Ceramic Particles Stabilized Aluminum Foams. Norbert Babcsán. Theses of Ph.D. dissertation



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Theses of Ph.D. dissertation Ceramic Particles Stabilized Aluminum Foams Norbert Babcsán Supervisors: Prof. P. Bárczy, University of Miskolc Prof. H.P. Degischer, Technical University of Vienna Miskolc, Mat. Sci. and Tech. Ph.D. School Kerpely Antal 2003

BACKGROUND AND AIMS Metal foams belong to the most challenging materials developed recently. A number of manufacturing technologies for foamed metals have been developed, mostly based on empiricism instead on a profound scientific knowledge. Despite their quality improvement in the last 10 years the resulting metal foams still suffer from non-uniformities and other deficiencies. Metal foams can be characterized by three expressions: profitability, safety and noise reduction. By exclusive combination of gas bubbles and metallic materials one can implement: a) an extra increase of the price of a product, b) new economically important energy absorbing materials increasing safety of the cars and the buildings, c) noise reduction by sound absorption and vibration damping. The volume fraction of gas bubbles in the metal is a simple variable to tailor the properties for the costumer requirements. The wide range of possible properties can lead to innovative applications, which is a strong driving force for the improvement of metal foam production technologies. Several types of metal foams have been produced since the first one patented in 1948 [1, 2, 3]. In the 1990 s it was clarified that direct foaming of metallic melt or the indirect foaming of metal powder compact can produce metal foams cost efficiently. Nearly all metals can be foamed but aluminum has the highest importance. The main challenge of recent research is to achieve a uniform cellular structure, to perfect reproducibility in manufacture and to control foam architecture. In 2000 D. Leitlmeier and coworkers at LKR, Austria reinvestigated the direct foaming process and successfully developed aluminum foams with homogeneous cell size distribution, now called METCOMB â [4, 5]. The first metal foam from CYMAT â was shown to me by Prof. Bárczy in 1998. At that time my students and I started to learn about aqueous foam stability and heat conductivity of polymeric foams. Under my supervision three student-research works [6, 7, 8] and two diploma works [9, 10] have been executed on aqueous, polymeric and metal foams. In 2000 and 2001 as an AMTT user I carried out measurements of metallic foam heat conductivity and oxide layer examination by TEM at ARC Seibersdorf, Austria. In September 2001 I became the leader of a new foam stability project with financial support of LKR, Austria. The project is strongly related to industrial development under a confidentially agreement. Since that time I partly worked in Austria with Prof. Degischer and partly in Miskolc and I had the fortune to experience both the phenomenon (academy) and the purpose (industry) oriented research [11]. The project has been finished by the end of 2002. In summary I attempted to answer the following questions related to ceramic particle stabilized aluminum foams: 1. What is the apparent surface tension of particle-reinforced aluminum melt? 2. How do the process parameters influence the cell wall structure? 3. What is the effect of the blowing gas? 4. How is this liquid-aluminum foam stabilized? 1 2

EXPERIMENTS AND EXAMINATION METHODS The materials selected for investigation can be divided into 5 groups. Pure aluminum alloys without particles, Duralcan metal matrix composites (MMC), further alloyed Duralcan MMCs, MMCs produced by LKR and CYMAT foam. All the MMCs had a wrought or cast aluminum alloy matrix and were reinforced by 10-20 µm size Al 2 O 3 or SiC particles. Differential Scanning Calorimeters were applied to determine the solidus and liquidus temperature of the MMCs. The measurements were carried out in nitrogen atmosphere with 5 K/min heating and cooling rate. Considering the advantages and disadvantages of various high temperature surface tension measurement methods, a self constructed High Temperature Maximum Bubble Pressure Tensiometer (HTMBPT) was built at the University of Miskolc. Apparent surface tension measurements were performed on Al 2 O 3 stabilized wrought alloy series and pure aluminum. Prior to the foaming experiments single cell wall pull out tests demonstrated the stability of liquid MMC films and the instabilities of particle-free liquid-aluminum alloys. Aluminum liquid foam was produced in an adiabatic furnace of LKR Austria by gas injection into an MMC melt. The applied foaming equipment was constructed for these experiments. Oxygen, air and nitrogen with 3 ppm oxygen were used as foaming gases. Due to the special gas injector the bubble formation was well controlled. After foam production the liquid-metal foam was held isothermally and solidified then in air or quenched in water. 3 The following structural examination methods were applied in order to determine the cell wall geometry and the microstructure of these solid aluminum foams: micrometer, light optical microscopy, scanning electron microscopy, image analysis, x-ray diffraction and transmission electron microscopy. SCIENTIFIC THESES 1. The apparent surface tension of foamable liquid aluminum can be determined applying the self-constructed High Temperature Maximum Bubble Pressure Tensiometer. Increasing Al 2 O 3 particle concentration has a decreasing effect on surface tension (Fig. 1). s, N/m 1.0 0.9 Bubble rupture 0.8 0.7 0.6 0.5 Foam 0.4 0 2 4 6 8 10 Particle volume, % Fig. 1. Surface tension of Al MMCs in function of Al 2 O 3 particle content of the melt at 700 C 4

2. The effect of process parameters on the geometrical and microstructure of the Al foams was described. It was shown that at foaming temperature (700 C) Al 2 O 3 particles reacted with liquid aluminum (forming spinel) if the Mg content of the alloy was higher than 0.3 at %. High Si content suppressed the spinel formation. The size of the dendrite arms was similar to the particle size in the quenched samples. Thus the observed particle distribution is considered as it was in the liquid. The particle concentration in the cell walls is considerably higher than in the original melt. In the case of foaming by nitrogen the cell wall surfaces are further enriched by particles, whereas surface segregation was not significant foaming with air or oxygen. The lognormal thickness distribution of cell walls was demonstrated by 400 individual thickness measurements on each of the foam samples. The cell wall thicknesses are almost independent of the type of blowing gas but slightly depend on alloying elements and foaming temperature. They are almost twice as thick for Al 2 O 3 containing matrixes than for SiC reinforcements: in the range of 100 µm (about 10 times the Al 2 O 3 particles diameter, if spinel was formed at the interface) and 50 µm (about 5 SiC diameters), respectively. There is some evidence that in absence of the interface spinel the cell wall thickness is somewhat smaller. The observed cell wall thickness remained constant even when solidification was delayed. Beyond the characteristic cell wall thickness drainage effects did not occur even after 100 min isothermal holding. 3. Using oxygen containing blowing gas produces oxide skins on the cell wall surfaces, which stabilize the foam structure by their mechanical rigidity. The thickness of that oxide skin depends on the foaming gas and the wall material in the way listed in Table 1. 5 Short-term oxidation mostly produced homogeneous oxide layer, which most probably built up from g-al 2 O 3 grains. After long-term oxidation primary and secondary oxides are present in the skin. Table 1. The oxide layer thickness of METCOMB foams measured by TEM N 2 foamed AlSi9Mg0.6/ Air foamed AlSi9Mg0.6/ O 2 foamed AlSi9Mg0.6/ O 2 foamed AlSi9Mg1.2/ Average thickness, nm 12 ± 1 37 ± 6 62 ± 31 28 ± 9 4. The critical parameters influencing foam stability of particle-reinforced aluminum melts are summarized: In order to have stable liquid-aluminum foam both a suitable amount (more than 5 vol%) of poor wetting particles and sufficiently thick oxide layer (more than 20 nm) are necessary. Foam stability is directly connected with largely reduced surface tension. Stability is also influenced by technology dependent reaction layers on particles, but nearly independent of the alloy, foaming temperature and time. UTILIZATION The results can be used for understanding particle stabilized aluminum foaming and designing higher quality aluminum foams. They have already been applied to improve the models of particle-stabilized foams [12, 13]. 6

OUTLOOK Further investigation will be carried out: Experiments on understanding the role of wettability of particles in liquid foam stability. Effect of nanosize particles on foam stability of powder metallurgically produced MMCs. In-situ investigation of cell wall thinning and rupture by X-ray radiography. SCIENTIFIC PUBLICATIONS Abstracts N. Babcsán, P. Bárczy: On correlation of foam development kinetics and materials properties, Book of abstracts, Metfoam 99, Bremen, 14-16.06.1999 N. Babcsán, D. Leitlmeier, H. P. Degischer and H. J. Flankl: Foamability of Particle Reinforced Aluminium Melts, Book of abstracts, Eurofoam2002, Manchester, 08-10.07.2002 N. Babcsán and I. Mészáros: Thermal and electrical conductivity measurements on metal foams, Book of abstracts on the Internet www.junior-euromat.fems.org, Junior Euromat 2002, Lausanne, 02-05.09.2002 Papers N. Babcsán: Some Examples on Foam Structure and Materials Properties, (ISBN 963-661-353-2) microcad 99 Conference Proceedings, Miskolc, 24-25.02.1999. pp. 1-6. D. Leitlmeier, H. P. Degischer, N. Babcsán and H. J. Flankl: Development of a Melt Foaming Process with Particulate Reinforced Aluminum Alloys, In: Light Metals 2002 Métaux Légers, Edited by T.Lewis, ISBN: 1894475216, (2002) 575-588 N. Babcsán, I. Mészáros and N. Hegman: Thermal and electrical conductivity measurements on metal foams, Proceedings of 2 nd Int. Meeting on Space and Aerospace Materials Technology, Seibersdorf, 04.11.2002. pp. 90-93 N. Babcsán, Habosított fém, Természet Világa, 2003. Január, pp. 36-38 N. Babcsán, D. Leitlmeier and H. P. Degischer: Foamability of Particle Reinforced Aluminum Melts, Materialwissenschaft und Werkstofftechnik 34, (2003) pp. 22-29 N. Babcsán, I. Mészáros and N. Hegman: Thermal and electrical conductivity measurements on metal foams, Materialwissenschaft und Werkstofftechnik 34, (2003) pp. 391-394 SCIENTIFIC PRESENTATIONS Poster Presentations N. Babcsán, P. Bárczy: On correlation of foam development kinetics and materials properties, Metfoam 99, Bremen, 14-16.06.1999 N. Babcsán: Metal foams, Tavaszi Szél Conference, Gödöllő, 12-14.04.2002 N. Babcsán: Heat conductivity of metal foams, MINING, METALLURGY @ 3.MILLENNIUM M3 Conference, Vienna, 29.05-01.06.2002 7 8

N. Babcsán: The stability of melt metal foam, MINING, METALLURGY @ 3.MILLENNIUM M3 Conference, Vienna 29.05-01.06.2002 N. Babcsán: Részecskestabilizált alumínium habok, Anyag és Kohómérnöki Kar Tudományos Konferenciája, Miskolc 29-31.08.2002 N. Babcsán and I. Mészáros: Thermal and electrical conductivity measurements on metal foams, Junior Euromat 2002, Lausanne, 02-05.09.2002 Oral Presentations N. Babcsán: Some Examples on Foam Structure and Materials Properties, microcad 99 Conference, Miskolc, 24-25.02.1999 N. Babcsán: The Structure of SiC Particle Reinforced Al Alloy Foam, Microcad Conference, Miskolc, 07.03.2002 N. Babcsán: Fémhabok, az előállítástól a felhasználásig, KFKI Budapest 22.03.2002 N. Babcsán, D. Leitlmeier, H. P. Degischer and H. J. Flankl: Foamability of Particle Reinforced Aluminium Melts, Eurofoam2002, Manchester, 08-10.07.2002 D. Leitlmeier, H. P. Degischer, N. Babcsán and H. J. Flankl: Development of a Melt Foaming Process with Particulate Reinforced Aluminum Alloys, MET SOC. 41st Annual Conference of Metallurgists of CIM August 11-14, 2002 Montreal, Canada N. Babcsán: Alumíniumhabok, Anyagtudományi Őszi Iskola, Visegrád 24.09.2002 N. Babcsán, I. Mészáros and N. Hegman: Thermal and electrical conductivity measurements on metal foams, 2 nd Int. Meeting on Space and Aerospace Materials Technology, Seibersdorf, 04.11.2002 LITERATURE [1] H. P. Degischer and B. Kriszt, Handbook of cellular metals, WILEY Verlag GmbH, Weinheim (2002) [2] V. Gergely, H.P. Degischer and T.W. Clyne, Recycling of MMCs and production of metallic foams, Comprehensive Composite Materials, 3 (2000) 797-820 [3] J. Banhart and D. Weaire, On the Road Again: Metal Foams Find Favor, Physics Today July (2002) 37-42 [4] D. Leitlmeier, H.P. Degischer and H.J. Flankl, Development of a foaming process for particulate reinforced aluminum melts, Adv. Eng. Mat., 4, No. 10 (2002) 735-740 [5] D. Leitlmeier, H. Flankl: "Development of a New Processing Technique for Net-shape Foam Parts based on the Melt Route", In: Cellular Metals and Metal Foaming Technology (Ed.: J. Banhart, M.F. Ashby, N.A. Fleck), Verlag MIT, Bremen (2001), 171-174 [6] A. Szemanik, E. Nagy, Habok vizsgálata, TDK dolgozat, University of Miskolc, 1998 [7] L. Kollár and M. Kollár, Poliuretán kemény és lágyhabok, TDK dolgozat, University of Miskolc, 2000 [8] A. Szemanik, Fémhabok előállítása és vizsgálata, TDK dolgozat, University of Miskolc, 2000 [9] A. Szemanik, Fémhabok előállítása és vizsgálata, Diploma work, University of Miskolc, Department of Non-metallic Materials, 2000 [10] Zs. Pyka, Beltéri ajtó tervezése fémhabból, Diploma work, University of Industrial Art, Budapest, 2001 [11] P. Bárczy, Materials Science or Materials Design, Materials Science Forum, 414-415 (2003) 1-8 [12] G.Kaptay: DSc Thesis, Miskolc, 2003 (manuscript) [13] G. Kaptay, Interfacial criteria to stabilize liquid foams by solid particles, submitted to Colloid and Surfaces A (2003) 9 10