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Journal articles on the topic 'Interphase boundary'

Author: Grafiati

Published: 28 May 2022

Last updated: 30 July 2025

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1

Liu, Y. J., N. Xu, and J. F. Luo. "Modeling of Interphases in Fiber-Reinforced Composites Under Transverse Loading Using the Boundary Element Method." Journal of Applied Mechanics 67, no. 1 (1999): 41–49. http://dx.doi.org/10.1115/1.321150.

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In this paper, interphases in unidirectional fiber-reinforced composites under transverse loading are modeled by an advanced boundary element method based on the elasticity theory. The interphases are regarded as elastic layers between the fiber and matrix, as opposed to the spring-like models in the boundary element method literature. Both cylinder and square unit cell models of the fiber-interphase-matrix systems are considered. The effects of varying the modulus and thickness (including nonuniform thickness) of the interphases with different fiber volume fractions are investigated. Numerica

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2

Nesterenko, A. I., and N. G. Nesterenko. "Pushing of Interstitial Elements in the Transition Zone under the Growing Diffusion Layers." Фізика і хімія твердого тіла 16, no. 1 (2015): 202–6. http://dx.doi.org/10.15330/pcss.16.1.202-206.

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The kinetics of diffusion of interstitial elements on the example of diffusion saturation with boron and silicon iron- carbon matrix (- iron) was considered . The layers of intermetallic Fe - B - Si are formed and grow in diffusion saturation , and carbon is pushed deep into the matrix. Linear , parabolic and logarithmic laws of motion of the interface boundary between the intermetallic layers and steel matrix was considered and solved the problem of the diffusion redistribution of carbon in the transition zone. Found that in all these cases is due to pushing of carbon its concentration are in

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3

Poletaev, Gennady, Darya Novoselova, Mikhail D. Starostenkov, Vladimir Tsellermaer, and Viktor Kovalenko. "The Study of Inhibition of Atom-Atom Collisions Cascades by Ni-Al (100) Interphase Boundary." Key Engineering Materials 685 (February 2016): 8–12. http://dx.doi.org/10.4028/www.scientific.net/kem.685.8.

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The interaction of atom-atom collisions cascades with Ni-Al interphase boundary was studied by the method of molecular dynamics. It was shown that the interphase boundary partially absorbs the cascade energy. The degree of energy absorption of the cascade by the interphase boundary increases with the growth of the structural imperfection of the boundary and density of the misfit dislocations, and also with increase of distance between the boundary and the place of the cascade initiation.

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4

Sancaktar, E., and P. Zhang. "Nonlinear Viscoelastic Modelling of the Fiber-Matrix Interphase in Composite Materials." Journal of Mechanical Design 112, no. 4 (1990): 605–19. http://dx.doi.org/10.1115/1.2912653.

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A nonlinear viscoelastic analysis of the carbon fiber-thermoset (or thermoplastic) matrix interphase is presented. The second order nonlinear partial differential equation governing the state of stress at the fiber-matrix interphase is solved by using an iterative scheme involving successive differentiation and Taylor expansions to satisfy the boundary conditions. Additional iteration is used for the case with nonlinear viscoelastic matrix material. The results reveal that the thickness and material properties of the interphase have strong influence in reducing the shear stress magnitudes and

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5

Benveniste, Y., and G. Baum. "An interface model of a graded three-dimensional anisotropic curved interphase." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 463, no. 2078 (2006): 419–34. http://dx.doi.org/10.1098/rspa.2006.1777.

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A three-dimensional, generally curved, constant thickness interphase whose properties vary across its thickness is considered. This graded interphase is modelled by an interface that is located at its mid-surface and which comes now into direct contact with the media that were adjacent to it. The derivation is carried out in the setting of heat conduction, and appropriate jump conditions for the temperature and normal heat flux across the interface are derived, which characterize the interface model. The inhomogeneity of the interphase becomes a major motivation for its replacement by an inter

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6

Huang, Yunhao, Jincheng Wang, Zhijun Wang, and Junjie Li. "Atomic structures and migration mechanisms of interphase boundaries during body- to face-centered cubic phase transformations." Journal of Applied Crystallography 52, no. 5 (2019): 1176–88. http://dx.doi.org/10.1107/s1600576719011889.

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Atomic structures and migration mechanisms of interphase boundaries have been of scientific interest for many years owing to their significance in the field of phase transformations. Though the interphase boundary structures can be deduced from crystallographic investigations, the detailed atomic structures and migration mechanisms of interphase boundaries during phase transformations are still poorly understood. In this study, a systematic study on atomic structures and migration mechanisms of interphase boundaries in a body-centered cubic (b.c.c.) to face-centered cubic (f.c.c.) massive tran

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7

Pond, R. C., M. Aindow, and W. A. T. Clark. "Hexagonal crystallography and interphase boundary dislocations." Scripta Metallurgica 21, no. 7 (1987): 971–74. http://dx.doi.org/10.1016/0036-9748(87)90136-0.

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8

Militzer, M., and A. N. Orlov. "Interphase-boundary dislocations and particle growth." Scripta Metallurgica 23, no. 7 (1989): 1173–76. http://dx.doi.org/10.1016/0036-9748(89)90321-9.

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9

Jia, Tao, Run Ni, Hanle Wang, Jicheng Shen, and Zhaodong Wang. "Investigation on the Formation of Cr-Rich Precipitates at the Interphase Boundary in Type 430 Stainless Steel Based on Austenite–Ferrite Transformation Kinetics." Metals 9, no. 10 (2019): 1045. http://dx.doi.org/10.3390/met9101045.

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The Cr-rich precipitates at the interphase boundary in stainless steels not only lead to the sensitization, which further induces the intergranular corrosion and intergranular stress corrosion cracking, but also significantly deteriorate the ductility and toughness. In this work, the formation of Cr-rich precipitates at the interphase boundary in type 430 stainless steel was investigated from the perspective of austenite–ferrite transformation kinetics. Cyclic heat treatment was firstly conducted to reveal the kinetic mode of transformation behavior, i.e., local equilibrium or para equilibrium

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10

Topolnikov, A. S. "Numerical Modeling of Evolution of Boundary Between Incompressible Gas and Liquid in Two-Dimensional Region." Proceedings of the Mavlyutov Institute of Mechanics 4 (2006): 224–36. http://dx.doi.org/10.21662/uim2006.1.020.

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The paper is devoted to numerical modeling of Navier–Stokes equations for incompressible media in the case, when there exist gas and liquid inside the rectangular calculation region, which are separated by interphase boundary. The set of equations for incompressible liquid accounting for viscous, gravitational and surface (capillary) forces is solved by finite-difference scheme on the spaced grid, for description of interphase boundary the ideology of Level Set Method is used. By developed numerical code the set of hydrodynamic problems is solved, which describe the motion of two-phase incompr

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11

Gnatchenko, S. L., N. F. Kharchenko, A. B. Chizhik, V. V. Eremenko, and R. Shimchak. "Investigation of the motion of the interphase magnetic domain boundary in DyFeO3." Soviet Journal of Low Temperature Physics 12, no. 10 (1986): 628–29. https://doi.org/10.1063/10.0031597.

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The field-dependence of the velocity of steady-state motion of an interphase magnetic domain wall in dysprosium orthoferrite is studied. Characteristic features of the motion of the interphase wall were observed: increase in the differential mobility accompanying an increase in the intensity of the driving field and asymmetry of the field-dependence of the velocity of the wall relative to the phase-transition field. It is shown that these features of the dynamics of the interphase wall are linked with the expansion of the wall when the applied field is different from the phase-transition field

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12

Poletaev G. M. and Rakitin R. Y. "Influence of the orientation of Ti-Al interphase boundary on the mutual diffusion rate at the solid and liquid states of aluminium: molecular dynamics simulation." Physics of the Solid State 64, no. 4 (2022): 398. http://dx.doi.org/10.21883/pss.2022.04.53495.247.

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The influence of the orientation of Ti-Al interphase boundary on the intensity of mutual diffusion at solid-phase and solid-liquid-phase contacts was studied by the method of molecular dynamics. Four orientations of the boundary with respect to the Ti (hcp) and Al (fcc) lattices were considered: (0001) : (111), (0001) : (001), (1010) : (111), (1011) : (001). At solid-phase contact, an important phenomenon influencing the intensity of mutual diffusion was the formation, due to the mismatch of the lattices of Ti and Al, of grain boundaries in Al parallel to the interphase boundary. This boundary

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13

Pędzich, Zbigniew, Krzysztof Haberko, Marek Faryna, and Krzystof Sztwiertnia. "Interphase Boundary in Zirconia – Carbide Particulate Composites." Key Engineering Materials 223 (February 2002): 221–26. http://dx.doi.org/10.4028/www.scientific.net/kem.223.221.

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14

Dorfman, Simon, David Fuks, Alex Gordon, A. V. Postnikov, and G. Borstel. "Movement of the interphase boundary inKNbO3under pressure." Physical Review B 52, no. 10 (1995): 7135–41. http://dx.doi.org/10.1103/physrevb.52.7135.

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15

Kubíček, Petr, and Libor Mrázek. "Diffusion in melt with nonstationary interphase boundary." Czechoslovak Journal of Physics 46, no. 6 (1996): 509–24. http://dx.doi.org/10.1007/bf01690672.

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16

Huang, Yunhao, Jincheng Wang, Zhijun Wang, and Junjie Li. "One-dimensional ledges and migration mechanism of incoherent interphase boundaries." Journal of Applied Crystallography 54, no. 1 (2021): 211–16. http://dx.doi.org/10.1107/s1600576720015587.

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Since the edge-to-edge matching relationship of close-packed planes on an incoherent interphase boundary was found, the one-dimensional ledge migration mechanism has been put forward. However, owing to the lack of direct experimental evidence, the existence of the one-dimensional ledge is still questioned and it is thus usually treated as just an assumption. In this study, focusing on the existence of one-dimensional ledges and the migration mechanism of incoherent interphase boundaries, an atomic scale investigation on the migration of incoherent interphase boundaries in a body- to face-cente

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17

Achenbach, J. D., and H. Zhu. "Effect of Interphases on Micro and Macromechanical Behavior of Hexagonal-Array Fiber Composites." Journal of Applied Mechanics 57, no. 4 (1990): 956–63. http://dx.doi.org/10.1115/1.2897667.

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The effect of interphase stiffness on microstresses and macromechanical behavior has been investigated for transverse loading of an hexagonal-array unidirectional fiber composite. The interphase is modeled by a layer which resists radial extension and circumferential shear deformation. Taking advantage of the periodicity of the medium, the states of stress, and deformation in a basic cell have been analyzed numerically by the use of the boundary element method. The circumferential tensile stress along the matrix side of the interphase and the radial stress in the interphase have been analyzed

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18

Cheng, S. C., and S. Sheinin. "Diffraction contrast images of interphase boundaries in cobalt." Proceedings, annual meeting, Electron Microscopy Society of America 48, no. 4 (1990): 364–65. http://dx.doi.org/10.1017/s0424820100174953.

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The boundaries between HCP and FCC phases in cobalt are generally expected to be of the type {111}FCC ‖ {001}HCP. Observations carried out by the authors indicate that the contrast exhibited by this type of boundary is very similar to the contrast exhibited by twin boundaries, as discussed by Sheinin and Corbett. These authors showed that images of twin boundaries consist of two intersecting sets of fringes with the possibility that one set is suppressed under certain diffraction conditions. The purpose of the work presented in this paper is to investigate the contrast exhibited by boundaries

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19

Eib, Wilhelm. "Interphase Diffusion with Curved Phase Boundaries." Defect and Diffusion Forum 258-260 (October 2006): 113–17. http://dx.doi.org/10.4028/www.scientific.net/ddf.258-260.113.

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The liquid phase of adhesives is most readily described by the theory of solutions. Adhesives act on phase boundaries. Yet right there, the fact that an adhesive is a solution does not fully describe its special performance. Some of the outstanding properties of adhesives are designed by the use non- soluble components, like Nanofillers, fibre reinforcements, color pigments, additives for the improvement of electrical and heat conductivity, etc. We would like to compare near phase boundary properties inside adhesives and outside near the substrates. We expect a relation between rheology and th

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20

Dzhezherya, Yu I., A. O. Khrebtov, D. P. Azarkh, and S. P. Kruchinin. "Sharp-pointed susceptibility of ferromagnetic films with magnetic anisotropy inhomogeneous in thickness." International Journal of Modern Physics B 32, no. 17 (2018): 1840034. http://dx.doi.org/10.1142/s0217979218400349.

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It is shown that in ferromagnetic films with anisotropy inhomogeneous in thickness, an interphase boundary can be formed for certain values and directions of the magnetic field. This boundary has a stable magnetic configuration. It is oriented parallel to the film plane and separates the regions with different orientations of the magnetization. In an alternating magnetic field, the interphase boundary oscillates, which may be accompanied by a resonance. The field and frequency dependences of the components of the magnetic susceptibility tensor are determined. It is shown that the susceptibilit

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21

Gulyaev, Yu V., and N. S. Shevyakhov. "Leaky Stoneley waves at a moving interphase boundary." Acoustical Physics 47, no. 5 (2001): 552–55. http://dx.doi.org/10.1134/1.1403544.

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22

Furuhara, T., and H. I. Aaronson. "On the mechanisms of interphase boundary carbide precipitation." Scripta Metallurgica 22, no. 10 (1988): 1635–37. http://dx.doi.org/10.1016/s0036-9748(88)80256-4.

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23

Hyland, R. W., M. Asta, S. M. Foiles, and C. L. Rohrer. "Al(f.c.c.):Al3Sc(L12) interphase boundary energy calculations." Acta Materialia 46, no. 10 (1998): 3667–78. http://dx.doi.org/10.1016/s1359-6454(98)00039-1.

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24

Liang, Q., and W. T. Reynolds. "Determining interphase boundary orientations from near-coincidence sites." Metallurgical and Materials Transactions A 29, no. 8 (1998): 2059–72. http://dx.doi.org/10.1007/s11661-998-0032-2.

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25

Kubíček, Petr, and Libor Mrázek. "Diffusion in solid phase with nonstationary interphase boundary." Czechoslovak Journal of Physics 46, no. 10 (1996): 931–41. http://dx.doi.org/10.1007/bf01795142.

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26

Hoyt, J. J. "Atomistic simulations of grain and interphase boundary mobility." Modelling and Simulation in Materials Science and Engineering 22, no. 3 (2014): 033001. http://dx.doi.org/10.1088/0965-0393/22/3/033001.

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27

Fuks, David, Simon Dorfman, Joshua Felsteiner, Alex Gordon, A. V. Postnikov, and G. Borstel. "Dynamics of the perovskite interphase boundary under pressure." Surface Science 352-354 (May 1996): 879–82. http://dx.doi.org/10.1016/0039-6028(95)01325-3.

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28

Полетаев, Г. М., та Р. Ю. Ракитин. "Влияние ориентации межфазной границы Ti-Al на скорость взаимной диффузии при твердом и жидком состояниях алюминия: молекулярно-динамическое моделирование". Физика твердого тела 64, № 4 (2022): 412. http://dx.doi.org/10.21883/ftt.2022.04.52180.247.

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The influence of the orientation of Ti-Al interphase boundary on the intensity of mutual diffusion at solid-phase and solid-liquid-phase contacts was studied by the method of molecular dynamics. Four orientations of the boundary with respect to the Ti (hcp) and Al (fcc) lattices were considered: (0001):(111), (0001):(001), (101 ̅0):(111), (101 ̅1):(001). At solid-phase contact, an important phenomenon influencing the intensity of mutual diffusion was the formation, due to the mismatch of the lattices of Ti and Al, of grain boundaries in Al parallel to the interphase boundary. This boundary was

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29

Xu, Wen, Qing Hua Zeng, Ai Bing Yu, and Donald R. Paul. "Determination of Interphase Thickness and Mechanical Properties of Effective Nanofillers in Polymer Nanocomposites by Molecular Dynamic Simulation." Materials Science Forum 654-656 (June 2010): 1654–57. http://dx.doi.org/10.4028/www.scientific.net/msf.654-656.1654.

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The properties of interphase in polymer composites are often different from those of bulk polymer matrix, which may include chemical, physical, microstructural, and mechanical properties. The nature of interphase is critical to the overall properties and performance of polymer materials, in particular in nanofiller reinforced composites. Experimental efforts have been made to determine the effective interphase thickness and its properties, for example, by nanoindentation and nanoscratch techniques. Yet, it is very difficult to quantify the interphase and its properties because of its nanoscale

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30

Furuhara, T., T. Maki, and K. Oishi. "Interphase boundary structure with irrational orientation relationship formed in grain boundary precipitation." Metallurgical and Materials Transactions A 33, no. 8 (2002): 2327–35. http://dx.doi.org/10.1007/s11661-002-0356-2.

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31

Lim, Joong Yeon, Han-Wool Kim, and Min-Wook Park. "Effect of interphase parameters on elastic modulus prediction for cellulose nanocrystal fiber reinforced polymer composite." Science and Engineering of Composite Materials 27, no. 1 (2020): 226–35. http://dx.doi.org/10.1515/secm-2020-0024.

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AbstractIn this study, the effective elastic modulus (Ec) of a cellulose nanocrystal fiber reinforced polymer composite was evaluated using the Mori-Tanaka and finite element (FE) model. The FE model was generated using a representative volume element with a periodic boundary condition. The mass fractions of the fiber in the composites (MFf) were set to 1, 2, and 3 wt.%. Elastic modulus values for interphase were input and were either uniform or exhibited a gradient. The E c for the uniform interphase region increased significantly with MFf, but was relatively low for interphase regions exhibi

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32

Апеков, Аслан Мартинович, and Ирина Гусейновна Шебзухова. "ORIENTATIONAL DEPENDENCE OF THE INTERPHASE ENERGY OF LOW-TEMPERATURE MODIFICATION OF TITANIUM AT THE BOUNDARY WITH AN ORGANIC LIQUID." Physical and Chemical Aspects of the Study of Clusters, Nanostructures and Nanomaterials, no. 14 (December 15, 2022): 17–23. http://dx.doi.org/10.26456/pcascnn/2022.14.017.

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В рамках электронно-статистического метода проведены вычисления межфазной энергии низкотемпературной модификации титана на границе с неполярными органическими жидкостями, получены поправки к межфазной энергии на дисперсионное взаимодействие ячеек Вигнера-Зейтца и осцилляцию электронной плотности в переходном слое, поляризацию поверхностных ионов металла и органической жидкости в поле полубесконечного металла. При расчете межфазной энергии рассматриваются изменения всех компонентов энергии металлической связи в переходном слое - собственные энергии электронного газа, энергии взаимодействия элек

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33

Muktepavela, Faina, and N. Zaporina. "Role of Diffusion in Superplasticity and Brittleness of Fine-Grained Binary Eutectics." Defect and Diffusion Forum 237-240 (April 2005): 745–50. http://dx.doi.org/10.4028/www.scientific.net/ddf.237-240.745.

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Mechanical properties of interphase boundaries (IB), stability of defects and microstructure in heavily deformed binary eutectics (Al-Sn, Zn-Sn, Pb-Sn, Cd-Sn, Bi-Sn) have been investigated at room temperature. Experiments were carried out on atomically clean surfaces of alloys and on bimetallic joints with clean interface. It has been shown that after severe deformation the phases are strengthened and relaxation processes occur mainly on the boundaries in all eutectics. For superplastic eutectics with low interphase boundary energy the intensive development of the diffusion – controlled proces

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34

Montheillet, Frank, and David Piot. "Combined Effects of Grain Boundary Convection and Migration in Dynamic Phase Transformations." Materials Science Forum 879 (November 2016): 72–77. http://dx.doi.org/10.4028/www.scientific.net/msf.879.72.

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During large strain deformation of polycrystals, grain or interphase boundaries are driven by the material flow, which is a convection movement. By contrast, upon static recrystallization or grain growth, their motion takes place with respect to matter, which is referred to as grain boundary or interphase migration. During hot working, where dynamic phase transformations commonly occur, convection and migration operate simultaneously. According to local geometrical (e.g., prescribed velocity field, grain boundary curvature) and physical (e.g., grain boundary mobility, dislocation densities) co

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35

Bojadjiev, Chr. "Nonlinear mass transfer and hydrodynamic stability in solubility phenomena." Pure and Applied Chemistry 74, no. 10 (2002): 1801–10. http://dx.doi.org/10.1351/pac200274101801.

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The dissolution of gases, liquids,or solids in liquids is a heterogeneous reaction, and in many cases, the reaction rate is limited by a diffusive transfer of substance in the boundary layer at the face interphase. In modern industry, intensive interphase mass transfer processes are accomplished by large concentration gradients. This can result in a set of nonlinear effects and the difference between experimental data and predictions of the linear mass transfer theory. One of the main nonlinear effects is a result of the induction of a secondary flow at the interface boundary. This can lead to

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36

Cheng, Zhao Gang, Xin Hua Ni, and Xie Quan Liu. "The Mechanical-Stress-Field of Matrix in Eutectic Ceramic Composite." Applied Mechanics and Materials 121-126 (October 2011): 3607–11. http://dx.doi.org/10.4028/www.scientific.net/amm.121-126.3607.

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Based on the interaction between nano-fiber and eutectic interphase, forth-phase mode is used to get the mechanical stress field of matrix in eutectic composite ceramics. The effective flexibility increment tensor of eutectic ceramic composite is obtained by the volumetric average strain. The remote stress boundary condition of the eutectic composite ceramis is accounted for getting the mechanical stress field in matrix. The results show the mechanical stress field of the matrix is associated with the stiffness and the volume fractions of each component in eutectic composite ceramic , the shap

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37

Maksymova, S. V., P. V. Kovalchuk, and V. V. Voronov. "Morphology of Barrier Coatings and Formation of an Interphase Boundary by Brazing of Dissimilar Alloys." METALLOFIZIKA I NOVEISHIE TEKHNOLOGII 45, no. 8 (2024): 963–74. http://dx.doi.org/10.15407/mfint.45.08.0963.

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38

Liu, Bin, Jianhua Liu, and Yongming Zhang. "A numerical study of the natural transition in a gas–liquid two-phase boundary layer over a flat plate taking account of interphase slip." AIP Advances 12, no. 8 (2022): 085218. http://dx.doi.org/10.1063/5.0096623.

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The natural transition in a gas–liquid two-phase boundary layer over an underwater flat plate is studied, taking into account the interphase slip between gas and liquid. An interphase slip model is proposed to determine the dynamic viscosity of the two-phase flow based on the physical origins of fluid viscosity. The model is then applied to laminar flow calculation, instability analysis, transition prediction, and prediction of the spectrum of wall fluctuating pressure in the laminar region. Numerical calculations are conducted for boundary layers for different void fractions, including liquid

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39

FURUHARA, Tadashi. "Interphase Boundary Structures in Phase Transformation and Precipitation Processes." Tetsu-to-Hagane 81, no. 2 (1995): 98–104. http://dx.doi.org/10.2355/tetsutohagane1955.81.2_98.

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40

Moritani, Tomokazu, Tadashi Furuhara, and Tadashi Maki. "Interphase Boundary Structure of Upper Bainite in Ferrous Alloy." Materia Japan 42, no. 12 (2003): 879. http://dx.doi.org/10.2320/materia.42.879.

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41

Kotova, O., S. Sun, E. Kotova, A. Ponariaydov, and R. Brodskaya. "Aluminosilicates: interphase boundary interactions and nature engineering of nanostructures." Journal of Physics: Conference Series 2315, no. 1 (2022): 012003. http://dx.doi.org/10.1088/1742-6596/2315/1/012003.

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Abstract The scientific basis for the development of innovative materials (microporous, nanostructured, composite) based on natural (technogenic and synthetic) aluminosilicate raw materials determine prototypes of new technologies in modern industry. Inspired by this, we studied interphase boundary interactions of the “aluminosicate resource – nanoproduct” type system as a key factor of aggregation and nanostructuring in the processes of mineral formation and synthesis. To study features of the heterogeneity of the structure and their correlations with the thermodynamic parameters of the forma

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42

Tadayon, K., R. Lemanis, B. Bar-On, and I. Zlotnikov. "Semi-empirical formulation of contact with an interphase boundary." Extreme Mechanics Letters 50 (January 2022): 101541. http://dx.doi.org/10.1016/j.eml.2021.101541.

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43

Belyaev, A. P., V. P. Rubets, and V. V. Antipov. "Formation of an interphase boundary under highly nonequilibrium conditions." Semiconductors 41, no. 12 (2007): 1457–59. http://dx.doi.org/10.1134/s1063782607120147.

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44

Boikov, Yu A., V. A. Danilov, I. T. Serenkov, V. I. Sakharov, and M. P. Volkov. "Electro- and Magnetotransport near a LaAlO3/SrTiO3 Interphase Boundary." Physics of the Solid State 60, no. 6 (2018): 1235–38. http://dx.doi.org/10.1134/s1063783418060082.

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45

Howe, J. "Aspects of interphase boundary structure in diffusional phase transformations." Acta Materialia 48, no. 15 (2000): 3977–84. http://dx.doi.org/10.1016/s1359-6454(00)00183-x.

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Poldushov, M. A., A. V. Polyanin, V. A. Moskalev, et al. "Assessment of Interphase Interaction at the Shungite/Elastomer Boundary." International Polymer Science and Technology 41, no. 3 (2014): 33–36. http://dx.doi.org/10.1177/0307174x1404100308.

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Brauner, Christian, Sawsane Nakouzi, Lucian Zweifel, and Jens Tresch. "Co-curing behaviour of thermoset composites with a thermoplastic boundary layer for welding purposes." Advanced Composites Letters 29 (January 1, 2020): 2633366X2090277. http://dx.doi.org/10.1177/2633366x20902777.

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The primary objective of this study is to determine the interphase behaviour of a thermoset epoxy resin that is commercially used for carbon fibre–reinforced composite materials in aerospace structures and a suitable thermoplastic material that can be used as a boundary layer. The thermoplastic boundary layer will be used for welding purposes to join structural components with a fraction of the effort compared to conventional gluing processes. In this study, the interphase formation of an epoxy resin with several thermoplastic materials, namely, polyetheretherketone, polyvinylidenfluoride, pol

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Mishuris, Gennady, Wiktoria Miszuris, and Andreas Öchsner. "Finite Element Verification of Transmission Conditions for 2D Heat Conduction Problems." Materials Science Forum 553 (August 2007): 93–99. http://dx.doi.org/10.4028/www.scientific.net/msf.553.93.

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Imperfect transmission conditions modelling a thin 2D intermediate layer between two bonded materials in a dissimilar strip have been derived and analytically analysed in another paper of this issue. In this paper, the validity of these transmission conditions for heat conduction problems has been investigated due to the finite element method (FEM) for various cases: namely, steady-state under uniform boundary conditions with constant or functional- dependent, i.e. temperature or spatial coordinate, conductivities of the interphase, non-uniform boundary conditions and finally for transient ana

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Howe, J. M., T. M. Murray, K. T. Moore, et al. "Understanding Interphase Boundary Dynamics by In Situ High-Resolution and Energy-Filtering Transmission Electron Microscopy and Real-Time Image Simulation." Microscopy and Microanalysis 4, no. 3 (1998): 235–47. http://dx.doi.org/10.1017/s1431927698980230.

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This study discusses the use of in situ high-resolution transmission electron microscropy (HRTEM) techniques to determine the structure, composition, and interphase boundary dynamics during phase transformations at the atomic level. Three main in situ HRTEM techniques are described: (1) in situ HRTEM dynamic studies that are performed on the same precipitate plates from different viewing directions to determine the three-dimensional structure of the interfaces; (2) in situ compositional mapping of precipitate interfaces obtained by energy-filtering TEM experiments at temperature in a HRTEM, an

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Peschanskiĭ, V. G., J. A. Roldan Lopez, and J. Idrogo. "Quantum oscillation effects in a thin layer of a normal metal in contact with a superconductor." Low Temperature Physics 22, no. 4 (1996): 327–30. https://doi.org/10.1063/10.0033978.

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The role of Andreev reflection of charge carriers at the interphase boundary in quantum magnetic size effects is considered for the magnetization of a thin layer of a normal metal on a superconducting substrate.

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