A Review on Polymer Crystallization Theories
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2 a Primer on Polymer Colloids: Structure, Synthesis and Colloidal Stability
A. Al Shboul, F. Pierre, and J. P. Claverie 2 A primer on polymer colloids: structure, synthesis and colloidal stability 2.1 Introduction A colloid is a dispersion of very fine objects in a fluid [1]. These objects can be solids, liquids or gas, and the corresponding colloidal dispersion is then referred to as sus- pension, emulsion or foam. Colloids possess unique characteristics. For example, as their size is smaller than the wavelength of light, they scatter light. They also offer a large interfacial surface area, meaning that interfacial phenomena are of paramount importance in these dispersions. The weight of each dispersed particle being small, gravity and buoyancy forces are not sufficient to counteract the thermal random mo- tion of the particle, named Brownian motion (in tribute to the 19th century botanist Robert Brown who first characterized it). The particles do not remain in a dispersed state indefinitely: they will sooner or later aggregate (phase separation). Thus, thecol- loidal state is in general metastable and colloidal stability is one of the key features to take into account when working with colloids. Among all colloids, the polymer colloid family is one of the most widely inves- tigated [2]. Polymer colloids are used for a large number of applications, ranging from coatings, adhesives, inks, impact modifiers, drug-delivery vehicles, etc. The particles range in size from about 10 nm to 1 000 nm (1 μm) in diameter. They are usually spherical, but numerous other shapes have been observed. Polymer colloids are not uncommon in nature. For example, natural rubber latex, the secretion of the Hevea brasiliensis tree, is in fact a dispersion of polyisoprene nanoparticles in wa- ter. -
Entropy Driven Phase Transition in Polymer Gels: Mean Field Theory
entropy Article Entropy Driven Phase Transition in Polymer Gels: Mean Field Theory Miron Kaufman Physics Department, Cleveland State University, Cleveland, OH 44115, USA; [email protected] Received: 16 April 2018; Accepted: 27 June 2018; Published: 30 June 2018 Abstract: We present a mean field model of a gel consisting of P polymers, each of length L and Nz polyfunctional monomers. Each polyfunctional monomer forms z covalent bonds with the 2P bifunctional monomers at the ends of the linear polymers. We find that the entropy dependence on the number of polyfunctional monomers exhibits an abrupt change at Nz = 2P/z due to the saturation of possible crosslinks. This non-analytical dependence of entropy on the number of polyfunctionals generates a first-order phase transition between two gel phases: one poor and the other rich in poly-functional molecules. Keywords: crosslinking entropy; saturation; discontinuous phase transition 1. Motivation A polymer gel like polyacrylamide changes the volumes by a large factor of ~1000 when a small quantity of solvent like acetone is added to the solution or when the temperature is varied slightly. Central to the understanding of this phase transition are the covalent crosslinks [1–5] between the linear chains. Polymer chains, such as in hydroxypropylcellulose (HPC) immersed in a water solution, form hydrogen bonds with the water. As the temperature, the pH, or some other external condition is varied, there is a change in the strength of the hydrogen bonds that results in the formation or destruction of aggregates of crosslinked polymer chains. Light scattering experiments [6,7] are used to study the influence of the amount of crosslinkers on the properties of the gel phases. -
Assessment of Styrene Emission Controls for FRP/C
Assessment of Styrene Emission Controls for FRP/C and Boat Building Industries FINAL REPORT by: Emery J. Kong, Mark A. Bahner, and Sonji L. Turner Research Triangle Institute P.O. Box 12194 Research Triangle Park, NC 27709 EPA Contract 68-D1-0118, W.A. 156 EPA Project Officer: Norman Kaplan Air Pollution Prevention and Control Division National Risk Management Research Laboratory U.S. Environmental Protection Agency Research Triangle Park, NC 27711 Prepared for U.S. Environmental Protection Agency Office of Research and Development Washington, D.C. 20460 Abstract Styrene emissions from open molding processes in fiberglass-reinforced plastics/composites (FRP/C) and fiberglass boat building facilities are typically diluted by general ventilation to ensure that worker exposures do not exceed Occupational Safety and Health Administration (OSHA) standards. This practice tends to increase the potential cost to the facility of add-on controls. Furthermore, add-on styrene emission controls are currently not generally mandated by regulations. Therefore, emission controls are infrequently used in these industries at present. To provide technical and cost information to companies that might choose emission controls to reduce styrene emissions, several conventional and novel emission control technologies that have been used to treat styrene emissions in the United States and abroad and a few emerging technologies were examined. Control costs for these conventional and novel technologies were developed and compared for three hypothetical plant sizes. The results of this cost analysis indicate that increasing styrene concentration (i.e., lowering flow rate) of the exhaust streams can significantly reduce cost per ton of styrene removed for all technologies examined, because capital and operating costs increase with increasing flow rate. -
Fluorocarbon-Based Polymer Lamination Coating Film and Method of Manufacturing the Same
Europaisches Patentamt European Patent Office © Publication number: 0 484 886 A1 Office europeen des brevets EUROPEAN PATENT APPLICATION © Application number: 91118847.2 int. CIA B05D 1/20, C09D 127/12 @ Date of filing: 05.11.91 ® Priority: 06.11.90 JP 302021/90 4-6-8-806, Senrioka Higashi Settsu-shi, Osaka 566(JP) @ Date of publication of application: Inventor: Ogawa, Kazufumi 13.05.92 Bulletin 92/20 30-5, Higashi Nakafuri 1-chome Hirakata-shi, Osaka 573(JP) © Designated Contracting States: Inventor: Mochizuki, Yusuke DE FR GB IT 79-206, 9-ban, Mitsuigaoka 4-chome Neyagawa-shi, Osaka 572(JP) © Applicant: MATSUSHITA ELECTRIC Inventor: Shibata, Tsuneo INDUSTRIAL CO., LTD. 3-3-44, Suimeidai 1006, Oaza Kadoma Kawanishi-shi, Hyogo-ken 666-1 (JP) Kadoma-shi, Osaka-fu, 571 (JP) @ Inventor: Soga, Mamoru © Representative: Patentanwalte Grunecker, 1-22, Saikudani 1-chome Kinkeldey, Stockmair & Partner Tennoji-ku, Osaka-shi 543(JP) Maximilianstrasse 58 Inventor: Mino, Norihisa W-8000 Munchen 22(DE) © Fluorocarbon-based polymer lamination coating film and method of manufacturing the same. © The invention seeks to provide a substrate such as metal, ceramic, plastic, and glass material having a fluorine-based coating film having strong adhesion to a surface of the substrate. The substrate material comprises a monomolecular or polymer adsorption film formed on a base substrate surface and having siloxane bonds and a fluorine-based coating film provided on the adsoprtion film. The invention also seeks to provide a method of manufacturing a substrate material having a fluorine coating, which is simple and does not involve any electrolytic etching step. -
Soft Condensed Matter Physics Programme Course 6 Credits Mjuka Material TFYA37 Valid From: 2018 Spring Semester
1(9) Soft Condensed Matter Physics Programme course 6 credits Mjuka material TFYA37 Valid from: 2018 Spring semester Determined by Board of Studies for Electrical Engineering, Physics and Mathematics Date determined LINKÖPING UNIVERSITY FACULTY OF SCIENCE AND ENGINEERING LINKÖPING UNIVERSITY SOFT CONDENSED MATTER PHYSICS FACULTY OF SCIENCE AND ENGINEERING 2(9) Main field of study Applied Physics, Physics Course level Second cycle Advancement level A1X Course offered for Biomedical Engineering, M Sc in Engineering Engineering Biology, M Sc in Engineering Entry requirements Note: Admission requirements for non-programme students usually also include admission requirements for the programme and threshold requirements for progression within the programme, or corresponding. Prerequisites Mandatory courses in mathematics and physics for the Y-program or equal. Intended learning outcomes The course will ive the student knowledge of the statistical physics of polymers, the chemical, geometrical and electronic structure of polymers as well as the structure, dynamics and processing of polymer solids. We will discuss condensed matter in the form of colloids, amphiphiles, liquid crystals, molecular crystals and biological matter. After the course, the student should be able to describe the geometry of polymer chains and their dynamics, and the mathematical description of these phenomena utilize thermodynamical analysis of phase transitions in polymers and polymer blends LINKÖPING UNIVERSITY SOFT CONDENSED MATTER PHYSICS FACULTY OF SCIENCE AND ENGINEERING 3(9) describe micro and nanostructure of polymer solutions and polymer blends describe amphiphile materials, colloids, foams and gels, liquid crystals Course content Polymers: terminology, chemical structures and polymerization, solid state structures, polymers in solution, colligative properties. Statistical physics of polymer chains: random coils, entropy measures, rubber physics. -
Shape Memory and Actuation Behavior of Semicrystalline Polymer Networks
Dipl.-Phys. Martin Bothe Shape Memory and Actuation Behavior of Semicrystalline Polymer Networks BAM-Dissertationsreihe • Band 121 Berlin 2014 Die vorliegende Arbeit entstand an der BAM Bundesanstalt für Materialforschung und -prüfung. Impressum Shape Memory and Actuation Behavior of Semicrystalline Polymer Networks 2014 Herausgeber: BAM Bundesanstalt für Materialforschung und -prüfung Unter den Eichen 87 12205 Berlin Telefon: +49 30 8104-0 Telefax: +49 30 8112029 E-Mail: [email protected] Internet: www.bam.de Copyright © 2014 by BAM Bundesanstalt für Materialforschung und -prüfung Layout: BAM-Referat Z.8 ISSN 1613-4249 ISBN 978-3-9816668-1-6 Shape Memory and Actuation Behavior of Semicrystalline Polymer Networks vorgelegt von Dipl.-Phys. Martin Bothe aus Tubingen¨ von der Fakult¨at II – Mathematik und Naturwissenschaften der Technischen Universit¨at Berlin zur Erlangung des akademischen Grades Doktor der Naturwissenschaften – Dr. rer. nat. – genehmigte Dissertation Promotionsausschuss: Vorsitzender: Prof. Dr.-Ing. Matthias Bickermann Gutachter: Prof. Dr. rer. nat. Michael Gradzielski Gutachter: Prof. Dr. rer. nat. Michael Maskos Tag der wissenschaftlichen Aussprache: 16.07.2014 Berlin 2014 D 83 Für meine Familie Abstract Shape memory polymers (SMPs) can change their shape on application of a suitable stimulus. To enable such behavior, a ‘programming’ procedure fixes a deformation, yielding a stable tem- porary shape. In thermoresponsive SMPs, subsequent heating triggers entropy-elastic recovery of the initial shape. An additional shape change on cooling, i.e. thermoreversible two-way actuation, can be stimulated by a crystallization phenomenon. In this thesis, cyclic thermomechanical measurements systematically determined (1) the shape memory and (2) the actuation behavior under constant load as well as under stress-free condi- tions. -
Polymer Exemption Guidance Manual POLYMER EXEMPTION GUIDANCE MANUAL
United States Office of Pollution EPA 744-B-97-001 Environmental Protection Prevention and Toxics June 1997 Agency (7406) Polymer Exemption Guidance Manual POLYMER EXEMPTION GUIDANCE MANUAL 5/22/97 A technical manual to accompany, but not supersede the "Premanufacture Notification Exemptions; Revisions of Exemptions for Polymers; Final Rule" found at 40 CFR Part 723, (60) FR 16316-16336, published Wednesday, March 29, 1995 Environmental Protection Agency Office of Pollution Prevention and Toxics 401 M St., SW., Washington, DC 20460-0001 Copies of this document are available through the TSCA Assistance Information Service at (202) 554-1404 or by faxing requests to (202) 554-5603. TABLE OF CONTENTS LIST OF EQUATIONS............................ ii LIST OF FIGURES............................. ii LIST OF TABLES ............................. ii 1. INTRODUCTION ............................ 1 2. HISTORY............................... 2 3. DEFINITIONS............................. 3 4. ELIGIBILITY REQUIREMENTS ...................... 4 4.1. MEETING THE DEFINITION OF A POLYMER AT 40 CFR §723.250(b)... 5 4.2. SUBSTANCES EXCLUDED FROM THE EXEMPTION AT 40 CFR §723.250(d) . 7 4.2.1. EXCLUSIONS FOR CATIONIC AND POTENTIALLY CATIONIC POLYMERS ....................... 8 4.2.1.1. CATIONIC POLYMERS NOT EXCLUDED FROM EXEMPTION 8 4.2.2. EXCLUSIONS FOR ELEMENTAL CRITERIA........... 9 4.2.3. EXCLUSIONS FOR DEGRADABLE OR UNSTABLE POLYMERS .... 9 4.2.4. EXCLUSIONS BY REACTANTS................ 9 4.2.5. EXCLUSIONS FOR WATER-ABSORBING POLYMERS........ 10 4.3. CATEGORIES WHICH ARE NO LONGER EXCLUDED FROM EXEMPTION .... 10 4.4. MEETING EXEMPTION CRITERIA AT 40 CFR §723.250(e) ....... 10 4.4.1. THE (e)(1) EXEMPTION CRITERIA............. 10 4.4.1.1. LOW-CONCERN FUNCTIONAL GROUPS AND THE (e)(1) EXEMPTION................. -
Inertial Mass of an Elementary Particle from the Holographic Scenario
Document downloaded from: http://hdl.handle.net/10459.1/62944 The final publication is available at: https://doi.org/10.1142/S0217751X17500439 Copyright (c) World Scientific Publishing, 2017 Inertial mass of an elementary particle from the holographic scenario Jaume Gin´e Departament de Matem`atica, Universitat de Lleida, Catalonia, Spain. E{mail: [email protected] Abstract Various attempts have been made to fully explain the mechanism by which a body has inertial mass. Recently it has been proposed that this mechanism is as follows: when an object accelerates in one direction a dy- namical Rindler event horizon forms in the opposite direction, suppressing Unruh radiation on that side by a Rindler-scale Casimir effect whereas the radiation in the other side is only slightly reduce by a Hubble-scale Casimir effect. This produces a net Unruh radiation pressure force that always op- poses the acceleration, just like inertia, although the masses predicted are twice those expected, see [17]. In a later work an error was corrected so that its prediction improves to within 26% of the Planck mass, see [10]. In this paper the expression of the inertial mass of a elementary particle is derived from the holographic scenario giving the exact value of the mass of a Planck particle when it is applied to a Planck particle. Keywords: inertial mass; Unruh radiation; holographic scenario, Dark matter, Dark energy, cosmology. PACS 98.80.-k - Cosmology PACS 04.62.+v - Quantum fields in curved spacetime PACS 06.30.Dr - Mass and density 1 Introduction The equivalence principle introduced by Einstein in 1907 assumes the com- plete local physical equivalence of a gravitational field and a corresponding non- inertial (accelerated) frame of reference (Einstein was thinking of his famous elevator experiment). -
Quantization of Black Holes Is One of the Important Issues in Physics [1], and There Has Been No Satisfactory Solution Yet
Quantization of Black Holes Xiao-Gang He1, 2, 3, 4, ∗ and Bo-Qiang Ma1, 2, 4, † 1School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871 2Department of Physics and Center for Theoretical Sciences, National Taiwan University, Taipei 10617 3Institute of Particle Physics and Cosmology, Department of Physics, Shanghai JiaoTong University, Shanghai 200240 4Center for High-Energy Physics, Peking University, Beijing 100871 Abstract We show that black holes can be quantized in an intuitive and elegant way with results in agreement with conventional knowledge of black holes by using Bohr’s idea of quantizing the motion of an electron inside the atom in quantum mechanics. We find that properties of black holes can be also derived from an Ansatz of quantized entropy ∆S = 4πk∆R/λ, which was suggested in a previous work to unify the black hole entropy formula and Verlinde’s conjecture to explain gravity as an entropic force. Such an Ansatz also explains gravity as an entropic force from quantum effect. This suggests a way to unify gravity with quantum theory. Several interesting and surprising results of black holes are given from which we predict the existence of primordial black holes ranging from Planck scale both in size and energy to big ones in size but with low energy behaviors. PACS numbers: 04.70.Dy, 03.67.-a, 04.70.-s, 04.90.+e arXiv:1003.2510v3 [hep-th] 5 Apr 2010 ∗Electronic address: [email protected] †Electronic address: [email protected] 1 The quantization of black holes is one of the important issues in physics [1], and there has been no satisfactory solution yet. -
Statistical Mechanics of Entropic Forces: Disassembling a Toy
Home Search Collections Journals About Contact us My IOPscience Statistical mechanics of entropic forces: disassembling a toy This article has been downloaded from IOPscience. Please scroll down to see the full text article. 2010 Eur. J. Phys. 31 1353 (http://iopscience.iop.org/0143-0807/31/6/005) View the table of contents for this issue, or go to the journal homepage for more Download details: IP Address: 132.239.16.142 The article was downloaded on 06/12/2011 at 21:15 Please note that terms and conditions apply. IOP PUBLISHING EUROPEAN JOURNAL OF PHYSICS Eur. J. Phys. 31 (2010) 1353–1367 doi:10.1088/0143-0807/31/6/005 Statistical mechanics of entropic forces: disassembling a toy Igor M Sokolov Institut fur¨ Physik, Humboldt-Universitat¨ zu Berlin, Newtonstraße 15, D-12489 Berlin, Germany E-mail: [email protected] Received 21 June 2010, in final form 9 August 2010 Published 23 September 2010 Online at stacks.iop.org/EJP/31/1353 Abstract The notion of entropic forces often stays mysterious to students, especially to ones coming from outside physics. Although thermodynamics works perfectly in all cases when the notion of entropic force is used, no effort is typically made to explain the mechanical nature of the forces. In this paper we discuss the nature of entropic forces as conditional means of constraint forces in systems where interactions are taken into account as mechanical constraints and discuss several examples of such forces. We moreover demonstrate how these forces appear within the standard formalism of statistical thermodynamics and within the mechanical approach based on the Pope–Ching equation, making evident their connection with the equipartition of energy. -
As a Solid Polymer Electrolyte for Lithium Ion Batteries
UPTEC K 16013 Examensarbete 30 hp Juli 2016 A study of poly(vinyl alcohol) as a solid polymer electrolyte for lithium ion batteries Gustav Ek Abstract A study of poly(vinyl alcohol) as a solid polymer electrolyte for lithium ion batteries Gustav Ek Teknisk- naturvetenskaplig fakultet UTH-enheten The use of solid polymer electrolytes in lithium-ion batteries has the advantage in terms of safety and processability, however they often lack in terms of performance. Besöksadress: This is of major concern in applications where high current densities or rapidly Ångströmlaboratoriet Lägerhyddsvägen 1 changing currents are important. Such applications include electrical vehicles and Hus 4, Plan 0 energy storage of the electrical grid to accommodate fluctuations when using renewable energy sources such as wind and solar. Postadress: Box 536 751 21 Uppsala In this study, the use of commercial poly(vinyl alcohol) (PVA) as a solid polymer electrolyte for use in lithium-ion batteries has been evaluated. Films were prepared Telefon: using various lithium salts such as lithium bis(trifluoromethane)sulfonimide (LiTFSI) 018 – 471 30 03 and casting techniques. Solvent free films were produced by substituting the solvent Telefax: Dimethyl sulfoxide (DMSO) with water and rigouros drying or by employing a 018 – 471 30 00 hot-pressing technique. The best performing system studied was PVA-LiTFSI-DMSO, which reached ionic conductivities of 4.5E-5 S/cm at room temperature and 0.45 Hemsida: mS/cm at 60 °C. The solvent free films showed a drop of ionic conductivity by http://www.teknat.uu.se/student roughly one order of magnitude compared to films with residual DMSO present. -
Polymer Colloid Science
Polymer Colloid Science Jung-Hyun Kim Ph. D. Nanosphere Process & Technology Lab. Department of Chemical Engineering, Yonsei University National Research Laboratory Project the financial support of the Korea Institute of S&T Evaluation and Planning (KISTEP) made in the program year of 1999 기능성 초미립자 공정연구실 Colloidal Aspects 기능성 초미립자 공정연구실 ♣ What is a polymer colloids ? . Small polymer particles suspended in a continuous media (usually water) . EXAMPLES - Latex paints - Natural plant fluids such as natural rubber latex - Water-based adhesives - Non-aqueous dispersions . COLLOIDS - The world of forgotten dimensions - Larger than molecules but too small to be seen in an optical microscope 기능성 초미립자 공정연구실 ♣ What does the term “stability/coagulation imply? . There is no change in the number of particles with time. A system is said to be colloidally unstable if collisions lead to the formation of aggregates; such a process is called coagulation or flocculation. ♣ Two ways to prevent particles from forming aggregates with one another during their colliding 1) Electrostatic stabilization by charged group on the particle surface - Origin of the charged group - initiator fragment (COOH, OSO3 , NH4, OH, etc) ionic surfactant (cationic or anionic) ionic co-monomer (AA, MAA, etc) 2) Steric stabilization by an adsorbed layer of some substance 3) Solvation stabilization 기능성 초미립자 공정연구실 기능성 초미립자 공정연구실 Stabilization Mechanism Electrostatic stabilization - Electrostatic stabilization Balancing the charge on the particle surface by the charges on small ions