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Journal articles on the topic 'Glassy state'

Author: Grafiati

Published: 4 June 2021

Last updated: 25 July 2025

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1

Huang, Dong Ya, Xiang Jin Zhao, Tao Zhang, and Vincent Ji. "Air Oxidation Kinetics Study of Zr₅₈Nb₃Cu₁₆Ni₁₃Al₁₀ Bulk Metallic Glass." Defect and Diffusion Forum 283-286 (March 2009): 209–13. http://dx.doi.org/10.4028/www.scientific.net/ddf.283-286.209.

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The isothermal oxidation behavior of Zr58Nb3Cu16Ni13Al10 bulk metallic glass (BMG) under dry air in the glassy state and the supercooled liquid state (SLS) was studied by the thermogravimetric method. The oxidation rate and thickness growth speed in the SLS were both hugely higher than in the glassy state. The oxidation kinetics of BMG in both states for 1.5 hours was different, the parabolic law was followed in the glassy state at 300°C and 350°C, contrarily the linear law was followed in SLS at 400 °C. After the oxidation for 126 hours in SLS, the oxidation kinetics possessed two stages, the

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2

Huang, Dong Ya, Bin Wang, Vincent Ji, and Tao Zhang. "Initial Oxidation Behavior of Zr₅₅Cu₃₀Al₁₀Ni₅ Bulk Metallic Glass in Short-Term Stage." Materials Science Forum 675-677 (February 2011): 209–12. http://dx.doi.org/10.4028/www.scientific.net/msf.675-677.209.

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The isothermal initial oxidation kinetics of Zr55Cu30Al10Ni5 bulk metallic glass in glassy state (lower than Tg = 685K) and in surpercooled liquid state (Tg = 685 K < T < Tx=774 K) is investigated under dry air by thermogravimetric method in short-term stage (for 1.5 hours). A protective parabolic law is followed in glassy state, except at 573 K where a linear law is followed. The self-limiting oxidation kinetics evolves from a short linear stage to a steady mild growth stage in supercooled liquid state at 723 K, which is induced mainly by crystallization and by the fast growth of dense

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3

El-Eskandarany, M. Sherif, Satoru Ishihara, and A. Inoue. "Mechanism of solid-state reaction for fabrication of new glassy V45Zr22Ni22Cu11 alloy powders and subsequent consolidation." Journal of Materials Research 18, no. 10 (2003): 2435–45. http://dx.doi.org/10.1557/jmr.2003.0339.

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A single glassy phase of V45Zr22Ni22Cu11 alloy powders was synthesized by milling the elemental alloying powders in an argon atmosphere using a low-energy ball-milling technique. During the early and intermediate stages of milling, the atoms of Zr, Ni, and Cu migrated and diffused into the V (base material) lattice to form a body-centered-cubic (bcc) solid-solution, which transformed into a glassy phase with the same composition upon annealing at 850 K for 300 s in an argon atmosphere differential scanning calorimeter (thermally-enhanced glass formation reaction). As the milling time increased

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4

Leopold, A. Carl, Wendell Q. Sun, and Irma Bernal-Lugo. "The glassy state in seeds: analysis and function." Seed Science Research 4, no. 3 (1994): 267–74. http://dx.doi.org/10.1017/s0960258500002294.

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AbstractIn view of the finding that dry seeds may exist in the glassy state, a brief review of the commonest methods of detection and quantification of the glass transition is presented. While the glassy state may contribute to seed tolerance of desiccation, it does not appear to account for desiccation tolerance. Its major function in dry seeds may be its contribution to the stability of the seed components during storage.

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5

El-Eskandarany, M. Sherif, M. Omori, and A. Inoue. "Solid-state synthesis of new glassy Co65Ti20W15 alloy powders and subsequent densification into a fully dense bulk glass." Journal of Materials Research 20, no. 10 (2005): 2845–53. http://dx.doi.org/10.1557/jmr.2005.0344.

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The mechanical alloying method was used to synthesize a single glassy phase of Co65Ti20W15 alloy powders, using a high-energy ball mill. The glass transition temperature of the end-product, which was obtained after 173 ks of milling time, lies at 786 K, whereas the crystallization takes place at 878 K through a single sharp exothermic peak with an enthalpy change of crystallization of −4.37 kJ/mol. The reduced glass transition temperature was found to be 0.51. This glassy alloy powders exhibit a very large supercooled liquid region (92 K) for a ternary metallic system. The spark plasma sinteri

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6

Luque, Patricia, and Antonio Heredia. "Glassy State in Plant Cuticles during Growth." Zeitschrift für Naturforschung C 49, no. 3-4 (1994): 273–75. http://dx.doi.org/10.1515/znc-1994-3-419.

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The existence of a glassy state in isolated tomato fruit cuticles was investigated using differential scanning calorimetry. Tomato fruit cuticular membranes showed a glass transition temperature at -30 °C and an additional second order transition temperature near 30 °C. Changes in these temperatures during fruit growth were also studied

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7

El-Eskandarany, M. Sherif, Wei Zhang, and A. Inoue. "Mechanically induced solid-state reaction for synthesizing glassy Co75Ti25 soft magnet alloy powders with a wide supercooled liquid region." Journal of Materials Research 17, no. 9 (2002): 2447–56. http://dx.doi.org/10.1557/jmr.2002.0357.

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A single phase of glassy Co75Ti25 alloy powders was synthesized by high-energy ball milling the elemental powders at room temperature, using the mechanical alloying method. The final product of the glassy alloy, which is obtained after ball milling for 86 ks, exhibits soft magnetic properties with polarization and coercivity values of 0.67 T and 2.98 kA/m, respectively. This binary glassy alloy, in which its glass transition temperature (Tg) lies at a rather high temperature (833 K), transforms into face-centered-cubic Co3Ti (ordered phase) at 889 K through a single sharp exothermic reaction w

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8

Kvashnin, Vyacheslav I., Dina V. Dudina, Arina V. Ukhina, Guilherme Yuuki Koga, and Konstantinos Georgarakis. "The Benefit of the Glassy State of Reinforcing Particles for the Densification of Aluminum Matrix Composites." Journal of Composites Science 6, no. 5 (2022): 135. http://dx.doi.org/10.3390/jcs6050135.

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In metallic glass-reinforced metal matrix composites, the glassy phase can serve a dual purpose: (i) it can behave as soft binder and porosity remover during consolidation; and (ii) it can act as the hard reinforcing phase after densification. The present work aimed to demonstrate the benefit of the glassy reinforcing particles for the densification of aluminum matrix composites. The consolidation behavior of Al–50 vol.% Fe-based alloy mixtures prepared using a glassy Fe66Cr10Nb5B19 alloy powder (Tg = 521 °C, Tx = 573 °C) or a crystalline Fe62Cr10Nb12B16 alloy powder was studied under spark pl

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9

Panayiotou, Costas. "Thermodynamics of the Glassy Polymer State: Equilibrium and Non-Equilibrium Aspects." Polymers 16, no. 2 (2024): 298. http://dx.doi.org/10.3390/polym16020298.

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This work examines, first, the non-equilibrium character of the glassy state of polymer systems and its significance in the development of novel materials for important technological applications. Subsequently, it summarizes the essentials of the generalized lattice fluid approach for the description of this highly complex non-equilibrium behavior with an approximate and simple, yet analytically powerful formalism. The working equations are derived in a straightforward and consistent manner by clearly defining the universal and specific variables needed to describe the discussed properties. Th

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10

Bernal-Lugo, I., and A. C. Leopold. "Seed stability during storage: Raffinose content and seed glassy state." Seed Science Research 5, no. 2 (1995): 75–80. http://dx.doi.org/10.1017/s0960258500002646.

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AbstractIt has been proposed that sucrose and raffinose play a role in the storability of maize seeds. The levels of these sugars in the embryos and the glassy state were compared in maize seeds of contrasting storage stability to determine the relationship between sugar composition, glassy state and the storability of the seed. Sucrose was the predominant sugar but its content was not correlated with good storage. The content of raffinose as a mass fraction of total sugars and the magnitude of the glassy state showed positive correlations with storage stability. It is suggested that in maize

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11

SURYANARAYANA, C., and SATYAJEET SHARMA. "GLASS FORMATION IN MECHANICALLY ALLOYED Fe-BASED SYSTEMS." Functional Materials Letters 02, no. 04 (2009): 147–55. http://dx.doi.org/10.1142/s1793604709000727.

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Rapid solidification processing of metallic melts has been traditionally employed to synthesize metallic glasses in several alloy systems. However, in recent years, solid-state processing methods, and more specifically, mechanical alloying, have become popular methods to synthesize glassy phases in metallic alloy systems. Although a large number of criteria have been developed to identify alloy compositions that can be solidified into the glassy state, very few attempts have been made to predict the glass-forming ability by solid-state processing methods. To evaluate if some clear criteria cou

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12

Gugov, Ivailo B. "The glass, the glassy state and the Alice number." Thermochimica Acta 280-281 (July 1996): 15–23. http://dx.doi.org/10.1016/0040-6031(95)02633-9.

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13

Wang, Yu, Xiao Bing Ren, and Kazuhiro Otsuka. "Strain Glass: Glassy Martensite." Materials Science Forum 583 (May 2008): 67–84. http://dx.doi.org/10.4028/www.scientific.net/msf.583.67.

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“Glass”, a frozen disordered-state, has been found in areas as diverse as amorphous solids, magnetic alloys, ferroelectrics, superconductors, and even in models of biological evolutions. In the present review we introduce a new class of glass–the “strain-glass”, which was discovered very recently. Strain glass is derived from a martensitic system, where the local-strain is frozen in disordered configuration. The first example of strain glass was found in the well-studied Ni-rich Ti50-xNi50+x martensitic system in its “non-transforming” composition regime (x>1.5). Contrasting to the familiar

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14

Muraishi, Shinji, Hirono Naito, Jhi Shi, Yoshio Nakamura, and Tatsuhiko Aizawa. "Controlled Elasticity in Nano-Structured Metallic Glass by Ion Implantation Method." Materials Science Forum 561-565 (October 2007): 1315–18. http://dx.doi.org/10.4028/www.scientific.net/msf.561-565.1315.

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Different reactivity of ions has been implanted into Zr-Cu metallic glass to obtain nano-structured surface with controlled elasticity. The penetration of glass forming element of Ni+ into crystalline Zr-Cu stabilizes glassy phase to induce crystalline-amorphous (c-a) transition during implantation process. In the meanwhile, penetration of N+ into glassy matrix induces precipitation of (Zr, Cu)N at the mean penetration depth of N. Critical N concentration for nitride formation is estimated to be (Zr,Cu)-20at%N, which also suggests existing of N solid solution of glassy phase. Inert element of

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15

Boucher, Virginie M., Daniele Cangialosi, Angel Alegría, and Juan Colmenero. "Reaching the ideal glass transition by aging polymer films." Physical Chemistry Chemical Physics 19, no. 2 (2017): 961–65. http://dx.doi.org/10.1039/c6cp07139b.

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16

Kato, Kazuaki, Tomoki Mizusawa, Akihiro Ohara, and Kohzo Ito. "Direct enhancement of intercomponent interactions in polyrotaxane and its pronounced effects on glass state properties." Chemical Communications 57, no. 93 (2021): 12472–75. http://dx.doi.org/10.1039/d1cc05516j.

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17

Scriven, Fiona. "The glassy state in foods." Trends in Food Science & Technology 5, no. 5 (1994): 176. http://dx.doi.org/10.1016/0924-2244(94)90128-7.

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18

Kantor, Y. "Glassy State of Polymerized Membranes." Europhysics Letters (EPL) 20, no. 4 (1992): 337–42. http://dx.doi.org/10.1209/0295-5075/20/4/009.

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19

BUZZACCHI, M., E. DEL GIUDICE, and G. PREPARATA. "COHERENCE OF THE GLASSY STATE." International Journal of Modern Physics B 16, no. 25 (2002): 3771–86. http://dx.doi.org/10.1142/s0217979202012116.

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Glasses are known to possess some puzzling features among condensed matter systems, as shown by the Kauzmann paradox. We show that if the coherent interaction mechanisms of Quantum Electrodynamics are taken into account, glasses are nothing but molecular liquids in which a large fraction of the molecules enter a collective, coherent state. In this conceptual framework the temperature of glass formation can be identified with the temperature at which the non-coherent fraction vanishes. Using a recently developed treatment of liquid water where QED interactions are not neglected, we suggest a po

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20

Hassan, Mohammad A., Naji M. Najib, and Mohammad S. Suleiman. "Characterization of glibenclamide glassy state." International Journal of Pharmaceutics 67, no. 2 (1991): 131–37. http://dx.doi.org/10.1016/0378-5173(91)90425-n.

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21

Jowitt, Ronald. "The glassy state in foods." Journal of Food Engineering 28, no. 3-4 (1996): 373–77. http://dx.doi.org/10.1016/0260-8774(96)88326-9.

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22

G’Sell, Christian, and Abdelhamid Souahi. "Influence of Crosslinking on the Plastic Behavior of Amorphous Polymers at Large Strains." Journal of Engineering Materials and Technology 119, no. 3 (1997): 223–27. http://dx.doi.org/10.1115/1.2812248.

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The mechanical properties of three grades of PMMA, one linear and two crosslinked, are investigated in tension below and above the glass transition temperature. It is found that strain-hardening decreases gradually with temperature in the glassy state, but keeps a significant value in the rubbery state. The results are analyzed in terms of an entropy-based statistical model (van der Giessen and Wu, 1992) which describes the stress-strain response of a chain network. The junctions of the network are not only associated with the chemical crosslinks, but additionally with physical entanglements,

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23

Bruni, F., and A. C. Leopold. "Cytoplasmic glass formation in maize embryos." Seed Science Research 2, no. 4 (1992): 251–53. http://dx.doi.org/10.1017/s0960258500001446.

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AbstractIn order to examine the occurrence of a glassy state in the cytoplasm of maize embryos as a function of water content, isolated embryos were examined using spin-probe electron spin resonance. The glass transition temperature was determined at various degrees of hydration (h) in the range 0.05–0.25 g H2O g−1 dry sample weight. The obtained phase diagram indicates that, at standard storage temperature (−5°C), the cytoplasm of embryos drier than 0.15 g H2O g−1 is in a glassy state.

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24

Cofré, Daniela Celis, Manuel Ignacio Azócar, Javier Enrione, Maritza Páez, and Silvia Matiacevich. "Influence of Glassy or Rubbery State on the Antimicrobial Activity of Chitosan-gelatin Films." Journal of Food Research 1, no. 4 (2012): 184. http://dx.doi.org/10.5539/jfr.v1n4p184.

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The aim was to study if the antimicrobial activity of chitosan incorporated into edible films based on gelatin could be affected by the molecular mobility (glassy or rubbery state) of the matrix. Films were obtained from film-forming suspensions (FFS) of bovine and salmon gelatins (7% w/w) and chitosan (0; 0.25; 0.5; 1% w/w) equilibrated at 33% y 85% of relative humidities. Antimicrobial properties against <em>Escherichia coli, Listeria monocytogenes </em>and <em>Salmonella thyphimurium </em>were determined. The results showed that both FFS and films had antimicrobial e

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25

Kato, H., A. Inoue, and H. S. Chen. "Fictive stress model calculations of viscoelastic behaviors in a Zr‐based glassy alloy." Strength, Fracture and Complexity: An International Journal 2, no. 1 (2004): 21–33. https://doi.org/10.3233/sfc-2004-027.

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Viscoelastic behaviors of a Zr‐based glassy alloy in the glass transition region were investigated with uni‐axial compression tests. The transition between the linear and the nonlinear viscoelasticity was observed just as it was observed in other glassy materials. The transition is considered to be due to a structural change in the glassy structure. Using the relationship taken from experimental results between the steady‐state flow stress and their relaxation time at various temperatures, we make the steady‐state flow stress, which is named fictive stress, stand for the flow structure during

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26

Yuan, G. C., Q. G. Wu, Guo Xun Zeng, and Z. Y. Ling. "Characterization of Ultrafine Glassy Powder for Al-Si-Ca-P-O-F Polynary System by Liquid Precipitation." Advanced Materials Research 177 (December 2010): 433–36. http://dx.doi.org/10.4028/www.scientific.net/amr.177.433.

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The ultrafine glassy powder of Al-Si-Ca-P-O-F polynary system was prepared by liquid precipitation method with several inorganic compounds as reactants containing the ions such as Al3+, SiO32-, P3O105-, Ca2+, F-, respectively. The powder was heat-treated in the range of temperature from 773 to 1173K and its crystallized processes were ascertained. The morphology, composition, bonding state and structure, crystallized behavior of the glassy powder were characterized by means of TEM, XRD, EDAX, IR, DSC etc methods. The results show that the powder containing Al, Si, Ca, P, O, F elements belongs

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27

Baustian, K. J., M. E. Wise, E. J. Jensen, G. P. Schill, M. A. Freedman, and M. A. Tolbert. "State transformations and ice nucleation in glassy or (semi-)solid amorphous organic aerosol." Atmospheric Chemistry and Physics Discussions 12, no. 10 (2012): 27333–66. http://dx.doi.org/10.5194/acpd-12-27333-2012.

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Abstract. Glassy or amorphous (semi-)solid organic aerosol particles have the potential to serve as surfaces for heterogeneous ice nucleation in cirrus clouds. Raman spectroscopy and optical microscopy have been used in conjunction with a cold stage to examine water uptake and ice nucleation on individual aqueous organic glass particles at atmospherically relevant temperatures (200–273 K). Three organic compounds considered proxies for atmospheric secondary organic aerosol (SOA) were used in this investigation: sucrose, citric acid and glucose. Internally mixed particles consisting of each org

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28

Tong, H. J., J. P. Reid, D. L. Bones, B. P. Luo, and U. K. Krieger. "Measurements of the timescales for the mass transfer of water in glassy aerosol at low relative humidity and ambient temperature." Atmospheric Chemistry and Physics 11, no. 10 (2011): 4739–54. http://dx.doi.org/10.5194/acp-11-4739-2011.

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Abstract. The influence of glassy states and highly viscous solution phases on the timescale of aerosol particle equilibration with water vapour is examined. In particular, the kinetics of mass transfer of water between the condensed and gas phases has been studied for sucrose solution droplets under conditions above and below the glass transition relative humidity (RH). Above the glass transition, sucrose droplets are shown to equilibrate on a timescale comparable to the change in RH. Below the glass transition, the timescale for mass transfer is shown to be extremely slow, with particles rem

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29

Qian, Xiao-Long, Jian Kang, Bo Lu, Shi-Xun Cao, and Jin-Cang Zhang. "Kinetics of glass transition, negative magnetization and exchange bias effects in Sm1−xBixCrO3." RSC Advances 6, no. 13 (2016): 10677–82. http://dx.doi.org/10.1039/c5ra25006d.

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DC magnetization and magnetic relaxation studies of polycrystalline Sm<sub>1−x</sub>Bi<sub>x</sub>CrO<sub>3</sub> (x = 0, 0.1) demonstrated the kinetics of magnetic glass behaviour in SmCrO<sub>3</sub>: the frozen antiferromagnetic state was dominant to the glassy transition state.

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30

Monnier, Xavier, Sara Marina, Xabier Lopez de Pariza, Haritz Sardón, Jaime Martin, and Daniele Cangialosi. "Physical Aging Behavior of a Glassy Polyether." Polymers 13, no. 6 (2021): 954. http://dx.doi.org/10.3390/polym13060954.

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The present work aims to provide insights on recent findings indicating the presence of multiple equilibration mechanisms in physical aging of glasses. To this aim, we have investigated a glass forming polyether, poly(1-4 cyclohexane di-methanol) (PCDM), by following the evolution of the enthalpic state during physical aging by fast scanning calorimetry (FSC). The main results of our study indicate that physical aging persists at temperatures way below the glass transition temperature and, in a narrow temperature range, is characterized by a two steps evolution of the enthalpic state. Altogeth

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31

FUKUOKA, Eihei, Midori MAKITA, and Shigeo YAMAMURA. "Glassy state of pharmaceuticals. III. Thermal properties and stability of glassy pharmaceuticals and their binary glass systems." CHEMICAL & PHARMACEUTICAL BULLETIN 37, no. 4 (1989): 1047–50. http://dx.doi.org/10.1248/cpb.37.1047.

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32

FUKUOKA, EIHEI, MIDORI MAKITA, and SHIGEO YAMAMURA. "Glassy state of pharmaceuticals. II. Bioinequivalence of glassy and crystalline indomethacin." CHEMICAL & PHARMACEUTICAL BULLETIN 35, no. 7 (1987): 2943–48. http://dx.doi.org/10.1248/cpb.35.2943.

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33

Sharifi, Soheil, and Jahanbakhsh Mashaiekhy Asl. "Secondary Relaxation inside the Glass." ISRN Materials Science 2011 (July 20, 2011): 1–10. http://dx.doi.org/10.5402/2011/764874.

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The physical properties of the glass depend on the procedure used to produce the glass. In particular, if the glass is obtained through the variation of external thermodynamic parameters, the specific way in which the parameters are varied (thermodynamic history) has influence on the final properties. In this work, we studied the effect of thermodynamic history on secondary relaxation inside the glassy state on different molecular glass forming, namely, PPGE(poly[(phenyl glycidyl ether)-co-formaldehyde]), 1,18-bis (p methoxyphenyl) cyclohexane (BMPC), poly(propylene glycol)—(PPG400), phenolpht

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34

Wisitsorasak, Apiwat, and Peter G. Wolynes. "Dynamical Heterogeneity of the Glassy State." Journal of Physical Chemistry B 118, no. 28 (2014): 7835–47. http://dx.doi.org/10.1021/jp4125777.

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35

Williams, Robert J., and A. Carl Leopold. "The Glassy State in Corn Embryos." Plant Physiology 89, no. 3 (1989): 977–81. http://dx.doi.org/10.1104/pp.89.3.977.

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36

Mauro, John C., Roger J. Loucks, and Prabhat K. Gupta. "Fictive Temperature and the Glassy State." Journal of the American Ceramic Society 92, no. 1 (2009): 75–86. http://dx.doi.org/10.1111/j.1551-2916.2008.02851.x.

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37

Gevorkian, S. G., A. E. Allahverdyan, D. S. Gevorgyan, and C. K. Hu. "Glassy state of native collagen fibril?" EPL (Europhysics Letters) 95, no. 2 (2011): 23001. http://dx.doi.org/10.1209/0295-5075/95/23001.

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38

Vleeshouwers, S., and E. Nies. "Stochastic theory for the glassy state." Colloid & Polymer Science 274, no. 2 (1996): 105–11. http://dx.doi.org/10.1007/bf00663442.

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39

Bouda, V. "The nature of glassy state instability." Polymer Degradation and Stability 24, no. 4 (1989): 319–26. http://dx.doi.org/10.1016/0141-3910(89)90042-6.

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40

Saunders, J. "A Glassy State of Supersolid Helium." Science 324, no. 5927 (2009): 601–2. http://dx.doi.org/10.1126/science.1172973.

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41

Nieuwenhuizen, Th M. "Thermodynamic picture of the glassy state." Journal of Physics: Condensed Matter 12, no. 29 (2000): 6543–52. http://dx.doi.org/10.1088/0953-8984/12/29/326.

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42

Gurevich, A. Vl, and R. G. Mints. "Superconducting glassy state induced by twins." Physica C: Superconductivity and its Applications 162-164 (December 1989): 233–34. http://dx.doi.org/10.1016/0921-4534(89)91003-4.

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43

Gerna, Davide, Daniel Ballesteros, Erwann Arc, et al. "Does oxygen affect ageing mechanisms of Pinus densiflora seeds? A matter of cytoplasmic physical state." Journal of Experimental Botany 73, no. 8 (2022): 2631–49. http://dx.doi.org/10.1093/jxb/erac024.

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Abstract During desiccation, the cytoplasm of orthodox seeds solidifies into an intracellular glass with highly restricted diffusion and molecular mobility. Temperature and water content govern seed ageing rates, while oxygen (O2) can promote deteriorative reactions. However, whether the cytoplasmic physical state affects involvement of O2 in seed ageing remains unresolved. We aged Pinus densiflora seeds by controlled deterioration (CD) at 45 °C and distinct relative humidity (RH), resulting in cells with a glassy (11% and 30% RH) or fluid (60% and 80% RH) cytoplasm. Hypoxic conditions (0.4% O

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44

Lebedev, M. P., O. V. Startsev, T. V. Koval, and I. M. Veligodsky. "Multiplet relaxation transitions in fluorurethane coating after climate aging." Doklady Rossijskoj akademii nauk. Himiâ, nauki o materialah. 516, no. 1 (2024): 45–51. http://dx.doi.org/10.31857/s2686953524030068.

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The relaxation transition from a glassy to a highly elastic state (α-transition) of a fluoropolyurethane coating deposited on the surface of VPS-48/778 glass fiber reinforced plastic was studied using the method of dynamic mechanical analysis. It is shown that the relaxation maximum of the dynamic loss modulus in the initial state is a superposition of α1-, α2-, α3-transitions, corresponding, respectively, to transitions from the glassy to highly elastic state of VE-69 enamel and EP-0215 epoxy primer. The transition temperature α1, which is the glass transition temperature of fluoropolyurethan

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45

Perez-Pirotto, Claudia, Gemma Moraga, Isabel Hernando, Sonia Cozzano, and Patricia Arcia. "Sorption Isotherms, Glass Transition and Bioactive Compounds of Ingredients Enriched with Soluble Fibre from Orange Pomace." Foods 11, no. 22 (2022): 3615. http://dx.doi.org/10.3390/foods11223615.

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Citrus fruits are one of the main crops worldwide. Its industrialization, primarily juice production, produces large amounts of byproducts, composed of seeds and peels, that can be used to obtain new ingredients. In this study, sorption behaviour, glass transition, mechanical properties, colour and bioactives of four different soluble fibre-enriched powders obtained from orange pomace using green technologies were studied. Powders were equilibrated at water activities between 0.113 and 0.680 for fifteen weeks at 20 °C, and studies were performed to indicate the best storing conditions to ensur

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Chen, Dongjie, and Gregory B. McKenna. "Deep glassy state dynamic data challenge glass models: Configurational entropy models." Journal of Non-Crystalline Solids 566 (August 2021): 120871. http://dx.doi.org/10.1016/j.jnoncrysol.2021.120871.

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Rim, Y. H., S. M. Lee, M. Kim, and Y. S. Yang. "Dielectric dispersive behaviors of lithium-silicate glass in the glassy state." Journal of the Korean Physical Society 60, no. 2 (2012): 301–5. http://dx.doi.org/10.3938/jkps.60.301.

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SAPRU, V., and T. P. LABUZA. "Glassy State in Bacterial Spores Predicted by Polymer Glass-Transition Theory." Journal of Food Science 58, no. 2 (1993): 445–48. http://dx.doi.org/10.1111/j.1365-2621.1993.tb04294.x.

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Wu, Junhua. "The glassy state, ideal glass transition, and second-order phase transition." Journal of Applied Polymer Science 71, no. 1 (1999): 143–50. http://dx.doi.org/10.1002/(sici)1097-4628(19990103)71:1<143::aid-app17>3.0.co;2-i.

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Wheaton, Jacob, Stuart Leland, and Steve Martin. "Towards a Degradation-Free Solid-State Lithium-Sulfur Battery Using Sulfide Glassy Solid-State Electrolytes." ECS Meeting Abstracts MA2024-02, no. 67 (2024): 4548. https://doi.org/10.1149/ma2024-02674548mtgabs.

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Solid-state batteries present several possible advantages over current lithium-ion batteries, including their enabling of higher capacity lithium anodes, and their removal of flammable organic liquid electrolytes. Sulfide glasses are of particular interest due to their high conductivity, low processing temperatures, and their ability to be formed without grain boundaries. Glasses in the Li2S – SiS2 – LixMOy phase space are being studied for use in lithium-sulfur batteries. While these glasses may appear to be stable against lithium metal during symmetric cell cycling and cyclic voltammetry, th

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