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Prof. Dr. George Kaptay List of publications and independent citations (August, 2012)

(in the format, requested by the Hungarian Academy of Sciences)

Summarized scientific results

h-index1 = 16 (based on independent citations2), dh/dt = 1/year since the year of 2000, Cumulative impact factor3: around 115 (end of 2011: 76), Partial cumulative impact factor4: around 73 (end of 2011: 43), Publications: 158 journal papers, 1 book, 9 book chapters, 117 proceedings papers + 16 other

papers = 301 published items, Cited papers: 146 (average 7.1 citations / cited paper), ratio of cited papers: 49 %. Independent citations: 1039 (3.5 citations / published item).

Content Journal papers 2 Book chapters 85 Edited books or special journal issues 88 Papers on non-scientific subjects 89 Proceedings papers 91 Selected manuscripts 119 Statistics for publications and citations 121 h-index count 122 Cumulative impact factor count 125 Pink: not uploaded to MTMT databank yet, black: uploaded to MTMT.

1 H-index is the number of papers, each with at least the same number of independent citations: see the following

16+2 papers: J84 – J102 – J46 – J87 - J11 – P41 – J48 – J90 – P79 – P77 – J57 – P65 – J95 – J23 – J28 – J94 – J96 - P96.

2 Independent citations: none of the authors overlap in the citing and cited papers. Citations, published in any journal, proceedings, book chapters or Thesis count, except those Thesis, for which I am a supervisor.

3 Cumulative impact factor = the sum of the impact factors of the journal in the year (except the last year, extrapolated from the data of the previous year) of publication of each given paper.

4 Partial cumulative impact factor = the sum of the ratio of the impact factors of the journal in the year (except the last year, extrapolated from the data of the previous year) of publication of the given paper, divided by the number of authors of the same paper.

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J. Journal papers (IF = journal impact factors) J158. G.Kaptay: The essence of equilibrium of materials in 17 short statements – Mater Sci Eng, 2012, vol.37, No.2, pp.37-42. (IF = 0). J157. G.Kaptay: On the interfacial energy of coherent interfaces. Acta Mater, doi: 10.1016/j.actamat.2012.09.002 (2011-IF = 3.755). J156. P. Baumli, J. Sychev, I. Budai, J.T. Szabo, G.Kaptay: Fabrication of carbon fiber reinforced aluminum matrix composites via a titanium-ion containing flux. Composites A, doi: 10.1016/j.compositesa.2012.08.021 (2011 IF = 2.695) J155. G.Kaptay: On the order–disorder surface phase transition and critical temperature of pure liquid metals originating from bcc, fcc and hcp crystal structures – Int. J. Thermophysics, 2012, DOI: 10.1007/s10765-012-1270-5. (2011-IF = 0,953). J154. T. Sándor, C. Mekler, J. Dobránszky, G. Kaptay: An improved theoretical model for A-TIG welding based on surface phase transition and reversed Marangoni flow – Metall Mater Trans A, 2012, doi: 10.1007/s11661-012-1367-2. (2011-IF = 1.545). J153. G.Kaptay: Nano-Calphad: extension of the Calphad method to systems with nano-phases and complexions - J Mater Sci, 2012, DOI: 10.1007/s10853-012-6772-9. (2011-IF = 2.015) J.152. Kaptay Gy.: Hány alapmértékegységre van szükségünk az általunk ismert világ leírásához? Magyar Tudomány, 2012, No.7, pp.856-860. (IF = 0) J.151. D. Janovszky, K.Tomolya, A.Sycheva, G. Kaptay: Stable miscibility gap in liquid Cu-Zr-Ag ternary alloy, J Alloys Compds, 2012, vol.541, pp.353-358. (2011-IF = 2,289). J.150. Zs. Baji, A. Szanyo, Gy. Molnár, A.L. Toth, G. Pető, K. Frey, E. Kotai, G. Kaptay: Formation of Nanoparticles by Ion Beam Irradiation of Thin Films. JNN (Journal of Nanoscience and Nanotechnology), 2012, vol. 12, No.6, pp. 5009-5015 (2011-IF = 1.563). J.149. O.Z.Nagy, J.T.Szabo, G.Kaptay: Stabilization of metallic emulsions by in-situ precipitating intermetallic layers – Intermetallics, 2012, vol.26, pp.26-30. (2011-IF = 1.649). J.148. G.Kaptay: On the size and shape dependence of the solubility of nano-particles in solutions – Int. J. Pharmaceutics (IJP), 2012, vol.430, pp.253-257. (2011-IF = 3.350). J.147. K. L. Juhasz, P. Baumli, G. Kaptay: Fabrication of carbon fibre reinforced, aluminium matrix composite by potassium iodide (KI) – potassium hexafluorotitanate (K2TiF6) flux, Mater.-wiss. Werkstofftech. 2012, vol. 43, No. 4, pp.310-314. (2011-IF = 0.543) J.146. G.Kaptay: The Gibbs equation versus the Kelvin and the Gibbs-Thomson equations to describe nucleation and equilibrium of nano-materials, JNN (Journal of Nanoscience and Nanotechnology), 2012, vol.12, No.3, pp. 2625-2633 (2011-IF = 1.563).

http://www.ingentaconnect.com/content/asp/jnn;jsessionid=5gonqwfyhi5l.victoriahttp://www.ingentaconnect.com/content/asp/jnn;jsessionid=5gonqwfyhi5l.victoria

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J.145. G. Kaptay: On the atomic masses (weights?) of the elements, J. Min. Metall. B, 2012, vol.48, pp. 153-159 (2011-IF = 1.317). J144. G.Kaptay: Interfacial Forces in Dispersion Science and Technology - Journal of Dispersion Science and Technology, 2012, vol.33, pp.130-140 (2011-IF = 0.560). J143. G.Kaptay: On the optimum contact angle of stability of foams by particles – Advances in Colloid and Interface Science, 2012, vol.170, pp. 87-88 (2011-IF = 8.120). J.142. G.Kaptay: The conversion of phase diagrams of solid solution type into electrochemical synthesis diagrams for binary metallic systems on inert cathodes - Electrochimica Acta, 2012, vol.60, pp.401-409. (2011-IF = 3.832) J.141. Y. Tang, Y. Du, L. Zhang, X. Yuan, G.Kaptay: Thermodynamic description of the Al–Mg–Si system using a new formulation for the excess Gibbs energy – Thermochimica Acta, 2012, vol.527, pp.131-142. (2011-IF = 1.805). J.140. G.Kaptay: On the tendency of solutions to tend toward ideal solutions at high temperatures – Metall Mater Trans A, 2012, vol.43, pp. 531-543. (2011-IF = 1.545). J.139. G.Kaptay: Interfacial phenomena in producing metallic materials. Part 5: The interfacial spreading force (in Hungarian). – BKL Kohászat, 2011., vol.144., No.5., pp. 9-13. (IF = 0) J.138. G.Kaptay: On the five base quantities of nature and SI (The International system of Units) – JMM B, 2011, vol47, No.2, pp.241-246. (IF = 1.317). J138-c1. KW Craig: No child left behind: teaching the metric system in US schools – Int J Appl Sci Technol,

2012, vol.2, No.4, pp.40-48. – „Although there are seven base units in SI, “it is claimed that five is the smallest number of base quantities that is sufficient to define all derived quantities and allows the description of all natural phenomena … length, mass, time, temperature and electric charge … The first four … coincide with the current list of base quantities in SI” (Kaptay, 2011, p. 242). There is a proposal to replace electric current with electric charge and to eliminate both the amount of substance and luminous intensity.” – p.41.

J.137. D.Madarasz, I.Budai, G.Kaptay: Fabrication of SiC-particles shielded Al-spheres upon recycling Al/SiC composites – Metal Mater Trans A, 2011, Volume 42, Number 6, 1439-1443 (IF = 1.545). J137-c1. Baumli P.: Fémmátrixú kompozitok előállítása öntészeti módszerekkel – CD-Proc. of 26. Int. Sci. Conf.

microCAD, 29-30 March, 2012. – „A NaCl-KCl-KF típusú sókeverékkel az alumínium olvadékban lévő SiC szemcsék is eltávolíthatóak [J137].” – 4.o.

J136. I.Budai, O.Z.Nagy, G.Kaptay: Inversion of a liquid Bi/Al metallic emulsion stabilized by solid SiC particles, Coll Surf A, 2011, vol.377, pp.325-329 (IF = 2.236) J.135. O.Verezub, Z.Kálazi, A.Sytcheva, L.Kuzsella, G.Buza, N.V.Verezub, A.Fedorov, G.Kaptay: Performance of a cutting tool made of steel matrix surface nano-composite produced by in-situ laser melt injection technology – J Mater Process Technol., 2011, vol.211, pp.750-758 (IF = 1.783)

http://www.springerlink.com/content/1073-5623/42/6/

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J135-c1. Baumli P.: Fémmátrixú kompozitok előállítása öntészeti módszerekkel – CD-Proc. of 26. Int Sci Conf microCAD, 29-30 March, 2012. – „Lézer segítségével felületi kompozitok állíthatóak elő. Ebben az esetben a mátrix anyagául szolgáló fém felületét lézerrel megolvasztják, és az így kialakult fémtócsába megfelelő sebességgel lövik az erősítő fázisnak szánt szemcséket [J135].” – 4.o.

J135-c2. C.W.Rejil, I.Dinaharan, S.J.Vijay, N.Murugan: Microstructure and sliding wear behavior of AA6360/(TiC+B4C) hybrid surface composite layer synthesized by friction stir processing on aluminum substrate. Mater Sci Eng A, 2012, vol.552, pp.336-344. „SCLs (surface composite layers) are fabricated using conventional liquid phase processing methods such as high energy laser melt injection [J135], etc… „ – p.336.

J134. I.Budai, G.Kaptay: Monotectic Al/Cd alloys with homogeneously dispersed Cd-droplets stabilized by strontium aluminide precipitates – Intermetallics, 2011, vol.19. pp.423-425 (IF = 1.649). J.133. Kaptay Gy.: Határfelületi jelenségek a fémesanyaggyártásban. 4.rész. A határfelületi gradiens erő – BKL Kohászat, 2010., 143. évf., 5. szám, 45-54.o. (IF = 0) J.132. G.Kaptay: The Extension of the Phase Rule to Nano-Systems and on the Quaternary Point in One-Component Nano Phase Diagrams - J. Nanosci. Nanotechnol., 2010, vol.10, pp.8164–8170. (IF = 1.352). J.131. M.Reger, B.Vero, I.Kardos, E.R.Fabian, G.Kaptay: Diffusion of carbon in the centerline region of continuous cast slabs – Mater Sci Forum, 2010, vol.659, pp.441-446 (IF = 0) J.130. Kaptay Gy.: Határfelületi jelenségek a fémesanyaggyártásban. 3.rész. A görbület indukálta határfelületi erő – BKL Kohászat, 2010., 143. évf., 3. szám, 33-38. (IF = 0) J.129. P.Baumli, J.Sytchev, G.Kaptay: Perfect wettability of carbon by liquid aluminum achieved by a multifunctional flux. J Mater Sci, 2010, vol.45, pp.5177-5190. (IF = 1.859). J129-c1. I.N.Orbulov: Infiltration of ceramic microballons by liquid metals – research plan for SCIEX-NMS,

February, 2011, 12 pp. – „There are many papers in the professional literature which are dealing with the phenomenon of infiltartion [J129]” – p.9.

J129-c2. Lévai Gábor (tud. vez.: dr. Török Tamás): Acéllemezek színes tűzi horganyzása, 6. doktori szeminárium, 2011, június 14., 28 oldal. – “Kaptay és mtsai több alkalommal publikáltak pozitív eredményeket alumíniumnak K2TiF6 sóval történő ötvözéséről [129]”. – p.19.

J129-c3. W.Xi, R.L. Peng, W. Wu, N. Li, S. Wang, S. Johansson: Al2O3 nanoparticle reinforced Fe-based alloys synthesized by thermite reaction – J Mater Sci, 2012, vol.47, pp.3585-3591 – „Many studies demonstrate that a low interfacial energy between ceramic particles and metal matrix is the most important condition for obtaining homogeneous distribution of ceramic particles in the metal matrix when a metal matrix components is produced by solidification process [J129]” – p.3588.

J.128. Á.E. Horváth, F. Járai-Szabó, G.Kaptay, R.Vajtai, Z.Néda: Pattern formation and selection in nanotube arrays - Univ Polit Bucharest Sci Bull – Ser A - Appl Math Phys, 2010, vol.72, Iss.1, pp.27-32. (IF = 0.253). J.127. I.Budai, G.Kaptay: Wettability of SiC and alumina particles by liquid Bi under liquid Al – J. Mater Sci, 2010, vol.45, pp.2090-2098. (IF = 1.859) J127-c1. I.Kaban, M.Köhler, W.Hoyer, L.Ratke: Catalytic efficiency of oxide particles on heterogeneous

nucleation in aluminium alloy with miscibility gap – Hig Temperatures – High Pressures, 2010, vol.39, pp.347-355. – „In this case, the advancing contact angle is around 10 degrees and the receeding contact angle is around zero, which correlates with the results of work [J127] were the perfect wetting of alumina by Bi- and Pb-rich phase has been reported” – p.352.

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J127-c2. I.Kaban, M.Köhler, L.Ratke, W.Hoyer, N.Mattern, J.Eckert, A.L.Geer: Interfacial tension, wetting and nucleation in Al-Bi and Al-Pb monotectic alloys – Acta mater, 2011, vol.59, pp. 6880-6889 – „Budai and Kaptay [J127] found that Al2O3 particles were perfectly wetted by the Bi-rich phase in a solidified Al-Bi alloy.” – p.6881.

J.126. Kaptay Gy.: Határfelületi jelenségek a fémesanyaggyártásban. 2.rész. A határfelületi összehúzó erő – BKL Kohászat, 2009., 142. évf., 6. szám, 37-46. (IF = 0)

J.125. J.Sytchev, G.Kaptay: Influence of alkali metal on the erosion of a graphite cathode and morphology of carbon nanotubes – Electrochim Acta, 2009, vol.54, pp. 6725-6731. (IF = 3.325) J125-c1. C.Schwandt, A.T.Dimitrov, D.J.Fray: The preparation of nano-structured carbon materials by

electrolysis of molten lithium chloride at graphite electrodes – J Electroanal Chem, 2010, vol.647, pp.150-158 – „Kaptay and co-workers also investigated the electrolytic preparation method. Carbonaceous products were prepared by using various molten salt electrolytes and fundamental studies likewise suggested alkali metal intercalation into graphite as an essntial step of the process [J125]” – p.151

J125-c2. A.R.Kamali, D.J.Fray, C.Schwandt: Thermokinetic characterisation of lithium chloride – J Therm Anal Calorim, 2011, vol.104, pp.619-626. “More recent investigations have shown that intercalation of lithium into graphite may also proceed at elevated temperatures as high as 625 to 900 C [J125]” – p.619.

J125-c3. AR Kamali, C Schwandt, DJ Fray: Effect of graphite electrode material on the characteristics of molten salt electrolitically produced carbon nanomaterials – Mater Charact, 2011, vol.62, pp. 987-994. – „Fundamental investigations have reveasled that the molten salt electrolytic formation of carbon nanomaterials commences with the intercalation of alkali metal from the molten salt electrolyte into the graphitic cathode [J125]” – p.987.

J125-c4. C.Schwandt, AT Dimitrov, DJ Fray: High yield synthesis of multi-walled carbon nanotubes from graphite by molten salt electrolysis – Carbon, 2012, vol.50, pp. 1311-1315 – „It is generally accepted that the first step of the cathodic reduction is the intercalation of the alkali metal into the spacings between the graphitic layers and the formation of intercalation compounds, MeCx [J125]” – p.1311.

J125-c5. A. Juhasz-Szalai, E. Kiss-Toth-Dojcsak, P. Koska, J. Szebeni, B. Fodor: Characteristic features of carbon nanotubes and their application in living systems – Egészségtudományi Közlemények, 2012, vol.2, No.1, pp.105-111 – “Several techniques have been developed for the synthesis of CNTs, including …. molten chloride electrolysis [J125]…” – p.106.

J125-c6. Hui Huang, Yang Xia, Xinyong Tao, Jun Du, Junwu Fang, Yongping Gan and Wenkui Zhang: Highly efficient electrolytic exfoliation of graphite into graphene sheets based on Li ions intercalation–expansion–microexplosion mechanism - J. Mater. Chem., 2012, vol.22, pp. 10452-10456.

J125-c7. A.R. Kamali, G. Divitini, C. Schwandt, D.J. Fray, Correlation between microstructure and thermokinetic characteristics of electrolytic carbon nanomaterials, Corrosion Science (2012), doi: http://dx.doi.org/ - „…the reaction commences with the diffusion-controlled intercalation of Li into the bulk of the graphite cathode, and it has also been considered that Li is simply deposited onto the surface of the graphite cathode in case the rate of Li generation is faster than that of Li inward diffusion [J125].”

J.124. O. Verezub, Z. Kálazi, G. Buza, N. V. Verezub, G. Kaptay: Classification of laser beam induced surface engineering technologies and in situ synthesis of steel matrix surface nanocomposites - Surface Engineering, 2011, vol.27, No.6, pp. 428-435 (2010-IF = 0.633) J.123. Kaptay György: Határfelületi jelenségek a fémesanyaggyártásban. 1. rész. A határfelületi erők osztályozása. BKL Kohászat, 2009., 142. évf., 3. szám, 39-46.o. Helyreigazítás: 2009., 142. évf., 5. szám, 43. o. J.122. O. Verezub, Z. Kálazi, G. Buza, N.V. Verezub, G. Kaptay: In-situ synthesis of a carbide reinforced steel matrix surface nanocomposite by laser melt injection technology and subsequent heat treatment, Surface & Coatings Technology, 2009, vol. 203, pp.3049-3057. (IF = 1.793)

http://dx.doi.org/

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J122-c1. E.Laszlo, A.Sytcheva, J.Szucs: Drilling of aluminium alloys and composites – Diáktudomány, A Miskolci Egyetem tudományos diákköri munkáiból, 2010, Miskolc, pp.87-98, ISBN 978-963-661-932-9 – “A kompozitok és nano-kompozitok fejlesztése az egyik fontos mérnöki feladat anyagtudomány és gépgyártástechnológia határterületén [J122]”.

J122-c2. M.J.Hamedi, M.J.Torkamany, J.Sabbaghzadeh: Effect of pulsed laser parameters on in-situ TiC synthesis in laser surface treatment – Opt Lasers Eng, 2011, vol.49, pp.557-563. – “Recently, the applications of the titanium carbide (TiC) composites have been increased … [J122]..” – p.557.

J122-c3. B.S. Yilbas, S.S. Akhtar, A. Matthews, C. Karatas: Laser treatment of carbon film coated steel surface, Surface Eng, 2012, vol.28, No.1, pp.57-67.

J122-c4. Baumli P.: Fémmátrixú kompozitok előállítása öntészeti módszerekkel – CD-Proc. of 26. Int Sci Conf microCAD, 29-30 March, 2012. – „Lézer segítségével felületi kompozitok állíthatóak elő. Ebben az esetben a mátrix anyagául szolgáló fém felületét lézerrel megolvasztják, és az így kialakult fémtócsába megfelelő sebességgel lövik az erősítő fázisnak szánt szemcséket [J122].” – 4.o.

J122-c5. A.P.I. Popoola, B.A. Obadele, O.M. Popoola: Effects of TiC-particulate distribution in AISI 304L stainless steel matrix - Digest Journal of Nanomaterials and Biostructures, 2012, vol. 7, No. 3, pp. 1245 – 1252. „In the present investigations, TiC particulate reinforced austenitic stainless steel has been fabricated using laser processing. Lately, the applications of carbides especially titanium carbide (TiC) composites have increased. This is as a result of the new and promising materials for wearresistant parts and high temperature engineering structural components [J122], high specific strength, low density and high elastic modulus.” – p.1246.

J.121. I.Budai, G.Kaptay: A new class of engineering materials: particles stabilized metallic emulsions and monotectic alloys, Metall. Mater Trans A, 2009, vol.40A, pp.1524-1528. (IF = 1.564) J121-c1. S.E.Friberg: Foams from Non-aqueous systems – Curr Opinion Coll Interface Sci, 2010, vol.15,

pp.359-364 – “The analysis of stability and general properties of solid foams, on the other hand, has gained a separate place in the scientific literature against the fact that their properties are as much dependent on details of their preparation and manufacturing as on basic collid phenomena and the latter have first been adequately examined [J121].” – p.359, “In the area of metallic foams truly significant progress was made by Kaptay and collaborators [121]….” – p. 362.

J121-c2. I.Kaban, M.Köhler, W.Hoyer, L.Ratke: Catalytic efficiency of oxide particles on heterogeneous nucleation in aluminium alloy with miscibility gap – Hig Temperatures – High Pressures, 2010, vol.39, pp.347-355. – “Unfortunately, there are practically no data on the wetting of solids at the liquid-liquid interfaces in metallic monotectic alloys (a short view of the state of the art can be found in the recent work of Budai and Kaptay [J121])” – p.348. „In this case, the advancing contact angle is around 10 degrees and the receeding contact angle is around zero, which correlates with the results of work [J121] were the perfect wetting of alumina by Bi- and Pb-rich phase has been reported” – p.352.

J121-c3. I.Kaban, M.Köhler, L.Ratke, W.Hoyer, N.Mattern, J.Eckert, A.L.Geer: Interfacial tension, wetting and nucleation in Al-Bi and Al-Pb monotectic alloys – Acta mater, 2011, vol.59, pp.6880-6889 – „Budai and Kaptay [J121] found that Al2O3 particles were perfectly wetted by the Bi-rich phase in a solidified Al-Bi alloy. On the other hand, the contact angle with SiC particles at the interface between two solid phases in an Al-Bi-Si alloy was about 90o [J121]” – p.6881.

J121-c4. T.Frolov, KA Darling, LJ Kecskes, Y.Mishin: Stabilization and strengthening of nanocrystalline copper by alloying with tantalum – Acta Mater, 2010, vol.60, pp. 2158-2168 – “Alloying with immiscible elemenets is a promising approach to the design of materials with extraordinary structural stability and mechanical strength at high temperatures [J121]” – p.2158.

J.120. T.Gábor, F.H.Kármán, J.Sytchev, E.Kálmán, G.Kaptay: The separation of carbon nanotubes from chlorides – Carbon, 2009, vol.47, pp.1195-1198. (IF = 4.504) J120-c1. C.Schwandt, A.T.Dimitrov, D.J.Fray: The preparation of nano-structured carbon materials by

electrolysis of molten lithium chloride at graphite electrodes – J Electroanal Chem, 2010, vol.647, pp.150-158 – „The separation of the nano-structured components from residual salt and unreacted graphite needs to be optimized. In this context, the suitability of a recently developed extraction technique using ethil acetate [J120] will be ascertained” – p.158

J120-c2. Graham KA, Kulawiec M, Owens KM, Li XR, Desouki MM, Chandra D, Singh KK: NADPH oxidase 4 is an oncoprotein localized to mitochondria, CANCER BIOLOGY & THERAPY 10: (3) Paper 12207. (2010)

J120-c3. A. Juhasz-Szalai, E. Kiss-Toth-Dojcsak, P. Koska, J. Szebeni, B. Fodor: Characteristic features of carbon nanotubes and their application in living systems – Egészségtudományi Közlemények, 2012,

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vol.2, No.1, pp.105-111 – “Several techniques have been developed for the synthesis of CNTs, including …. molten chloride electrolysis [J120]…” – p.106.

J.119. O.N.Verezub, G.Kaptay, G.Buza, N.V.Verezub: The modification of surface layers of materials by laser alloying method. Part II. Laser melt injection technology of instrumental carbon steels - Journal of Functional Materials, 2008, vol.2, No.4, pp.137-143. (in Russian). (IF = 0) J.118. O.N.Verezub, G.Kaptay, G.Buza, N.V.Verezub: The modification of surface layers of materials by laser alloying method. Part I. Journal of Functional Materials, 2008, vol.2, No.3, pp.82-91. (in Russian). (IF = 0) J.117. P.Baumli, G.Kaptay: Wettability of carbon surfaces by pure molten alkali chlorides and their penetration into a porous graphite substrate – Mater Sci Eng A, 2008, vol.495, pp.192-196. (IF = 1.860) J117-c1. J.F.Cooper J.R.Selman: Electrochemical Oxidation of Carbon for Electric Power Generation: A Review

– Abstract Book of the 214th Meeting of the Electrochemical Society, October 2008 http://ecsmeet7.peerxpress.org/ms_files/ecsmeet7/2008/12/15/00001942/00/1942_0_art_0_kbxyy3.pdf - „A recent study of graphite wetting in molten chlorides indicates strong dependence on cationic composition and temperature [J117]”

J117-c2. N.Esutathopoulos, B.Drevet, S.Brandon, A.Virozub: Basic principles of capillarity in relation to crystal growth – Chapter 1 in: Crystal Growth Processes Based on Capillarity: Czochralski, Floating Zone, Shaping and Crucible Techniques, ed. by T.Duffar, 2010, John Wiley and Sons Ltd. – „The thermodynamic adhesion of molten halides on carbon is weak, as ensured solely by physical interactions [J117]. From modeling molten halide / graphite interactions, it was shown that for the same type of halides (for instance chlorides), when the surface tension decreases, the work of adhesion increases rapidly. According to the Young-Dupré equation, this implies a strong decrease in the contact angle (Table 1.8). Table 1.8 Reprinted with permission from [J117], copyright 2008 Elsevier Ltd.” – p.27.

J117-c3. X. Liu, Z. Wang, S. Zhang: Molten Salt Synthesis and Characterization of Titanium Carbide-Coated Graphite Flakes for Refractory Castable Applications – Int J Appl Ceram Technol, 2011, vol. 8, pp.911-919 – „Among the three molten salts, NaCl has the highest viscosity and wets graphite poorly [J117]; therefore, the transport of Ti to the surface of graphite will be hindered considerably. Although LiCl has the lowest viscosity it does not wet graphite [J117] and consequently the delivery of Ti to the reaction sites on the graphite surface becomes difficult. Differently from these two molten salts, KCl wets graphite well [J117] and has a low viscosity which facilitates the diffusion of Ti species in it and thus the rapid TiC coating formation. Thanks to the useful properties of KCl salt mentioned above, the KCl–LiCl eutectic salt was also effective in the MSS of TiC coatings”. p.914.

J117-c4. I.N.Orbulov, I.Kientzl, J.T.Blücher, Á.Németh, J.Dobránszky, J.Ginsztler: Production and investigation of a metal matrix composite pipe – in: Proc of 14th European Conf on Composite Materials, Paper ID: 262-ECCM14, 8 pp. – „Efforst have been done to reduce the contact angle either by coating of the fibers or by using three component reinforcement – salt – matrix systems [J117]” – p.2.

J117-c5. Kientzl I.: Alumíniummátrixú kompozithuzalok és kettős kompozit-szerkezetek – PhD értekezés, BME (tud. vez.: dr.Dobránszky János), 2010, 112.o. – „.. ha a porózus test egyforma, szorosan pakolt gömbökből van kirakva, akkor a kritikus peremszög 50,7o [], amire az első kísérleti bizonyíték Baumlitől származik [J117]” – 20.o.

J117-c6. I.N.Orbulov, Á.Németh: Infiltration characteristics of carbon fiber reinforced MMCs – Mater Sci Forum, 2010, vol.659, pp.229-234. – „Effort have been done to reduce the contact angle either by coating fibers or by using three component reinforcement – salt – matrix system [J117]” – p. 230.

J117-c7. Youliang Cheng, Tiehu Liy, Xianliang Hou, Deqi Jing, Qiang Zhuang, Tingkai Zhao: Effects of AlCl3-NaCl Content on the Formation of Mesocarbon Microbeads – Int J Chem Reactor Eng, 2010, vol.8, Note S7, pp. 1-12 – „Moreover, due to the low wettability of carbon and molten salt [J117], the morphology of obtained mesophase spheres gets more regular.” – p.5.

J117-c8. Korenko M, Simko F: Measurement of Interfacial Tension in Liquid-Liquid High-Temperature Systems – J Chem Eng Data, 2010, vol.55, issue 11, pp. 4561-4573. „Baumli and Kaptay [J117] used contact angle measurements for the evaluation of surface tension and wettability of several chlorides (KCl, NaCl, RbCl, CsCl) on graphite and glassy carbon substrates” – p.4570.

http://ecsmeet7.peerxpress.org/ms_files/ecsmeet7/2008/12/15/00001942/00/1942_0_art_0_kbxyy3.pdfhttp://apps.isiknowledge.com/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=P16igndinbI1C782E2O&name=Korenko%20M&ut=000284017600002&pos=1http://apps.isiknowledge.com/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=P16igndinbI1C782E2O&name=Simko%20F&ut=000284017600002&pos=2

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J117-c9. I.N.Orbulov: Infiltration of ceramic microballons by liquid metals – research plan for SCIEX-NMS, February, 2011, 12 pp. – „There are many papers int he professional literature which are dealing with the phenomenon of infiltartion [J117]” – p.9.

J117-c10. Z.Tao, Q.Guo, X.Gao, L.Liu: The wettability and interface thermal resitance of copper/graphite system with addition of chromium – Mater Chem, 2011, vol.128, pp.228-232 – „.. there exists a critical contact angle for spontaneous filling the surface pores of graphite material. This value is around 50 deg which has been demonstrated both by theory and experiment [J117]”

J.116. C.Mekler, G.Kaptay: Calculation of surface tension and surface phase transition line in binary Ga-Tl system – Mater Sci Eng A, 2008, vol.495, pp.65-69. (IF = 1.860) J116-c1. Zoltai László (+Dúl Jenő): Grafitcsírák keletkezési lehetőségének elméleti vizsglata – 3.

kutatószemináriumi dolgozat, Miskolci Egyetem, 2009. február, 48 oldal – „A β paraméter a felületi rétegben meglévő kötések hányada, ami 1-nél ksiebb pozitív szám, értéke 0,83 [J116]” – 31.o.

J116-c2. S.H.Sheng, R.F.Zhang, S.Veprek: Phase stabilities and decomposition mechanism in the Zr-Si-N system studied by combined ab initio DFT and thermodynamic calculation – Acta Mater, 2011, vol.59, pp.297-307 – “The so-called surface phase transition, which has been theoretically predicted by Cahn and recently elaborated in more detail by Kaptay et al [J116], essentially states that the system will decrease the high surface energy of the ionic transition metal nitride by wetting it with covalent Si3N4” – p.305.

J116-c3. A.Aqra, A.Ayyad, F.Takrori: Model calculation of the surface tension of liquid Ga-Bi alloy – Appl Surf Sci, 2011, vol.257, pp.3577-3580 – “It should be noted that the surface tension of liquid solders may be calculated by means of various methods such as Butler method [J116] – p.3578.

J116-c4. F.Aqra, A.Ayyad: Theoretical calculations of the surface tension of Ag-Cu liquid alloys – J Alloys Compounds, 2011, vol.509, pp.5736-5739 – “Many attempts have been made to predict the surface tension of liquid metals and alloys, such as computer simulation with Monte Carlo or molecular dynamics methods and models based on Butler's concept [J116]” – p.5736.

J116-c5. L.E.Gonzalez, D.J.Gonzalez: Orbital free ab initio simulation of surface freezing in a dilute Ga-Tl alloy – Eur. Phys. J. Special Topics, 2011, vol. 196, pp.15-26. – “A theoretical thermodynamic calculation of the surface phase transition line, separating the regions where the segregation of a Tl-rich nanolayer takes place or does not take place, has been pursued by Mekler and Kaptay [J116]. They obtained good agreement with the adsorpőtion measurements of Shim et al.” - pp.17-18.

J.115. G.Kaptay: A unified model for the cohesive enthalpy, critical temperature, surface tension and volume thermal expansion coefficient of liquid metals of bcc, fcc and hcp crystals – Mater Sci Eng A, 2008, vol.495, pp.19-26. (corrigendum: see Mater Sci Eng A, 2009, vol.501, p.255.) (IF = 1.860) J115-c1. Zoltai László (+Dúl Jenő): Grafitcsírák keletkezési lehetőségének elméleti vizsglata – 3.

kutatószemináriumi dolgozat, Miskolci Egyetem, 2009. február, 48 oldal – „Az irodalmi érték: σFe-g = 2470 – 0.32T mJ/,2 [J115]” – 30.o.

J115-c2. A.G.Cherevko: Nukleacionno-fluktuacionnii podhod k opredeleniiu temperaturnoi zavisimosti poverhnostnogo natiazheniia metallov – Kolloidnii zhurnal, 2009, vol.71, No.6, pp.852-859 (Nucleation-fluctuation approach to determining the temperature dependence of the surface tension of metals – Colloid Journal, 2009, vol.71, No. 6, pp. 869-876) – V rabotach [J115] bili naideni korreliacii poverhnostnogo natiazheniia vblizi temperaturi plavleniia s teplotoi plavleniia i moliarnim obiomom” – p.852.

J115-c3. V.Morel, A.Bultel, B.G.Cheron: The critical temperature of aluminum – Int J Thermophys, 2009, vol.30, pp.1853-1863 – „Recently, Kaptay [J115] has given a unified model linking the cohesive enthalpy of a liquid with the melting point of alkali metals. This model also yields fairly good results for other metals. The cohesive enthalpy is defined as the energy existing in the liquid resulting from the mutual atomic attractions, which vanishes when the critical temperature is reached… (2 equations)”- p.1858. “Table 4. New estimates of the critical temperature for aluminium. Method: cohesive enthalpy, Tc = 6548 K.” – p.1861. “Finally, the recommended critical temperature of aluminium, obtained as the average of our own results and the latter, is 6700 ± 800 K” – p.1862.

J115-c4. F.Aqra, A.Ayyad: Theoretical calculations of the surface tension of liquid transition metals – Metal Mater Trans B, 2011, vol.42B, pp.5-8 – “Few published models [J115]… ” – p.7.

J115-c5. F.Aqra, A.Ayyad: Surface tension of pure liquid bismuth and its temperature dependence: Theoretical calculations, Mater Letters, 2011, vol.65, pp.760-762 – “few established models [J115]…” – p.760.

J115-c6. F.Aqra, A.Ayyad: Surface energies of metals in both liquid and solid states – Appl Surf Sci, 2011, vol.257, pp.6372-6379. – “The surface tension of liquids is defined as the ratio of the excess surface Gibbs

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energy (expressed through excess surface enthalpy and excess surface entropy) divided by the molar surface area: Eq.(17-18) where f is a geometrical constant (approximately = 1.0) [J115]” – p.6375.

J115-c7. F.Aqra, A.Ayyad: Surface tension of liquid alkali, alkaline, and main group metals: theoretical treatment and relationship investigations – Metall Mater Trans A, 2011, vol.42A, pp.2680-2684 – „Establishing an accurate, successful, and universal theoretical model for calculating the surface tension of liquid metals is necessary [J115]” – p.2680

J115-c8. F.Aqra, A.Ayyad: Theoretical estimation of temperature-dependent surface tension of liquid antimony, boron and sulfur – Metall Mater Trans A, 2011, vol.42, pp.437-440 – „Few established models are universal [J115], but the agreement with experiment is not satisfactory” – p. 437.

J115-c9. F.Aqra, A.Ayyad: Theoretical temperature-dependence surface tension of pure liquid gold - Mater Letters, 2011, vol.65, pp.2124-2126 – „… it is still difficult to identify successfull model for which both accuracy and universality apply. Although few established models are universal [J115], but the agreement with experiment is not very satisfactory” – p. 2124.

J115-c10. F.Aqra, A.Ayyad: Surface tension, surface energy and crystal-melt interfacial energy of metals – Current Applied Phys, 2012, vol.12, pp.31-35 – „… it is still difficult to identify successfull model for which both accuracy and universality apply. Although few established models are universal [J115], but the agreement with experiment is not very satisfactory” – p. 34.

J115-c11. F.Aqra, A.Ayyad: Surface tension of pure liquid lanthanide and early actinide metals – Phys Chem Liquids, 2012, vol.50, pp. 336-345.

J.114. P.Baumli, G.Kaptay: Wettability of carbon surfaces by molten alkali chloride mixtures – Mater Sci Forum, 2008, vol.589, pp.355-359. (IF = 0)

J.113. G. Buza, V. Janó, M. Svéda, O. Verezub, Z. Kálazi, G. Kaptay, A. Roósz: On the possible mechanisms of porosity formation during laser melt injection (LMI) technology – Mater Sci Forum, 2008, vol.589, pp.79-84. (IF = 0) J.112. G.Kaptay: A CALPHAD-compatible method to calculate liquid/liquid interfacial energies in immiscible metallic systems – Calphad, 2008, vol.32, pp.338-352. (IF = 1.530) J112-c1. J.Lee, S.Min, J.Park: Effect of Ce and La on surface property of Bi-Cu-Sn alloys – PPT file of TOFA

2008, June 22-27, Krakow, Poland, 23 slides – „new equation and 2 graphs are taken from paper [J112]” – slide 18.

J112-c2. J.Park, S.Min, J.Lee: Effect of REM addition on the surface tension and the critical temperature of the immiscible liquid phase separation of the 60%Bi-24%Cu-16%Sn alloy – Korean J Mater Res, 2009, vol.19, pp. 111-114. – “Recently, Kaptay [J112] suggested a semiempirical equation to predict the interfacial tension between two immiscible liquids based on the models of Chatain et al. and Hoyer et al. Simply, the interfacial tension can be expressed as Eq.(2) … This equation successfully described the interfcial tension of the Ga-Pb and Al-Bi systems [J112]” – p.113. “Fig. Cacilated by Eq.(2)” – p.114.

J112-c3. J.Li, B.Ma, S.Min, J.Lee, Z.Yuan, L.Zang: Effect of Ce addition on macroscopic core-shell structure of Cu-Sn-Bi immiscible alloy – Mater Letteres, 2010, vol.64, pp.814-816 – “Kaptay [J112] suggested that the interfacial tension between two immiscible liquids could be expressed by the equation: …{Eq.2}… “ – p.2. Fig.4. Temperature dependence of interfacial tension of the 24Cu – 16Sn – 60 Bi alloy with 0.05 wt % Ce addition, calculated using Eq.(2)” – p.815.

J112-c4. Mende T.: Az ESTPHAD módszer fejlesztése és alkalmazása kettő-, három- és négyalkotós rendszerek likvidusz hőmérsékletének közelítésére, PhD értekezés, (tud. vez.: Roósz A.), 2010, Miskolc, 129 o. – “A 4.33 ábrán a szakirodalomból származó [J112] és a 31. egyenlettel számított szétválási görbe látható. 4.18. táblázat [J112]” – 65.o, „A reguláris elegymodellből levezethetően a szétválási hőmértésklet koncentráció-függésére a következő egyenlet írható fel [J112]: (34) egyenlet.” – 67.o.

J112-c5. Mende T., Roósz A.: Egyensúlyi fázisdiagramok nonvariáns pontjainak nagy pontossággú számítása Estphad módszerrel – BKL Kohászat, 2011, vol.144, No.3, pp.47-50.

J112-c6. L.Zhao, J. Zhao: Microstructure formation in a gas-atomized drop of Al-Pb Immiscible alloy – Metall Mater Trans A, 2012, doi: 10.1007/s11660-012-1313-3. – “”The critical temperature for a ternary immiscible alloy is determined by the alloy composition [J112]” -

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J111. G.Kaptay: Link between the semi-empirical Andrade and Shytil equations and the statictical-mechanical Born-Green equation for viscosity and surface tension of pure liquid metals – Metall Mater Trans B, 2008, vol.39B, pp.387-389. (IF = 0.798) J110. G.Kaptay: A new theoretical equation for temperature dependent self-diffusion coefficient of pure liquid metals – Int J. Mater Res. (formerly Z. Metallkunde), 2008, vol.99, pp.14-17. (IF = 0.819) J110-c1. S.Yang, X.Su, J.Wang, F.Yin, Z.Li, S.Chen, C.Liu: Temperature-evolution of structure and diffusion

properties of liquid transition metals – J Non-Crystalline Solids, 2010, vol.356, pp.1061-1069 – „… a recently derived predictive equation for temperature dependence of self-diffusion coefficients of liquid metals [J110] has been applied to give theoretical prediction. The new equation was derived combining a unified equation on the viscosity of pure liquid metals with the well known Sutherland-Einstein equation without any adjustable parameters. The perfect agreement of the prediction of this new equation with the experimental values measured under micro-gravity conditions confirms its applicability. The equation has been derived as: {Eq.4}… + 10 lines. The performance of the present MD study was evaluated by determining relative difference between the calculated and theoretical prediction values. .... The values are listed in Table 1. Table 1. Simulated self-diffusion coefficients of liquid transition metal – 1 coloumn is calculated by Eq.(4) [J110]”.

J110-c2. DL Beke: On the composition and pressure dependence of the self-diffusion coefficient in liquid metals – Int J Mater Res, 2010, vol.101, 353-355. - „In a very recent paper Kaptay [J110] presented a unified equation for the temperature dependence of the self-diffusioin coefficient, D, in liquid metals. It is mentioned in [J110] that the result is also a prepequisite for modeling of the composition and pressure dependence of D.” – p.353. “.. fortunately this data collection and trial to get a relation expressing at least the non-reduced values of D as the function of T was already done in [J110]. Thus it is worth to compare relation (5) with the results of [J110]: {2 equations, 9 lines copied from [J110]}. – p.354. “The use of the so-called “corrected” melting point for semi metals is a good trial in [J110]: indeed for these elements the melting point is not a good measure of the bonding strength because during melting there are changes in the electronic structure” – p.354.

J110-c3. Beke DL.: Composition and Pressure Dependence of the Diffusion Coefficients in Binary Liquid Alloys – Defect and Diffusion Forum, 2010, vol.297-301, pp.1371-1376. – „Data collection and trial to get a relation expressing at least the non-reduced values of D as the function of T* has already been done [J110]. … Furthermore it was shown in [J110] that in fact the logarithm of F2*(T*) is a good linear function of Tm/T (see Figs 1-2 in [J110].” – p.1373.

J110-c4. AA Simonova: Obespechenie neobhodimogo kachestva poverhnostnogo sloia obiomnich nanokristallicheskich metallov posle mechanicheskoi obrabotki – Naukovi Notatki (Inzhenerna mechanika), No.24, 2009, Luck, pp.500-506 – „Nabliudeniia, predstavlennie v rabote [J110] pokazali, shto….” – p.503.

J109. G.Kaptay: The threshold pressure of infiltration into fibrous preforms normal to the fiber’s axes – Composites Science and Technology, 2008, vol.68, pp.228-237. (IF = 2.533) J109-c1. I.Kientzl, J.Dobránszky: Production and behaviuour of aluminium matrix double composite structures –

Mater Sci Forum, 2008, vol.589, pp.105-110 – “Kaptay’s equation describes the threshold pressure as function of the contact angle and smallest separation of the fibers divided by the fibre diameter. The threshold pressure of non-wetting liquids is found to be inversely proportional to the smallest distance between the fibers although it is commonly beleived to be inversely proportional to the diameter of the fibres. Four different cases were distuinguished based on the wettability of fibres and the sapce between the fibres and the equations of thrshold pressures were worked out for all these cases [J109]” – p.105-106. „Based on Kaptay’s method the threshold pressure was calculated and plotted as function of the contact angle and relative distance between the fibers (Fig.2).” – p.107.

J109-c2. Orbulov I, Németh Á, Dobránszky J: Manufacturing of Composites by Pressure infiltration, Structure and Mechanical Properties. In: Penninger A, Váradi K, Vörös G (eds.), Gépészet 2008, Proceedings of Sixth Conference on Mechanical Engineering, BUTE Faculty of Mechanical Engineering – “This threshold pressure can be calculated by theoretical approaches for various systems [J109]” – p.1/9.

J109-c3. Orbulov IN, Németh Á, Dobránszky J: XRD and EDS Investigations of Metal Matrix Composites and Syntactic Foams. 13th European Conference on X-Ray Spectrometry, Cavtat, Croatia, 16-20 June 2008, In: EXRS 2008 Proceedings – “The main parameter in this case is the infiltration pressure, which can be approximated numerical calculations and is influenced by wetting” – p. 2/10.

J109-c4. Kientzl I.: Alumínium mátrixú kompozithuzalok és kettőskompozit szerkezetek – PhD értekezés, 2010., BME (tud. vezető: Dobránszky János). – „G. Kaptay azonban pontosan egy ilyen számítási módszert mutatott be cikkében határfelületi megfontolásokra alapozva munkáját [J109]. Az ebben a cikkben

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bemutatott számítási eljárást ismertetem a következőkben (+ 1 oldal, 2 ábra és 16 egyenlet a cikkből)” – 21-22. o., „… a szálak olvális keresztmetszetűek, hosszirányban 12 μm, keresztirányban 7 μm, így a Kaptay által adott módszer, ami kör keresztmetszetű szálakra lett kidolgozva, csak közelítő számításokra alkalmas ebben az esetben – 42. ábra” – 44.o.

J109-c5. I.N.Orbulov, I.Kientzl, J.T.Blücher, Á.Németh, J.Dobránszky, J.Ginsztler: Production and investigation of a metal matrix composite pipe – in: Proc of 14th European Conf on Composite Materials, Paper ID: 262-ECCM14, 8 pp. – „This threshold pressure can be estimated by theoretical approaches for various wetting or non-wetting systems [J109]” – p.2.

J109-c6. Qi LH, Xu R, Su LZ, Zhou JM, Guan JT: Dynamic measurement on infiltration process and formation mechanism of infiltration front – Trans. Nonferr Metals Soc China, 2010, vol.20, pp.980-986 – „As an indispensable step int he fabrication technologies of metal matrix composites (MMC), the liquid metal infitration process in porous preform, such as squeeze casting, vacuum infiltration, variable pressure infiltration and liquid infiltration-extrusion, have attracted research interest due to the significantly effective improvement int he properties of composite products [J109]” – p.980.

J109-c7. Kientzl I.: Alumíniummátrixú kompozithuzalok és kettős kompozit-szerkezetek – PhD értekezés, BME (tud. vez.: dr.Dobránszky János), 2010, 112.o. – „.. Kaptay a hengeres szálak közé való infiltrálást vizsgálta [J109]. Az eredmények szerint a szálakkal párhuzamosan a kritikus peremszög 90o, míg azokra merőlegesen sokkal kisebb 90o-nál. A konkrét peremszög értéke függ a szálak térkitöltésétől…” – 20.o. „Kaptay egy új számítási módszert mutatott be határfelületi megfontolásokra alapozva munkáját [J109] + 2 oldal + 14 egyenlet + 2 ábra idézet” – 21-23. o. „A Kaptay modell. 1,5 oldal elemzés… A Kaptay modell a folyamatos infiltrációhoz szükséges küszöbnyomást 0,20 – 0,77 MPa értékre becsüli. Ez a tartomány a kísérleti eredményekből származó 0,62-0,83 MPa intervallummal átfedésben van, tehát ez a modell magyarázatot ad a folyamatos infiltráció nyomás-szükségletére… Összefoglalva megállapítható, hogy a White-Mortensen és a Kaptay modellek közül csak a Kaptay-modell mutatott átfedést a mérési eredményeimmel” – 60-64. oldalak. „A Kaptay-model által adott küszöbnyomásfüggvény alapján a szálak ritkább elrendeződése esetén, még nagy peremszögek mellett sem nő jelentős mértékben a folyamatos infiltrációhoz szükséges küszöbnyomások értéke” – 83.o. „2.tézis. A küszöbnyomás 0,62-0,83 MPa-os intervallumát összevetettem két elméleti modellel… .. tehát a kísérleti eredményeim matematikai közelítésére a Kaptay modell alkalmas” – 84.o.

J109-c8. I.N.Orbulov, Á.Németh: Infiltration characteristics of carbon fiber reinforced MMCs – Mater Sci Forum, 2010, vol.659, pp.229-234. – The threshold pressure can be estimated by theoretical approaches for various wetting or non-wetting systems [J109]” – p. 230.

J109-c9. I Kientzl, J Dobránszky, Á Németh: Effect of the Infiltration Pressure on the Properties of Composite Wires- Materials Science Forum, 2010, vol. 659, pp.177-182. – „Kaptay's equations describe the threshold pressure as a function of the contact angle and smallest separation of the fibres divided by the fibre diameter [J109]. The threshold pressure of non-wetting liquids is found to be inversely proportional to the smallest distance between the fibers … „ p.177

J109-c10. L.H.Qi, L.Z.Su, J.M.Zhou, J.T.Guan, X.H.Hou, H.J.Li: Infiltration characteristics of liquid AZ91D alloy into short carbon fiber preform – J Alloys Compds, 2012, vol.527, pp.10-15. – „… much research work had also been conducted on the calculation of the threshold pressure for initiation of infiltration [J109]” – p.10.

J109-c11. Seung-Wook Han, Nak-Sam Choi and Min-Soo Lee: Analysis of glass fabric impregnation using a resin drop method - J Mechan Sci Technol, 2012, vol. 26, pp. 1477-1482 – “The interplay between the surface tension of the infiltrating liquid, the wettability of the fibers by the surrounding liquid and the morphological details of the preform fabric directly affects the integrity of the manufactured composites [J109]” – p.1477.

J109-c12. MA You-ping, LI Xiu-lan, WANG Cheng-hui, LU Lu: Microstructure and Impact Wear Resistance of TiN Reinforced High Manganese Steel Matrix – J Iron Steel Res Int. 2012, vol. 19, No. 7, pp. 60-65 – „The most common surface treatment route is the liquid metal infiltration …. Infiltration technique has been successfully applied in wear parts [J109]” – p.60.

J108. K.Wasai, G.Kaptay, K.Mukai, N.Shinozaki: Modified classical homogeneous nucleation theroy and a new minimum in free energy change 2. Behavior of free energy change with a minimum calculated for various systems - Fluid Phase Equilibria, 2007, vol.255, pp.55-61. (IF = 1.506)

http://apps.isiknowledge.com/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=V2ea4Loa92GGLC8fefO&name=Qi%20LH&ut=000279976100007&pos=1http://apps.isiknowledge.com/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=V2ea4Loa92GGLC8fefO&name=Xu%20R&ut=000279976100007&pos=2http://apps.isiknowledge.com/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=V2ea4Loa92GGLC8fefO&name=Su%20LZ&ut=000279976100007&pos=3http://apps.isiknowledge.com/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=V2ea4Loa92GGLC8fefO&name=Zhou%20JM&ut=000279976100007&pos=4http://apps.isiknowledge.com/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=V2ea4Loa92GGLC8fefO&name=Guan%20JT&ut=000279976100007&pos=5http://scholar.google.com/scholar_url?hl=en&q=http://www.scientific.net/MSF.659.177&oi=scholaralrt&ct=alrt&cd=3&sa=X&scisig=AAGBfm0uM-tFOn6GrjBDf90g4kMkXliklghttp://scholar.google.com/scholar_url?hl=en&q=http://www.scientific.net/MSF.659.177&oi=scholaralrt&ct=alrt&cd=3&sa=X&scisig=AAGBfm0uM-tFOn6GrjBDf90g4kMkXliklghttps://springerlink3.metapress.com/content/?Author=Seung-Wook+Hanhttps://springerlink3.metapress.com/content/?Author=Nak-Sam+Choihttps://springerlink3.metapress.com/content/?Author=Min-Soo+Leehttps://springerlink3.metapress.com/content/h6x1835rrmk8mw77/https://springerlink3.metapress.com/content/h6x1835rrmk8mw77/https://springerlink3.metapress.com/content/1738-494x/

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J108-c1. S.Min, J.Park, J.Lee: Surface tension of the 60%Bi-24%Cu-16%Sn alloy and the critical temperature of the immiscible liquid phase separation – Mater Lett, 2008, vol.62, pp.4464-4466 – „In order to control the structure of the core-shell lead-free solder ball, the surface tension and the interfacial tension between two immiscible liquid alloys are required [J108]” – p.4464.

J108-c2. Verezub O.: Lézeresen felületkezelt szerszámacél köszörülése – Gyártóeszközök, szerszámok, szerszámgépek, 2008, No.1, pp.65-68. – „A nanométer tartományba tartozó szemcsék kiválásának felételeiről lásd [J108]” – p.66.

J108-c3. Zoltai László (+Dúl Jenő): Grafitcsírák keletkezési lehetőségének elméleti vizsglata – 3. kutatószemináriumi dolgozat, Miskolci Egyetem, 2009. február, 48 oldal – „Mivel a SiC képződése során az olvadék Si- és C-tartalma csökken, a nano méretű SiC csírák stabiliázlása elméletileg lehetséges [J108]” – 2.o. „Wasai, Kaptay, Mukai és Shinozaki ismerték fel először [J108], hogy csíraképződés során az olvadékfázis Gibbs energiája változásának figyelmen kívül hagyása oda vezet, hogy a csíraképződési görbe egyébként létező minimum pontja nem jelenik meg… A levezetés [J108] a nemrég publikált cikkek egyszerűsített változata – 2 oldal egyenletek” – 40. o.

J.107. Gábor T., Kármánné H.F., J.Sytchev, Kaptay Gy., Kálmán E.: Sóolvadékok elektrolízise során kialakult szén nanocsövek kinyerése és minősítése – BKL Kohászat, 2007, vol.140., No.2, pp. 43-50. (IF = 0) J106. K.Wasai, G.Kaptay, K.Mukai, N.Shinozaki: Modified classical homogeneous nucleation theroy and a new minimum in free energy change 1. A new minimum and Kelvin equation – Fluid Phase Equilibria, 2007, vol.254, pp.67-74. (IF = 1.506) J106-c1. Verezub O.: Lézeresen felületkezelt szerszámacél köszörülése – Gyártóeszközök, szerszámok,

szerszámgépek, 2008, No.1, pp.65-68. – „A nanométer tartományba tartozó szemcsék kiválásának felételeiről lásd [J106]” – p.66.

J106-c2. Zoltai László (+Dúl Jenő): Grafitcsírák keletkezési lehetőségének elméleti vizsglata – 3. kutatószemináriumi dolgozat, Miskolci Egyetem, 2009. február, 48 oldal – „Mivel a SiC képződése során az olvadék Si- és C-tartalma csökken, a nano méretű SiC csírák stabiliázlása elméletileg lehetséges [J106]” – 2.o. „Wasai, Kaptay, Mukai és Shinozaki ismerték fel először [J106], hogy csíraképződés során az olvadékfázis Gibbs energiája változásának figyelmen kívül hagyása oda vezet, hogy a csíraképződési görbe egyébként létező minimum pontja nem jelenik meg… A levezetés [J106] a nemrég publikált cikkek egyszerűsített változata – 2 oldal egyenletek” – 40. o.

J106-c3. Carreon-Calderon B., Soria A., Romero-Martinez A.: Driving Force in First-Order Phase Transitions and Its Application to Gas Hydrate Nucleation from a Single Phase - AICHE Journal, 2009, vol.55, pp. 2433-2447. – „.. authors consider the nucleation work as a maximum of the free energy surface” – p.2434.

J106-c4. Teychene S., Biscans B.: Microfluidic Device for the Crystallization of Organic Molecules in Organic Solvents – Crystal growth & Design, 2011, vol.11, pp.4810-4818. -

J105. G.Kaptay: On the wettability, encapsulation and surface phase transition in monotectic liquid metallic systems – Materials Science Forum, 2007, vol.537-538, pp.527-532 (IF = 0) J105-c1. Svéda Mária: Monotektikus felületi rétegek létrehozása lézersugaras felületkezeléssel c. PhD

értekezéséhez (tudományos vezető: dr. Roósz András) – 2007. – „A nagyobb sűrűségű Pb olvadéknak az ötvözett zóna felszínén való elhelyezkedése a határfelületi jelenségekkel magyarázható [J105]” – p.87.

J104. I.Budai, M.Z.Benkő, G.Kaptay: Comparison of different theoretical models to experimental data on viscosity of binary liquid alloys – Materials Science Forum, 2007, vols.537-538, pp.489-496. (IF = 0) J104-c1. D.Zivkovic: Application of the Kaptay model in calculation of ternary liquid alloys viscosities – Int J

Mat Res, 2008, vol.99, pp.748-750 – „Kaptay’s approach to estimate the viscosity of liquid metallic alloys from viscosities of pure liquid metals and thermodynamic properties of the liquid alloy has been tested for different types of binary systems [J104], including those with considerable deviations from ideality” – pp.748-749.

J104-c2. D.Zivkovic: A new approach to estimate the viscosity of the ternary liquid alloys using the Budai-Benko-Kaptay equation – Metall Mater Trans B, 2008, vol.39, pp.395-398 – „The new Budai-benko-Kaptay (BBK) equation has been recently derived for estimation of the viscisity of liquid alloys and tested on numerous binary systems, showing a good agreement with experimentally obtained data. Equations…. … The presented new BBK equation for estimation of the viscosity of liquid metallic alloys has been

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already tested for different types of binary systems [J104], showing good compliance with experimental data in most cases. IN this article, the applicability of a new equation to ternary systems will be tested in examples of Au-Ag-Cu alloys. „ – p.395, „There is an agreement between the results of the BBK equation application, presented in this work and the experimental literature data… the ability to predict the viscosity, even if the viscosities of the pure componnets are not known, should be underlined int he application of the new BBK equation and taken as an advantage among other models int he case when these data are not known” – p.396. „The greatest advantage of the presented BBK equation is to be accetuated – such estimation of the viscosities of multicomponent liquid alloys demands just a few starting data for the calculation compared to the other known models, which makes it simple and easy to apply in different cases” – p.397.

J104-c3. V.Skliarchuk, A.Iakimovich, M.Dufanec: Rozrahunok viazkosti rozplaviv sistemi Al-Cu – Vseukrainska konferencia molodich vchonich “Suchasne materialoznavstvo: materiali ta technologii SMMT-2008. (PPT file of a conference talk) – “Modifikovane rivnannia Budai-Benko-Kaptay [J104] …. “ – p. 4, “Rozrahovani znacheniia viazkosti zgidno modeli Chabra i modifikovanogo rivnannia Budai-Benko-Kaptay dobre uzgodzhuiutsia z literaturnimi dannimi“ – p.9.

J104-c4. Sklyarchuk VM, Yakimovich AS, Dufanets' MV: Calculation on Viscosity of Al-Cu Liquid Alloys – Metallofizika i noveishie technologii, 2008, vol.30, pp., 315-321.

J104-c5. P.Terzieff: The viscosity of liquid alloys of polyvalent metals with Cu, Ag and Au: Theoretical treatments based on the enthalpy of mixing – Physica B, 2009, vol.404, pp. 2039-2044 – „The majority of the currently used viscosity models are of semi-empirical nature focused on thermodynamic quantities such as enthalpy of mixing [J104]” – 2039, “The extension toi the case of multi-component systems involves the volume of mixing and the enthalpy of mixing as additional input parameters [J104]: Eq.(3)” – p.2040, “Fig-s 1-10: “unified model”” – pp.2041-2033, “The least strenuous way to calculate viscosities is given by the unified equation of Kaptay and coworkers [J104]. Except for the Ag-Sb and some extent to Cu-Sb, the excess viscosities are in reasonable numerical agreement with the experimental values (Table 1). Apart from the model’s obvious overestimation of the viscosity of pure liquid Cu in Cu-BI, Cu-Pb and Cu-Sn (Figs 2, 3 and 5) or the disagreement in the values of undercooled Au in Au-Sn (Fig.10) the shapes of the viscosity isotherms are found to be adequately reproduced (curves b). However, it has to be also noted that the experimental values reported for liquid Cu differ from one author to the other by more than 1 mPaseven at the same temperature (Figs 3. and 4.). The additional isotherms (curves b’) shown for Cu-Bi, Cu-Sb, Ag-Ge and Ag-Sb were obtained by using the corrected melting temperatures for Ge (450 K), Sb (650 K) and Bi (450 K) as recommended by Kaptay [J104]. As compared to the isotherms obtained with the uncorrected melting temperatures (curves b) the improvemenets are extremely large for Ag-Ge (Fig.6), less pronounced for Cu-Sb and Ag-Sb (Figs 4, 8) and small for Cu-Bi (Fig.2).” – p.2043.

J104-c6. P.Terzieff: Some physico-chemical properties of liquid Ag-Sn-Zn – Physica B, Condensed Matter, 2010, vol.405, pp.2668-2672 – From a previous analysis it has been concluded that the semi-empirical apprach based on Kaptay’s unified equation [J104] is one of the most convenient methods to gain a first idea of the viscosity of muticomponent systems, even if the viscosities of the pure liquids are unknown. The application requires the melting temperatures of the components, their molar masses, and their molar volumes. The only requirements for alloy is the knowledge of the excess volume and the enthalpy of mixing : (Eq.10)” – p.2674.

J104-c7. Gasior W, Moser Z, Debski A: New data to the SURDAT-database of modeled and experimental physical properties of lead-free solder alloys – Arch Metall Mater, 2009, vol.54, pp. 1253-1259 – „..SURDAT database … experimental … and the viscosity calculated from the dependences proposed by … Kaptay [J104] : Eq.(6)” – p.1256. “Fig.4. Experimental (symbols) and calculated (lines) viscosity (Eq-s (1, 2, 5, 6, 7) of Ag-Sn (Fig.4a) and Sn-Zn (Fig.4b) alloys” – p.1257.

J104-c8. Knott S., Terzieff P.: Calculation of the viscosity of the liquid ternary Ag-Au-Sn system – Int. J. Mater. Res., 2010, vol.101, pp.834-838. – „Several viscosity models based on thermodynamic data exist, some of them apply adjustable parameters, while others make use of universal parameters [J104] which a re considered to be applicable to a large class of alloy systems” – p.834, “The expression for the viscosity, given by Budai et al. [J104] is based on Kaptay-s unified equation for pure liquid metals: Eq.(3)” – p.835. Fig-s 2, 4 and Table 2 are calculated by the model [J104] – pp.836-837. “…the unified equation yields a much better agreement for Ag-Au system” – p.836. “Conclusions: .. in case of missing experimental evidence the unified equation might give a first reasonable estimate of the viscosity in liquid multicomponent systems” – p.838.

J104-c9. Wunderlich RK; Fecht H-J: Surface tension and viscosity of NiAl catalytic precursor alloys from microgravity experiments – Int J Mater Res, 2011, vol.102, pp.1164-1173. „The Kaptay model was shown to provide better agreement with observed viscosities of binary alloys [J104] than the Moelwyn-Hughes model. In the Kaptay model the viscosity is given by: Eq-s.(15-16), Fig.11, Table 2.” – p.1170-1171.

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J104-c10. R.N.Singh, F.Sommer: Viscosity of liquid alloys: generalization of the Andrade’s equation – Monatsh Chem, 2012, vol.143, pp.1235-1242. – „Results obtained from these relations have been compared with new or given [J104] experimental viscosity data as a function of composition and temperature.” – p.1235. “A comparison of available semi-empirical models with experimental data of the viscosity of liquid alloys has been given recently [J104]” – p.1241.

J103. Baumli P., Sytchev J., Kaptay Gy.: SiC és Al2O3 kerámia szemcsék felületkezelése só olvadékban, kompozitok fejlesztése céljából – BKL Kohászat, 2006., 139. évf., 3.szám, 47-50. (IF = 0) J103-c1. Orbulov I., Kientzl I., Németh Á.: Fémhabok és kompozitok előállítása infiltrálásos eljárással – BKL

Kohászat, 2007, vol.140, No.5, pp.41-46. – „Nagyon fontos, hogy a fémmátrixú kompozitanyagok esetében is csak akkor kapunk megfelelő műszaki tulajdonságokat, ha megfelelő a kapcsolat az erősítőanyag és a mátrixanyag határfelületén [J103]” – p.41.

J103-c2. Orbulov I.: Szintaktikus fémhabok keménységmérése – Anyagvizsgálók lapja, 2009, No.1, pp.9-15. – „… vizsgálatok tárgyát képezték az erősítőanyagra felvihető különböző bevonatok is [J103].” – p.9.

J102. G.Kaptay: On the equation of the maximum capillary pressure induced by solid particles to stabilize emulsions and foams and on the emulsion stability diagram - Colloids and Surfaces A: Physicochem. Eng. Aspects, 2006, vol.282-283, pp.387-401. (IF = 1.611) J102-c1. Gonzenbach UT, Studart AR, Tervoort E, Gauckler LJ: Tailoring the microstructure of particle-

stabilized wet foams - LANGMUIR 23 (3): 1025-1032 JAN 30 2007 - „These results suggest that the preparation of wet foams that are stable against bubble coarsening and drainage requires particle sizes not larger than a few micrometers in diameter. Theoretical calculations based ont he adsoroption energy of particles at gas – liquid interface and the maximum capillary pressure developed at the interface showed that particles larger than about 3 microns are not able to stabilize foams for long period of time [J102]. These results are in the same order of magnitude as our experimental findings” – p.1029.

J102-c2. C.Körner: Integral Foam Molding of Light Metals – Physical and Technological Principles – Habilitation Thesis, Erlangen, 2007 (Ref. No.132) – “Kaptay was the first who realized that stabilization for these kind of particles is based on the development of 3D network structures which transfer forces from one interface to the other [J102].” – p.108.

J102-c3. Torres LG, Iturbe R, Snowden MJ, Chowdhry BZ, Leharne SA: Preparation of o/w emulsions stabilized by solid particles and their characterization by oscillatory rheology - COLLOIDS AND SURFACES A-PHYSICOCHEMICAL AND ENGINEERING ASPECTS 302 (1-3): 439-448 JUL 20 2007 – “The magnitude of the free energy required to remove a particle from the interface between two immiscible fluids does not provide an insight into the stability of the emulsions [J102]…. It is reported that the water fil between two drops of the discontinuous oil phase resists rupture if the contact angle of the stabilising particle is in the range of 15 – 90 degrees [J102]” – p.440.

J102-c4. Studart AR, Gonzenbach UT, Akartuna I, Tervoort E, Gauckler LJ: Materials from foams and emulsions stabilized by colloidal particles - JOURNAL OF MATERIALS CHEMISTRY 17 (31): 3283-3289 2007 – “… stabilization is achieved for intermediate contact angles ranging from 20 to 86 deg for oil-in-water emulsions and foams, and from 94 to 160 deg for water-in-oil emulsions and mists [J102]” – p.3285, “Besides the high energy of adsorption of particles at the interface, the remarkable resistance of particle-stabilized foams and emulsions against coalescence has also been attributed to the development of capillary forces that impede thinning down the liquid film between bubbles/droplets, as well as to the formation of an attractive network of particles throghout the continouos liquid phase [J102]” – p.3286.

J102-c5. SE Friberg, AA Bawab, AA Abdoh: Surface active inverse micelles – Colloid Polym Sci, 2007, vol.285, pp.1625-1630 (Ref. No.17) – “Finally Professor Kaptay [J102] has published a complete treatment on the influence of solid particles on the capillary pressure in their stabilization of emulsions and foams” – p.1628.

J102-c6. Orbulov I., Kientzl I., Németh Á.: Fémhabok és kompozitok előállítása infiltrálásos eljárással – BKL Kohászat, 2007, vol.140, No.5, pp.41-46. – „A másik csoportba sorolhatjuk azokat az anyagokat, amelyek létrehozásánál vagy csak a tömegcsökkentés, vagy valamilyen más különleges követelmény dominál. Ezek a porózus szerkezeti anyagok [J102]” – p.41.

J102-c7. L.Torres, R.Iturbe, MJ Snowden, B. Chowdhry, S.Lehrane: Can Pickering emulsion formation aid the removal of creosote DNAPL from porous media? – Cemosphere, 2008, vol.71, pp.123-132 – “There are, however, problems with the model that undepints the development of Eq.(1) (of Binks). For example the model does not explain experimental observation that particle stabilised emulsions are maximally stabilised when the particles display a contact angle less than 90o [J102]…. The role of the particles in

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film stabilisation can be incorporated into a model which then predicts that the film between two drops of the discontinuous oil phase resists rupture if the contact angle of the stabilising particlesis in the range between 15 and 90 deg [J102]” – p.125.

J.102-c8. TN Hunter, RJ Pugh, GV Franks, GJ Jameson: The role of particles in stabilizing foams and emulsions – Adv. Colloid Interface Sci., 2008, vol.137. pp.57-81 – “A recent review by Kaptay [J102] has brought this mechanism back into focus, and it will be briefly surmised here. Kaptay [J102] derived …. 61 lines + Figures 4-5 + Equation (2) ” – pp.62-63.

J102-c9. T.S. Horozov: Foams and foam films stabilised by solid particles - Curr Opinion in Colloid Interface Sci, 2008, vol.13, pp.134-140. – „Several recent works [J102, etc.] treat the problem of liquid film stability by solid particles theoretically, assuming either a bridging monolayer or a bilayer of hexagonally close-packed particles.” – p.137. „A recent review on this subject by Kaptay [J102] is worth to consider. There, previous and more recent theoretical results are analysed and semi-empirical equations for the dependence of max

cP on the particle contact angle are obtained with the toroidal pore model. Results calculated by these equations are compared in Fig.3….. description of Fig.3 (19 lines + 7 lines of figure caption [J102])…” – p.138, „Another mechanism of foam film stabilisation by a network of particle aggregates (gel) inside the film has also been discussed in [J102] (Fig.2.c). … description (7 lines)…” – p.138, „Link between the stability of particle stabilised aqueous films and that of particle-stabilised foams or oil-in-water (o/w) emulsions has also been discussed [J102] … description (15 lines)… . Semiquantitative arguments have been used to estimate the optimum contact angles for the highest foam (o/w emulsion) stability [J102]…decription (3 lines)…” – pp.138-139, „Smaller particles should stabilise the film better but their attachment to the liquid surface is weaker and vica versa [J102].” – p.139. „A good review of theoretical studies on liquid films stabilised by solid particles. Useful approximated equations for the dependence of critical capillary pressure for film rupture on the particle contact angle are obtained. Mechanism of liquid film stabilisation by solid particles are discussed” – p.140.

J102-c10. S Ata: Coalescence of bubbles covered by particles – Langmuir, 2008, vol.24, pp.6085-6091. – „The mechanism of film stabilisation has been explained by the capillary pressure between bubbles, given by {equation}. The theory was first proposed by Ivanov and co-workers and developed further by others [J102]” – p.6086-6087.

J102-c11. I.Akartuna, AR Studart, E.Tervoort, UT Gozenbach, LJ Gauckler: Stabilization of oil-in-water emulsions by colloid particles modified with short amphiphiles – Langmuir, 2008, vol.24, pp.7161-7168. – „The adsoroption energy increases monotonically with increasing contact angle reachin a maximum at 90 degrees. Besides a strong adsorption at the interafce, the stabilization of emulsions also requires that the adsorbed particles impede thinning of the liquid film between droplets. In contract to the adsorption energy, earlier studies have shown that the highest resistance against film thinning is achieved for particles forming contact angles approaching 0 and 180 degrees [J102]. COnsidering these opposite trends, optimum contact angles between 70 and 86 degrees and between 94 and 110 degrees have been suggested for the stabilization of oil-in-water and water-in-oil emuslions, respectively, using interfacial adsorbed particles [J102]. Under such conditions, particles should be able to sterically hinder the coalescence of droplets over long periods of time, which has been experimentally confirmed in a number of recent studies” – p.7161.

J102-c12. H.A.Wege, S.Kim, V.N.Paunov, Q.X.Zhong, O.D.Velev: Long-term stabilization of foams and emulsions with in-situ formed microparticles from hydrophobic cellulose – Langmuir, 2008, vol.24, pp.9245-9253. „Removing such particles from interface requires the expense of a significant transfer eneregz, whose magnitude can be estimated by [J102]: (Eq.1).” – p.9245.

J102-c13. C.Körner: Foam formation mechanism in particle suspensions applied to metallic foams – Mater Sci Eng A, 2008, vol.495, pp.227-235 – “Further progress to explain foam stability was made by Kaptay [J102] who uses a model of a three-dimensional network of solid, spherical particles to explain force transfer between two interfaces and in this way stability” – p.228.

J102-c14. A.J.Klinter, G. Mendoza-Suarez, R.A.L.Drew: Wetting of pure aluminum and selected alloys on polycrystalline alumina and sapphire – Mater Sci Eng A, 2008, vol.495, pp.147-152. – “Recently it has been derived that the most favorable ciontact angle range for a liquid foam to be stabilized by particles is between 70 and 86 degrees [J102]. An experimental simulation conducted by Sun et al employing ethanol/water mixture and polymeric particles supports this finding showing that the most stable foams were obtained when the liquid wetted the particles in a range of 70-85 degrees. Therefore, it is assumed that in order to produce stable aluminum foams, the aluminum alloy melt needs to wet the added ceramic particles in this optimum contact angle range of 70-86 degrees over the temperature span between that of the melt bath in the direct foaming method (typically around 750 – 800 Centigrades) and the solidification of the alloy” – p.148.

J102-c15. A.J.Klinter, R.A.L.Drew: Evaluation of the wetting behaviour of Al-7Cu and Al-11.5Si on SiC and sapphire in terms of Al-foam stability. In: METFOAM-2007, ed. by L.P.Lefebre, J.Banhart, D.C.Dunand,

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DEStech Publ. Inc, 2008, pp.23-26. – „During the early stages of Al-foam rersearch, it was found that alumina or SiC particles are essential in order to obtain stable aluminium foams. Originally it was believed that the stabilizing effect of these ceramic particles have on Al-foams was caused by an increase in bulk viscosity of the Al melt due to ceramic particles additions. In a very theoreticla approach, KAPTAY [P41, J84] later developed models suggesting that the improved foam stability was due to capillary effects between the melt and the particles, preventing the two liquid gas interfaces of a foam cell wall from touching, and the two adjacent cells from coalescencing….. KAPTAY concluded recently in a complex and theoretical study [J102] that the optimum contact angle for foam stabilization by a single or a closely packed double layer of particles is between 70 and 86 degrees” – p.23. „Fig-s 5 show that Al-11.5Si wets the substrate better than Al-Cu, however neither alloy reaches the optimum contact angle range for foam stabilization [J102]” – p.25. „Conclusions. … A number of researchers have shown that metal foams can be produced using a verity of aluminum alloy – ceramic particle combinations (including Al2O3, SiC and TiB2). Nevertheless, it is believed that foams with narrower pore size distribution and more homogeneous properties can be produced if alloy-particle combinations are chosen with wetting properties int he optimum contact angle range for foam stabilization by particles of 70 to 86 degrees derived by KAPTAY [J102]” – p.26.

J102-c16. C.Koerner: Integral Foam Molding of Light Metals – Springer, 2008, 224 pp. – „ Kaptay [J102] was the first who realized, that stabilization for this kind of particles is based on the development of 3D network structures which transfer forces from one interface to the other” – p. 100.

J102-c17. Hunter, T.N., Wanless, E.J., Jameson, G.J.: Effect of esterically bonded agents on the monolayer structure and foamability of nano-silica - Colloids and Surfaces A: Physicochemical and Engineering Aspects, 2009, vol. 334, pp. 181 – 190. – „Kaptay [J102] has theoretically weighted the effects of weakly and strongly hydrophobic particles and estimated that particles wit ha contact angle 70o would best stabilize foam films with a single layer of particles. For a bi-layer of particles, the contact angle for maximum stability changes to 85o [J102] (more in line with emulsions) suggesting concentration and conformation may affect the extent in which particles of different hydrophobicity stabilize a system” – p.181, “The weak stabilization of the SiO-dodecane dispersions highlights that the bubbles in the dynamic foams are likely not fully loaded, and as drainage continues, bubbles interact with only a single bridging layer of particles (giving theoretical maximum stability with particles near 70o [J102]).” – p.186, “Following on from Kaptay [J102] and the work tabled in a pre4vious review [], it appears dynamic foams are stabilised by species of intermediate hydrophobicity, where there is a balance of inter-bubble and steric stabilisation forces.” – p.188.

J102-c18. Hunter TN, Jameson GJ, Wanless EJ, Dupin D, Armes SP: Adsorption of Submicrometer-Sized Cationic Sterically Stabilized Polystyrene Latex at the Air-Water Interface: Contact Angle Determination by Ellipsometry - Langmuir, 2009, vol. 25, pp. 3440-3449. – „Less hydrphobic particles can also dynamically stabilize bubbles by altering threshold capillary pressure [J102]” – p.3441.

J102-c19. Fournier CO, Fradette L, Tanguy PA: Effect of dispersed phase viscosity on solid-stabilized emulsions – Chemical Engineering Research & Design, 2009, vol. 87, pp. 499-506. – „As a general rule, a hydrophobic particle favors a water-in-oil emulsion while a hydroplhilic particle generates an oil-in-water emulsion. However, this rule may be broken depending on the number of layers the solid particles will form at the oil-water interface. Based on the energy and maximum capillary pressure considerations, Kaptay (2006) showed that for an emulsion stabilized by a single layer of particles, the contact angle for o/w emulsions must be between 15 and 90 degrees and for w/o emulsions, the contact angle must be between 90 and 165 degrees. For emulsions stabilized by a double layer of particles, o/w emulsions are stable for contact angle values between 15 and 129.3 degrees and w/o emulsions are stable for contact angle values between 50.7 and 165 degrees. Furthermore, the interval of optimum contact angle, for both single and double particles layer appears to be between 70 and 86 degrees for o/w emulsions and between 94 and 110 degrees for w/o emulsions” – pp.499-500.

J102-c20. J.Frelichowska: Emulsions stabilisees par des particules solides: etudes physico-chmiques et evaluation pour l’application cutanee, PhD, L’Universite Claude Bernard Lyon 1, 2009 Jan – “La stabilite du film de phase continue entre les gouttelettes peut aussi empecher la coalescence. Le film peut etre stabilise par des forces capillaires et/ou les proprietes theologiques de l’intergace elle-meme [J102] – p.59.

J102-c21. A.J.Klinter, C.A.Leon-Patino, R.A.L. Drew: The optimum contact angle range for metal foam stabilization: an experimental evaluation of theory – Abstract book of 6th HTC conference, 6-9 May, 2009, Athens, Greece, p.75 – „From the measured values, contact angle vs. Temperature curves were generated, some of which satisfy the contact angle requirement between liquid metal and ceramic particles for optimum metal foam stabilization proposed by Kaptay (70 to 86 degrees) [J102]. …. Comparing the experimentally observed liquid foam stability and the resulting foam morphology with the obtained

http://mail.elsevier-alerts.com/go.asp?/bESJ001/mTX06Y8/qBX0FY8/uVZA56/x4SUOY8/cutf-8http://mail.elsevier-alerts.com/go.asp?/bESJ001/mTX06Y8/qBX0FY8/uVZA56/x4SUOY8/cutf-8http://apps.wosportal.om.hu/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=T1B4Hm@Iiji89i8hGe8&name=Hunter%20TN&ut=000264145000022&pos=1http://apps.wosportal.om.hu/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=T1B4Hm@Iiji89i8hGe8&name=Jameson%20GJ&ut=000264145000022&pos=2http://apps.wosportal.om.hu/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=T1B4Hm@Iiji89i8hGe8&name=Wanless%20EJ&ut=000264145000022&pos=3http://apps.wosportal.om.hu/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=T1B4Hm@Iiji89i8hGe8&name=Dupin%20D&ut=000264145000022&pos=4http://apps.wosportal.om.hu/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=T1B4Hm@Iiji89i8hGe8&name=Armes%20SP&ut=000264145000022&pos=5http://apps.wosportal.om.hu/full_record.do?product=WOS&search_mode=CitedRefIndex&qid=2&SID=T1B4Hm@Iiji89i8hGe8&page=1&doc=1http://apps.wosportal.om.hu/full_record.do?product=WOS&search_mode=CitedRefIndex&qid=2&SID=T1B4Hm@Iiji89i8hGe8&page=1&doc=1http://apps.wosportal.om.hu/full_record.do?product=WOS&search_mode=CitedRefIndex&qid=2&SID=T1B4Hm@Iiji89i8hGe8&page=1&doc=1http://apps.wosportal.om.hu/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=X1BfMlK6dNbdIk29mK7&name=Fournier%20CO&ut=000264913500017&pos=1http://apps.wosportal.om.hu/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=X1BfMlK6dNbdIk29mK7&name=Fradette%20L&ut=000264913500017&pos=2http://apps.wosportal.om.hu/DaisyOneClickSearch.do?product=WOS&search_mode=DaisyOneClickSearch&db_id=&SID=X1BfMlK6dNbdIk29mK7&name=Tanguy%20PA&ut=000264913500017&pos=3

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contact angle vs. Temperature curves allows an evaluation of Kaptay’s theooretically derived requirements for optimum foam stabilization by ceramic particles [J102]” – p.75.

J102-c22. SE Friberg: Effect of relative humidity on the evaporation path from a phenethyl alcohol emulsion – J Coll Interface Sci, 2009, vol.336, pp.786-792 – „Emulsions are one of the most important vehicles both for their own processing as well as their application in a large number of industries such as pharmaceutics, cosmetics, preparation of nano-particles and others. Hence, general treatments ar ereadily available and there heas been significant progress in the more fundamental aspects of the related science [J102]” – p.786.

J102-c23. Fournier CO, Fradette L, Tanguy PA: Effect of dispersed phase viscosity on solid-stabilized emulsions – 13th European Conference on Mixing, London, 14-17 April, 2009, Proceedings, 8 pp. – „As a general rule, a hydrophobic particle favors a water-in-oil emulsion while a hydroplhilic particle generates an oil-in-water emulsion. However, this rule may be broken depending on the number of layers the solid particles will form at the oil-water interface. Based on the energy and maximum capillary pressure considerations, Kaptay (2006) showed that for an emulsion stabilized by a single layer of particles, the contact angle for o/w emulsions must be between 15 and 90 degrees and for w/o emulsions, the contact angle must be between 90 and 165 degrees. For emulsions stabilized by a double layer of particles, o/w emulsions are stable for contact angle values between 15 and 129.3 degrees and w/o emulsions are stable for contact angle values between 50.7 and 165 degrees. Furthermore, the interval of optimum contact angle, for both single and double particles layer appears to be between 70 and 86 degrees for o/w emulsions and between 94 and 110 degrees for w/o emulsions” – p.1.

J.102-c24. I.Akartuna: porous materials and capsules from particle-stabilized emulsions – PhD dissertation, Chapter 2. Zurich, 2009 – “Optimum contact angles between 70 and 86 degrees, and between 94 and 110 degrees have been suggested for the stabilization of oil-in-water and water-in-oil emulsions, respectively, using interfacially adsorbed particles [J102]” – p.16.

J.102-c25. I.Akartuna: porous materials and capsules from particle-stabilized emulsions – PhD dissertation, Chapter 3. Zurich, 2009 – “The adsorption of colloidal particles to liquid-liquid interfaces can be achieved by adjusting their wettability in the liquid media or, in other words, their contact angle at the liquid interface. In general, particles with contact angles lower than 90 degrees tend to stabilize oil-in-water emulsions, whereas particles exhibiting contact angles higher than 90 degrees yield water-in-oil emulsiopns [J102]” – p.42.

J102-c26. S.N.Tan, Y.Yang, R.G.Horn: Thinning of a vertical free-draining aqueous film incorporating colloidal particles – Langmuir, 2010, vol.26, No.1, pp.63-73. – “Various possible film stabilization mechanisms of particle stabilized films have been suggested in the literature: film stabilized by bridging particles, bilayer of hexagonally close packed particlesand network of particles aggregates (gel) inside the film [J102].” – p.71. “Kaptay [J102] used a thermodynamic approach to explain the role of particles in film stability… 12 lines of description” – p.72.

J102-c27. Á.Detrich, A.Deák, E.Hild, A.L.Kovács, Z.Hórvölgyi: Langmuir and Langmuir-Blodgett films of bidisperse silica nanoparticles – Langmuir, 2010, vol.26, pp.2694-2699, doi: 10.1021/1a9027207. – The stabilizing effect of fine particles in foaming and emulsification has been extensively studied during the past decades” – p.2694

J102-c28. S.Kubowicz, J.Daillant, M.Dubois, M.Delsanti, J-M. Verbavatz, H.Möhwald: Mixed-Monolayer-Protected Gold Nanoparticles for Emulsion Stabilization – Langmuir, 2010, vol.26, No.3, pp 1642–1648.

J102-c29. A.J.Klinter, C.A.Leon, R.A.L.Drew: The optimum contact angle range for metal foam stabilization: an experimental comparison with the theory – J. Mater Sci., 2010, vol.45, pp.2174-2180 – „Kaptay [102] developed different models of particle arrangement – detailed description of the model in 20 lines + Fig.1” – p.1-2/7. „From particle-stabilized foams presented by other researchers it can be seen that the closely packedd double layer or complex 3-dimensional network models proposed by Kaptay [102] are the most representative for aluminium foams” – p.2/7. “Using the PM method, the present work aims to evaluate the possibility to predict foam expansion performance based on wetting behaviour and Kaptay’s [102] model” – p.2/7. „Assuming the closely packed double layer model (Fig.1) [102], those liquid metal/solid particle combinations should form the most stable foams that exhibit contact angles in the range of 85-90 degrees.” – p,5/7. “This is in agreement with .. , as well as Kaptay [102] and must be interpreted as improved wetting … “ – p.5/7. “Thus, base don the contact angle behaviour of the tested metal/Al2O3 combinations, Kaptay’s closely packed double layer model (Fig.1) predicts the foam stability/quality sequence among these combinations correctly, with exception of Al-1Mg/Al2O3, which should yield foams of similar quality and expansion as Al-11.5Si/Al2O3.” – p.5/7. „It can be therefore stated that the model … is conclusive. Nevertheless, it