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Journal articles on the topic 'Binary phase diagram'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Sangster, James Malcolm. "Calculation of phase diagrams and thermodynamic properties of 18 binary common-ion systems of Na,K,Ba//F,MoO4,WO4." Canadian Journal of Chemistry 74, no. 3 (1996): 402–18. http://dx.doi.org/10.1139/v96-045.

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Phase diagram and thermodynamic data of 18 binary common-ion molten salt systems in Na,K,Ba//F,MoO4,WO4 were optimized by computer algorithm. The phase diagram data as well as single-salt data were retrieved from an extensive critical literature search. Expressions for the excess properties of solution phases and thermodynamic properties of intermediate compounds were thereby obtained. These data were used to generate a "best" phase diagram for each binary system considered. Key words: molten salts, phase diagrams, thermodynamic properties.

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2

Tkachenko, Alexei V. "Generic phase diagram of binary superlattices." Proceedings of the National Academy of Sciences 113, no. 37 (2016): 10269–74. http://dx.doi.org/10.1073/pnas.1525358113.

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Emergence of a large variety of self-assembled superlattices is a dramatic recent trend in the fields of nanoparticle and colloidal sciences. Motivated by this development, we propose a model that combines simplicity with a remarkably rich phase behavior applicable to a wide range of such self-assembled systems. Those systems include nanoparticle and colloidal assemblies driven by DNA-mediated interactions, electrostatics, and possibly, controlled drying. In our model, a binary system of large and small hard spheres (L and S, respectively) interacts via selective short-range (“sticky”) attraction. In its simplest version, this binary sticky sphere model features attraction only between S and L particles. We show that, in the limit when this attraction is sufficiently strong compared with kT, the problem becomes purely geometrical: the thermodynamically preferred state should maximize the number of LS contacts. A general procedure for constructing the phase diagram as a function of system composition f and particle size ratio r is outlined. In this way, the global phase behavior can be calculated very efficiently for a given set of plausible candidate phases. Furthermore, the geometric nature of the problem enables us to generate those candidate phases through a well-defined and intuitive construction. We calculate the phase diagrams for both 2D and 3D systems and compare the results with existing experiments. Most of the 3D superlattices observed to date are featured in our phase diagram, whereas several more are predicted for future discovery.

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3

Wicaksono, Yudi, Dwi Setyawan, and S. Siswandono. "Diagram Fase dan Sifat Termodinamik Campuran Biner Ketoprofen-Asam Suksinat." Jurnal ILMU DASAR 19, no. 2 (2018): 99. http://dx.doi.org/10.19184/jid.v19i2.5521.

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The equilibrium phase diagram and thermodynamic properties of a mixture of drugs and additives are information related to various possible interaction processes between components. Therefore, we conducted a study of the phase diagrams and thermodynamic properties of binary mixtures of ketoprofen-succinic acid to estimate the types of interactions that may occur between these materials. The solid-liquid phase diagram of ketoprofen-succinic acid binary mixtures was determined by differential scanning calorimetry and composition of eutectic system was determined accurately using a Tamman diagram. The measurement of binary mixtures of ketoprofen-succinic acid with differential scanning calorimeter obtained the value of melting temperature and heat of fusion of ketoprofen- succinic acid system. The solid-liquid phase diagram of ketoprofen- succinic acid showed the formation of eutectic type phase diagram. The Tamman diagram showed accurately composition of the eutectic system of the Kp-SA binary mixtures at the mole fraction of Kp 0.87 and temperature 96.9oC.Keywords: ketoprofen, phase diagram, eutectic system, Tamman diagram

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4

Kim, Han Gyeol, Joonho Lee, and Guy Makov. "Phase Diagram of Binary Alloy Nanoparticles under High Pressure." Materials 14, no. 11 (2021): 2929. http://dx.doi.org/10.3390/ma14112929.

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CALPHAD (CALculation of PHAse Diagram) is a useful tool to construct phase diagrams of various materials under different thermodynamic conditions. Researchers have extended the use of the CALPHAD method to nanophase diagrams and pressure phase diagrams. In this study, the phase diagram of an arbitrary A–B nanoparticle system under pressure was investigated. The effects of the interaction parameter and excess volume were investigated with increasing pressure. The eutectic temperature was found to decrease in most cases, except when the interaction parameter in the liquid was zero and that in the solid was positive, while the excess volume parameter of the liquid was positive. Under these conditions, the eutectic temperature increased with increasing pressure.

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5

Travesset, Alex. "Binary nanoparticle superlattices of soft-particle systems." Proceedings of the National Academy of Sciences 112, no. 31 (2015): 9563–67. http://dx.doi.org/10.1073/pnas.1504677112.

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The solid-phase diagram of binary systems consisting of particles of diameter σA=σ and σB=γσ (γ≤1) interacting with an inverse p = 12 power law is investigated as a paradigm of a soft potential. In addition to the diameter ratio γ that characterizes hard-sphere models, the phase diagram is a function of an additional parameter that controls the relative interaction strength between the different particle types. Phase diagrams are determined from extremes of thermodynamic functions by considering 15 candidate lattices. In general, it is shown that the phase diagram of a soft repulsive potential leads to the morphological diversity observed in experiments with binary nanoparticles, thus providing a general framework to understand their phase diagrams. Particular emphasis is given to the two most successful crystallization strategies so far: evaporation of solvent from nanoparticles with grafted hydrocarbon ligands and DNA programmable self-assembly.

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6

Sanders, Philip C., James H. Reeves, and Michael Messina. "The Binary Temperature–Composition Phase Diagram." Journal of Chemical Education 83, no. 1 (2006): 150. http://dx.doi.org/10.1021/ed083p150.

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7

Mckenney, Robert, and Thomas Krawietz. "Binary Phase Diagram Series: HMX/RDX." Journal of Energetic Materials 21, no. 3 (2003): 141–66. http://dx.doi.org/10.1080/716100385.

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8

Okamoto, H., and T. B. Massalski. "guidelines for binary phase diagram assessment." Journal of Phase Equilibria 14, no. 3 (1993): 316–35. http://dx.doi.org/10.1007/bf02668229.

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9

Legendre, B., and F. Querniard. "Glossary for Binary Phase Diagram Reactions." Journal of Phase Equilibria and Diffusion 35, no. 1 (2013): 11–14. http://dx.doi.org/10.1007/s11669-013-0266-6.

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10

Ramirez, Antonio J., and Sérgio Duarte Brandi. "Weldability Approach to Duplex Stainless Steels Using Multicomponent Phase Diagrams." Materials Science Forum 475-479 (January 2005): 2765–68. http://dx.doi.org/10.4028/www.scientific.net/msf.475-479.2765.

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Welding is a non-equilibrium process. However, some weldability issues, as the extension of the heat-affected zone (HAZ) can be addressed using equilibrium phase diagrams. The 70 wt% Fe-Cr-Ni pseudo-binary phase diagram is commonly used to establish the phase transformations during welding of duplex stainless steels. The predicted results are assumed to be reasonably good for most of the duplex stainless steels. Thermodynamic calculations were used to determine multicomponent phase diagrams and volumetric fraction of phases present as a function of temperature several commercial duplex stainless steels. Results showed that simplified pseudobinary phase diagram approach is valid to estimate welded joint microstructures only for the low alloy duplex stainless steels as UNS S32304, but phase transformations and mainly solidification paths of high alloy duplex stainless steels should predicted only using a multi-component phase diagram.

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11

Tatárka, Eszter, Tamás Mende, and András Roósz. "Liquidus Temperature Calculation in Sn-Bi-Cd System by ESTPHAD Method." Materials Science Forum 790-791 (May 2014): 265–70. http://dx.doi.org/10.4028/www.scientific.net/msf.790-791.265.

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This paper includes the binary and ternary liquidus temperature calculations of Sn-Bi-Cd system. The calculation was performed in cases of the surfaces of Sn, Bi and Cd phases too. First of all the liquidus curves were calculated in the binary systems (Bi phase in Bi-Cd and Bi-Sn systems, Sn phase in Sn-Cd and Sn-Bi systems, Cd phase in Cd-Sn and Cd-Bi systems). By using the calculated coefficients of the binary phase diagrams and the data from the digitalized ternary phase diagram, the liquidus temperature of Sn, Bi and the Cd phases were calculated. Finally the eutectic point of the binary liquidus curves and the eutectic valley of the Sn and the Bi surfaces were calculated by means of an iteration method.

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12

Jian-Ling, Zhang, Liu Xiao-Di, Wu Ke-Zhong, Zhang Jian-Jun, and He Shu-Mei. "Phase Diagram of Binary System NPG-TAM." Acta Physico-Chimica Sinica 16, no. 07 (2000): 652–57. http://dx.doi.org/10.3866/pku.whxb20000714.

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13

Guo-Yan, Huo. "Phase Diagram of Cr-Ni Binary System." Acta Physico-Chimica Sinica 18, no. 12 (2002): 1093–98. http://dx.doi.org/10.3866/pku.whxb20021208.

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14

Hosoya, Yuji, Takayuki Terai, Satoru Tanaka, and Yoichi Takahashi. "Phase Diagram of NdCl3-NaCl Binary System." Netsu Bussei 10, no. 4 (1996): 96–101. http://dx.doi.org/10.2963/jjtp.10.96.

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15

Mimkes, J., and M. Wuttig. "Diffusion and phase diagram in binary alloys." Thermochimica Acta 282-283 (July 1996): 165–73. http://dx.doi.org/10.1016/0040-6031(96)02815-8.

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16

Wu, Kezhong, Ping Zuo, Xiaodi Liu, and Yajuan Li. "Subsolidus binary phase diagram of C10Zn/C12Zn." Thermochimica Acta 397, no. 1-2 (2003): 49–53. http://dx.doi.org/10.1016/s0040-6031(02)00316-7.

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17

Espeau, P., HAJ Oonk, PR van der Linde, X. Alcobe, and Y. Haget. "Experimental binary phase diagram of pentadecane-heneicosane." Journal de Chimie Physique 92 (1995): 747–57. http://dx.doi.org/10.1051/jcp/1995920747.

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18

Liang, L. H., D. Liu, and Q. Jiang. "Size-dependent continuous binary solution phase diagram." Nanotechnology 14, no. 4 (2003): 438–42. http://dx.doi.org/10.1088/0957-4484/14/4/306.

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19

SADIQ, A., K. YALDRAM, and M. DAD. "PHASE DIAGRAM OF A DILUTE BINARY SYSTEM." International Journal of Modern Physics C 03, no. 02 (1992): 297–305. http://dx.doi.org/10.1142/s0129183192000245.

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Phase diagram of a binary system with quenched impurities has been studied with Monte Carlo computer simulation technique. Use of Swendsen-Wang algorithm makes it possi-ble to explore the vicinity of percolation transition which was difficult to explore with the traditional Metropolis method. For small vacancy concentration υ(υ=1−p, where p is the spin concentration) the critical temperature, Tc, decreases linearly with υ consistent with earlier results on this system. For larger values of v departure from linearity is observed with Tc decreasing to zero sharply near the percolation threshold. An estimate of the critical exponent describing this sharp drop of Tc is also given.

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20

Martínez Casado, F. J., M. Ramos Riesco, and J. A. R. Cheda. "Rubidium and lithium butanoates binary phase diagram." Journal of Thermal Analysis and Calorimetry 87, no. 1 (2006): 73–77. http://dx.doi.org/10.1007/s10973-006-7819-4.

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21

Sun, Yimin, Shihua Wang, Zhiyu Qiao, and Meitian Wang. "Phase Diagram of EuI2–KI Binary System." Journal of Solid State Chemistry 136, no. 1 (1998): 134–36. http://dx.doi.org/10.1006/jssc.1997.7634.

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22

Igarashi, K., H. Ohtani, and J. Mochinaga. "Phase Diagram of the System LaCl3-CaCl2-NaCl." Zeitschrift für Naturforschung A 42, no. 12 (1987): 1421–24. http://dx.doi.org/10.1515/zna-1987-1212.

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The phase diagram of ternary system LaCl3-CaCl2-NaCl has been constructed from the phase diagrams of the three binary systems and of thirteen quasi-binary systems determined by DTA. For the binaries LaCl3-CaCl2 and CaCl2-NaCl eutectic points were observed at 651 °C , 35.1 mol% LaCl3 and at 508 °C , 49.9 mol% NaCl, respectively. For LaCl3-NaCl, a peritectic point besides the eutectic point at 545 °C , 36.1 mol% LaCl3 was found at 690 °C , 57.5 mol%, which is attributable to the formation of the peritectic compound 3 LaCl3 · NaCl. The phase diagram of the ternary system has a ternary eutetic point and a ternary peritectic point due to 3 LaCl3-NaCl, the form er at 462 °C and 12.1 - 3 9 .7 - 4 8 .2 mol% (LaCl3-CaCl2-NaCl) and the latter at 612 °C and 26.9 - 55.1 - 18.0 mol%.

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23

Minic, Dusko, Dragan Manasijevic, Dragana Zivkovic, Nada Strbac, and Zvonimir Stankovic. "Prediction of phase equilibria in the In-Sb-Pb system." Journal of the Serbian Chemical Society 73, no. 3 (2008): 377–84. http://dx.doi.org/10.2298/jsc0803377m.

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Binary thermodynamic data, successfully used for phase diagram calculations of the binary systems In-Sb, Pb-Sb and In-Pb, were used for the prediction of the phase equilibria in the ternary In-Sb-Pb system. The predicted equilibrium phase diagram of the vertical Pb-InSb section was compared with the results of differential thermal analysis (DTA) and optical microscopy. The calculated phase diagram of the isothermal section at 300 ?C was compared with the experimentally (SEM, EDX) determined composition of phases in the chosen alloys after annealing. Very good agreement between the binary-based thermodynamic prediction and the experimental data was found in all cases. The calculated liquidus projection of the ternary In-Sb-Pb system is also presented.

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24

Yang, Hui Min, Liang Shun Luo, Mei Hui Song, Hai Qun Qi, Chun Yan Wang, and Chuang Yang. "Calculation of Aluminum Equivalent Based on Thermo-Calc Software in Ti-Al-Nb Ternary System." Materials Science Forum 788 (April 2014): 144–49. http://dx.doi.org/10.4028/www.scientific.net/msf.788.144.

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Ti-Al-Nb ternary phase diagrams were calculated by Thermo-Calc software. The analysis of the calculated vertical sections of Ti-Al-Nb phase diagram indicated that when Nb content is fixed at 5at.% and Al content is lower than 52.3at.%, the primary phase would be β phase during solidification. With 10 at.%Nb and Al content lower than 55.8at.%, or with 15 at.%Nb and Al content lower than 56.9at.%, the primary phase would be β phase. The vertical sections of Ti-Al-Nb ternary phase diagram were further simplified into pseudo-Ti-Al binary phase diagram. According to the pseudo-Ti-Al diagram, the expression of the aluminum equivalent was obtained in Ti-Al-5Nb ternary alloys.

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25

Cherkasov, Dmitry G., та Varvara D. Parfenova. "Phase diagram of the β-alanine – water binary system". Izvestiya of Saratov University. New Series. Series: Chemistry. Biology. Ecology 21, № 1 (2021): 44–47. http://dx.doi.org/10.18500/1816-9775-2021-21-1-44-47.

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The phase diagram of the β-alanine–water binary system was studied using the visual polythermal method and the method of time–temperature curves in а temperature range of -20–90°С. There is a eutectic equilibrium at -18.3°С in the system; the solid phases of this equilibrium are ice and individual β-alanine. For the first time, the composition of the liquid phase of the eutectic state was determined.

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26

Homolová, Viera. "Prediction of Ternary Fe-B-Cr Phase Diagram." Materials Science Forum 782 (April 2014): 45–50. http://dx.doi.org/10.4028/www.scientific.net/msf.782.45.

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Fe-B-Cr ternary system and its binary subsystems have been studied with aim to develop database of parameters for various thermodynamic calculations of complex systems with boron (for example modified ferritic and austenitic steels for energy industry). All corresponding binary phase diagram were calculated with software THERMO-CALC. Prediction of ternary phase diagram for the Fe-B-Cr system was modelled with using binary data of corresponding subsystems. The prediction was compared with available literature experimental results of phase analysis. The experimental results were used for modifying of the phase diagram prediction by Calphad-method. In future the modified prediction is going to be compared with our experimental results of phase analysis of prepared model alloys to receive most reliable phase diagram of the system.

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27

Kainzbauer, Peter, Klaus W. Richter, and Herbert Ipser. "The Binary Bi-Rh Phase Diagram: Stable and Metastable Phases." Journal of Phase Equilibria and Diffusion 39, no. 1 (2017): 17–34. http://dx.doi.org/10.1007/s11669-017-0600-5.

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28

Gabriel, Armand, and Arthur D. Pelton. "Phase diagram measurements and thermodynamic analysis of the PbCl2–NaCl, PbCl2–KCl, and PbCl2–KCl–NaCl systems." Canadian Journal of Chemistry 63, no. 11 (1985): 3276–82. http://dx.doi.org/10.1139/v85-542.

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The phase diagrams of the PbCl2–NaCl and PbCl2–KCl systems have been measured by the cooling curve technique. In addition, a number of measurements at compositions in the ternary system PbCl2–KCl–NaCl have been made. The binary data have been analysed along with other available thermodynamic data for the binary systems in order to obtain mathematical expressions for the binary thermodynamic properties. Various estimation procedures were then used to calculate the Gibbs energy of the ternary liquid from the binary expressions, and the ternary phase diagram calculated therefrom was compared to the experimental ternary points. In the case of the Conformal Ionic Solution equation, agreement was within 3 °C at all measured points. In the case of two "geometric" estimation techniques, the Kohler and Toop equations, agreement was within 10 °C but could be brought to within 3 °C by the addition of only one small adjustable ternary correction term. The technique of coupled thermodynamic/phase diagram analysis permits a large reduction in the amount of experimental work necessary to measure the ternary diagram. In addition, the ternary thermodynamic expressions developed can be used to calculate all thermodynamic properties of the ternary liquid.

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29

Zhou, Guo Jun, and De Chang Zeng. "Thermodynamic Evaluation of the Fe-Pr Binary System." Materials Science Forum 654-656 (June 2010): 2442–45. http://dx.doi.org/10.4028/www.scientific.net/msf.654-656.2442.

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The Fe–Pr binary system was thermodynamic evaluation by means of the CALPHAD method based on phase diagram experimental data from the literature and a few values of the mixing enthalpy in the liquid phase obtained by the Miedema theory technique. Each of the selected data values is given a certain weight, which is chosen and adjusted based on the thermodynamic data and diagram phase data. A consistent thermodynamic description of the Fe–Pr binary system is presented: only one intermediate compound, Fe17Pr2, is stable in the system and forms peritectically at 1371K. An eutectic reaction L↔Pr+ Fe17Pr2 occurs at 939K and the eutectic liquid contains 82 at% Pr, five solid solution phases (Fe-rich αFe, γFe and δFe, Pr-rich αPr and βPr) and the liquid solution phase were considered in the evaluation. The intermediate phase was treated as stoichiometric compound, the solid solutions as ideal and the liquid solution phase by the Redlich–Kister formalism. The calculated phase diagram and thermodynamic properties are in good agreement with available experimental data.

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30

Bosholm, O., H. Oppermann, and S. Däbritz. "Chemischer Transport intermetallischer Phasen IV: Das System Fe - Ge/Chemical Vapour Transport of Intermetallic Phases IV: The System Fe - Ge." Zeitschrift für Naturforschung B 56, no. 4-5 (2001): 329–36. http://dx.doi.org/10.1515/znb-2001-4-501.

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Abstract Six phases exist in the binary system iron-germanium Fe3Ge, β, η, Fe6Ge5, FeGe and FeGe2. All phases could be prepared by chemical transport with iodine as transport agent in the temperature range between T1 (600 °C) and T2 (950 °C). Two phase diagrams have been known in the literature from specific experiments of chemical vapour transport. It is now possible to decide which phase diagram is the most valid description.

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31

Li, Yandong, Tongsheng Zhang, Yefeng Feng, Chengjun Liu, and Maofa Jiang. "Liquid Regions of Lanthanum-Bearing Aluminosilicates." Materials 13, no. 2 (2020): 450. http://dx.doi.org/10.3390/ma13020450.

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The Al2O3-SiO2, La2O3-Al2O3, and La2O3-SiO2 binary phase diagrams were estimated by Redlich–Kister expression. La4.67Si3O13 (=La4.67(SiO4)3O) was introduced to improve the existing phase diagrams. The Al2O3-SiO2-La2O3 ternary phase diagram extrapolated by Kohler method was optimized. Then, the liquidus of Al2O3-SiO2-La2O3 system at 1600 °C was compared with Al2O3-SiO2-RE2O3 (RE = Rare Earth Elements) systems and experimental results in other literature. The high temperature experiments were conducted in the tube furnace at 1500 °C. Then the field emission scanning electron microscope (FE-SEM), energy dispersive spectrometer (EDS), and X-ray diffraction (XRD) were employed to verify the calculated liquid region and precipitates phase at 1500 °C. Moreover, the liquidus of binary systems were compared with FactSage results and experiments. The optimized ternary phase diagram shows the relatively reliable region of liquid phase, and it is significant to the seal glass of solid oxide fuel cells and other fields being related to RE containing silicates.

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32

LOPES, J. N. CANONGIA. "Phase equilibra in binary Lennard-Jones mixtures: phase diagram simulation." Molecular Physics 96, no. 11 (1999): 1649–58. http://dx.doi.org/10.1080/00268979909483108.

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33

Lee, S. Y., C. P. Kim, J. D. Almer, U. Lienert, E. Ustundag та W. L. Johnson. "Pseudo-binary phase diagram for Zr-based in situ β phase composites". Journal of Materials Research 22, № 2 (2007): 538–43. http://dx.doi.org/10.1557/jmr.2007.0066.

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The pseudo-binary (quasi-equilibrium) phase diagram for Zr-based bulk metallic glasses with crystalline in situ precipitates (β phase) has been constructed from high-temperature phase information and chemical composition analysis. The phase evolution was detected in situ by high-energy synchrotron x-ray diffraction followed by Rietveld analysis of the data for volume fraction estimation. The phase diagram delineates phase fields and allows the control of phase fractions. Combined with related previous work by the authors, this diagram offers a unique opportunity to control both the morphology and volume of the dendritic β phase precipitates to enhance the properties of the composites.

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34

Råberg, Mathias, Dan Boström, Anders Nordin, Erik Rosén, and Björn Warnqvist. "Improvement of the Binary Phase Diagram Na2CO3−Na2S." Energy & Fuels 17, no. 6 (2003): 1591–94. http://dx.doi.org/10.1021/ef0340256.

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35

Heimburg, Thomas, Ulrich Würz, and Derek Marsh. "Binary phase diagram of hydrated dimyristoylglycerol-dimyristoylphosphatidylcholine mixtures." Biophysical Journal 63, no. 5 (1992): 1369–78. http://dx.doi.org/10.1016/s0006-3495(92)81714-9.

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36

Kambara, M., M. Nakamura, Y. Shiohara, and T. Umeda. "Quasi-binary phase diagram of Nd4Ba2Cu2O10Ba3Cu5O8 system." Physica C: Superconductivity 275, no. 1-2 (1997): 127–34. http://dx.doi.org/10.1016/s0921-4534(96)00681-8.

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37

Zhang, Wei, Kozo Osamura, and Shojiro Ochiai. "Phase Diagram of the BaO-CuO Binary System." Journal of the American Ceramic Society 73, no. 7 (1990): 1958–64. http://dx.doi.org/10.1111/j.1151-2916.1990.tb05252.x.

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38

Rycerz, L., and M. Gaune-Escard. "Phase Diagram of the TbBr3-KBr Binary System." Zeitschrift für Naturforschung A 59, no. 1-2 (2004): 84–90. http://dx.doi.org/10.1515/zna-2004-1-212.

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The phase equilibrium of the TbBr3-KBr has been established by Differential Scanning Calorimetry. This system has the three compounds K3TbBr6, K2TbBr5, and KTb2Br7 and two eutectics located at (χTb = 0.163 (885 K) and (χTb = 0.433 (697 K). K3TbBr6 undergoes a solid-solid phase transition at 691 K and melts congruently at 983 K with the corresponding enthalpies 8.0 and 48.0 kJ mol−1. K2TbBr5 melts incongruently at 725 K, and KTb2Br7 at 741 K. The latter forms at 694 K, a temperature very close to that (697 K) of one of the two eutectics also existing in the binary system.

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39

Richter, Klaus W., and Herbert Ipser. "Reinvestigation of the binary FeSb phase diagram." Journal of Alloys and Compounds 247, no. 1-2 (1997): 247–49. http://dx.doi.org/10.1016/s0925-8388(96)02597-2.

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40

Son, L. "Nonergodic correction to a binary mixture phase diagram." Physica A: Statistical Mechanics and its Applications 449 (May 2016): 395–400. http://dx.doi.org/10.1016/j.physa.2015.12.112.

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41

Dewaele, Agnès, Angelika D. Rosa, and Nicolas Guignot. "Argon-neon binary diagram and ArNe2 Laves phase." Journal of Chemical Physics 151, no. 12 (2019): 124708. http://dx.doi.org/10.1063/1.5119419.

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42

Delica, Serafin, Melvin Estonactoc, Mary Claire Micaller, Leorina Cada, and Zenaida Domingo. "PHASE DIAGRAM OF BINARY MIXTURE TM74A:E48 LIQUID CRYSTALS." Molecular Crystals and Liquid Crystals Science and Technology. Section A. Molecular Crystals and Liquid Crystals 366, no. 1 (2001): 101–6. http://dx.doi.org/10.1080/10587250108023952.

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43

Mishra, Pankaj, Manjori Mukherjee, and Sanat Kumar. "Phase diagram of two-dimensional binary Yukawa mixtures." Molecular Physics 114, no. 6 (2015): 741–56. http://dx.doi.org/10.1080/00268976.2015.1116714.

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44

Schuster, Julius C., and Martin Palm. "Reassessment of the binary Aluminum-Titanium phase diagram." Journal of Phase Equilibria and Diffusion 27, no. 3 (2006): 255–77. http://dx.doi.org/10.1361/154770306x109809.

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Yao, Qingrong, Yanchun Wang, and Huaiying Zhou. "Phase diagram of the Tb–Ni binary system." Journal of Alloys and Compounds 395, no. 1-2 (2005): 98–100. http://dx.doi.org/10.1016/j.jallcom.2004.11.043.

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Massalski, T. B. "The ASM/NBS Binary Phase Diagram Evaluation Program." JOM 37, no. 11 (1985): 42. http://dx.doi.org/10.1007/bf03258742.

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Chien, W. M., D. Chandra, A. K. Helmy, J. Franklin, and C. J. Rawn. "Experimental determination of NH4NO3-KNO3 binary phase diagram." Journal of Phase Equilibria and Diffusion 26, no. 2 (2005): 115–23. http://dx.doi.org/10.1007/s11669-005-0130-4.

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Lim, S. S., P. L. Rossiter, and J. E. Tibballs. "Assessment of the Al-Ag binary phase diagram." Calphad 19, no. 2 (1995): 131–41. http://dx.doi.org/10.1016/0364-5916(95)00014-6.

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Xu, Ch F., K. H. Chen, Z. F. Gu, et al. "Phase diagram of the Nd2Fe14B–Sm2Fe14B pseudo-binary system." Journal of Applied Crystallography 49, no. 1 (2016): 64–68. http://dx.doi.org/10.1107/s1600576715022062.

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Abstract:

The phase relations in the (1−x)Nd2Fe14B–xSm2Fe14B system over the whole concentration range have been studied by means of X-ray powder diffraction (XRD), differential thermal analysis (DTA) and scanning electron microscopy with energy-dispersive X-ray spectroscopy. Crystal structure parameters for all studied compositions of (Nd1−xSmx)2Fe14B have been determined by full-profile Rietveld refinements. These results revealed that all intermediate alloys of (Nd1−xSmx)2Fe14B are similar to the end member of the investigated system, Nd2Fe14B, with a tetragonal structure (space groupP42/mnm). The formation of continuous solid solutions has been found in this system. The normalized lattice parameters and unit-cell volumes of (Nd1−xSmx)2Fe14B solid solutions decrease linearly with increasing Sm content. The DTA measurements show that the melting temperature of (Nd1−xSmx)2Fe14B increases linearly with increasing Sm content and no metastable phases were detected. Based on the DTA data and XRD results, a tentative phase diagram for the pseudo-binary system Nd2Fe14B–Sm2Fe14B has been constructed.

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Lu, Yong, Zheng Jiang, Qiao Qiao Tang, Cui Ping Wang, and Xing Jun Liu. "Steady-State Dynamic Phase Diagram Calculation of U-Ti and U-V Binary System under Irradiation." Materials Science Forum 993 (May 2020): 996–1003. http://dx.doi.org/10.4028/www.scientific.net/msf.993.996.

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Abstract:

In this paper, by considering the irradiation-enhanced diffusion, a combination of effective free energy model and the thermodynamic model was used for studying the phase relationships in the U-Ti and U-V binary system under irradiation. The steady-state dynamical phase diagrams of U-Ti and U-V binary alloys under different irradiation intensities were calculated and compared with the conventional thermodynamic equilibrium phase diagram. The calculated results show that under irradiation the high-temperature stable (βTi, γU) and (γU,V) phases were stabilized at relatively low temperature resulting in invariant reactions at relatively low temperature. In addition, with the increase of the irradiation intensity, the temperature of the invariant reactions increased, and the phase regions of the (βTi, γU) and (γU,V) also increased.

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