COST 507 - Repositório Aberto da Universidade do Porto

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BCC B2«2 TIRL TIRL RL3M D022 TIRL RL3M D022 BCC Β2·2 TIRL RL3M D022 BCC B2Ì2 RL3M_D022 PLBVS BCC B2t RL3M_D022 RLBV5 RL3M_D022 RL3M_D022 FCC_P1 PL10V RL3M D022 FCC fil RL10V RL3M_D022 RL10V RL3M_D022 RL7V RL311_D022 PL7V RL23V4 RL3h_D022 PL7V RL23V4 RL3M_D022 BCC B2»2 T13RL TIRL BCC_B2»2 TI3RL TI3RL BCC B2#2 BCC_B2#2 HCP_R3 0.2 0.4 0.6 MOLE FRACTION AL Figure 13 0.2 0.4 0.6 0.8 MOLE FRACTION V 1 .0 Figure 14: Calculated A2B2 boundary 1573K873K 244
0.2 0.3 0.4 0.5 X(LIQ,V) Figure 15 Calculated liquidus surface 4 References [60Kub] 0 Kubaschewski, C Wainwright, F J Kirby, J.Inst. Metals,1960, 89, .139-144. [68Kor] 11 Kornilov, M A Volkova, Izvestia Akad. Nuak, S.S.S.R., 1968, Met (1), 176-180. [68Tsu] T Tsuijimoto, Trans. Japanese Institute of Metals, 1969, 10, 281-286, translated from Journal of the Japanese Institute of Metals 1968, 32(10), 970-975. [85Has] K Hashimoto, H Doi, T Tsuijimoto, Trans. Japanese Institute of Metals, 1986, 27(10), 741-749, translated from Journal of the Japanese Institute of Metals, 1985, 49(6), 410-416. [88Mae] T.Maeda, Ph.D. Thesis, Imperial College, University of London (1988). [91Par] M Paruchuri, T B Massalski, Materials Research Society Symposium Proceedings 1991, 213, 143-149. [93Hay] F H Hayes, 'TernaryAlloys', Volume 8, ed. G Petzow and G Effenberg , pub VCH Verlagsgesellschaft, Weinheim, Germany, 426-455, 1993. [93Nak] H Nakamura, M Takeyama, L Wei, Y Yamabe, M Kikuchi, Symposium on Intermetallic Compounds for High Temperature Structural Applications, 3 rd Japanese Int. SAMPE Symposium, December 1993, Scripta Met. &Mat., 1993,28,997-1002. [94Ahml] Τ Ahmed, Η M Flower, Materials Science and Technology, 1994, 10, 272-288. [94Ahm2] Τ Ahmed, H.J.Rack, H.M.Flower, Materials Science and Technology, 1994,10, 681-690. [94Hay] F H Hayes, COST 507 I Project Final Report, Thermodynamic Assessment of the Ti-Al-V system, June 1994. [95Sau] N.Saunders, Thermodynamic Database for Light Metal Alloys, ed. I Ansara COST 507, Concerted Action on Materials Sciences, European Commission, DG XII, Luxembourg, 1995. [95Hay] F H Hayes, J.Phase Equilibria, 1995, 16 (2), 163-176. 245 -
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European Commission COST European c
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European Commission COST European c
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Preface The Final Workshop of the C
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COST 507 STRUCTURE Measurement and
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GRl: Mirtee S.A., Volos Mr.P.Polati
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D9 Dll Fl GR2 II NI S3 SF1 "Thermop
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A Summary of the COST 507 Action an
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Aluminium-based systems Titanium-ba
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An Example using the COST 507 Datab
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Appendix COST 507: Some Key Meeting
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Al - 0.5 Fe, 1 Mg, 0.8 Mn, 0.2 Si (
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Fig 4 Aluminium beverage cans. The
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Fig 6 High pressure compressor vane
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INTRODUCTION All of us are aware of
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In the interaction with materials a
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There was a first warning more than
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Some time ago, the well-known physi
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Today there is a whole range of ins
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The dimension of this reservoir inc
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REFERENCES [ 1 ] G. Petzow, "Man, M
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Trends in Application of Materials
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Raw Materials The Cycle of Material
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i LÌ i.'»Af·· iù^ VV.V.X. iTTa
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1600 OJ 1200 .« 1100 d 1000 900 Si
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Al Phase Relations in the Aluminium
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oundaries of the single phase regio
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Table 1 : Crystallographic Data of
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order to facilitate the evaluation
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(especially around 33 at% Mg) in or
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3.System Ti-Sn-Al-N. The investigat
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6) N.Durlu, U.Gruber, M.Pietzka, H.
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Summary of final report Directional
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calculate the thermodynamic mixing
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Introduction It is the aim of this
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Thermodynamic evaluations for high
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Figure 5 presents the calculated li
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There is a complete lack in the lit
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a.B5 ø.ia 0.15 0.20 0.25 0.30 0.35
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700 [53Phi] 800 +[90Kuz21 ]iquld a
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Thermodynamic Assessments, Experime
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AIN and TiNi_ x is also given. Vari
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satisfied the three requirements of
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84Bey R. Beyers, R. Sinclair, and M
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Material and Methods 2.1 Fabricatio
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3.4 Electronmicroscopy (SEM) and X-
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Tab. 3: Density of the Ti20Albase
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Tab.5. continued TÌ20A1 5CulONi Ti
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Fig. 3: ESMA and Xray diffraction
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Fig.7: Wetting angle of Ti 15A1 lOC
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Thermophysical Properties of Light
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Tab.2 Chemical composition of terna
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700 (AI)+AIFeS¡«_600 KS1275.1 l
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4.2 Thermal conductivity of industr
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4.3 AlSiZn alloys Electrical re
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94Jar/Bra G.Jaroma-Weiland, R.Brand
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MgZn9 (C 14) and Mg2Zn u in the Al
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The three Laves phases were describ
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References [13Ege] G. Eger, Z. Meta
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0.30 0.35 0.40 0.45 0.50 mole fract
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□ [48Koe] 600 500 400 0 0.1 0
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MggZn,, this work □ Single phase,
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Temperatures in °C 0.05 0.10 mole
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Table 2 : Alloy compositions Alloy
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All. Dy 50 Cpexp °C Cpadd Table 5
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Zn ¿Kl Si Fig. 2 : Position of the
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22.5 ■■ 7.5 Temperature ICI Tem
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.to 2.5 "lõõ soo iÍOõ dOõ rtõ
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GR2 Differential Scanning Calorimet
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Time (x10 3 sec) Fig. 1. DSC Thermo
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solidification. It can be seen that
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4. Conclusions Differential scannin
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COST 507 - ROUND Π UNIT II SEZIONE
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[96Sac] The Rrich regions of the
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List of publications in the framewo
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2Contributions: oral or posters p
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1996 REPORT 2 s ' PART: ACTIVITY CA
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[96Sei] Excess Gibbs energy coeffic
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List of publications in the framewo
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Proc. :7 th Meeting on "Syntheses a
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2.1 Solid solubility measurements T
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eviews by Rivlin and Raynor [81 Riv
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inaires. Thesis, Universite Scienti
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Table 1. Review of the ternary phas
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L) Liq+bcc=FeSi+t_1 M) Liq+t 1=FeSi
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Extrapolations based on Ti-C-N S3 B
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value has been accepted in all thre
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with high precision whereas Jonsson
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only fit the hightemperature asym
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Jonsson combined his descriptions o
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Table II. Solubility product of TiC
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Ti-C, Z.Metallkd. 86 (1995) 5 319
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1000 1500 2000 2500 3000 Τ (K) Fig
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o Oí o 3 4 5 6 7
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M^øD^ O Kelley(1944) • Kelley an
Page 197 and 198: — cale, with Dumitrescu (1997) -
Page 199 and 200: € gfc-π m-, .-π-, π-π .-saa J
Page 201 and 202: +graph 0 TiN 0.2 0.4 0.6 X TiC 0.8
Page 203 and 204: Binder et al (1992) TiN 1423 K ■
Page 205 and 206: 0.08 600°C 700°C 800°C 900°C 10
Page 207 and 208: [59Sto]: Ä600°C □ 70D°C O8Q0°
Page 209 and 210: 2000 Cale, with Saunders (1997) —
Page 211 and 212: An Experimental Investigation of th
Page 213 and 214: An Experimental Investigation of th
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Page 217 and 218: EXPERIMENTAL INVESTIGATION OF THE C
Page 219 and 220: Fig.1 SEM micrographs of CuMgZr
Page 221 and 222: ■ 888 24 HSM^«" 16—19 3 À I
Page 223 and 224: Thermodynamic Evaluations of the Al
Page 225 and 226: Fcc_Al aves_C15 ONU ΔΝ12 αΝ13
Page 227 and 228: 2.2 Assessment The optimisation of
Page 229 and 230: 0.50 0.45 CulOZr7/ 0. 40 Or ^ 0.3
Page 231 and 232: References [71Kri] Kripyakevich, P.
Page 233 and 234: Kejun Zeng and Marko Hämäläinen,
Page 235 and 236: for detennining phase boundary and
Page 237 and 238: Table 2 Al-Fe-Mn results wt%Fe 0.5
Page 239 and 240: •00 Γ Ι I I I ~ LIQUID S^ 7iO
Page 241 and 242: the observed A2-B2 ordering. This p
Page 243 and 244: 1473K Ahmed & Flower [94 Ahmi] 0.2
Page 245 and 246: 900K Paruchuri & Massalski [91Par]
Page 247: BCC_B2#2 TI3RL TIPL BCC B2#2 TIRL
Page 251 and 252: 1 Introduction and Overview of the
Page 253 and 254: at least 95% by Fe, possibly 99%, a
Page 255 and 256: 8 References 43Phi H W L Phillips,
Page 257 and 258: 1050 1000 Isopleth, Al - Si - 4 wt
Page 259 and 260: Al-Mn-Si 873 K 0.90 Liquid 0.80 0.7
Page 261 and 262: A Thermochemical Assessment of Data
Page 263 and 264: certainly due to the appearance of
Page 265 and 266: Materials Science Centre, November
Page 267 and 268: 1400 Al-Mn Fig 2 Calculated partial
Page 269 and 270: 1000 ι AlMn I Ι 950 Liquid E ω
Page 271 and 272: Al-Fe-Mn 843 K 0.90 0.80 0.70 0.60
Page 273 and 274: AlFeMn section at 2 wt% Mn co
Page 275: 0.50 0.45 0.40-1 LU £ 0.35 LU 0.30
Page 279: European Commission EUR 18171 —CO
Page 284: NOTICE TO THE READER Information on
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