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Journal articles on the topic 'Binary liquid; Transport; Surface'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Limbu, H. K., K. K. Mishra, A. K. Sah, I. S. Jha, and D. Adhikari. "Theoretical investigation of mixing properties of Sb-Sn binary liquid alloy at 905K." BIBECHANA 15 (December 19, 2017): 1–10. http://dx.doi.org/10.3126/bibechana.v15i0.18306.

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The thermodynamic, microscopic, surface and transport properties of Sb-Sn liquid alloy at 905K have been studied using regular solution model. In thermodynamic properties, free energy of mixing(GM) , activity(a), entropy of mixing(SM), heat of mixing (HM) have been studied. To understand structural behavior of the liquid alloys concentration fluctuations in the long wavelength limit i.e. (Scc(0)) and short range order parameter (α1) have been computed. Surface property is studied with the help of Butler’s model while transport property is computed from Moelwyn-Hughes equation. The theoretical and experimental values of thermodynamic and microscopic properties of Sb-Sn liquid alloy at 905K have been compared. In present work the value of interchange energy (w) is found to be negative suggesting that there is a tendency of unlike atoms pairing (i.e. Sb-Sn) as the nearest neighbor indicating the ordering behavior in Sb-Sn liquid alloy. The symmetric behavior of concentration fluctuations of the liquid alloy has been well explained by the model. The temperature dependence of interchange energy (w) has been found during the computation of entropy of mixing (SM) and heat of mixing (HM) of the liquid alloy.BIBECHANA 15 (2018) 1-10

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2

Mishra, K. K., H. K. Limbu, B. Yadav, A. K. Khan, I. S. Jha, and D. Adhikari. "Thermodynamic, structural, surface and transport properties of Zn-Cd liquid alloy at 800 K." BIBECHANA 14 (November 28, 2016): 54–65. http://dx.doi.org/10.3126/bibechana.v14i0.15715.

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The mixing thermodynamic and structural properties of Zn-Cd liquid at 800K has been studied using Flory’s model. To explain the mixing properties of binary liquid alloys, size factor (ф) and ordering energy (ω) are taken into account. Thermodynamic properties like free energy of mixing (GM), activity (a), Heat of mixing (HM) and entropy of mixing (SM) and the microscopic properties like concentration fluctuation in the long wave length limit (Scc(0)) and chemical short range order parameter (α1) have been calculated. Surface property has also been studied with the help of Buttler’s model. The viscosity of the melt has been computed from Kaptay equation and BBK models. Both the viscosity and surface tension of the alloy increase with addition of zinc- component. BIBECHANA 14 (2017) 54-65

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3

Luo, Jian, Shen J. Dillon, and Martin P. Harmer. "Interface Stabilized Nanoscale Quasi-Liquid Films." Microscopy Today 17, no. 4 (June 26, 2009): 22–27. http://dx.doi.org/10.1017/s1551929509000121.

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A unique class of impurity-based quasi-liquid films has been widely observed at free surfaces, grain boundaries (GBs), and hetero-phase interfaces in ceramic and metallic materials (Figure 1). These nanometer-thick interfacial films can be alternatively understood to be: (a) quasi-liquid layers that adopt an “equilibrium” thickness in response to a balance of attractive and repulsive interfacial forces (in a high-temperature colloidal theory) or (b) multilayer adsorbates with thickness and average composition set by bulk dopant activities [1–2]. In several model binary systems, such quasi-liquid, interfacial films are found to be thermodynamically stable well below the bulk solidus lines, provoking analogies to the simpler interfacial phenomena of premelting in unary systems [3] and prewetting in binary de-mixed liquids [4]. These interfacial films exhibit structures and compositions that are neither observed nor stable as bulk phases, as well as transport, mechanical, and physical properties that are markedly different from bulk phases.

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4

Malinowski, Robert, Ivan P. Parkin, and Giorgio Volpe. "Nonmonotonic contactless manipulation of binary droplets via sensing of localized vapor sources on pristine substrates." Science Advances 6, no. 40 (September 2020): eaba3636. http://dx.doi.org/10.1126/sciadv.aba3636.

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Droplet motion on surfaces influences phenomena as diverse as microfluidic liquid handling, printing technology, and energy harvesting. Typically, droplets are set in motion by inducing energy gradients on a substrate or flow on their free surface. Current configurations for controllable droplet manipulation have limited applicability as they rely on carefully tailored wettability gradients and/or bespoke substrates. Here, we demonstrate the nonmonotonic contactless long-range manipulation of binary droplets on pristine substrates due to the sensing of localized water vapor sources. The droplet-source system presents an unexpected off-centered equilibrium position. We capture the underlying mechanism behind this symmetry breaking with a simplified model based on the full two-dimensional functional form of the surface tension gradient induced by the source on the droplet’s free surface. This insight on the transport mechanism enables us to demonstrate its versatility for applications by printing, aligning, and reacting materials controllably in space and time on pristine substrates.

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5

Ehrl, Andreas, Johannes Landesfeind, Wolfgang A. Wall, and Hubert A. Gasteiger. "Determination of Transport Parameters in Liquid Binary Lithium Ion Battery Electrolytes." Journal of The Electrochemical Society 164, no. 4 (2017): A826—A836. http://dx.doi.org/10.1149/2.1131704jes.

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6

Ehrl, Andreas, Johannes Landesfeind, Wolfgang A. Wall, and Hubert A. Gasteiger. "Determination of Transport Parameters in Liquid Binary Electrolytes: Part II. Transference Number." Journal of The Electrochemical Society 164, no. 12 (2017): A2716—A2731. http://dx.doi.org/10.1149/2.1681712jes.

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7

Anjum, Aisha, Sadaf Masood, Muhammad Farooq, Naila Rafiq, and Muhammad Yousaf Malik. "Investigation of binary chemical reaction in magnetohydrodynamic nanofluid flow with double stratification." Advances in Mechanical Engineering 13, no. 5 (May 2021): 168781402110162. http://dx.doi.org/10.1177/16878140211016264.

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This article addresses MHD nanofluid flow induced by stretched surface. Heat transport features are elaborated by implementing double diffusive stratification. Chemically reactive species is implemented in order to explore the properties of nanofluid through Brownian motion and thermophoresis. Activation energy concept is utilized for nano liquid. Further zero mass flux is assumed at the sheet’s surface for better and high accuracy of the out-turn. Trasnformations are used to reconstruct the partial differential equations into ordinary differential equations. Homotopy analysis method is utilized to obtain the solution. Physical features like flow, heat and mass are elaborated through graphs. Thermal stratified parameter reduces the temperature as well as concentration profile. Also decay in concentration field is noticed for larger reaction rate parameter. Both temperature and concentration grows for Thermophoresis parameter. To check the heat transfer rate, graphical exposition of Nusselt number are also discussed and interpret. It is noticed that amount of heat transfer decreases with the increment in Hartmann number. Numerical results shows that drag force increased for enlarged Hartmann number.

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8

Mahanthesh, B. "Magnetohydrodynamic flow of Carreau liquid over a stretchable sheet with a variable thickness." Multidiscipline Modeling in Materials and Structures 16, no. 5 (March 4, 2020): 1277–93. http://dx.doi.org/10.1108/mmms-11-2019-0205.

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PurposeThe magnetohydrodynamic (MHD) flow problems are important in the field of biomedical applications such as magnetic resonance imaging, inductive heat treatment of tumours, MHD-derived biomedical sensors, micropumps for drug delivery, MHD micromixers, magnetorelaxometry and actuators. Therefore, there is the impact of the magnetic field on the transport of non-Newtonian Carreau fluid in the presence of binary chemical reaction and activation energy over an extendable surface having a variable thickness. The significance of irregular heat source/sink and cross-diffusion effects is also explored.Design/methodology/approachThe leading governing equations are constructed by retaining the effects of binary chemical reaction and activation energy. Suitable similarity transformations are used to transform the governing partial differential equations into ordinary differential equations. Subsequent nonlinear two-point boundary value problem is treated numerically by using the shooting method based on Runge–Kutta–Fehlberg. Graphical results are presented to analyze the behaviour of effective parameters involved in the problem. The numerical values of the mass transfer rate (Sherwood number) and heat transfer rate (Nusselt number) are also calculated. Furthermore, the slope of the linear regression line through the data points is determined in order to quantify the outcome.FindingsIt is established that the external magnetic field restricts the flow strongly and serves as a potential control mechanism. It can be concluded that an applied magnetic field will play a major role in applications like micropumps, actuators and biomedical sensors. The heat transfer rate is enhanced due to Arrhenius activation energy mechanism. The boundary layer thickness is suppressed by strengthening the thickness of the sheet, resulting in higher values of Nusselt and Sherwood numbers.Originality/valueThe effects of magnetic field, binary chemical reaction and activation energy on heat and mass transfer of non-Newtonian Carreau liquid over an extendable surface with variable thickness are investigated for the first time.

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9

Frisken, B. J., Andrea J. Liu, and David S. Cannell. "Critical Fluids in Porous Media." MRS Bulletin 19, no. 5 (May 1994): 19–24. http://dx.doi.org/10.1557/s0883769400036526.

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The behavior of fluids confined in porous materials has been of interest to engineers and scientists for many decades. Among the applications driving this research are the use of porous membranes to achieve liquid-liquid separations and to deionize water, the use of porous materials as beds for catalysis, and the need to extract liquids (especially oil and water) from such media. Many of these applications depend on transport, which is governed by flow or diffusion in the imbibed fluids. Both the flow and diffusion of multiphase fluids in porous media, however, strongly depend on the morphology of phase-separated domains, and on the kinetics of domain growth. Thus, it is worthwhile to study the behavior of multiphase fluids in porous media in the absence of flow. Recently, much attention has focused on even simpler systems that still capture these essential features, namely, near-critical binary liquid mixtures and vapor-liquid systems in model porous media, such as Vycor and dilute silica gels. Although near-critical fluids may seem rather artificial as models for multiphase liquids, there are several advantages associated with them. In general, domain morphology and growth kinetics are governed primarily by competition between interfacial tension and the preferential attraction of one phase to the surface of the medium. In near-critical fluids, the relative strength of these two energy scales is sensitive to temperature, and can therefore be altered in a controlled fashion. In addition, the kinetics of domain growth are sensitive to the temperature quench depth, and can be controlled.

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10

Koirala, I., IS Jha, and BP Singh. "Theoretical investigation on ordering nature of Cd-Bi alloys in the molten state." BIBECHANA 11 (May 8, 2014): 70–78. http://dx.doi.org/10.3126/bibechana.v11i0.10382.

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Experimental determination of thermo-physical mixing properties of binary liquid alloys is a long and expensive task that becomes more complicated for some system which may be chemically active or radioactive or even may contain scarce components. Theoretical method, on the other hand reduces the time and efforts required, and are of great importance in predicting the properties. Now we have focused on theoretical model to study of the alloying behaviour of Cd-Bi alloys in the molten state at 773K. We have used simple statistical model to report the ordering nature of Cd-Bi liquid alloys through the study of surface properties, transport properties and various thermodynamic and microscopic functions. The knowledge of surface phenomena like surface segregation and surface tension is essential for the processing of materials and productions in the metallurgical industry. At the microscopic level, transport properties such as viscosity and diffusion coefficient help to understand about the mixing behaviour of the alloys forming molten metals. Thermodynamic properties provide information on the interaction, stability and bonding strength among the constituent atoms in the alloys. The microscopic properties are useful in obtaining the microscopic information on structure of molten alloys. Our theoretical analysis gives the negative energy parameter, which is found to be temperature dependent. Negative deviation from Raoultian behaviour is observed in the computed surface tension, thermodynamic and structural parameters of the alloys. But in case of viscosity isotherm positive deviation from ideality is observed. The computed results are in good agreement with experimental data. The analysis concluded that the alloy is of weakly interacting and heterocoordinating system. DOI: http://dx.doi.org/10.3126/bibechana.v11i0.10382 BIBECHANA 11(1) (2014) 70-78

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11

Hatton, D. C., and A. W. Woods. "Diffusion-controlled dissolution of a binary solid into a ternary liquid with partially molten zone formation." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 464, no. 2094 (March 10, 2008): 1615–37. http://dx.doi.org/10.1098/rspa.2007.0241.

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We build a theoretical model of equilibrium dissolution of a homogeneous, solid mixture of two salts A and B, KCl and NaCl being used as the type example, into an aqueous solution of the two salts, with diffusive transport. We find that there are two sharp dissolution fronts, separating fluid, a partially molten zone containing a single solid and mixed solid. The phase change happens almost entirely at the two sharp fronts. In equilibrium, the leading front exhibits a small amount of precipitation of NaCl, simultaneous with complete dissolution of KCl. There is a unique surface in the space of far-field fluid KCl concentration, far-field fluid NaCl concentration and solid composition, dividing conditions where NaCl is the solid in the partially molten zone, from conditions where KCl is the solid in the partially molten zone. The movement rates of the dissolution fronts decrease as the concentration of either salt in the far-field fluid is increased. The movement rates of the dissolution fronts increase as either far-field temperature is increased, but this effect is smaller than that of concentration. In most circumstances, the dissolution front for a given salt moves more slowly, the more of that salt is present in the original solid, although the mass dissolution rate is not greatly affected by the solid composition.

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12

Alexandrov, Dmitri V., and Peter K. Galenko. "A review on the theory of stable dendritic growth." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 379, no. 2205 (July 19, 2021): 20200325. http://dx.doi.org/10.1098/rsta.2020.0325.

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This review article summarizes the main outcomes following from recently developed theories of stable dendritic growth in undercooled one-component and binary melts. The nonlinear heat and mass transfer mechanisms that control the crystal growth process are connected with hydrodynamic flows (forced and natural convection), as well as with the non-local diffusion transport of dissolved impurities in the undercooled liquid phase. The main conclusions following from stability analysis, solvability and selection theories are presented. The sharp interface model and stability criteria for various crystallization conditions and crystalline symmetries met in actual practice are formulated and discussed. The review is also focused on the determination of the main process parameters—the tip velocity and diameter of dendritic crystals as functions of the melt undercooling, which define the structural states and transitions in materials science (e.g. monocrystalline-polycrystalline structures). Selection criteria of stable dendritic growth mode for conductive and convective heat and mass fluxes at the crystal surface are stitched together into a single criterion valid for an arbitrary undercooling. This article is part of the theme issue ‘Transport phenomena in complex systems (part 1)’.

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13

Ehrl, Andreas, Johannes Landesfeind, Wolfgang A. Wall, and Hubert A. Gasteiger. "Erratum: Determination of Transport Parameters in Liquid Binary Lithium Ion Battery Electrolytes: I. Diffusion Coefficient [J. Electrochem. Soc., 164, A826 (2017)]." Journal of The Electrochemical Society 165, no. 11 (2018): X12. http://dx.doi.org/10.1149/2.1171811jes.

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14

Gervasi, Natalie R., David O. Topping, and Andreas Zuend. "A predictive group-contribution model for the viscosity of aqueous organic aerosol." Atmospheric Chemistry and Physics 20, no. 5 (March 12, 2020): 2987–3008. http://dx.doi.org/10.5194/acp-20-2987-2020.

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Abstract. The viscosity of primary and secondary organic aerosol (SOA) has important implications for the processing of aqueous organic aerosol phases in the atmosphere, their involvement in climate forcing, and transboundary pollution. Here we introduce a new thermodynamics-based group-contribution model, which is capable of accurately predicting the dynamic viscosity of a mixture over several orders of magnitude (∼10-3 to >1012 Pa s) as a function of temperature and mixture composition, accounting for the effect of relative humidity on aerosol water content. The mixture viscosity modelling framework builds on the thermodynamic activity coefficient model AIOMFAC (Aerosol Inorganic–Organic Mixtures Functional groups Activity Coefficients) for predictions of liquid mixture non-ideality, including liquid–liquid phase separation, and the calorimetric glass transition temperature model by DeRieux et al. (2018) for pure-component viscosity values of organic components. Comparing this new model with simplified modelling approaches reveals that the group-contribution method is the most accurate in predicting mixture viscosity, although accurate pure-component viscosity predictions (and associated experimental data) are key and one of the main sources of uncertainties in current models, including the model presented here. Nonetheless, we find excellent agreement between the viscosity predictions and measurements for systems in which mixture constituents have a molar mass below 350 g mol−1. As such, we demonstrate the validity of the model in quantifying mixture viscosity for aqueous binary mixtures (glycerol, citric acid, sucrose, and trehalose), aqueous multicomponent mixtures (citric acid plus sucrose and a mixture of nine dicarboxylic acids), and aqueous SOA surrogate mixtures derived from the oxidation of α-pinene, toluene, or isoprene. We also use the model to assess the expected change in SOA particle viscosity during idealized adiabatic air parcel transport from the surface to higher altitudes within the troposphere. This work demonstrates the capability and flexibility of our model in predicting the viscosity for organic mixtures of varying degrees of complexity and its applicability for modelling SOA viscosity over a wide range of temperatures and relative humidities.

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15

Li, Jienan, Seanna M. Forrester, and Daniel A. Knopf. "Heterogeneous oxidation of amorphous organic aerosol surrogates by O<sub>3</sub>, NO<sub>3</sub>, and OH at typical tropospheric temperatures." Atmospheric Chemistry and Physics 20, no. 10 (May 25, 2020): 6055–80. http://dx.doi.org/10.5194/acp-20-6055-2020.

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Abstract. Typical tropospheric temperatures render possible phase states of amorphous organic aerosol (OA) particles of solid, semisolid, and liquid. This will affect the multiphase oxidation kinetics involving the organic condensed-phase and gaseous oxidants and radicals. To quantify this effect, we determined the reactive uptake coefficients (γ) of O3, NO3, and OH by substrate films composed of single and binary OA surrogate species under dry conditions for temperatures from 213 to 313 K. A temperature-controlled coated-wall flow reactor coupled to a chemical ionization mass spectrometer was applied to determine γ with consideration of gas diffusion transport limitation and gas flow entrance effects, which can impact heterogeneous reaction kinetics. The phase state of the organic substrates was probed via the poke-flow technique, allowing the estimation of the substrates' glass transition temperatures. γ values for O3 and OH uptake to a canola oil substrate, NO3 uptake to a levoglucosan and a levoglucosan / xylitol substrate, and OH uptake to a glucose and glucose / 1,2,6-hexanetriol substrate have been determined as a function of temperature. We observed the greatest changes in γ with temperature for substrates that experienced the largest changes in viscosity as a result of a solid-to-liquid phase transition. Organic substrates that maintain a semisolid or solid phase state and as such a relatively higher viscosity do not display large variations in heterogeneous reactivity. From 213 to 293 K, γ values of O3 with canola oil, of NO3 with a levoglucosan / xylitol mixture, and of OH with a glucose / 1,2,6-hexanetriol mixture and canola oil, increase by about a factor of 34, 3, 2, and 5, respectively, due to a solid-to-liquid phase transition of the substrate. These results demonstrate that the surface and bulk lifetime of the OA surrogate species can significantly increase due to the slowed heterogeneous kinetics when OA species are solid or highly viscous in the middle and upper troposphere. This experimental study will further our understanding of the chemical evolution of OA particles with subsequent important consequences for source apportionment, air quality, and climate.

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16

Borsoi, Giovanni, Barbara Lubelli, Rob van Hees, Rosário Veiga, and António Santos Silva. "Application Protocol for the Consolidation of Calcareous Substrates by the Use of Nanolimes: From Laboratory Research to Practice." Restoration of Buildings and Monuments 22, no. 4-6 (February 23, 2018): 99–109. http://dx.doi.org/10.1515/rbm-2016-0008.

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Abstract Calcareous materials such as limestone and lime-based mortars, widely used in the Built Heritage, are often subjected to degradation processes that can lead to loss of cohesion and material loss. Consolidation of these materials with liquid products via the surface is a common practice; however, the most used consolidation products (e. g. TEOS-based) show a poor physical-chemical compatibility with calcareous substrates. For application on calcareous materials, the so-called nanolimes, i. e. dispersions of lime nanoparticles in alcohols, are an alternative to TEOS-based products, thanks to their chemical compatibility with lime-based substrates. Nanolimes can help to recover a superficial loss of cohesion. However, their in-depth consolidation effect is not always satisfactory. Previous work has shown that a better deposition of lime nanoparticles in depth can be achieved by adapting the properties of the nanolime dispersion (kinetic stability and evaporation rate) to the moisture transport properties of the substrate, through optimization of the solvent. In this paper, freshly synthetized nanolimes were dispersed in pure ethanol and/or in binary mixture of ethanol (95 %) and water (5 %). These nanolimes were applied on Maastricht limestone and on a lime-based mortar by capillary absorption (method commonly used for laboratory tests) and by nebulization (method widely used in situ). The aim of this research is to fill the gap between laboratory tests and on site application, providing an application protocol for restorers and professionals in the field. The research shows that results obtained by application by capillary absorption do not always correspond to those obtained by nebulization. This fact should be considered when deciding on the use of a consolidation surface treatment in practice.

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17

Bringuier, E. "Transport of volume in a binary liquid." Physica A: Statistical Mechanics and its Applications 391, no. 21 (November 2012): 5064–75. http://dx.doi.org/10.1016/j.physa.2012.05.065.

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18

Jain, K. C., N. Gupta, and N. S. Saxena. "Transport Properties in Liquid Metal Binary Alloys." physica status solidi (b) 178, no. 1 (July 1, 1993): 109–14. http://dx.doi.org/10.1002/pssb.2221780109.

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19

Douillard, J. M., R. Bennes, M. Privat, and L. Tenebre. "Surface transitions in binary liquid mixtures." Journal of Colloid and Interface Science 106, no. 1 (July 1985): 146–53. http://dx.doi.org/10.1016/0021-9797(85)90390-x.

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20

Papaioannou, D., and C. Panayiotou. "Surface tension of binary liquid mixtures." Journal of Colloid and Interface Science 130, no. 2 (July 1989): 432–38. http://dx.doi.org/10.1016/0021-9797(89)90120-3.

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21

Speiser, R., D. R. Poirier, and K. Yeum. "Surface tension of binary liquid alloys." Scripta Metallurgica 21, no. 5 (May 1987): 687–92. http://dx.doi.org/10.1016/0036-9748(87)90385-1.

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22

Bhuiyan, G. M., I. Ali, and S. M. Mujibur Rahman. "Atomic transport properties of AgIn liquid binary alloys." Physica B: Condensed Matter 334, no. 1-2 (June 2003): 147–59. http://dx.doi.org/10.1016/s0921-4526(03)00040-1.

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23

MacGowan, David, and Denis J. Evans. "Heat and matter transport in binary liquid mixtures." Physical Review A 34, no. 3 (September 1, 1986): 2133–42. http://dx.doi.org/10.1103/physreva.34.2133.

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24

Nattland, Detlef, Andrei Turchanin, and Werner Freyland. "Surface freezing transitions in liquid binary alloys." Journal of Non-Crystalline Solids 312-314 (October 2002): 464–71. http://dx.doi.org/10.1016/s0022-3093(02)01716-7.

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25

Baumgärtl, Martin, Andreas Jentys, and Johannes A. Lercher. "Surface Effects Determining Transport in Binary Xylene Mixtures." Journal of Physical Chemistry C 124, no. 49 (December 1, 2020): 26814–20. http://dx.doi.org/10.1021/acs.jpcc.0c08477.

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26

Bhuiyan, E. H., A. Z. Ziauddin Ahmed, G. M. Bhuiyan, and M. Shahjahan. "Atomic transport properties of AgxSn1−x liquid binary alloys." Physica B: Condensed Matter 403, no. 10-11 (May 2008): 1695–703. http://dx.doi.org/10.1016/j.physb.2007.09.090.

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27

Vora, Aditya M. "Electrical Transport Properties of Liquid Rb1–XCsX Binary Alloys." Journal of Advanced Physics 4, no. 2 (June 1, 2015): 164–68. http://dx.doi.org/10.1166/jap.2015.1182.

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Hadkar, Ulhas Balkrishna, and Munira Aunali Loliwala. "Surface Tension Prediction of Organic Binary Liquid Mixtures." Asian Journal of Pharmacy and Technology 5, no. 2 (2015): 107. http://dx.doi.org/10.5958/2231-5713.2015.00016.1.

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Schmitz, J., J. Brillo, I. Egry, and R. Schmid-Fetzer. "Surface tension of liquid Al–Cu binary alloys." International Journal of Materials Research 100, no. 11 (November 2009): 1529–35. http://dx.doi.org/10.3139/146.110221.

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Brillo, Jürgen, Giorgio Lauletta, Luca Vaianella, Elisabetta Arato, Donatella Giuranno, Rada Novakovic, and Enrica Ricci. "Surface Tension of Liquid Ag–Cu Binary Alloys." ISIJ International 54, no. 9 (2014): 2115–19. http://dx.doi.org/10.2355/isijinternational.54.2115.

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Bardavid, S. M., G. C. Pedrosa, and M. Katz. "Surface Tensions of Some Nonelectrolyte Binary Liquid Mixtures." Journal of Colloid and Interface Science 165, no. 2 (July 1994): 264–68. http://dx.doi.org/10.1006/jcis.1994.1229.

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32

Ghasemian Lemraski, Ensieh, and Zohre Pouyanfar. "Surface Tension Prediction of Ionic Liquid Binary Solutions." Journal of Chemical & Engineering Data 59, no. 12 (December 2014): 3982–87. http://dx.doi.org/10.1021/je500479f.

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Brillo, J., and G. Kolland. "Surface tension of liquid Al–Au binary alloys." Journal of Materials Science 51, no. 10 (February 18, 2016): 4888–901. http://dx.doi.org/10.1007/s10853-016-9794-x.

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Kobatake, Hidekazu, Jürgen Brillo, Julianna Schmitz, and Pierre-Yves Pichon. "Surface tension of binary Al–Si liquid alloys." Journal of Materials Science 50, no. 9 (February 13, 2015): 3351–60. http://dx.doi.org/10.1007/s10853-015-8883-6.

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Whitmer, J. K., S. B. Kiselev, and B. M. Law. "Adsorption at the liquid-vapor surface of a binary liquid mixture." Journal of Chemical Physics 123, no. 20 (November 22, 2005): 204720. http://dx.doi.org/10.1063/1.2128705.

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36

Machunsky, Stefanie, and Urs Alexander Peuker. "Liquid-Liquid Interfacial Transport of Nanoparticles." Physical Separation in Science and Engineering 2007 (January 8, 2007): 1–7. http://dx.doi.org/10.1155/2007/34832.

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The study presents the transfer of nanoparticles from the aqueous phase to the second nonmiscible nonaqueous liquid phase. The transfer is based on the sedimentation of the dispersed particles through a liquid-liquid interface. First, the colloidal aqueous dispersion is destabilised to flocculate the particles. The agglomeration is reversible and the flocs are large enough to sediment in a centrifugal field. The aqueous dispersion is laminated above the receiving organic liquid phase. When the particles start to penetrate into the liquid-liquid interface, the particle surface is covered with the stabilising surfactant. The sorption of the surfactant onto the surface of the primary particles leads to the disintegration of the flocs. This phase transfer process allows for a very low surfactant concentration within the receiving organic liquid, which is important for further application, that is, synthesis for polymer-nanocomposite materials. Furthermore, the phase transfer of the nanoparticles shows a high efficiency up to 100% yield. The particle size within the organosol corresponds to the primary particle size of the nanoparticles.

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Nasyedkin, K. A., V. E. Sivokon, Yu P. Monarkha, and S. S. Sokolov. "Nonlinear surface electron transport over liquid helium." Low Temperature Physics 35, no. 10 (October 2009): 757–65. http://dx.doi.org/10.1063/1.3253395.

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Wu, Mingqiu, Johannes G. Khinast, and Stefan Radl. "Liquid transport rates during binary collisions of unequally-sized particles." Powder Technology 309 (March 2017): 95–109. http://dx.doi.org/10.1016/j.powtec.2016.12.080.

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39

Molin, Dafne, and Roberto Mauri. "Enhanced heat transport during phase separation of liquid binary mixtures." Physics of Fluids 19, no. 7 (July 2007): 074102. http://dx.doi.org/10.1063/1.2749810.

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40

Evans, Denis J., and David MacGowan. "Addendum to ‘‘Heat and matter transport in binary liquid mixtures’’." Physical Review A 36, no. 2 (July 1, 1987): 948–50. http://dx.doi.org/10.1103/physreva.36.948.

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41

Vora, Aditya M. "Electrical Transport Properties of K-Based Alkali Liquid Binary Alloys." International Letters of Chemistry, Physics and Astronomy 54 (July 2015): 56–72. http://dx.doi.org/10.18052/www.scipress.com/ilcpa.54.56.

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Abstract:

The electrical transport properties viz. the electrical resistivity (ρ), the thermoelectric power (TEP) and thermal conductivity (σ) of three K-based alkali liquid binary alloys viz. K1-XNaX, K1-XRbX and K1-XCsX were calculated from the pseudopotential form factors and Percus-Yevic (PY) hard sphere structure factors of Ashcroft and Langreth. The well recognized empty core model (EMC) pseudopotential of Ashcroft is used for the first time with seven local field correction functions due to Hartree (H), Hubbard-Sham (HS), Vashishta-Singwi (VS), Taylor (T), Ichimaru-Utsumi (IU), Farid et al. (F) and Sarkar et al. (S) in the present computation and found suitable for such study. It is conclude that, the comparison of present and experimental findings is highly encouraging.

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Szpakowska, Mariola, Zaklad Chemii Fizycznej, and Ottó B. Nagy. "Copper(II) Ion Transport Through Mono and Binary Liquid Membranes." Bulletin des Sociétés Chimiques Belges 99, no. 4 (September 1, 2010): 243–53. http://dx.doi.org/10.1002/bscb.19900990406.

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Szpakowska, Mariola, and Ottó B. Nagy. "Facilitated passive copper(II) ion transport through binary liquid membrane." Bulletin des Sociétés Chimiques Belges 99, no. 11-12 (September 1, 2010): 889–93. http://dx.doi.org/10.1002/bscb.19900991105.

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Antion, Caroline, and Dominique Chatain. "Liquid surface and liquid/liquid interface energies of binary subregular alloys and wetting transitions." Surface Science 601, no. 10 (May 2007): 2232–44. http://dx.doi.org/10.1016/j.susc.2007.03.026.

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Anusionwu, B. C. "Surface properties of some sodium-based binary liquid alloys." Journal of Alloys and Compounds 359, no. 1-2 (September 2003): 172–79. http://dx.doi.org/10.1016/s0925-8388(03)00213-5.

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Brillo, J., D. Chatain, and I. Egry. "Surface tension of liquid binary alloys – theory versus experiment." International Journal of Materials Research 100, no. 1 (January 2009): 53–58. http://dx.doi.org/10.3139/146.101787.

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Rudakov, O. B., D. S. Belyaev, E. A. Khorokhordina, and E. A. Podolina. "Surface tension of binary mobile phases for liquid chromatography." Russian Journal of Physical Chemistry A 81, no. 3 (March 2007): 366–69. http://dx.doi.org/10.1134/s0036024407030107.

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Kahl, Heike, Tino Wadewitz, and Jochen Winkelmann. "Surface Tension of Pure Liquids and Binary Liquid Mixtures." Journal of Chemical & Engineering Data 48, no. 3 (May 2003): 580–86. http://dx.doi.org/10.1021/je0201323.

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DiMasi, E., H. Tostmann, O. G. Shpyrko, M. Deutsch, P. S. Pershan, and B. M. Ocko. "Surface-induced order in liquid metals and binary alloys." Journal of Physics: Condensed Matter 12, no. 8A (February 17, 2000): A209—A214. http://dx.doi.org/10.1088/0953-8984/12/8a/325.

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Yeum, K. S., R. Speiser, and D. R. Poirier. "Estimation of the surface tensions of binary liquid alloys." Metallurgical Transactions B 20, no. 5 (October 1989): 693–703. http://dx.doi.org/10.1007/bf02655927.

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