Rheological Evaluation of Gelatin-Xanthan Gum System With

Total Page:16

File Type:pdf, Size:1020Kb

Rheological Evaluation of Gelatin-Xanthan Gum System With Food Hydrocolloids 28 (2012) 141e150 Contents lists available at SciVerse ScienceDirect Food Hydrocolloids journal homepage: www.elsevier.com/locate/foodhyd Rheological evaluation of gelatinexanthan gum system with high levels of co-solutes in the rubber-to-glass transition region Filiz Altay a, Sundaram Gunasekaran b,* a Istanbul Technical University, Faculty of Chemical and Metallurgical, Department of Food Engineering, Maslak, Istanbul 34469, Turkey b University of WisconsineMadison, Department of Biological Systems Engineering, 460 Henry Mall, Madison, WI 53706, USA article info abstract Article history: Effects of moisture content, xanthan gum (XG) addition, and glucose syrup (GS):sucrose ratio on the Received 20 October 2011 gelation of gelatin-XG systems with high levels of co-solutes were investigated in the rubbery and the Accepted 8 December 2011 glass transition regions. Frequency sweep tests were performed between 0.1 and 100 rad and the storage (G0) and loss (G00) moduli of the system were measured in the temperature range of 60 to À15 C. The Keywords: onset of glass transition region increased with decreasing moisture content. The timeetemperature Gelatin superposition yielded master curves of G0 and G00 as a function of timescale of measurement. G00 and Xanthan gum 00 G were superimposed with the horizontal shift factor aT, which was temperature dependent according Tg e e WLF equation to the Williams Landel Ferry (WLF) equation. Glass transition temperature (Tg) of the samples were Free volume determined by dynamic mechanical analysis (DMA) from the peak of tan d. Tg decreased with XG addition. The energy of vitrification of samples with XG increased compared to samples containing only gelatin. Relaxation spectra of the samples were calculated from rheological measurements using the first and second approximations. The Rouse theory was more closely followed with the second approximation. Ó 2011 Elsevier Ltd. All rights reserved. 1. Introduction constructing master curves of mechanical spectra, spanning many decades of frequency. Isothermal data obtained by frequency Dynamic mechanical measurements are widely used to probe sweeps at different temperatures are shifted along the frequency structureeproperty relationships in amorphous synthetic polymers axis and overlaid to obtain a master curve at an arbitrarily chosen during vitrification. The synthetic polymer approach, in which the reference temperature. TTS can express the effects of time and idea of molecular mobility governing the kinetics of phase/state temperature on viscoelastic properties separately by enlarging the transitions and chemical reactions is applied, has been extended to effective time or frequency scale available for experimental food biopolymers (Kasapis, Al-Marhoob, & Deszczynski, Mitchell, & measurements. The superposition of curves from frequency sweeps Abeysekara, 2003; Kasapis, Al-Marhoobi, & Sworn, 2001; Levine & at constant temperature intervals yields the shift factor (aT), which Slade, 1988). This approach has been applied extensively together indicates how much the time scale of measurement shifts with with free volume theory to high-concentration mixtures of sugars temperature (Ferry, 1980). The underlying basis of TTS is the and biopolymers (Deszczynski, Kasapis, MacNaughton, & Mitchell, equivalence between time (or frequency) and temperature as they 2003; Kasapis, Al-Marhoobi, & Giannouli, 1999; Kasapis, Des- affect molecular processes that influence the viscoelastic behavior brieres, Al-Marhoobi, & Rinaudo, 2002; Kasapis et al., 2001; Kasapis of polymeric materials and glass-forming small molecules (Slade & & Sworn, 2000) and it has been reported that small addition of Levine, 1993). The criteria for the applicability of TTS are as follows polysaccharides to sugar-containing systems accelerate their vitri- (Ferry, Fitzgerald, Johnson, & Grandine, 1951): (a) shapes of adja- fication (Kasapis et al., 2001). cent curves should match exactly, (b) the same values of aT must The synthetic polymer approach includes the application of the superpose all the viscoelastic functions, and (c) the temperature principle of timeetemperature superposition (TTS), which is also dependence of aT must have a reasonable form consistent with known as the method of reduced variables. TTS has been used for experience. For the last criterion, Williams, Landel, and Ferry (1955) proposed an empirical relationship known as the Williams-Landel- Ferry (WLF) equation. * Corresponding author. Tel.: þ1 608 262 1019; fax: þ1 608 262 1228. The glass transition is relevant to the behavior of food materials E-mail address: [email protected] (S. Gunasekaran). for several reasons. For both polymers and low molecular weight 0268-005X/$ e see front matter Ó 2011 Elsevier Ltd. All rights reserved. doi:10.1016/j.foodhyd.2011.12.007 142 F. Altay, S. Gunasekaran / Food Hydrocolloids 28 (2012) 141e150 glasses, there is a large change in material properties while going 2. Materials and methods through the glass transition. Functional behavior of the material is affected by the dramatic slowing of diffusive processes as a material 2.1. Materials is cooled towards Tg. This slowing will affect stability to crystalli- zation and time-dependent processes associated with crystalliza- Pigskin gelatin (Type B) and laboratory grade sucrose were tion, drying/rehydration and spoilage, when the rate-limiting step purchased from EM Science and Fischer Chemicals, respectively. is the rate of diffusion encountered between substrates or enzyme Glucose syrup, with dextrose equivalent of 43.4 and total solids of and substrate (Noel, Ring, & Whittam, 1993). In addition, it has been 80.5%, was obtained from Cargill, IA, USA (lot number C007138). presumed that at temperatures below Tg amorphous sugars in foods The water content of GS was taken into account in calculating the are stable. Food products are subject to changes in moisture content sample composition. Food-grade XG (lot number 3D0724A) was and temperature during processing and storage, both of which obtained from CP Kelco U.S. Inc., Chicago, IL, USA. decrease stability of amorphous compounds in their rubbery state by increasing temperature difference (T À T )(Roos & Karel, 1993). g 2.2. Sample preparation A glass forms when a typical liquid, a state with a disordered molecular structure, is cooled to a temperature generally w100 C Several gelatin-XG systems were prepared. For each, the below its equilibrium crystalline melting temperature (T )or m required amount of gelatin and XG were dissolved separately in freezing point, at a cooling rate sufficiently high to avoid crystalli- deionized water to prepare 10% solution at 75 C and 600 rpm for zation of the liquid. This solidification process, known as vitrifica- 20 min and 4% solution at 60 C and 425 rpm for 2 h, respectively. tion, results in immobilization of the disordered structure of the The required amount of sucrose was mixed with 1/3 part of water in liquid such that the resulting glassy solid is spatially homogeneous, a temperature-controlled kettle. Then GS, gelatin, and XG solution but without any long-range lattice order, and is incapable of were added into the sucrose solution. The mixture was stirred at exhibiting any long-range, cooperative relaxation behavior (e.g., about 90 C for 30e60 min depending on the desired level of total translational mobility) on a practical time scale. The most impor- solids, which was checked by a refractometer (Atago N-3E, Japan). tant distinction between dimensionally extended (a) relaxations, Total solids content of the gels, which were cured overnight in which give rise to the glass transition as translational motions a refrigerator at 0 C, were determined using the AOAC method become restricted at T , and small-scale (b and g) relaxations, for g (AOAC, 1990); the moisture contents were calculated by subtracting which small-scale rotational motions do not become restricted as T total solids content from one hundred. The compositions of all falls below T , is the cooperative nature of a relaxations (Slade & g samples tested are presented in Table 1. Levine, 1993). The gelatin-XG systems were investigated at two moisture Fitting the master curves to WLF equation enables predicting contents (20 and 25%), three gelatin:XG ratios (5:0, 9:1, and 4:1) the T . It has been proposed that the rheological T is a point g g and three GS:sucrose ratios (<1, 1 and >1) at each moisture between the T region and the glassy state. The T can signify the g g content. For each sample, two batches were prepared and tested. transformation from free-volume phenomena of the polymeric backbone in the Tg region to an energetic barrier to motions in the glassy state involving stretching and bending of chemical bonds 2.3. Rheological measurements (Kasapis et al., 2001). Free volume can be defined as holes of the order of molecular (monomeric) dimensions or smaller voids 2.3.1. SAOS associated with packing irregularities. Many properties of liquids, The small amplitude oscillatory shear (SAOS) technique was whether polymeric or not, can be attributed to the presence of used to determine the dependence of viscoelastic behavior on a substantial proportion of free volume. The thermal expansion temperature and time. Freshly prepared samples were loaded onto coefficient of liquids represents the creation of additional free a controlled-stress dynamic rheometer (Bohlin CVOR, Malvern Inc., volume with rising temperature. At high temperatures, where local Southampton, MA) equipped
Recommended publications
  • Predicting Polymers' Glass Transition Temperature by a Chemical
    polymers Article Predicting Polymers’ Glass Transition Temperature by a Chemical Language Processing Model Guang Chen 1 , Lei Tao 1 and Ying Li 1,2,* 1 Department of Mechanical Engineering, University of Connecticut, Storrs, CT 06269, USA; [email protected] (G.C.); [email protected] (L.T.) 2 Polymer Program, Institute of Materials Science, University of Connecticut, Storrs, CT 06269, USA * Correspondence: [email protected] Abstract: We propose a chemical language processing model to predict polymers’ glass transition temperature (Tg) through a polymer language (SMILES, Simplified Molecular Input Line Entry System) embedding and recurrent neural network. This model only receives the SMILES strings of a polymer’s repeat units as inputs and considers the SMILES strings as sequential data at the character level. Using this method, there is no need to calculate any additional molecular descriptors or fingerprints of polymers, and thereby, being very computationally efficient. More importantly, it avoids the difficulties to generate molecular descriptors for repeat units containing polymerization point ‘*’. Results show that the trained model demonstrates reasonable prediction performance on unseen polymer’s Tg. Besides, this model is further applied for high-throughput screening on an unlabeled polymer database to identify high-temperature polymers that are desired for applications in extreme environments. Our work demonstrates that the SMILES strings of polymer repeat units can be used as an effective feature representation to develop a chemical language processing model for predictions of polymer Tg. The framework of this model is general and can be used to construct structure–property relationships for other polymer properties. Citation: Chen, G.; Tao, L.; Li, Y.
    [Show full text]
  • Colorless and Transparent High – Temperature-Resistant Polymer Optical Films – Current Status and Potential Applications in Optoelectronic Fabrications
    Chapter 3 Colorless and Transparent high – Temperature-Resistant Polymer Optical Films – Current Status and Potential Applications in Optoelectronic Fabrications Jin-gang Liu, Hong-jiang Ni, Zhen-he Wang, Shi-yong Yang and Wei-feng Zhou Additional information is available at the end of the chapter http://dx.doi.org/10.5772/60432 Abstract Recent research and development of colorless and transparent high-temperature- resistant polymer optical films (CHTPFs) have been reviewed. CHTPF films possess the merits of both common polymer optical film and aromatic high-temperature- resistant polymer films and thus have been widely investigated as components for microelectronic and optoelectronic fabrications. The current paper reviews the latest research and development for CHTPF films, including their synthesis chemistry, manufacturing process, and engineering applications. Especially, this review focuses on the applications of CHTPF films as flexible substrates for optoelectrical devices, such as flexible active matrix organic light-emitting display devices (AMOLEDs), flexible printing circuit boards (FPCBs), and flexible solar cells. Keywords: colorless polymer films, high temperature, synthesis, flexible substrates 1. Introduction Various polymer optical films have been widely applied in the fabrication of optoelectronic devices [1]. Recently, with the ever-increasing demands of high reliability, high integration, high wiring density, and high signal transmission speed for optoelectronic fabrications, the service temperatures of polymer optical films have dramatically increased [2, 3]. For instance, © 2015 The Author(s). Licensee InTech. This chapter is distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/3.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
    [Show full text]
  • 3 About the Nature of the Structural Glass Transition: an Experimental Approach
    3 About the Nature of the Structural Glass Transition: An Experimental Approach J. K. Kr¨uger1,2, P. Alnot1,3, J. Baller1,2, R. Bactavatchalou1,2,3,4, S. Dorosz1,3, M. Henkel1,3, M. Kolle1,4,S.P.Kr¨uger1,3,U.M¨uller1,2,4, M. Philipp1,2,4,W.Possart1,5, R. Sanctuary1,2, Ch. Vergnat1,4 1 Laboratoire Europ´een de Recherche, Universitaire Sarre-Lorraine-(Luxembourg) [email protected] 2 Universit´edu Luxembourg, Laboratoire de Physique des Mat´eriaux,162a, avenue de la Fa¨ıencerie, L-1511 Luxembourg, Luxembourg 3 Universit´eHenriPoincar´e, Nancy 1, Boulevard des Aiguillettes, Nancy, France 4 Universit¨atdes Saarlandes, Experimentalphysik, POB 151150, D-66041 Saarbr¨ucken, Germany 5 Universit¨at des Saarlandes, Werkstoffwissenschaften, POB 151150, D-66041 Saarbr¨ucken, Germany Abstract. The nature of the glassy state and of the glass transition of structural glasses is still a matter of debate. This debate stems predominantly from the kinetic features of the thermal glass transition. However the glass transition has at least two faces: the kinetic one which becomes apparent in the regime of low relaxation frequencies and a static one observed in static or frequency-clamped linear and non-linear susceptibilities. New results concerning the so-called α-relaxation process show that the historical view of an unavoidable cross-over of this relaxation time with the experimental time scale is probably wrong and support instead the existence of an intrinsic glass transition. In order to prove this, three different experimental strategies have been applied: studying the glass transition at extremely long time scales, the investigation of properties which are not sensitive to the kinetics of the glass transition and studying glass transitions which do not depend at all on a forced external time scale.
    [Show full text]
  • Lecture #16 Glass-Ceramics: Nature, Properties and Processing Edgar Dutra Zanotto Federal University of São Carlos, Brazil [email protected] Spring 2015
    Glass Processing Lecture #16 Glass-ceramics: Nature, properties and processing Edgar Dutra Zanotto Federal University of São Carlos, Brazil [email protected] Spring 2015 Lectures available at: www.lehigh.edu/imi Sponsored by US National Science Foundation (DMR-0844014) 1 Glass-ceramics: nature, applications and processing (2.5 h) 1- High temperature reactions, melting, homogeneization and fining 2- Glass forming: previous lectures 3- Glass-ceramics: definition & applications (March 19) Today, March 24: 4- Composition and properties - examples 5- Thermal treatments – Sintering (of glass powder compactd) or -Controlled nucleation and growth in the glass bulk 6- Micro and nano structure development April 16 7- Sophisticated processing techniques 8- GC types and applications 9- Concluding remmarks 2 Review of Lecture 15 Glass-ceramics -Definition -History -Nature, main characteristics -Statistics on papers / patents - Properties, thermal treatments micro/ nanostructure design 3 Reading assignments E. D. Zanotto – Am. Ceram. Soc. Bull., October 2010 Zanotto 4 The discovery of GC Natural glass-ceramics, such as some types of obsidian “always” existed. René F. Réaumur – 1739 “porcelain” experiments… In 1953, Stanley D. Stookey, then a young researcher at Corning Glass Works, USA, made a serendipitous discovery ...… 5 <rms> 1nm Zanotto 6 Transparent GC for domestic uses Zanotto 7 Company Products Crystal type Applications Photosensitive and etched patterned Foturan® Lithium-silicate materials SCHOTT, Zerodur® β-quartz ss Telescope mirrors Germany
    [Show full text]
  • Movement Between Bonded Optics
    MOVEMENT BETWEEN BONDED OPTICS Andrew Bachmann, Dr. John Arnold and Nicole Langer DYMAX Corporation, September 13, 2001 INTRODUCTION Controlling the movement of bonded optical parts depends, in large measure, on the properties of the adhesives used. Common issues include both shrinkage during cure and expansion during thermal excursions. Designers have historically had to limit their designs to optics whose thermal range fell below the then-available “high” glass transition temperature (Tg) epoxies; i.e., operating below the adhesive’s Tg. However, many of today’s optical devices employ even higher operating temperatures and require greater resistance to environmental conditions. The common minus 50ºC to plus 200ºC microelectronic test operating range challenges even classical “High Tg” optical epoxies. The NO SHRINK™ family of Optical Positioning adhesives features low total movement between bonded parts either on cure or when the optical device is thermally cycled. NO SHRINK™ products are based on novel, patent- applied-for technology. This technology was incorporated into light curing urethane-acrylics to create products with thermal characteristics that are different from those of older technology adhesives. Table 1. Dimensional changes (measured at 25ºC) Adhesive OP-60-LS Adhesive OP-64-LS < 0.1% (during UV Cure) < 0.1% (during UV Cure) < 0.1% (after 24 hr, 120°C) < 0.1% (after 24 hr, 120°C) Tg ~ 50ºC Tg ~ 125ºC “Rules of thumb” for comparing epoxy resins are not accurate for comparing other resins or other resins with epoxies. Novel NO SHRINK™ UV and visible light curing adhesives exhibit less total movement over a temperature range regardless of the Tg.
    [Show full text]
  • Effect of Cladding Layer Glass Transition Temperature on Thermal Resistance of Graded-Index Plastic Optical fibers
    Polymer Journal (2014) 46, 823–826 & 2014 The Society of Polymer Science, Japan (SPSJ) All rights reserved 0032-3896/14 www.nature.com/pj NOTE Effect of cladding layer glass transition temperature on thermal resistance of graded-index plastic optical fibers Hirotsugu Yoshida1, Ryosuke Nakao1, Yuki Masabe1, Kotaro Koike2 and Yasuhiro Koike2 Polymer Journal (2014) 46, 823–826; doi:10.1038/pj.2014.75; published online 27 August 2014 INTRODUCTION maleimide (cHMI) doped with diphenyl sulfide, and the cladding and Graded-index plastic optical fibers (GI POFs)1 are a highly over-cladding polymers were poly(methyl mathacrylate) and competitive transmission medium for short-range communications poly(carbonate), respectively. In this study, we used two types of such as local area networks and interconnections. Because GI POFs commercial poly(methyl mathacrylate) resins with different Tg values have a parabolic refractive index profile in the core region, modal and compared the long-term thermal reliability of the GI POFs in dispersion is minimized and high-speed data transmission of over a terms of fiber attenuation. gigabit per second is possible. Currently, most suppliers produce GI 2 POFs via coextrusion and a dopant diffusion method; the core EXPERIMENTAL PROCEDURE polymer, which contains a diffusible dopant that has a higher Materials refractive index than that of the base polymer, and the cladding TClEMA and cHMI were purchased from Osaka Organic Chemical Industry polymer are concentrically extruded. The core and cladding (Osaka, Japan) and Nippon Shokubai (Osaka, Japan), respectively. Diphenyl polymers flow together into a diffusion zone, and the dopant from sulfide and lauryl mercaptan were purchased from Sigma-Aldrich Japan the core layer diffuses toward the cladding layer, forming the (Tokyo, Japan), and di-tert-hexyl peroxide was purchased from NOF Corpora- GI profile.
    [Show full text]
  • Crystalline Phase Characterization of Glass-Ceramic Glazes M.G
    CORE Metadata, citation and similar papers at core.ac.uk Provided by Estudo Geral Ceramics International 33 (2007) 345–354 www.elsevier.com/locate/ceramint Crystalline phase characterization of glass-ceramic glazes M.G. Rasteiro a,*, Tiago Gassman b, R. Santos c, E. Antunes a a Chemical Engineering Department, Coimbra University, Po´lo II, Pinhal de Marrocos, 3030-290 Coimbra, Portugal b Colorobbia Portugal, Anadia, Portugal c Centro Tecnolo´gico da Ceraˆmica e do Vidro, Coimbra, Portugal Received 6 May 2005; received in revised form 2 September 2005; accepted 3 October 2005 Available online 18 January 2006 Abstract The firing process of five raw crystalline frits was investigated by means of DTA, XRD, heating microscopy and dilatometry. The chemical composition of the frits was determined by FAAS, to define the main glass-ceramic system of each frit. The final crystalline structure detected for the sintered frits conformed to the temperatures for which transformations were obtained during heating. The existence of a relationship between the crystallization process and sintering behaviour was confirmed. During devitrification, the sintering process stops, confirming that crystalline formation affects the sintering behaviour of the frits. In this case, the thermal properties of the final product are not only dependent on oxide composition but also on the crystalline phases. It was established that the addition of adequate compounds could induce the formation of crystalline phases on some glass-ceramic frits. # 2005 Elsevier Ltd and Techna Group S.r.l. All rights reserved. Keywords: A. Sintering; D. Glass-ceramics; D. Glass; Crystallization 1. Introduction Glazes are commonly applied on surfaces as aqueous suspensions of frits and other additives, also called enamels [2].
    [Show full text]
  • Makrolon Product Range Typical Values 2 ® Important Economic Regionsimportant Are the World
    ® Product range Typical values Makrolon ® Makrolon® is the brand name of our polycarbonate, which we produce in all the major economic regions of the world. For Makrolon®, the most important economic regions are Asia­Pacific (APAC), Europe, Middle East, Africa and Latin America (EMEA/LA), and North America and Mexico (NAFTA). Makrolon 2 Characterization Compared with other thermoplastics, the amor- dimensional stability coupled with a high creep phous material Makrolon® has a very unique modulus and good electrical insulation properties. property profile. It is noted above all for its high Glass fiber reinforced Makrolon® has particularly transparency, heat resistance, toughness and high stiffness and outstanding dimensional stability. Makrolon® is available in: Grades for special applications Optical storage media General purpose grades Optical lenses Food contact grades Light guides Impact modified grades Lighting Flame retardant grades Automotive lighting Glass fiber reinforced (milled fiber) grades Automotive glazing Blow molding Glass fiber reinforced (normal fiber) grades Furniture Extrusion Structural foam Medical devices Nomenclature ..06 So-called “food contact“ grades that The non-reinforced, general purpose and food comply with the regulations of the EU and contact grades of Makrolon® are available in its member states with regard to plastics different viscosity classes. The first two digits in contact with foodstuffs, conform to the in the type designation usually characterize the relevant FDA regulations and also meet the
    [Show full text]
  • A Review of Liquid-Glass Transitions
    A Review of Liquid-Glass Transitions Anne C. Hanna∗ December 14, 2006 Abstract Supercooling of almost any liquid can induce a transition to an amorphous solid phase. This does not appear to be a phase transition in the usual sense — it does not involved sharp discontinuities in any system parameters and does not occur at a well-defined temperature — instead, it is due to a rapid increase in the relaxation time of the material, which prevents it from reaching equilibrium on timescales accessible to experimentation. I will examine various models of this transition, including elastic, mode-coupling, and frustration-based explanations, and discuss some of the problems and apparent paradoxes found in these models. ∗University of Illinois at Urbana-Champaign, Department of Physics, email: [email protected] 1 Introduction While silicate glasses have been a part of human technology for millenia, it has only been known since the 1920s that any supercooled liquid can in fact be caused to enter an amor- phous solid “glass” phase by further reduction of its temperature. In addition to silicates, materials ranging from metallic alloys to organic liquids and salt solutions, and having widely varying types of intramolecular interactions, can also be good glass-formers. Also, the glass transition can be characterized in terms of a small dimensionless parameter which is different on either side of the transition: γ = Dρ/η, where D is the molecular diffusion constant, ρ is the liquid density, and η is the viscosity. This all seems to suggest that there may be some universal aspect to the glass transition which does not depend on the specific microscopic properties of the material in question, and a significant amount of research has been done to determine what an appropriate universal model might be.
    [Show full text]
  • An Experimental Investigation of Glass Transition Temperature of Composite Materials Using Bending Test
    Journal of Energy and Power Engineering 10 (2016) 39-44 doi: 10.17265/1934-8975/2016.01.005 D DAVID PUBLISHING An Experimental Investigation of Glass Transition Temperature of Composite Materials Using Bending Test Noori Hassoon Mohammed Al-Saadi1 and Ammar Fadhil Hussein Al-Maliki2 1. Building and Construction Engineering Department, Dijlah University College, Baghdad 10001, Iraq 2. Mechanical Engineering Department, Al-Mustansiriyah University, Baghdad 10001, Iraq Received: October 29, 2015 / Accepted: November 27, 2015 / Published: January 31, 2016. Abstract: In this study, the bending test is used to investigate the glass transition temperature for epoxy reinforced with three types of fibers, fiberglass, Kevlar and synthetic wool, these materials have a wide used in many application which they are used composite materials. The glass transition temperature can be measured at the point of inflection for the curve of variation of the deflection and temperature. The results show that, the glass transition temperature is affected by the type of the reinforcement of the composites. On the other hand, the glass transition temperature of the wool composite is higher than the other. Key words: Glass transition, composite materials, bending test. 1. Introduction transition temperature (Tg), but since the transition often occurs over a broad temperature range, the use of The glass transition of a polymer matrix composite is a single temperature to characterize it may give rise to a temperature-induced change in the matrix material some confusion. The experimental technique used to from the glassy to the rubbery state during heating or obtain the T must be described in detail, especially from a rubber to a glass during cooling.
    [Show full text]
  • Effect of Glass Transition Temperature of Polymeric Binders on Properties Ceramic Materials
    Journal of Thermal Analysis and Calorimetry, Vol. 77 (2004) 319–327 EFFECT OF GLASS TRANSITION TEMPERATURE OF POLYMERIC BINDERS ON PROPERTIES CERAMIC MATERIALS M. Szafran, P. Wiíniewski* and G. Rokicki Faculty of Chemistry, Warsaw University of Technology, ul. Noakowskiego 3, 00-664 Warsaw, Poland Abstract In the paper are presented the studies of the effect of glass transition temperature of new water- thinnable polymeric binders on the properties of ceramic materials obtained by die pressing. The pa- rameters of ceramic samples comprising polymeric binders have been compared with those of sam- ples comprising poly(vinyl alcohol) (PVA) – water-soluble binder. When using poly(acrylic- styrene) (AS), poly(acrylic-allyl) (AA) and poly(vinyl-allyl) (VA) water-thinnable binders, materi- als of greater density and mechanical strength were obtained in the green state as well as after sintering than those in the case of using PVA. The dependence of the chemical structure of the bind- ers applied on the properties of samples such as the glass transition temperature and hydropho- bic–hydrophilic balance of the copolymers has been discussed. Keywords: alumina, die pressing, DSC, glass transition temperature, polymeric dispersions, PVA, Weibull modulus Introduction In modern ceramics, different polymeric binders of various chemical structure are ap- plied for different molding methods. A narrow range of water-soluble organic bind- ers, such as poly(vinyl alcohol) and poly(oxyethylene) glycol, are most often used in the molding process. The samples obtained with the binders mentioned are character- ized by a relatively small density (<63% of theoretical value) and small mechanical strength before and after sintering [1–3].
    [Show full text]
  • Advanced Vitreous State: the Structure of Glass
    Advanced Vitreous State: The Structure of Glass Section 1: Lecture 1 - Fundamentals of the Glass Transition: The Glass Transition is a Kinetic Transition with Thermodynamic Signatures • Examine the differences between a kinetic and thermodynamic transition • Develop the affect of the “internal” and “external” timescales and how each can lead to glass formation • Investigate the affect of cooling rate on the volume of glass • Recognize the origin of the hysteresis affect in the glass transition • Distinguish the “Thermodynamic Signatures” of the glass transition • The Enthalpy and heat capacity functions in the glass transition region • The Entropy function in the glass transition region Fundamentals of the Glass Transition The Glass Transition is a Kinetic Transition Continuous changes in structure and properties Between the liquid and solid (glassy) states As the liquid is (typically) cooled Structure and properties are continuous with temperature Structures and properties can be changed continuously by changing the kinetics of the cooled or reheated liquid There is no “Thermodynamic driving force” for the glass transition The glass transition occurs simply because of a dramatically diverging difference between timescales internal and external to the cooling liquid Advance Vitreous State: The Structure of Glass Section 1: Lecture 1 - Fundamentals of the Glassy State SWMartin 2 Fundamentals of the Glass Transition Melting and Crystallization are: Thermodynamic Transitions Discontinuous changes in structure and properties at
    [Show full text]