Polymer Colloid Science
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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. -
Controlled/Living Radical Polymerization in Aqueous Media: Homogeneous and Heterogeneous Systems
Prog. Polym. Sci. 26 =2001) 2083±2134 www.elsevier.com/locate/ppolysci Controlled/living radical polymerization in aqueous media: homogeneous and heterogeneous systems Jian Qiua, Bernadette Charleuxb,*, KrzysztofMatyjaszewski a aDepartment of Chemistry, Center for Macromolecular Engineering, Carnegie Mellon University, 4400 Fifth Avenue, Pittsburgh, PA 15213, USA bLaboratoire de Chimie MacromoleÂculaire, Unite Mixte associeÂe au CNRS, UMR 7610, Universite Pierre et Marie Curie, Tour 44, 1er eÂtage, 4, Place Jussieu, 75252 Paris cedex 05, France Received 27 July 2001; accepted 30 August 2001 Abstract Controlled/living radical polymerizations carried out in the presence ofwater have been examined. These aqueous systems include both the homogeneous solutions and the various heterogeneous media, namely disper- sion, suspension, emulsion and miniemulsion. Among them, the most common methods allowing control ofthe radical polymerization, such as nitroxide-mediated polymerization, atom transfer radical polymerization and reversible transfer, are presented in detail. q 2001 Elsevier Science Ltd. All rights reserved. Keywords: Aqueous solution; Suspension; Emulsion; Miniemulsion; Nitroxide; Atom transfer radical polymerization; Reversible transfer; Reversible addition-fragmentation transfer Contents 1. Introduction ..................................................................2084 2. General aspects ofconventional radical polymerization in aqueous media .....................2089 2.1. Homogeneous polymerization .................................................2089 -
„Polymer-Dispersionen“
„Polymer-Dispersionen“ Klaus Tauer Definitions Meaning & properties of polymer dispersions Preparation of polymer dispersions Polymer Dispersions Polymer: any of a class of natural or synthetic substances composed of very large molecules, called macromolecules, that are multiples of simpler chemical units called monomers. Polymers make up also many of the materials in living organisms, including, for example, proteins, cellulose, and nucleic acids. Dispersion: (physical chemistry) a special form of a colloid: i.e. very fine particles (of a second phase) dispersed in a continuous medium the most popular / famous / best-known case of a polymer dispersion is a LATEX a latex is produced by heterophase polymerization, where the most important technique is emulsion polymerization *) *) *) 1 DM = 1.95583 € Molecular Composition polymer dispersionen: high concentration of polymer with low viscosity thickener (BASF AG, Ludwigshafen) Virtual EASE 2003/1 „Thickening agent“ Sterocoll is an acidic aqueous polymer dispersion containing polymer particles rich in caroxylic acid groups. It is used as thickening agent. First the polymer dispersion is diluted with water to lower the polymer content from 30 % to 5 %. It is still a white liquid having low viscosity. By addition of a small amount of an aqueous sodium hydroxide solution the pH is increased and the caroxylic acid groups are negatively charged. This makes the polymer particles soluble in water and a polymer solution is formed. At the same time the viscosity strongly increases due to the unfolding of the polymer molecules. At the end a clear gel is obtained. important application properties: viscosity viscosity-psd dilatancy (BASF AG, Ludwigshafen) „Dilatancy“ Dilatancy is a rheological phenomenon. -
Plasmofluidic Single-Molecule Surface-Enhanced Raman
ARTICLE Received 24 Feb 2014 | Accepted 9 Jun 2014 | Published 7 Jul 2014 DOI: 10.1038/ncomms5357 Plasmofluidic single-molecule surface-enhanced Raman scattering from dynamic assembly of plasmonic nanoparticles Partha Pratim Patra1, Rohit Chikkaraddy1, Ravi P.N. Tripathi1, Arindam Dasgupta1 & G.V. Pavan Kumar1 Single-molecule surface-enhanced Raman scattering (SM-SERS) is one of the vital applications of plasmonic nanoparticles. The SM-SERS sensitivity critically depends on plasmonic hot-spots created at the vicinity of such nanoparticles. In conventional fluid-phase SM-SERS experiments, plasmonic hot-spots are facilitated by chemical aggregation of nanoparticles. Such aggregation is usually irreversible, and hence, nanoparticles cannot be re-dispersed in the fluid for further use. Here, we show how to combine SM-SERS with plasmon polariton-assisted, reversible assembly of plasmonic nanoparticles at an unstructured metal–fluid interface. One of the unique features of our method is that we use a single evanescent-wave optical excitation for nanoparticle assembly, manipulation and SM-SERS measurements. Furthermore, by utilizing dual excitation of plasmons at metal–fluid interface, we create interacting assemblies of metal nanoparticles, which may be further harnessed in dynamic lithography of dispersed nanostructures. Our work will have implications in realizing optically addressable, plasmofluidic, single-molecule detection platforms. 1 Photonics and Optical Nanoscopy Laboratory, h-cross, Indian Institute of Science Education and Research, Pune 411008, India. Correspondence and requests for materials should be addressed to G.V.P.K. (email: [email protected]). NATURE COMMUNICATIONS | 5:4357 | DOI: 10.1038/ncomms5357 | www.nature.com/naturecommunications 1 & 2014 Macmillan Publishers Limited. All rights reserved. -
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. -
Generation and Stability of Size-Adjustable Bulk Nanobubbles
www.nature.com/scientificreports OPEN Generation and Stability of Size-Adjustable Bulk Nanobubbles Based on Periodic Pressure Received: 10 September 2018 Accepted: 18 December 2018 Change Published: xx xx xxxx Qiaozhi Wang, Hui Zhao, Na Qi, Yan Qin, Xuejie Zhang & Ying Li Recently, bulk nanobubbles have attracted intensive attention due to the unique physicochemical properties and important potential applications in various felds. In this study, periodic pressure change was introduced to generate bulk nanobubbles. N2 nanobubbles with bimodal distribution and excellent stabilization were fabricated in nitrogen-saturated water solution. O2 and CO2 nanobubbles have also been created using this method and both have good stability. The infuence of the action time of periodic pressure change on the generated N2 nanobubbles size was studied. It was interestingly found that, the size of the formed nanobubbles decreases with the increase of action time under constant frequency, which could be explained by the diference in the shrinkage and growth rate under diferent pressure conditions, thereby size-adjustable nanobubbles can be formed by regulating operating time. This study might provide valuable methodology for further investigations about properties and performances of bulk nanobubbles. Nanobubbles are gaseous domains which could be found at the solid/liquid interface or in solution, known as surface nanobubbles (SNBs)1,2 and bulk nanobubbles (BNBs)3, respectively. For BNBs, generally recognized as spherical bubbles with the diameter of less than 1μm surrounded by liquid, though it has been observed frstly in 19814, the existence of long-lived BNBs is still a controversial subject as it is contrary to the classical theory5,6. -
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. -
Initiator Systems Effect on Particle Coagulation and Particle Size Distribution in One-Step Emulsion Polymerization of Styrene
polymers Article Initiator Systems Effect on Particle Coagulation and Particle Size Distribution in One-Step Emulsion Polymerization of Styrene Baijun Liu 1, Yajun Wang 1, Mingyao Zhang 1,* and Huixuan Zhang 1,2 1 School of Chemical Engineering, Changchun University of Technology, Changchun 130012, China; [email protected] (B.L.); [email protected] (Y.W.); [email protected] (H.Z.) 2 Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, China * Correspondence: [email protected]; Tel.: +86-431-8571-6465 Academic Editor: Haruma Kawaguchi Received: 6 December 2015; Accepted: 15 February 2016; Published: 19 February 2016 Abstract: Particle coagulation is a facile approach to produce large-scale polymer latex particles. This approach has been widely used in academic and industrial research owing to its higher polymerization rate and one-step polymerization process. Our work was motivated to control the extent (or time) of particle coagulation. Depending on reaction parameters, particle coagulation is also able to produce narrowly dispersed latex particles. In this study, a series of experiments were performed to investigate the role of the initiator system in determining particle coagulation and particle size distribution. Under the optimal initiation conditions, such as cationic initiator systems or higher reaction temperature, the time of particle coagulation would be advanced to particle nucleation period, leading to the narrowly dispersed polymer latex particles. By using a combination of the Smoluchowski equation and the electrostatic stability theory, the relationship between the particle size distribution and particle coagulation was established: the earlier the particle coagulation, the narrower the particle size distribution, while the larger the extent of particle coagulation, the larger the average particle size. -
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................. -
Preparation of Ultra Fine Poly(Methyl Methacrylate) Microspheres in Methanol-Enriched Aqueous Medium
Macromolecular Research, Vol. 12, No. 2, pp 240-245 (2004) Preparation of Ultra Fine Poly(methyl methacrylate) Microspheres in Methanol-enriched Aqueous Medium Sang Eun Shim, Kijung Kim, Sejin Oh, and Soonja Choe* Department of Chemical Engineering, Inha University, Yonghyun 253, Namgu, Incheon 402-751, Korea Received March 17, 2004; Revised April 6, 2004 Abstract: Monodisperse PMMA microspheres are prepared by means of a simple soap-free emulsion polymerization in methanol-enriched aqueous medium in a single step process. The size and uniformity of the microspheres are dependent on the polymerization temperature. In a stable system, the uniformity is improved with the polymerization time. The most uniform and stable microspheres are obtained under mild agitation speed of 100 rpm at 70 oC. The monodisperse PMMA microspheres in the size range of 1.4-2.0 µm having less than 5% size variation are successfully achieved with varying concentrations of monomer and initiator. As the monomer and initiator concentrations increase, the larger microspheres with enhanced uniformity are obtained. However, the decreased amount of water induces the polydisperse PMMA particles due to the generation of secondary particles. Keywords: monodisperse microspheres, poly(methyl methacrylate), soap-free emulsion polymerization. Introduction micron-sized polymer colloids have been exploited and found that they allow to shift the stop-band in NIR and IR region.21 Since the seminal concept of the photonic band-gap In the synthesis of micron-sized polymer colloids via (PBG) crystals was proposed by Yablonovich1 and John,2 emulsion polymerization, several attempts have been made. explosive researches have been flushed in the fabrication Homola et al. -
Batch Emulsion Polymerization of Vinyl Chloride
Batch Emulsion Polymerization of Vinyl Chloride: Application of Experimental Design to Investigate the Effects of Operating Variables on Particle Size and Particle Size Distribution Mahdi Pourmehr, Amir H. Navarchian Department of Chemical Engineering, University of Isfahan, Isfahan, Iran Received 4 May 2008; accepted 7 July 2008 DOI 10.1002/app.29079 Published online 3 October 2008 in Wiley InterScience (www.interscience.wiley.com). ABSTRACT: In this article, the influences of operating effects in the range of levels investigated in this study. variables on the particle size (PS) and particle size distribu- Except initiator concentration, all factors have important tion (PSD) of emulsion poly(vinyl chloride) in batch reactor influence on the PSD (significance sequence: S > R > T > were investigated using Taguchi experimental design [E]). It is implied from the greater influence of agitation approach. The variables were temperature (T), water to speed relative to temperature on PSD that the shear coagula- monomer weight ratio (R), concentrations of initiator ([I]) tion predominates the Brownian coagulation in this system. and emulsifier ([E]), and agitation speed (S). Scanning elec- The relative optimum condition for a typical paste applica- tron microscope was used together with image analysis soft- tion was also determined using overall evaluation criteria. ware to determine the PS and PSD. Statistical analysis of VC 2008 Wiley Periodicals, Inc. J Appl Polym Sci 111: 338–347, 2009 results revealed that the PS of emulsion poly(vinyl chloride)