic. Similarly, if the alignment is small, the material is almost isotropic. The phase transition of a nematic liquid crystal is demonstrated in the following movie provided by Dr. Mary Neubert, LCI−KSU. The nematic phase is seen as the marbled texture. Watch as the temperature of the material is raised, causing a transition to the black, isotropic liquid. A special class of nematic liquid crystals is called chiral nematic. Chiral refers to the unique ability to selectively reflect one component of circularly polarized light. The term chiral nematic is used interchangeably with cholesteric. Refer to the section on cholesteric liquid crystals for more information about this mesophase. Smectic Phases The word "smectic" is derived from the Greek word for soap. This seemingly ambiguous origin is explained by the fact that the thick, slippery substance often found at the bottom of a soap dish is actually a type of smectic liquid crystal.
    [Show full text]
  • Modeling Complex Liquid Crystals Mixtures: from Polymer Dispersed
    Modeling Complex Liquid Crystals Mixtures: From Polymer Dispersed Mesophase to Nematic Nanocolloids Ezequiel R. Soule and Alejandro D. Rey 1. Institute of Materials Science and Technology (INTEMA), University of Mar del Plata and National Research Council (CONICET), J. B. Justo 4302, 7600 Mar del Plata, Argentina 2. Department of Chemical Engineering, McGill University, Montreal, Quebec H3A 2B2, Canada Abstract Liquid crystals are synthetic and biological viscoelastic anisotropic soft matter materials that combine liquid fluidity with crystal anisotropy and find use in optical devices, sensor/actuators, lubrication, super-fibers. Frequently mesogens are mixed with colloidal and nanoparticles, other mesogens, isotropic solvents, thermoplastic polymers, cross- linkable monomers, among others. This comprehensive review present recent progress on meso and macro scale thermodynamic modelling, highlighting the (i) novelties in spinodal and binodal lines in the various phase diagrams, (ii) the growth laws under phase transitions and phase separation, (iii) the ubiquitous role of metastability and its manifestation in complex droplet interfaces, (iv) the various spinodal decompositions due to composition and order fluctuations, (v) the formation of novel material architectures such as colloidal crystals, (vi) the particle rich phase behaviour in liquid crystal nanocomposites, (vii) the use of topological defects to absorb and organize nanoparticles, and (viii) the ability of faceted nanoparticles to link into strings and organize into lattices. Emphasis is given to highlight dominant mechanisms and driving forces, and to link them to specific terms in the free energies of these complex mixtures. The novelties of incorporating mesophases into blends, solutions, dispersions and mixtures is revealed by using theory, modelling , computation, and visualization.
    [Show full text]
  • CHAPTER I Introduction to Liquid Crystals: Phase Types, Structures and Applications
    CHAPTER I Introduction to liquid crystals: phase types, structures and applications I. 1 Introduction Liquid crystal (LC) phases represent a unique state of matter characterized by both mobility and order on a molecular and at the supramolecular levels. This behaviour appears under given conditions, when phases with a characteristic order intermediate to that of a three dimensionally ordered solid and a completely disordered liquid are formed. Molecules in the crystalline state possess orientational and three dimensional positional orders. That is the constituent molecules of highly structured solids occupy specific sites in a three dimensional lattice and points their axes in fixed directions as illustrated in Fig.1.1a. Liquid crystal phases possess orientational order (tendency of the molecules to point along a common direction called the director n) and in some cases positional order in one or two dimensions as shown in Fig I.1b and I.1c. On the other hand, in the isotropic liquid state, the molecules move randomly and rotate freely about all possible directions (see Fig. I.1d). Thus, liquid crystals (LCs) have been defined as “orientationally ordered liquids” or “positionally disordered crystals” that combine the properties of both the crystalline (optical and electrical anisotropy) and the liquid (molecular mobility and fluidity) states [1] Figure I. 1 Schematic representation of molecular packing in the a) crystals b & c) liquid crystals and d) liquid state. 1. 2. Classification of liquid crystals The liquid crystal state(s) can be attained either by the action of heat on mesogens or by action of solvent on amphiphilic systems. The mesophases obtained by temperature variation are called thermotropic.
    [Show full text]
  • The Significant Structure Theory Applied to a Mesophase System
    Proc. Nat. Acad. Sci. USA Vol. 72, No. 1, pp. 78-82, January 1975 The Significant Structure Theory Applied to a Mesophase System (compressibility/coefficient of expansion/specific heat/cooperative phenomenon/liquid crystal) SHAO-MU MA AND H. EYRING Department of Chemistry, University of Utah, Salt Lake City, Utah 84112 Contributed by Henry Eyring, August 19, 1974 ABSTRACT The significant structure theory of liquids melting point to the boiling point of the material under in- is extended to the mesophase system with p-azoxyanisole vestigation. as an example. This compound has two different structures, a nematic phase and an isotropic phase, in its liquid state. (2) It gives the volume dependency as well as the tempera- In this study the nematic phase is treated as subject to a ture dependency of the Helmholtz free energy and therefore second volume and temperature-dependent degeneracy of the thermodynamic properties of liquids that depend on formally like that due to melting. The isotropic phase is both volume and temperature. treated as a normal liquid. The specific heat, thermal ex- pansion coefficient, compressibility, volume, entropy of transitions, and heat of transitions are calculated and compared to the observed values. This analysis differs from THEORY previous ones in including the volume dependence as well as the temperature dependence in one explicit expression According to the significant structure theory, there are three for the Helmholtz free energy. important contributions to liquid structure. (1) Molecules with solid-like degrees of freedom. The significant structure theory, which was first proposed by (2) Positional degeneracy in the solid-like structure.
    [Show full text]
  • Rapid Crystallization and Mesophase Formation of Poly(L-Lactic Acid)
    e-Polymers 2018; 18(4): 331–337 Muhammad Syazwan and Takashi Sasaki* Rapid crystallization and mesophase formation of poly(L-lactic acid) during precipitation from a solution https://doi.org/10.1515/epoly-2017-0247 is to control the degree of crystallinity. However, it has Received November 24, 2017; accepted January 13, 2018; previously been revealed that PLLA is rather intractable because of published online February 14, 2018 its slow crystallization tendency compared with common crystallizable polymers (1, 2). Efforts have been under- Abstract: Very rapid crystallization behaviors of taken to overcome this problem. Nucleation agents poly(L-lactic acid) (PLLA) are observed at room tempera- and plasticizers are often used as common methods to ture when it is precipitated from a chloroform solution into promote the crystallization (3–7). Other techniques such a large amount of alcohols (non-solvents). The resulting as freeze-drying (8, 9), and solvent-induced crystalliza- crystalline phase contains both a highly ordered (α) and tion (10) have also been reported. In addition, it is worth less ordered (α′) modifications, and the fraction of these noting that interface and geometrical nano-confinement phases depends on the alcohols used as the non-solvents: significantly affect the crystallization process of PLLA methanol tends to produce the highly ordered phase. The (11–14). degree of crystallinity tends to be high for lower alcohols. To promote the polymer crystallization rate, it is When the precipitation occurs in n-hexane, almost no important to clarify its fundamental mechanism. It has crystalline phase is formed, but a mesomorphic phase is been reported that a mesomorphic phase (mesophase), formed as a precursor to the crystalline phase.
    [Show full text]
  • Polymer Crystallization in Droplets and Confined Layers Using Multilayered Films
    POLYMER CRYSTALLIZATION IN DROPLETS AND CONFINED LAYERS USING MULTILAYERED FILMS by Deepak Langhe Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy Dissertation Advisers: Prof. Eric Baer and Prof. Anne Hiltner Department of Chemical Engineering CASE WESTERN RESERVE UNIVERSITY January, 2012 CASE WESTERN RESERVE UNIVERSITY SCHOOL OF GRADUATE STUDIES We hereby approve the thesis/dissertation of _______Deepak Langhe______________________________ candidate for the Ph.D. degree *. (signed) __Prof. Eric Baer_______________________ (chair of the committee) Prof. James Anderson___________________ Prof. David Schiraldi____________________ Prof. LaShanda Korley___________________ (date) ____September 20, 2011_____________ *We also certify that written approval has been obtained for any proprietary material contained therein. Copyright © 2011 by Deepak Langhe All rights reserved Dedicated to my grandparents and parents TABLE OF CONTENTS LIST OF TABLES………………………………………………………………… ii LIST OF FIGURES……………………………………………………………….. iii ACKNOWLEDGEMENTS……………………………………………………….. xiv ABSTRACT………………………………………………………………………… xvi CHAPTER PART I 1. STRUCTURE AND CRYSTALLIZATION KINETICS OF HOMOGENEOUSLY NUCLEATED POLYPROPYLENE DROPLETS AT HIGH UNDERCOOLINGS………………………….. 2 2. TRANSFORMATION OF ISOTACTIC POLYPROPYLENE 32 DROPLETS FROM THE MESOPHASE INTO THE Α-PHASE…….. 3. FRACTIONATED CRYSTALLIZATION OF α- AND β- 65 NUCLEATED POLYPROPYLENE DROPLETS……………………... 4. EFFECT OF ADDITIVES, CATALYST RESIDUES AND CONFINING SUBSTRATES ON THE
    [Show full text]
  • Assisted Development of Mesophase Pitch with Dispersed Graphene and Its Resulting Carbon Fibers
    University of Kentucky UKnowledge Theses and Dissertations--Mechanical Engineering Mechanical Engineering 2018 ASSISTED DEVELOPMENT OF MESOPHASE PITCH WITH DISPERSED GRAPHENE AND ITS RESULTING CARBON FIBERS Aaron Owen University of Kentucky, [email protected] Author ORCID Identifier: https://orcid.org/0000-0003-0858-3151 Digital Object Identifier: https://doi.org/10.13023/etd.2018.454 Right click to open a feedback form in a new tab to let us know how this document benefits ou.y Recommended Citation Owen, Aaron, "ASSISTED DEVELOPMENT OF MESOPHASE PITCH WITH DISPERSED GRAPHENE AND ITS RESULTING CARBON FIBERS" (2018). Theses and Dissertations--Mechanical Engineering. 126. https://uknowledge.uky.edu/me_etds/126 This Master's Thesis is brought to you for free and open access by the Mechanical Engineering at UKnowledge. It has been accepted for inclusion in Theses and Dissertations--Mechanical Engineering by an authorized administrator of UKnowledge. For more information, please contact [email protected]. STUDENT AGREEMENT: I represent that my thesis or dissertation and abstract are my original work. Proper attribution has been given to all outside sources. I understand that I am solely responsible for obtaining any needed copyright permissions. I have obtained needed written permission statement(s) from the owner(s) of each third-party copyrighted matter to be included in my work, allowing electronic distribution (if such use is not permitted by the fair use doctrine) which will be submitted to UKnowledge as Additional File. I hereby grant to The University of Kentucky and its agents the irrevocable, non-exclusive, and royalty-free license to archive and make accessible my work in whole or in part in all forms of media, now or hereafter known.
    [Show full text]