Page 1
CALPHAD Vol. 11, No. 4, pp. 395-406, 1987 Printed in the USA.
SUBJECT INDEX
CALPHAD: Computer Coupling of Phase
VOLUME 11,1987
C. Bernard
0364-5916/87 $3.00 t .OO (c) 1987 Pergamon Journals Ltd.
Diagrams and Thermochemistry
Laboratoire de Thermodynamique
et Physico-Chimie Metallurgiques
ENSEEG, Domaine Universitaire B.P.44,
38401 St. Martin d'Heres, FRANCE
231
AN ALGORITHM AND COMPUTER PROGRAM FOR CALCULATING COMPOSITION PHASE DIAGRAMS
CONNOLLY J.A.O./KERRICK O.M./
CALPHAO. 1987. 11. (I). l-55. ---_--_-___-____________________________-~~--~~~~~
232
A THERMODYNAMIC DESCRIPTION AN0 PHASE RELATIONSHIPS OF THE FE-CR SYSTEM: PART
I THE BCC PHASE AND THE SIGMA PHASE
CHUANG YING-VU./LIN JEN-CHWEN./CHANG A.Y./
CALPHAO. 1987. 11. (1). 57-72. ____________________~____~~~~~~~~~~~~~~~__~~__~___
233
A THERMODYNAMIC DESCRIPTION AND PHASE RELATIONSHIPS OF THE FE-CR SYSTEM: PART
II . THE LIOUIO PHASE AND THE FCC PHASE
LIN JEN-CHWEN./CHUANG YING-YU./HSIEH KER-CHANG./CHANG A.V./
CATLPHAO. 1987, 11. (I). 73-81. __________________________________________________
234
THERMODYNAMIC PROPERTIES OF THE CR-FE SYSTEM
ANOERSSON J.-O./SUNOMAN BO/
CALPHAD. 1987. 11. (I). 83-92. ________________________________________~~~~~~~~~_
235
A NEW METHOD OF DESCRIBING LATTICE STABILITIES .
ANOERSSON J.-O./FERNANOEZ GUILLERMET A./GUSTAFSDN P./HILLERT M./JANSSON B./
JDNSSON B./SUNOMAN B./AGREN J./
CALPHAO. 1987. 11. (1). 93-98. ____________________------_-______________________
236
REGION-OF-OEMIXING CALCULATIONS ON HP 15 C CALCULATOR CALCULATION OF
SPINOOAL AND BINODAL .
VAN EKEREN P.J./OONK H.A.J./
CALPHAO. 1987. 11. (I). 99. _________________________~~~~~~~~~~~~~~~____~_____
237
CALCULATION OF EOUILIBRIA BETWEEN TWO MIXED STATES ON HP 15 C CALCULATOR
VAN EKEREN P.J./OONK H.A.d./
CALPHAD. 1987, 11. (1). 101. _________________________~~~~~~~~~_~~~_~___~______
236
CALCULATION OF TERNARY PHASE DIAGRAMS WITH BINARY DATA
BHANSALI A.S./MALLIK A.K./
CALPHAD. 1987. 11. (2). 105-116. ____________________~~~~~-~~-~~~-~~~~~~~~~~~~~~~~~
Page 2
396 C. BERNARD
239
CALCULATION OF LIOUID MISCIBILITY GAP IN CD-PB-ZN SYSTEM .
BHANSALI A.S./MALLIK A.K./ CALPHAD. 1987. 11. (2). 117-126.
____________________~_~__________~__~~~~~~~~~ _____
240 A NEW ASSESSMENT OF THE FE-N PHASE DIAGRAM .
FRISK K./
CALPHAO. 1987. 11. (2). 127-134. ______________________~_____________~~~~~~~~~~~~~~
241 A THERMODYNAMIC ASSESSMENT OF THE CU-SI SYSTEM . LUDECKE D./
CALPHAD. 1987. 11. (2). 135-142. ___________________~~~~~~__~~~~~~~~~~~~~~~--------
242 THE APPLICATION OF R FUNCTION TO PREDICTING TERNARY THERMODYNAMIC PROPERTiES
ZHOU GUO-ZHl / CALPHAG. 1987. 11. (2). 143-148.
____________________-~-~-_~~~~~~~~~~~~~~~~~~--~---
243 STABLE AND METASTABLE EDlJlLIBRlA IN THE FE-RICH CORNER OF THE FE-C-S] SYSTEM . CHUEH S.-C./SMITH J.F./
CALPHAD. 1987. 11. (2). 149-158. ________________________~~~~~~~~~~~~~~~--~~-------
244 THE OBSERVATION OF A NON-EOUILIBRIUM CLOSE PACKED HEXAGONAL PHASE IN ALLOYS
OF COPPER WITH GROUP III-VB ELEMENTS
SAUNDERS N./MIOOOWNIK A.P./
CALPHAD. 1987. 11. (2). 159-161. ____________~~______~~~~~_______~__~~~~~~~~~~~~~~~
245 ON THE NATURE OF BONDING IN TRANSITION METAL-PHOSPHORUS ALLOYS
CHANDRASEKARAN L./SAUNDERS N./MIODOWNIK A.P./
CALPHAO. 1987, 11. (2). 163-164. ____________________~~___~~~~~~~~~~~~~~~~~~ __--_--
246 A THERMODYNAMIC STUDY OF AN ASSOCIATED SOLUTION MODEL FOR LIQUID ALLOYS .
SCHMID R./CHANG A.V./ CALPHAD. 1987. 11. (2). 165-166.
_______________________~~______________~_~~~~~~~~~
247 OPTIMIZATION OF THERMOOVNAMIC DATA FOR SILICON BORIDES
DIRKX R.R./SPEAR K.E./
CALPHAO. 1987. 11. (2). 167-175. __________________________________________________
248 A THERMODYNAMIC ANALYSIS OF THE 81-S SYSTEM BY AN ASSOCIATED SOLUTION MODEL .
SHARYA R.C./LIN J.-C./CHANG A.V./ CALPHAD. 1987. 11. (2). 177-182.
________________________________________----------
249 AN ASSESSMENT OF THE FE-MN SYSTEM
WEIMING HUANG./ CALPHAD. 1987. 11. (2). 183-186.
_________________________________~~~~~~~~~~~~-~~--
250 A THERWOOVNAMIC ANALYSIS OF THE TI-H SYSTEM
KIVILAHTI J.K./MIETTINEN J.M./ CALPHAO. 1987. 11. (2). 187-199.
Page 3
SUBJECT INDEX 397
251
A THERMODYNAMIC EVALUATION OF THE C-FE-N1 SYSTEM
GABRIEL A./GUSTAFSON P./ANSARA I./
CALPHAO. 1967. 11. (3). 203-218.
252
APPLICATION OF TH HOCH-ARPSHOFEN MODEL TO TERNARY, OUATERNARY. AND LARGER SYSTEMS
HOCH M./
CALPHAD. 1987. 11. (3). 219-224. __________________________________________________
253
THE APPLICATION OF THE HOCH-ARPSHDFEN MDDEL TO LIOUID SYSTEMS WITH
COMPOUND-FORMING TENDENCIES AND A MISCIBILITY GAP
HOCH M./
CALPHAD. 1987. 11. (3). 225-23T6. __~_________________~__________________~~~~~~~~~~
254
APPLICATION OF THE HDCH-ARPSHDFEN MODEL TO THE THERMODYNAMICS OF THE
CU-NI-SN, CU-FE-NIB CU-MG-AL. AND CU-MG-ZN SYSTEMS
HOCH M./
CALPHAD. 1987, 11. (3). 237-246. ------.__________________----____-________________
255
APPLICABILITY DF VARIOUS FORMALISMS IN INTERPRETATION OF THERMODYNAMIC
PROPERTIES AND PHASE EOUILIBRIA IN ZN-BASED SYSTEMS
HAJRA J.P./SINHA A.K./
CALPHAD. 1987. 11. (3). 247-252. _________________________~~~~~~____~~_____________
256
FORMULATION OF THE A2/E2/D03 ATOMIC ORDERING ENERGY AND A THERMODYNAMIC
ANALYSIS OF THE FE-S1 SYSTEM .
LEE BYEDNG-JOO./LEE SEH KWANG./LEE DONG NYUNG./
CALPHAD. 1987. 11. (3). 253-270.
257
THERMODYNAMIC PROPERTIES OF CR-C
ANDERSSON J.-O./
CALPHAD. 1987. 11. (3). 271-276.
258
MEASUREMENT AND CALCULATION OF THE PHASE DIAGRAM OF THE LICL-BACLP-SRCLZ SYSTEM
ZHIYU OIAO./SANGSTER J./PELTON A.D./
CALPHAD. 1987. 11. (3). 277-286.
259
THE CALCULATION AND APPLICATION OF R FUNCTION IN TERNARY SYSTEMS .
CHOU K.-C./
CALPHAD. 1987. 11. (3). 287-292. ____________________~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
260
A NEW SOLUTION MODEL FOR PREOICTING TERNARY THERMODYNAMIC PROPERTIES .
CHOU K.-C./
CALPHAD. 1987. 11. (3). 293-300. _________________________~~~~~~~~~~~~~~~~~~~~~~~~~
261
SUMMARY DF THE PROCEEDINGS OF THE SIXTEENTH CALPHAD MEETING .
KAUFMAN L./
CALPHAD. 1987. 11. (4). 303-321. __~~________________~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
Page 4
398 C. BERNARD
262
A DATA BASE FOR ENTHALPIES OF FORMATION OF TRANSITION RARE-EARTH METAL ALLOYS
COLINET C./PASTUREL A./ CALPHAD. 1987. 11. (4). 323-334.
___________________________________~_~_~_~~~~~~~~-
263 TRENDS IN COHESIVE ENERGY OF TRANSITION RARE EARTH METAL ALLOYS
COLINET C./PASTUREL A./
CALPHAD. 1987. 11. (4). 335-348. __________________________________________--------
264 THERMODYNAMIC MODEL OF THE SDLIDIFICATIDN PROCESS OF ALLOYS . PART I
GENERAL TREATMENT FOR COMPLETE EOUILI6RIUH
KUNDRAT D.M./
CALPHAD. 1987. 11. (4). 349-354. ____________________________________________------
265
THERMODYNAMIC MODEL OF THE SDLIDiFICATION PROCESS OF ALLOYS . PART II
GENERAL TREATMENT OF SEGREGATION AS THE PRECIPITATION OF A SOLID PHASE IN A CLOSED SYSTEM
KUNDRAT D.M./
CALPHAD. 1987. 11. (41. 355-360. .____________________~--~~~~~.~~~~~~~~~~~~~~~~-~~~
266
ON THE LATTICE STABILITIES FOR CR, MO AND U
ANDERSSON J.-D./FERNANDEZ GUILLERMET A./GUSTAFSDN P./
CALPHAD. 1987. 11. (4). 361-364. .___________________------------------------------
267
A RECIPROCAL MODEL FOR LIOUID M-C SOLUTIONS
ANDERSSON J.O./
CALPHAD. 1987. 11. IO). 365-367. __________________________________________________
260 CALCULAiED PHASE DIAGRAMS OF CU-W. AG-W AND AU-W BINARY SYSTEMS . VIJAYAKUMAR H./SRIRAMAMURTHY A.M./NAGENDER NAIDU S.V./
CALPHAD. 1987. 11. (4). 369-374. _____________________~~______________~_~_~~~~~~~~~
269
A THERMODYNAMIC STUDY C’F THE CHROMIUM-CARBON SYSTEM .
BERKANE R./GACHDN J.C./CHARLES J./HERTZ J./ CALPHAD. 1987. 11. (4). 375-382.
____________________________________________-__-__
270 A NETWORK YODEL FOR THE THERMODYNAMICS OF MULTICOMPONENT SILICATE MELTS . I . BINARY MIXTURES MO-S102
WICHELS M.A.J./WESKER E./ CALPHAD. 1987. 11. (4). 383-393.
.___________________~~~~~________~__~_~~~~~~~~~~~~
Page 5
SUBJECT INDEX 399
[email protected] w.
261 L- GD. CONVEX PROGRAM, METASTAELE NB-
261 :N LIOUID ALLOYS, ZR- C. I-IF- C. TI- C.
261 .ITH TL. KCL- CACLZ. FE- C- E. FE- ZN-
261 CD- Nl. V- NI- FE, TI- AL- V. NI- V-
254 :ODEL. CU- NI- SN. CU- FE- NT. CU- MG-
244 .E PACKED HEXAGONAL PHASE, CU- ZN. CU-
261 .ILIBRIA. ANTIPHASE BOUNDARIES FOR FE-
261 MONTE-CARLO CALCULATIONS FOR FE- CD-
261 F ORDERING. ATOMIC RELAXATION FOR NI-
261 :U- ZN. NI- SI- B- CR- FE, AL- FE. NI-
261 .FE. AL- FE, NI- AL, W- NI- CU. MG- Y-
261 ., CALORIMETER DETERMINATIONS, AL- LA.
261 AL, W- NI- CU. MG- Y- AL, Y- AL- SI.
261 :METER DETERMINATIONS, AL- LA. AL- CE.
261 LLOVS. CA- PU- ZN. NI- Sl- B- CR- FE,
2Gl .TERMINATIDNS. AL- LA, AL- CE, AL- ER.
261 .v, LU- v. CALORIMETER DETERMINATIONS.
261 Y- AL. Y- AL- SI. AL- CU- X. AL- MG.
261 CU. MG- Y- AL, V- AL- ST. AL- CU- X,
261 FE, Nl- AL, W- NI- CU. MG- Y- AL. Y-
261 NI- V- CR. V- CO- NI. V- NI- FE. TI-
261 .ODEL. SI3N4 COMPOSITE MATERIAL, T102-
261 .2- SID2- Y203. HF02- SIO2- MGO. TID2-
261 .- MGO- SIO2. T102- AL203- 5102. TIO2-
261 .- AL203- HFD2. TI02- MGO- 5102. TID2-
231 . . . . . . . . . . . . . ..c......................
261 .TE CARLO HEXAGONAL BINARY ALLDYS WITH
261..)IN(l-YISB. SURFACE PHASE EOUILIBRIA.
261.. CA(l-X)MG(X)COB AN0 CO(l-X)MN(X)COB.
244.. , cu- SI. CU- GE, CU- SN. CU- GA. CU-
261... MG- LX. CU- FE- NI. SE- SE. SN- TE.
26l..ON DIFFRACTION MEASUREMENTS ON LIOUIO
248.................................61- S. 246.......................................
256.......................................
26l..C INTERACTIONS, KINETICS OF ORDERING.
26l..TL. KCL- CACLZ. FE- C- 6. FE- ZN- AL.
261..OSE PATTERNS, FE- CR MISCIBILITY GAP,
266..........................CU- W. AG- W.
26l..TY GAP. AU- SI BASED TERNARY SYSTEMS.
261..RY ALLOYS WITH TL. KCL- CACLZ. FE- C-
261.. SYSTEMS, AU- ZN. SN- SE. PD- TI. PD-
247....................................SI-
26l..UDOBINARY ALLOYS, CA- PU- ZN. NI- SI-
256..................................LICL-
253..DEL. MGO- 5102. CAO- SI02. SID- SI02.
261.. TID2- AL203- SIO2. TI02- AL203- MGO.
261..TERNS. FE- CR MISCIBILITY GAP. AU- SI
232................................CR- FE,
236..................MO- V- W. CO- PB- SN. 248.......................................
245
26T
261
. . . . . . . .._................... NATURE OF
.,................ RECIPROCAL MODEL FE-
.THIRD TRANSITION SERIES ELEMENTS. NB-
AG- W. AU- W............................... . . . . . . ...266
AL ALLOYS. NBAL. NE3AL. CAI I-X)MG(X)CDB AND COt I-X)..261
AL(X)GA(Y)IN(l-YISE. SURFACE PHASE E~JUILIERIA. ANTI..261
AL. AU- GA. MONTE CARLO FOR CONFIGURATIONAL ENTROPY..261
AL. CO- CR- V. MIEDEMA APPRDXIMATIDNS. ND- V. SM- V..261
AL. CU- MG- ZN, . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...254
AL. cu- SI. CU- GE. CU- SN. CU- GA. CU- AS. CU- SE,..244
AL. GRAIN BOUNDARY STRUCTURE DIFFUSION. LATTICE STA..261
AL. MONTE CARLO FOR ALLDYS INTERACTIONS AND CORRELA..261
AL. ORDERING EFFECT FOR STEEL. ISING MODEL, HEISEMB..261
AL. W- NT- CU. MG- t- AL, Y- AL- SI. AL- CU- X. AL-..261
AL. Y- AL- SI. AL- CU- X. AL- MG. AL- LI. MG- LI. C..261 AL- CE. AL- ER. AL- GD. CONVEX PROGRAM, METASTABLE ..261
AL- CU- X. AL- MG. AL- LI. MG- LI. CU- FE- NI. SB- ..261 AL- ER. AL- GD. CONVEX PROGRAM. METASTAELE NE- AL A..261
AL- FE. NI- AL, W- NI- CU. MG- V- AL. Y- AL- SI. AL..261
AL- GD. CONVEX PROGRAM, METASTABLE NB- AL ALLOYS. N..261
AL- LA, AL- CE. AL- ER. AL- GD. CONVEX PROGRAM, MET..261 AL- LI. MG- LT. CU- FE- NI. SE- SE. SN- TE. AS2SE3-..261 AL- MG. AL- LI. MG- LI. CU- FE- NI. SE- SE. SN- TE...261
AL- SI. AL- CU- X. AL- MG. AL- LI. MG- LI. CU- FE- ..261
AL- V. NI- V- AL, CO- CR- V. MIEOEMA APPROXIMATIONS..261
AL203, TI02- SIO2. TID2- Y203. HF02- i!R02- CAO. HF0..261
AL203- HFD2. TI02- MGD- SIO2. TI02- AL203- SIO2. TI..261
AL203- MGO. BAO- UO2- i!R02- MOOZ. MICROALLOYED STEE..261 AL203- SI02. TI02- AL203- MGO. BAD- UD2- ZR02- M002..261
ALGORITHM AND COMPUTER PROGRAM, . . . . . . . . . . . . . . . . . . ...231
ANISOTROPIC INTERACTIONS, KINETICS OF ORDERING, AT0..261
ANTIPHASE BOUNDARIES FOR FE- AL. GRAIN BOUNDARY STR. 261
AOUEOUS SDLUTIDNS. CACOB- MGCDS- H20. MONTE-CARLO C. 261
AS. CU- SE. CU- P....................................244
AS2SE3- SE2SE3- SE SYSTEM............................261
AS50GA50 AND CD50TE50. INTERFACIAL ENERGY, MARTENS1 261
ASSOCIATED SOLUTION MODEL, ........................
ASSOCIATED SOLUTION MODEL ..........................
ATOMIC ORDERING REACTIONS, FE- SI ..................
ATOMIC RELAXATION FOR NI- AL, ORDERING EFFECT FOR S
248 246
256
261
AU- GA. MDNTE CARLO FOR CONFIGURATIONAL ENTROPY, NE AU- SI BASED TERNARY SYSTEMS, AU- ZN. SN- SE. PO- T
AU- W ..............................................
AU- 2N. SN- SE. PD- TI. PD- B. GA- TL. BINARY ALLOY
6. FE- ZN- AL, AU- GA, MONTE CARLO FOR CONFIGURATIO
Ea. GA- TL. BINARY ALLDYS WITH TL. KCL- CACLP. FE- C 6 ..................................................
6- CR- FE, AL- FE, NI- AL, W- NI- CU. MG- Y- AL, Y-
261 261
268
261
261
261
247 261
BACLZ- SRCLZ. .....................................
BAD- SI02. FE- FE01.5. ............................
BAD- UO2- 2R02- M002, MICRCALLOYED STEELS: DUPLEX P
256
253
261
SASED TERNARY SYSTEMS. AU- 2N. SN- SE. PD- TI. PO- 261
BCC AND SIGMA PHASES, MAGNETIC CONTRIBUTION ........
EI- CD- SN. .......................................
El- s. ASSOCIATED SOLUTION MODEL. .................
BONDING, FE- P. MN- P. CR- P. RH- P. MO- P. PD- P.
232
230 240
245
C LIDUID SOLUTIONS ................................. 267
c. ................................................ 261
Page 6
400 C. BERNARD
261..- IN LIOUID ALLOYS, ZR- C. HF- C. TI-
261.. MODELING. FE- PD. FE- MN- f. FE- TI- 261................................ FE- CR- 261.. TATE PHASES MODELING, FE- PD. FE- MN- 261..FE- PD. FE- MN- C. FE- TI- C. FE- NB-
261 .PACIfY, CD- GA- IN L:OUID ALLOYS, ZR- 261.. CD- GA- IN LIOUID ALLOYS, ZR- C. HF- 257....................................CR-
269....................................CR-
26i..INAi?Y ALLOYS WITH TL. KCL- CACL2, FE-
251.......................................
243....................................FE-
C. ALIXIGALY tINI 1-Y 1%. SURFACE PHASE EOUILIBRIA. A. .261
C, FE- NE- C. FE- TI- N, FE- NE- N, LIOUIO LI- PE, ..261 C, FE- PD. METALLIC GLASSES CU- ZR. EKVI DATA GASE...26i
C. FE- TI- C. FE- NB- C. FE- TI- N. FE- NB- N. LIOU..261 C. FE- TI- N. FE- NB- N. LIOUID LI- PB. PB- NA. PB-..261 C. HF- C. TI- C. ALIX)GA(YbIN(l-YISE. SURFACE PHASE..261
C. TI- C. ALlXIGA(Y)IN(l-YISE. SURFACE PHASE EOUILI..261
~....................................................257
C....................................................26 9
C- 8. FE- ZN- AL. AU- GA. MONTE CARLO FOR CONFIGURA..26 1 C- FE- NI............................................25 1
c- SI. STABLE AND METASTABLE EOUILIBRIA..............24 3
261.. ETASTABLE NB- AL ALLOYS. NEAL. NBOAL.
26l..ANSFORMATION FOR PSEUDOBINARY ALLOYS.
261... GA- TL. BINARY ALLOYS WITH TL. KCL-
261.. D COtI-X)MN(XICOB, AOUEOUS SOLUTIONS,
261..IMATfONS, ND- Y, SNi- V. TM- 11. LU- V,
CAll-XIMG(XIC03 AN0 COII-XIHN(XJCC3. AOUEOIJS SOLUTI..261 CA- PU- ZN, NI- SI- B- CR- FE. AL- FE. NI- AL. W- N..261
CACL2. FE- C- 6. FE- ZN- AL, AU- GA. MONTE CARLD FO..261
CACO3- MGC03- H20. MONTE-CARLO CALCULATIONS FOR FE-..261
CALORIMETER OETER~INATIONS, AL- LA. AL- CE. AL- ER,..261
261... TIOZ- 5102. TIO2- Y203. HFO2- ZR02-
253..... ..HOCH-ARPSHOFEN MODEL. MGD- SI02.
261..N, LIGUIO LI- PB. PB- NA, PE- K. HEAT
CAO. HFO2- Y203- MGO. HFO2- SIO2- Y203. HF02- SIO2-..261 CAO- 5102. SIO- SIO2. E/LO- SI02, FE- FEOl.5, . . . . . ...253
261. .LI- PB. PB- NA. PB- K. HEAT CAPACITY. 23s......................_.......rdo- v- w.
239................ LIQUID MISCIBILITY GAP,
238............ ..MO- V- W. CO- PE- SN, BI-
261.. N MEASUREMENTS ON LIOUID ASSOGASO AND
261..LORIHETER DETERMINATIONS, AL- LA, AL-
CAPACITY, CD- GA- IN LIOUID ALLOYS. ZR- C. MF- C. T..261
CO- GA- IN LIOUID ALLOYS. ZR- C. HF- C, TI- C. AL(X..261
CD- PB- SN. BI- CD- SN, . . . . . . . . . . . . . . . . . . . . . . . . . . ...238 CD- PB- ZN, ..~_..._...,................,............ 239 CD- SN. ._......................*.................... 238
CD50TE50. INTERFACIAL ENERGY. MARTENSITIC TRANSFORM..261
244........................NON-EOUILIBRIUM
CE. AL- ER. AL- GD, CONVEX PROGRAM, METASTABLE NB- ..261
CLOSE PACKED HEXAGONAL PHASE. CU- ZN. CU- AL. CU- S-.244
26i..OYS. NEAL, NBSAL, CA{%-XlbiG(XbCO3 AND
26l..H20, MONTE-CARLO CALCULATIONS FOR FE-
261.. NI. V- NI- FE, TX- AL- V. NI- V- AL,
261.......................... FE- V- CR, V-
261.... FE- V- CR. V- CO- FE. NI- V- CR, V-
245.. P. MN- P. CR- P, RH- P. MO- P. PO- P.
263.......................................
CO(l-X~MN(X)CO3, AOUEOUS SOLUTIONS. CACO3- MGCO3- H..261 CO- AL. MONTE CARLO FOR ALLOYS INTERACTIONS AND CDR..261
CO- CR- V, NIEOEMA APPROXIMATIONS, ND- V, SN- V. TM..261
CO- FE, NI- V- CR, V- CO- NI, V- NI- FE. TX- AL- V...261
CO- NI. V- NI- FE. TI- AL- V. NI- V- AL, CO- CR- V...261
CO- P. NI- P, RU- P..................................245
COHESIVE ENERGY OF RARE-EARTH- TRANSITION METAL ALL..263
261.. MOOEL, COMPOUND- ENERGY MODEL. SI3N4
261.., FE- ZN- AL, AU- GA, MONTE CARLO FOR
261.. IONS. AL- LA. AL- CE. AL- ER. AL- GO.
26l..NTE CARLO FOR ALLOYS INTERACTIONS AND
COMPOSITE MATERIAL. T102- AL203. TI02- 5102, TIOZ- ..261
CONFIGURATIONAL ENTROPY, NEUTRON DIFFRACTION HEASUR..261
CONVEX PROGRAM, METASTABLE NB- AL ALLOYS, NEAL. NB3..261
CORRELATIONS, MONTE CARLO HEXAGONAL BINARY ALLOYS W..261
26l..S CALCULATIONS. PENROSE PATTERNS. FE- CR MISCIBILITY GAP. AU- SI BASED TERNARY SYSTEMS, A..261
266....................................... CR. MO AND W LATTICE STABILITIES. . . . . . . . . . . . . . . . . ...266
261......................._.........FE- V- CR, V- CO- FE. Nl- V- CR, V- CO- NI, V- NI- FE. TX-..261
261...... . . . ..FE- V- CR. V- CO- FE, NI- V- CR. V- CO- NI. V- NI- FE, TI- AL- V. NI- V- AL. CO-..261
26l....................................FE- CR- C. FE- PD. METALLIC GLASSES CU- ZR. EKVI DATA B..261
257....................................... CR- C................................................25~
269....................................... CR- c )......,........................................ 269 234....................................... CR- FE, . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...234
26l..BlNARY ALLOYS. CA- PU- ZN, NI- SI- B- CR- FE. AL- FE. NI- AL. W- NI- CU. MG- Y- AL, Y- AL..261
232....................................... CR- FE, BCC AND SlGMA PHASES. MAGNETIC CONTRIBUTION..232
233....................................... CR- FE, LIOUID AND FCC PHASES, METASTABLE EOUILIBRI..233
245.... . ..NATURE OF BONDING. FE- P, MN- P. CR- P, Rki- P. MO- P, PD- P, CO- P, NI- P, RU- P,.....246
261.. V- NI- FE. TX- AL- V. NI- V- AL. CO- CR- V. MIEDEMA APPROXIMATIONS, ND- V. SM- V. TM- V...261
261..SI- B- CR- FE, AL- FE, NI- AL, W- NI-
244.. CLOSE PACKED HEXAGONAL PHASE. CU- ZN.
244. .- AL, CU- SI. CU- GE. CU- SN. CU- GA,
254...... HOCH-ARPSHOFEN MODEL. CU- NI- SN,
261.. I, AL- CU- X. AL,- MC. AL- LX. MG- LI.
244. .- ZN. CU- AL. CU- Si, CU- GE. CU- SN.
244..AGONAL PHASE. CU- ZN. CU- AL. CU- SI.
CU. MG- Y- AL. V- AL- SI. AL- CU- X. AL- MG, AL- LI..261
CU- AL. CU- SI. CU- GE, CU- SN. CU- GA, ClJ- AS. CU-..244 CU- AS. CU- SB. CU- P................................244 CU- FE- NI, CiJ- MG- AL, CU- MG- ZN. . . . . . . . . . . . . . . ...254
CU- FE- NI, SB- SE. SN- TE. AS2SE3- SE2SE3- SE SVST..261 CU- GA. CU- AS. CU- SB. CU- P........................244
CU- GE. CU- SN, CU- GA, CU- AS. CU- SB, CU- P........244 254..SHOFEN MODEL, CU- NI- SN, CU- FE- NI. CU- MG- AL. C”- MU- LN, . . . . . . . . . . . . . . . . . . . . . . . . . . ...119
Page 7
SUBJECT INDEX 401
?54.. , CU- Nl- SN. CU- FE- NI. ClJ- MG- AL,
?54..................HOCH-ARPSHOFEN MODEL.
244..- GE, CU- SN. CU- GA. CU- AS. CU- SE,
244..- 51. CU- GE, CU- SN. CU- GA. CU- AS,
241....................................... 244..CKEO HEXAGONAL PHASE. CU- ZN. CU- AL.
244..HASE. CU- ZN. CU- AL. CU- Sl. CU- GE,
268.......................................
261.. W- Nl- CU. MG- Y- AL, Y- AL- SI. AL-
244..LIBRIUM CLOSE PACKED HEXAGONAL PHASE.
26l....FE- CR- C. FE- PO, METALLIC GLASSES
236. HP 15 COMPUTER PROGRAM FOR
261. FOR CONFIGURATIONAL ENTROPY, NEUTRON
261. FOR FE- AL, GRAIN BOUNDARY STRUCTURE
26l..UO2- ZRO?- M002. MICROALLOYED STEELS:
261..- C. FE- PD. METALLIC GLASSES CU- ZR.
261..R DETERMINATIONS. AL- LA, AL- CE. AL-
233.....................CR- FE. LIOUID AND
234. _.___.......___.._._ CR- 261. RY ALLOYS, CA- PU- ZN. NI- SI- B- CR-
232. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . CR-
233. .._.__.__........_......._........ CR-
261. S. CA- PU- 2N. NI- SI- B- CR- FE, AL-
261. . . . . . . . . . . . . . . . . . FE- V- CR, V- CO-
261. CO- FE. NI- V- CR. V- CO- NI. V- NI-
261. EOUILIBRIA. ANTIPHASE BOUNDARIES FOR
267. . . . . . . . . . . . . . . . . . . . . RECIPROCAL MODEL
261. L. BINARY ALLOYS WITH TL. KCL- CACLZ.
243. . .._._..........__....._.........._..
261. 03- H20. MONTE-CARLO CALCULATIONS FOR
261. IPLES CALCULATIONS, PENROSE PATTERNS, 261.......................................
253..102. CAO- S~Ia2. SIO- 5102. BAO- 5102. 249.......................................
261.. PRECIPITATE PHASES MOOELING. FE- PO. 240....................................... 261..OELING. FE- PO. FE- MN- C. FE- TI- C.
261..- C. FE- TI- C. FE- N6- C. FE- TI- N.
254..HOCH-ARPSHOFEN MODEL. CU- NI- SN. CU-
26l..L- CU- X. AL- MG. AL- LI. MG- LI. CU- 251.....................................c-
245.....................NATURE OF BONDING,
261..: DUPLEX PRECIPITATE PHASES MODELING. 261.............................FE- CR- C.
256.............ATOMIC ORDERING REACTIONS,
26l..E PHASES MODELING. FE- PO, FE- MN- C. 261.. PO. FE- MN- C. FE- TI- C, FE- NE- C.
261.......................................
26l..ALLOYS WITH TL. KCL- CACL2. FE- C- 8.
253.. CAO- SIO?. SIO- SiO2. BAO- SIO2. FE- FEOl.5. ..__._ _..._...._.......... 253
26l..ALLIC GLASSES CU- ZR. EKVI DATA BASE. FIRST PRINCIPLES CALCULATIONS, PENROSE PATTERNS. FE 261
255....................ZN- SN. ZN- IN, ZN-
244.. . CU- AL, CU- SI. CU- GE, CU- SN. CU- 26l..KCL- CACLZ. FE- C- B. FE- ZN- AL. AU-
26l..PE. PB- NA. PB- K. HEAT CAPACITY. CD-
261..STEMS. AU- ZN. SN- SE. PO- TI. PD- 6.
261.. PENROSE PATTERNS, FE- CR MISCIBILITY
235.....................LIOUID MISCIBILITY
26l..INATIONS. AL- LA, AL- CE. AL- ER, AL-
244..AL PHASE, CU- ZN. CU- AL, CU- SI. CU-
?61............FE- CR- C. FE- PO. METALLIC
GA, __.,._.,...__.__...._.._.......___.............
GA, CU- AS. CU- SB. cu- P..........................
GA. MONTE CARLO FOR CONFIGURATIONAL ENTROPY, NEUTRO
GA- IN LIOUID ALLOYS, ZR- C. HF- C. TI- C. AL(XIGA(
GA- TL. BINARY ALLOYS WITH TL. KCL- CACLP. FE- C- B
GAP, AU- 51 BASED TERNARY SYSTEMS, AU- 2N. SN- SE.
GAP. CD- PB- ZN. .._._...._.....__.____._..___.....
GO. CONVEX F’ROGRAM. METASTABLE NB- AL ALLOYS. NEAL.
255 244 261
261
261
GE. CU- SN. CU- GA, CU- AS. CU- SE. CU- P....
GLASSES CU- 2R. EKVI DATA BASE, FIRST PRINCIPLES CA
261
239
261
244
261
CU- MG- 2N. __...__.__........__... . . . . . . . . ...254
CU- Nl- SN. CU- FE- NI. CU- MS- AL. CU- MG- 2N. . . ...254
CU- P................................................244
cu- SE. CU- P........................................244
CU- 51. ._._..... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...241 CU- SI. CU- GE. CU- SN. CU- GA. CU- AS. CU- SB. CU-..244
CU- SN. CU- GA. CU- AS. CU- SE. CU- P...... . . . . . . ...244
CU- W. AG- W. AU- W..................................268
CU- X. AL- MG. AL- Ll. MG- LI. CU- FE- NI. SB- SE. ..261
CU- 2N. CU- AL. CU- SI. CU- GE, CU- SN. CU- GA. CU-..244
CU- 2R. EKVI DATA GASE. FIRST PRINCIPLES CALCULATIO..261
DEMIXING CALCULATIONS. . . . . . . . . . . . . . . . . . . . . . . . . . . . ...236
DIFFRACTION MEASUREMENTS ON LIOUID AS50GA50 AN0 CDS..261
DIFFUSION, LATTICE STAGILITIES FOR SECOND AND THIRD..261
DUPLEX PRECIPITATE PHASES MODELING. FE- PO, FE- MN-..261
EKVI DATA BASE. FIRST PRINCIPLES CALCULATIONS, PENR..261
ER.
FCC
FE.
FE. FE. FE.
FE.
FE. FE. FE-
FE- FE- FE-
FE- FE- FE- FE- FE-
FE- FE- FE- FE-
FE- FE-
FE-
FE- FE-
FE-
FE- FE-
FE- FE-
FE-
AL- GO, CONVEX PROGRAM. METASTABLE NB- AL ALLOY..261
PHASES. METASTABLE EOUILIERIA. . . . . . . . . . . . . . . . ...233
. . 234 AL- FE, NI- AL, W- NI- CU. MG- Y- AL. Y- AL- S1..261 KC AND SIGMA PHASES, MAGNETIC CONTRIBUTION,.....232
LIOUIO AND FCC PHASES, METASTAELE EOUILIBRIA. . ..233 NI- AL, W- NI- CU. MG- Y- AL, Y- AL- 51. AL- CU..261
NI- V- CR. V- CO- NI. V- NI- FE, TI- AL- V, NI-..261 TI- AL- V. NI- V- AL, CO- CR- V. MIEDEMA APPRDX..261
AL. GRAIN BOUNDARY STRUCTURE DIFFUSION, LATTICE..261 C LIOUID SOLUTIONS...............................267
c- B. FE- ZN- AL, AU- GA, MONTE CARLO FOR CONFI..261
c- SI. STABLE AND METASTABLE EOUILIBRIA..........243
CO- AL, MONTE CARLO FOR ALLOYS INTERACTIONS AND..261
CR MISCIBILITY GAP, AU- SI BASED TERNARY SYSTEM..261
CR- C. FE- PD. METALLIC GLASSES CU- 2R. EKVI DA..261 FE01.5. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...253 MN, . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...249
MN- C. FE- TI- C. FE- NB- C. FE- TI- N. FE- NE-..261 N................................................240
N6- C. FE- TI- N. FE- NB- N. LIOUIO LI- PB. PB-..261 NB- N. LIOUID LI- PB. PB- NA. PB- K. HEAT CAPAC..261
Nl . CU- MG- AL, CU- MG- 2N. :................... 254
NI . SE- SE. SN- TE. AS2SE3- SB2SE3- SE SYSTEM... 261
NI.............................................. 251
P. MN- P. CR- P. RH- P. MO- P. PO- P. CO- P. NI. 245
PO. FE- MN- C. FE- TI- C. FE- NB- C. FE- TI- N.. 261
PO. METALLIC GLASSES CU- 2R. EKVI DATA BASE, FI. 261 Sl............................................. 256
TI- C. FE- NB- C. FE- TI- N. FE- NE- N. LIOUIO 261
TI- N. FE- NB- N. LIOUIO LI- PE. PB- NA. PB- K. 261
V- CR, V- CO- FE, NI- V- CR, V- CO- NI. V- NI- 261
ZN- AL, AU- GA, MONTE CARLO FOR CONFIGURATIONAL 261
Page 8
402 C. BERNARD
261. .RIQ. ANTIPHASE BOUNDARIES FOR fE- AL. GRAIN BOUNOARY STRUCTURE DIFFUSION, LATTICE STAEILI..261
250....................................TI- H............................................,.......260
261. .CD3, AOJEOUS SOLUTIONS, CACO3- MGC03- H20. MONTE-CARLO CALCULATIONS FOR FE- CO- AL, MONTE..261
261.. NET- N. LIOUID LI- PE. PE- NA, PE- K, HEAT CAPACITY. CD- GA- IN LIOUXO ALLOyS. ZR- C. Hf-..261
261..OER1NG EFFECT FOR STEEL. IsING MODEL. HEISEMEERG MOOEL. COMPOUND- ENERGV MOOEL. SIJNJ COM..261
261..ACTIONS AND CORRELATIONS. MONTE CARLO HEXAGONAL BINARY ALLOYS WlTH ANISOTROPIC INTERACTI0..26:
244..... _.._ .NON-EOUILIBRIUM CLOSE PACKED HEXAGONAL PHASE. CU- ZN. CU- AL, CU- SI. CU- GE. CU..244
261..ITV. CD- GA- IN LIOUID ALLOYS, ZR- C. HF- C, TI- C. AL(XIGA(Y)IN(l-YISG, SURFACE PHASE EO..261
261..- Y203, HF02- SIO2- MGO. TI02- AL203- HFOZ. TIOZ- MGO- SIO2. TI02- AL203- 5102. TI02- AL2..261 261..0. HFO2- Y203- MGO. HF02- SIO2- y203, HFO2- S102- MGO. TI02- AL203- HF02. T102- HGO- SIO2..261 261..03, HFO2- ZRO2- CAO, HF02- Y203- MGO. HFO2- S102- Y203. HF02- SIOZ- MGO. T102- AL203- HFO..261 261..2- 5102. TI02- Y203. HF02- ZR02- CAO. HF02- Y203- MGO, HFO?- SI02- Y203. HFO?- 5X02- MG0...26l 261.. TI02- At203. T102- S102. T102- Y203. HFOZ- ZR02- CAO. HFO2- Y203- MGO, HFO2- S102- Y203,..26l
252 ....................................... HOCU-ARPSHOFEN MODEL. ............................. ..25 2 254 ....................................... HOCH-ARPSHOFEN MODEL. CU- NI- SN, CU- FE- NI. CU- M..25 4 253 ....................................... HOCH-ARPSHOFEN MODEL. MGO- 5102. CAO- SIO2. SIO- 51..25 3
?36....................................... HP 15 COMPUTER PROGRAM FOR OEMIXING CALCULATIONS, . ..236 237.......................,.. . . . . . . . . . . . . HP 15 COMPUTER PROGRAM FOR EOUILIBRIA CALCULATIONS..:237
261.. PB- NA. PB- K. HEAT CAPACITY, CD- GA- IN LIOUIO ALLOYS, ZR- C. HF- C. TI- C. AL(X)GA( 255............................ZN- SN. ZN- IN. ZN- GA, . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...255
261.. ENTS ON LIOUID AS50GA50 AND CD50TE50. INTERFACIAL ENERGY, MARTENSITIC TRANSFORMATION FOR ..261
261 ..OR NI- AL. ORDERING EFFECT FOR STEEL, ISING MODEL. HEISEMBERG MODEL. COMPOUND- ENERGY MOD..261
261.. FE- NB- N, LIPUID LI- PB. PB- NA, Pfl- K. HEAT CAPACITY. CD- GA- IN LIOUIO ALLOYS. ZR- C. ..261
261..PD- 5, GA- TL, BINARY ALLOYS WITH TL, KCL- CACLZ. FE- C- 6, FE- ZN- AL, AU- GA. MONTE CAR..261
26f..ALLOVS WITH ANISOTROPIC INTERACTIONS, KINETICS OF ORDERING, ATOMIC RELAXATION FOR NI- AL,..261
26l..U- V. CALORIMETER O~TERMINATIONS. AL- LA. AL- CE. AL- ER. AL- GO, CONVEX PROGRAM, METASTA..261
235....................................... LATTICE STABILITIES DESCRIPTION......................235
261.., GRA:N BOUNDARY STRUCTURE DIFFUSION. LATTICE STABILITIES FOR SECOND AND THIRD TRANSITION..261
266........................... CR. MO AND W LATTICE STABILITIES. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...266
261.. L- SI. A,_- CU- X. AL- MG. AL- LI. MG- LI. CU- FE- NI. SB- SE, SN- TE, AS2SE3- SB2SE3- SE ..261
261. .AL. Y- AL- SI. AL- CU- X. AL- MG. AL- LI. MG- LI. CU- FE- NI. SB- SE, SN- TE. AS2SE3- SB2..261
261..- NB- C. FE- TI- N. FE- NB- N. LIOUID LI- PB. PB- NA, PB- K. HEAT CAPACITY, CD- GA- IN LI..261
256...................,................... LICL- BACL2- SRCLZ. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...258
261.. APPROXIMATIONS. ND- V. SM- V. TM- V. LU- V. CALORIMETER DETERMINATIONS. AL- LA. AL- CE, ..2E1
232......... .CR- FE, ECC AND SIGMA PHASES, MAGNETIC CONTRIBUTION.......................... . . . ...232
261..&50 AND CO50TE50. INTERFACIAL ENERGY, NIARTENSITIC TRANSFORUATION FOR PSEUDOBINARY ALLOYS...261
233.........CR- FE. LIOUID AN0 FCC PHASES, METASTABLE EOUILISRIA. . . . . . . . . . . . . . . . . . . . . . . . . . . . ...233
243..................FE- C- 51. STABLE AND METASTABLE EOUILIBRIA,...............................243
26l..- CE. AL- ER. AL- GO, CONVEX PROGRAM. METASTABLE NB- AL ALLOYS, NBAL. NBOAL. CAii-X)MGfXl..261
261.. MG- Y- AL. Y- AL- 51. AL- CU- X. AL- MG. AL- LI. MG- LI, CU- FE- NI. SB- SE. SN- TE. AS2..261
254..EN MODEL. CU- NI- SN. CU- FE- NI. CU- MG- AL, CU- MG- ZN. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...254
26i..Y- AL- SI. AL- CU- X. AL- MG. AL- LI. MG- LI. CU- FE- NI. S6- SE. SN- TE. AS2SE3- SB2SE3-..261
261..B- CR- FE, AL- FE, NI- AL. W- NI- CU. MG- Y- AL. Y- AL- SI. AL- CU- X. AL- MC. AL- LI. FAG..261
254..- NI- SN. CU- FE- NI. CU- NG- AL. CU- MG- ZN, . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...254
261. .X)MN(n)C03. AOUEOUS SOLUTIONS. CACD3- MGCD3- H20. MONTE-CARLO CALCULATIONS FOR FE- CO- AL..261
Zb!. . SIOZ. TI02- AL203- SIO?. TI02- AL203- MGO. BAO- UO2- ZR02- MOD2. MlCROALLOYED STEELS: DUP..261
261..2- Y203. HFO2- ZR02- CAO. HF02- Y203- MGO , HF02- S10’2- Y203, HFOZ- SIO2- MGO. TI02- AL203..261
261. 3- MGO. HF02- 5X02- Y203. HFOZ- SIOZ- MGO . TI02- AL203- HFO?. T102- MGO- 5102. TI02- AL20..261
?53..................HOCH-ARPSHOFEN MODEC. MGO- 5102. CAO- 5102. SIO- SIO2. BAO- SIO2. FE- FEO..253
?6l..- sIO2- MGD. TIO2- AL203- HFO2. TI02- MGO- 5102. TID2- AL203- 5102, TI02- AL203- MGO. BAO..261
Page 9
SUBJECT INDEX 403
261..02- AL203- MGO. EAO- UO2- ZROZ- MOO2.
261.. FE, TI- AL- V. NI- V- Al. CO- CR- V,
26l..ALCULATIONS. PENROSE PATTERNS, FE- CR
239.................................LIOUIO
249....................................FE-
26l..CIPITATE PHASES MQOECING. FE- PO. FE-
245............. .NATURE OF BONOING. FE- P.
266.....................,..............CR. MO AN0 W LATTICE STAEILITIES, . . . . . . . . . . . . . . . . . . . . ...266 245.. EDNDING. FE- P, MN- P. CR- P. RH- P. MO- P. PO- P. CO- P. NI- P, RU- P,...................245 238....................................... MO- V- W. CD- PB- SN. EI- CD- SN, . . . . . . . . . . . . . . . . ...233
26?.............................RECIPRQCA L
248 ........... ..BI - 5. ASSOCIATED SOLUTION 252.........................HOCi+ARPSHOFE N
260.......................TERNARY SOLUTION 264................. SOLIDIFICATION PROCESS 265................ .SO!_IDIFICATION PROCESS 26l..CT FOR STEEL, ISING MODEL. HEISEMBERG
254.........................HOCn-ARPSnOFEN 26t.. AL. ORDERING EFFECT FOR STEEL. ISING 253.........................HOCH-ARPSHOFEN
26i..L, HEISEMBERG MODEL, COMPOUND- ENERGY
246....................ASSCkCIATEO SOLUTION ??O........‘ .MlJLTICOMPONENT SILICATE MELTS
26l..YEO STEELS: DUPLEX PRECIPITATE PHASES
MODEL FE- C LIOUID SOLUTIONS.........................267
MODEL,
MODEL,
MODEL
MODEL;
MODEL, MODEL.
MODEL,
MODEL.
MODEL. MODEL,
. . . . . . . . . .._..._......._......................248
. . . . . . . . . . . . . . . . . . . . . .._......................252
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...260
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...264
265 CoMPoutuo~‘;N;bc;.Moo;;l.sijN;‘CoMPas;;;.M;;E::26t
CU- NI- SN, CU- FE- NI, CU- MG- AL. CU- MG- ..254
HEISEMBERG MODEL. COMPOUND- ENERGY MODEL, S1..261
MGO- 5102. CAO- SI02. SIO- 5102. EAO- SIO2, ..253 S13N4 COMPOSITE MATERIAL. Ti02- AL203. TI02-..261
MODEL ...............................................
MODEL ............................................... 246
270
MODELING, FE- PD. FE- MN- C, FE- TI- C, FE- NB- C. 261
26l..TE-CARLO CALCULATIONS FOR FE- CO- AL, MONTE CARLO FOR ALLOYS INTERACTIONS AND CORRELATION. 261 261.. CACi2, FE- C- 6, FE- ZN- AL. AU- GA., MONTE CARLO FOR CONFIGURATIONAL ENTROPY. NEUTRON 51. 261 261..ALLOYS INTERACTIONS AND CORRELATIONS. MONTE CARLO HEXAGONAL BINARY ALLOYS WITH ANISQTROPI. 261
261..AQUEOUS SOLUTIONS, CACO’J- MGCOJ- ii20, MONTE-CARLO CALCULATIONS FOR FE- CO- AL, MONTE CARL. 261
261..02. TI02- AL203- MGCI. BAO- UO2- ZR02- 261
261.. UN- C. FE- TI- C. FE- NE- C. FE- TI- 261.. TI- c, FE- NB- C. FE- TX- N. FE- NB- 240................... . . . . . . . . . . . . . . ..FE-
261.. TI- N. FE- NE%- N. LIQUID LI- PE. PB-
245.......................................
M002. MICROALLOYED STEELS: DUPLEX PRECIPITATE PHASE.
N, FE- NB- N. LXOUID LI- PB. PE- NA, PE- K. HEAT CA. N, LIQUID LI- PB, PB- NA, Pe- K. HEAT CAPACITY, CD-.
N...................................................
261 261
240
NA. PB- K, HEAT CAPACITY. CD- GA- IN LIOUIO ALLOYS,..261
NATURE OF BONOING, FE- P. MN- P. CR- P. RH- P. MO- ..245
261. .R. AL- GO, CONVEX PROGRAM, METASTABLE NE- AL ALLOYS. NEAL. NBBAL. CA(l-XIMG(XIC03 AND CO(..261 26l..AND THIRD TRANSITION SERIES ELEMENTS, NE- C. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...261 26l..NG. FE- PD. FE- MN- C, FE- TI- C. FE- NB- C. FE- TI- N, FE- NB- N. LIQUID LI- PfI. PB- NA...261 261.. FE- TX- C, fE- NB- C. FE- TI- N, FE- NB- N, LIOUIO LI- PB. PB- NA. PB- K. HEAT CAPACITY...261
26l..GRAM. METASTABLE NB- AL ALLOYS, NBAL,
26l..EX PROGRAM. METASTABLE NB- AL ALLOYS.
N63AL. CA(l-X)MG(X)COB AND CO(l-XIMN(XICO3, AQUEOUS..261
NBAL, NB3AL, ~A(t-X)MG(XjCO3 AND CO(l-X)MN(X)C~3, A..261
26l..L. CO- CR- V. MIEDEMA APPROXIMATIONS, NO- V. SM- V. TM- V. LU- v. CALORIMETER DETERMINATI..261
2Gl..TE CARLO FOR CONFIGURATIONAL ENTROPY. NEUTRON DIFFRACTION MEASUREMENTS ON LIQUID AS50GA50..261
25J..-ARPSXOFEN MODEL. CU- NI- SN. Cu- FE- NI . CU- MG- AL. CU- Mt- ZN, . . . . . . . . . . . . . . . . . . . . . . ...254 26l..U- X, AL- MG. AL- LI, MG- LI. CU- FE- NI . SB- SE. SN- TE. AS2SE3- SB2SE3- SE SYSTEM........261
261..- V- CR. V- CO- FE, NI- V- CR. V- CO- NI. V- NX- FE, TI- AL- V. NI- V- AL, CO- CR- V. MIE..261
251.................................C- FE- Nl,..................................................251
26l..CS OF ORDERING, ATOMIC RELAXATION FOG NI- AL, ORDERING EFFECT FOR STEEL, ISING MODEL. HEI..
261. .A- PU- ZN, NI- SI- E- CR- FE, AL- FE, NI- AL, W- NI- CU. MG- V- AL, Y- AL- SI. AL- CU- X,..261
2Gl..NI- SI- 6- CR- FE, AL- FE, NI- AL. W- NI- CU. MG- Y- AL. V- AL- SI. AL- CU- X. AL- MG. AL..261
261... V- CO- FE. NI- V- CR, V- CO- NI. V- NI- FE. TI- AL- V, NI- V- AL. CO- CR- V. MIEDEHA AP..26t
245..P. CR- P. RH- P. MO- P, PD- P, CO- P. NI- P. RU- P.........................................245
261.. FOR PSEUDOEINhR~ ALLOYS. CA- PU- ZN. NI- SI- 6- CR- FE, AL- FE. NI- AL. W- NX- CU. MG- Y..261
254............. .HOCH-ARPSHOFEN MODEL. CU- NI- SN. CU- FE- NI. CU- MG- AL. CU- MG- ZN. . . . . . . ...254
2G1. CR. V- CO- NI. V- NI- FE. TI- AL- V. NI- V- AL, CO: CR- v. MIEDEMA APPROXIMATIONS. NO- v..261
26t..................FE- V- CR, V- CO- FE. NI- V- CR, V- CO- NI. V- NI- FE, TX- AL- V, NI- V- ..261
244....................................... NON-EOUILIBRIUM CLOSE PACKED HEXAGONAL PHASE. CU- 2 ,244
261. .DERING. ATOMIC RELAXATION FOR Nl- AL. ORDERING EFFECT FOR STEEL, 1SINC MODEL. HEISEMBERG ..261
MICROALLOYED STEELS DUPLEX PRECIPITATE PHASES MODE..261
MIEDEMA APPROXIMATIONS. ND- V. SM- V. TM- V. LU- V...26i
MISCIGILITY GAP. AU- SI EASED TERNARY SYSTEMS. AU- ..2rjt
MISCIBILITY CAP. CD- PB- ZN. . . . . . . . . . . . . . . . . . . . . . ...239
MN. MN_ c~.;;~‘;i~.t~‘..“..‘“.““.‘..““..’...,...’~~ 249 FE- NE- C, FE- TI- N. FE- NB- N. 261
MN- P. CR- P, RH- P. MO- P. PD- P. CO- P. NI- P, RU..245
Page 10
404 C. EER~ARD
?56........................ . . . . . . ..ATOMIC ORDERING REACTIONS, FE- Sl.......................... 256 261..ANISOTROPIC INTERACTIONS. KINETICS OF CRDERiNG. ATOMIC RELAXATION FOR NI- AL, DROERING Ef. 261
245 .E- P. MN- P. CR- P. RH- P. MO- P. PO-
245 .,. . . ..NAlURE OF BONDING. i-E- P. MN-
245 . . . . . . . . . . . . . . ..NATURE OF BONDING. FE- 145 OF BONDING. FE- P, MN- P, CR- P. RH-
245 .N- P. CR- P. PH- P. MO- P. PO- P. CO-
245 .OING. FE- P. MN- P. CR- F. RH- P. MD-
245 ..NATURE OF BONDING. FE- P. MN- P. CR-
245 .R- P. RH- P. MO. P. PD- P. CO- P. NI-
244 . CU- SN. CLJ- GA, CU- AS, CU- SC. CU-
245 .H- P. MO- P, PO- P. CO- P. NI- P. RU-
244..................NON-EQUILIBRIUM CLOSE
P. CO- P. NI- F. RU- P.....
P. CR- P. RH- F. MO- P. PO- P;.CO:‘P;.N;:.P:.R;:‘P;
P. MN- P. CR- P. KH- P. MO- P, PO- P, CO- P. NI- P, P, MO- P. PD- P. co- F, NI- P. RU- P............... P. NI- P, RU- P..... . . . P. PD- P. CO- P. NI- P. RU- i::::::::::::::::::::::
P, RH- P. MO- P, PD- P. co- P. NI- P. RU- P........ P. RU- P....... _... . . . . . . . . . . . . . . . . . P................... . . . . . . . . . . . . . . . . . . . . P................... . . . . . . . . ..__..._.........
PACKED HEXAGONAL PHASE, CU- ZN, CU- AL. CU- 51. CU-
PATTERNS, FE- CR MISCIBILITY GAP. AU- SI BASED TERN.
PE. PB- NA. PB- K. HEAT CAPACITY. CD- GA- IN LIOUIO. PB- K. HEAT CAPACITY. CD- GA- IN LIOUID ALLOYS. ZR-. PB- NA. PB- K. HEAT CAPACITY. CO- GA- IN LIQUIO ALL. PE- SN. BI- CD- SN. ._____...,._...___.._........_..
PB- ZN. ..,.........._.......................,......
245
245 145
245 245
245
24S 245
244
245
244
261..IRST PRINCIPLES CALCULATIONS. PENROSE 261
261..- C. FE- TI- N. FE- NE- N. LIOUID LI-
261.. N. FE- NB- N. LIOUID LI- PB. PB- NA. 261.. FE- TI- N. FE- NB- N. LIQUID LI- PE.
238..........................MD- V- W. CO-
239............ LIOUID MISCIEIlITY GAP, CD-
261..PLEX PRECIPITATE PHASES MOCELING. FE-
261.........................FE- CR- C. FE-
261..NARY SYSTEMS. AU- ZN. SN- SE. PD- TI.
245..G. FE- P. MN- P. CR- P. RH- P. MO- P.
261. ASED TERNARY SYSTEMS, AU- ZN. SN- SE,
261
261 261 238
239
261.. BASE. FIRST PRINCIPLES CALCULATIONS,
261..02- MOOP, MICROALLOYED STEELS: DUPLEX
242..IDN. TERNARY THERMOOYNAMIC PROPERTIES
PO. FE- MN- C. FE- TI- C. FE- NE- C, FE- TI- N. FE-.
PO. METALLIC GLASSES CU- ZR, EKVI DATA BASE, FIRST . PO- E. GA- TL. BINARY ALLOYS WITH TL, KCL- CACLP, F.
PO- P. CD- P. NI- P. RU- P..........................
PD- TI. PD- B, GA- TL. BINARY ALLOYS WITH TL. KCL-
PENROSE PATTERNS, FE- CR MISCIBILITY GAP. AU- SI EA.
PRECIPITATE PHASES MODELING. fE- PO. FE- MN- C. FE-.
261
26%
261 245
261
2Gl
261
PREDICTIONS, _............................~......... 242
26t..GLASSES CU- ZR. EKVI DATA BASE. FIRST PRINCIPLES CALCULATIONS. PENROSE PATTERNS, FE- CR M. 261
264.........................SOLIDIFICATION PROCESS MODEL, ..__..._.....................,...... 264
265.........................SOLIDIFICATION PROCESS MODEL, . . . . . . . . ..t......................... 265
236.........................tiP 15 COMPUTER PROGRAM FOR OEMIXING CALCULATIONS. . . . . . . . . . . . . . . . . 236
237.........................HP 15 COMPUTER PROGRAM FOR EQUILIBRIA CALCULATIONS, . . . . . . . . . . . . . . 237
231.................ALGORITHM AND COMPUTER PROGRAM. _....,._.._...............r........,t...... 231
261..L- LA. AL- CE. AL- ER, AL- GO. CONVEX PROGRAM. METASTAPBLE NB- AL ALLOYS. NBAL. NBIAL. CA{. 261
261..NERGY. MARTENSITIC TRANSFORMATION FOR
261..DRMATION FOR PSEUDOBINARY ALLOYS. CA-
PSEUDOBINARY ALLOYS. CA- PU- ZN, NI- SI- E- CR- FE,.
259.......................................
242.......................................
PU- ZN. NI- SI- B- CR- FE. AL- FE. NI- AL. w- NI- C.
R FUNCTION FOR TERNARY SYSTEMS. . . . . . . . . . . . . . . . . . . . .
R FUNCTION. TERNARY THERMODYNAMIC PROPERTIES PREDIC.
263.....................COHESIVE ENERGY OF RARE-EARTH- TRANSITION METAL ALLOYS, . . . . . . . . . . . . . .
262.............. .COMPOUNDS AND ALLOYS FOR RARE-EARTH- TRANSITION METALS SYSTEMS : ENTHALPIES
267.......,............................. RECIPROCAL MODEL FE- C LIQUIO SOLUTIONS............
26t
261
259
242
263
262
267
261
245
246
248
244 261
26l..ACTIONS. KINETICS OF ORDERING. ATOMIC
245..TURE OF BONDING, FE- P. MN- P. CR- P.
245..P. Rli- P. MO- P. PD- P, CO- P. NI- P.
248....................................BI-
244 . . CU- GE, CU- SN. CU- GA, CU- AS, CU-
261 ., AL- MG, AL- LI. MG- LI. CU- FE- NI.
261 _. CU- FE- NI. SB- SE. SN- TE. ASZSE3-
261 .- NI. SB- SE, SN- TE, AS2SE3- SBZSE3-
262 .SI BASED TERNARY SYSTEMS. AU- ZN. SN- 261 _- MG. AL- LI, MG- LI. CU- FE- NI, SE-
SE. cu- P..........................................
S6- SE. SN- TE. ASZSE3- SBZSE3- SE SYSTEM,.........
S&2SE3- SE SYSTEM................................... 261
SE SYSTEM,.....................,................... 261
SE, PO- TI. PD- E, GA- TL. BINARY ALLOVS WITH TL. K 261
SE. SN- TE. AS2SE3- SEZ?SE3- SE SYSTEM,............. 261
261..RE DIFFUSION. LATTICE STABILITIES FOR SECOND AND THIRD TRANSITION SERIES ELEMENTS. NB- C.. 261
RELAXATION FOR NI- AL, ORDERING EFFECT FOR STEEL, I.
RH- P. MO- P, PO- P. CD- P. NI- P. RU- P............
RU- P...............................................
5. ASSOCIATED SOLUTIDN MODEL, . . . . . . . . . . . . . ..r......
Page 11
SUBJECT INDEX 405
26l..ITIES FOR SECOND AND ThJRD TRANSITION SERIES ELEMENTS, NE- C. .
SI BASED TERNARY SYSTEMS. AU- ZN. SN- SE. PD- TI. P SI. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
SI. AL- CU- X. AL- MG. AL- LI. MG- LI. CU- FE- NI.
SI. CU- GE. CU- SN, CU- GA. CU- AS. CU- SE. CU- P..
51. SlABLE ANC METASTAELE EOUILIERIA............... SI.................................................
Sl- E...... ._...
SI- B- CR- FE. AL- FE. NI- AL, W- NI- CU. MG- Y- AL
261
26l..PATTERNS. FE- CR MISCIGILITY GAP. AU-
241.................. . . . . . . . . . . . . . . . ..cu- 261.. Nl- AL. W- NI- CU. MG- l- AL. Y- AL- 244.. HEXAGONAL PHASE. CU- ZN. CU- AL. CU- ?43...... . . . . . . . . . . . . . . . . . . . . . . . . ..FE- C-
256......... ATOMIC ORDERING REACTIONS, FE- 247.......................................
261.. PSEUOOEINARY ALLOYS, CA- PU- ZN. NI-
2Cl
24 1 361 244
243
256 247
261
26l..EMBERG MODEL, COMPOUND- ENERGY MODEL,
352........................CR- FE. BCC AND
SI3N4 COMPOSITE MATERIAL. TIO2- AL203. TIOZ- SIO2. 261
SIGMA PHASES, MAGNETIC CONTRIBUTION................’ 232
270.........................MULTICOMPONENT SILICATE MELTS MODEL............................... 270
253 RPSHOFEN MODEL, MGO- SIO2. CAO- SIO?.
253 FEN MODEL, MGO- SI02. CAO- SIO2. SIO-
253 HOCH-ARPSHOFEN MODEL. MGO-
253 MGl+:‘S;&‘:‘CAO- SIO2. SIO- SIO2. 6AO-
253 HOCH-ARPSHOFEN MODEL, MGO- SIO2. CAO-
261 - HF02. T102- MGO- SIO2. TI02- AL203-
261 2- MGO. TI02- AL203- HF02. TI02- MGO-
261 OMPOSITE MATERIAL, TI02- AL203. TIU2-
261 2- Y203- MGO. HF02- SIO2- Y203. HFO2-
261 02- ZR02- CAO. HF02- Y203- MGO. HF02-
261 CR- V. MIEDEMA APPROXIMATIONS. ND- V.
236 ._._____ MO- V- W. CD- PB- SN. Bi- CD-
236 . . . . . . . . . . . . . . . . . . ..MO- V- W. CD- PB-
254 HOCH-ARPSHOFEN MODEL, CU- NI- 244 ;‘ii:‘ii. CU- AL, CU- SI. CU- GE, CU- 355 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ..ZN-
261 AU- SI BASED TERNARY SYSTEMS, AU- EN.
261 , AL- LI. MG- LI. CU- FE- NI. SB- SE,
264.......................................
265.......................................
SIO- SIO2. BAO- SIO-7. FE- FE01.5. ..___.__.._ 253
5102. EAO- SIO2. FE- FE01.5. .._.._._._._____.__.._ SIO2. CAO- 5102. SIO- 5102. BAO- SIOZ. FE- FE01.5.
SIO2. FE- FE01.5. . .._....._.__._. SIO2, SIO- SIO2, BAO- 5102. FE- FE01.5, ________.._
SI02. TI02- AL203- MGO. BAO- UO2- ZR02- MD02. MICRO 5102. TI02- AL203- 5102. T102- AL203- MGO. BAO- U02 SIOZ. T102- Y203, HF02- ZR02- CAO. HFO2- V203- MGO. SIO2- MGO. TI02- AL203- HFO2. TI02- MGO- SIO2. TI02
s102- v203. HFC)Z- SIO2- MGO. TID2- AL203- HF02. TIO
SM- V. TM- V. LU- V. CALORIMETER DETERMINATIONS. AL
SN. ___.______._._.___.__.______..._____.___._,._,,
SN. BI- CD- SN. .._............._..__._.
SN. CU- FE- NI. CU- MG- AL, CU- MG- ZN. .
SN. CU- GA. CU- AS. CU- SB. CU- P.................. SN. ZN- IN. ZN- GA. . . . ..__..._. SN- SE, PD- TI. PD- B. GA- TL. BINARY ALLOYS WITH T SN- TE. AS2SE3- SE2SE3- SE SYSTEM,.................
SOLIDIFICATION PROCESS MODEL. _...__.__..___._.._,.
SOLIOIFICATION PROCESS MODEL, .
253 253
253 253
261 261 261 261 261
261
236
238
254 244
255 261 261
264 265
258...........................LICL- BACL?- SRCL2. .._........._........._.____.._____.._...... 256
243.............................FE- C- SI. STABLE AND METASTABLE EOUILIBRIA................... 243
26l..ATION FOR NI- AL, ORDERING EFFECT FOR
261..0. BAD- UO2- ZR02- M002. MICROALLOYED
STEEL. ISING MODEL, HEISEMBERG MODEL, COMPOUND- ENE
STEELS: DUPLEX PRECIPITATE PHASES MODELING. FE- PD.
261
261
26l..BOUNDARIES FOR FE- AL, GRAIN BOUNDARY STRUCTURE DIFFUSION. LATTICE STABILITIES FOR SECOND 261
261..C. HF- C. TI- C. AL(XJGA(YJIN(l-YJSB.
261..- LI. MG- LI. CU- FE- NI. SB- SE, SN-
SURFACE PHASE EOUILIBRIA. ANTIPHASE BOUNDARIES FOR
TE. AS2SE3- SE2SE3- SE SYSTEM......................
261
261
261. .N. LATTICE STABILITIES FOR SECOND AND
261.. TERNARY SYSTEMS. AU- ZN. SN- SE. PD- 261.. FE, NI- V- CR. V- CO- NI. V- NI- FE.
261..- GA- IN LIOUID ALLOYS, ZR- C. HF- C. 26l..ASES MODELING, FE- PD. FE- MN- C. FE-
250.......................................
261.. FE- MN- C. FE- TI- C. FE- NE- C. FE-
THIRD TRANSITION SERIES ELEMENTS. NB- C. .r._...... 261
TI . PD- E. GA- TL. BINARY ALLOYS WITH TL. KCL- CACL 261 TI- AL- V. NI- V- AL, CO- CR- V. MIEDEMA APPROXIMAT 261 TI- C. AL(XJGA(YJIN(l-YJSB. SURFACE PHASE EOUILIBRI 261 TI- C. FE- NE- C. FE- TI- N. FE- NB- N. LIOUID LI- 261 TI- H.............................................. 250 TI- N. FE- NB- N. LIOUID LI- PB. PB- NA. PB- K. HEA 261
261 .ERGV MODEL, SI3N4 COMPOSITE MATERIAL.
261 .O. HFOZ- SIO2- Y203. HFOZ- SIO2- MGO.
261 . . TIO;Z- MGO- 5102. TI02- AL203- SI02.
261 . . TIOZ- AL203- HFOZ. TI02- MGO- SIO2.
261 . . HFO2- S102- MGO. TI02- AL203- HF02.
261 . 13N4 COMPDSITE MATERIAL. TI02- A~203. 261 .TE MATERIAL, TI02- AL203. T102- SIO2.
TIO2- AL203. TI02- SIO2. T102- Y203. HF02- ZROZ- CA
TIOZ- AL203- HF02. TI02- MGO- SIO2. TI02- AL203- SI TIO2- AL203- MGO. BAD- UO2- ZR02- MOO2. MICROALLOYE
TI02- AL203- SIO2. TI02- AL203- MGO. BAO- UO2- ZRD2
TI02- MGO- 5102. TI02- AL203- 5102. TIOZ- AL203- MG
T102- SIO2. T102- Y203. HF02- ZR02- CAO. HF02- Y203
TI02- Y203. HF02- i!RJ2- CAO. HFOZ- Y203- MGO. HFO?-
261 261
261
261 261
261
261
261 .S. AU- ZN. SN- SE. PD- TI. PD- B. GA-
261 .TI. PD- E. GA- TL. BINARY ALLOYS WITH
261..MIEDEMA APPROXIMATIONS. ND- V. SM- V.
TL. EINARY ALLOYS WITH TL. KCL- CACL2. FE- C- B. FE
TL. KCL- CACL?. FE- C- B. FE- ZN- AL. AU- GA. MONTE
TM- V. LU- V. CALORIMETER DETERMINATIONS. AL- LA. A
261
261
26 1
Page 12
406 C. BERNARD
261
263 262 261
261
261 261 261 261 261 261 261 261 261 261
TE50. INTERFACIAL ENERGY, MARTENSITIC TRANSFORMATION FOR PSEUDOEINARY ALLOYS. CA- PU- ZN...261
.COHESIVC ENERGY OF RARE-EARTH- :COMPOUNDS ANO ALLOYS FOR RARE-EARTH-
TICE STAEILITIES FOR SECOND AND ‘IHIRG
TRANSITIClN METAL ALLOYS. . . . . . . . . . . . . . . . . . . . . . . . . . ...263 TRANSITION METALS SYSTEMS ENTHALPIES OF FORMATION. .26? TRANSITION SERIES ELEMENTS. NB- C. . . . . . . . . . ...261
- AL203- SID?. TI02- AL203- MGO. BAO-
ROXIMATIONS. ND- V. SM- v. TM- v. LU- EMA APPROXIMATIONS, NO- V. SM- V. TM- NI- FE. TI- AL- V. NI- V- AL, CO- CR-
V- CR. V- CO- NI. V- NI- FE. TI- AL- 0- CR- V. MIEDEMA APPROXIMATIONS. NO- V. MIEDEMA APPROXIMATIONS, ND- V. SM-
V- CO- NI. V- NI- FE. TI- AL- V. Nl- . . . . . . . . . . . . . . . . . . . . . . . . . ..FE- V- CR,
FE- V- CR. V- CO- FE. NI- V- CR. . . . . . . . . . . . . . . . . . . . . . . . . FE-
UD?- ZROZ- MOD?. MICROALLOYED STEELS. DUPLEX PRECIP..261
V. CALORIMETER DETERMINATIONS. AL- LA, AL- CE. AL- ..261
V. LU- v. CALORIMETER DETERMINAlIONS. AL- LA, AL- C..261
V. MIEDEMA APPROXIMATIONS. NO- V. SM- V. TM- V. LU-..261
V. NI- V- AL. CO- CR- V. MIEDEMA APPROXIMATIONS. ND..261
V, SM- V. TM- V. LU- V. CALORIMETER DETERMINATIONS...261
V. TM- V. LU- V. CALORIMETER DETERMINATIONS. AL- LA..261 v- AL. CO- CR- V. MIEOEMA APPROXIMATIONS. ND- V. SM..261 v- CD- FE, NI- V- CR, V- CO- NI. V- NI- FE, TI- AL-..261 V- CO- NI. V- NI- FE, TI- AL- V. NI- V- AL. CO- CR-..261 v- CR, V- CO- FE. NI- V- CR. V- CO- NI. V- NI- FE. ..261 v- CR, V- CD- NI. V- NI- FE. TI- AL- V. NI- V- AL, 261 v- NI- FE, TI- AL- V. NI- V- AL. CO- CR- V. MIEDEMA::261 v- W. CD- PB- SN. BI- CD- SN. . . . . . . . . . . . . . . . . . . . . ...233
261..............FE- V- CR. V- CD- FE, NI- 261.. CR. V- CO- FE. NI- V- CR. V- CD- NI. 23B....................................MO-
266.............................CR. MO AN0 26B....................................CU- 26B.............................CU- W. AG- 23B.................................MO- V- 268...... . . . . . . . . . . . . . ..CU- W. AG- W. AU- 261..N. NI- Si- B- CR- FE, AL- FE. NI- AL.
PCl.NB- AL ALLOYS. NEAL. NE3AL. CA(l-XlMGl 261. NB3AL. CA(l-XIMG(XICO3 AND COIl-X)MN(
W LATTICE STABILITIES. __._._.. . . . . . . . . . . . . . . . . . ...266 W. AG- W. AU- W................ . . . . . . . ...268
W. AU- W....................... . . . . . . . . . . . . . . . ...268 W. CO- PE- SN. BI- CD- SN. .._ . . . . . . . . . ...238 w.............................. . . . . . . . . ...268 W- NI- CU. MG- Y- AL. V- AL- SI AL- CU. X AL- MG...261
XJCO3 AND CO(l-XIMN(XICO3. AOUEOUS SOLUTIONS. CACO3..261 XICO3. AOUEOUS SOLUTIDNS. CACO3- MGCD3- H20. MONTE-..261
261.IOUIO ALLOYS, ZR- C. HF- C. TI- C. ALI
261..NI- CU. MG- Y- AL, Y- AL- SI. AL- CU-
XjGAiYIINcl-YISB. SURFACE PHASE EQUILIBRIA, ANTIPHI..
X. AL- MG. AL- LI. MG- LI. CU- FE- NI. SB- SE. SN- ..261
261. ALLOYS. ZR- C. I-IF- C. TX- C. AL(X)GA( V)IN(I-Y)SB, SURFACE PHASE EOUILIBRIA. ANTIPHASE 80..261
261..R- FE, AL- FE. NI- AL, W- NI- CU. MG- Y.. AL. Y- AL- SI. AL- CU- X. AL- MG. AL- LI. MG- LI..261
26l..AL- FE, NI- AL. W- NI- CU. MG- Y- AL. Y- AL- SI. AL- CU- A. AL- MG. AL- LI. MG- LI. CU- F..261’
261..02- CAO. HF02- V2D3- MGO. HF02- SID2- Y2D3. HF02- SIO2- MGO. TIO2- AL203- HFO2, TIO2- MGO..261
26l..ERIAL. TI02- AL203. TI02- 5102. TI02- Y203. HFD2- ZR02- CAO. HFO2- Y203- MGD. HFO2- SIO2-..261
261..?. TI02- Y203. HF02- ZR02- CAO. HF02- Y203- MGO. HF02- SIO2- Y203. HF02- SID2- MGO. TIO2-..261
239........ LIOUlD MISCIBILITY GAP, CD- P6- ZN. 254..- SN. CU- FE- NI. CU- MG- AL, CU- MG- 2N. 244..IUM CLOSE PACKED HEXAGONAL PHASE. CU- ZN. 261..TION FOR PSEUDOBINARY ALLOYS, CA- PU- ZN. 261..AP. AU- SI BASED TERNARY SYSTEMS, AU- ZN. 261..YS WITH TL. KCL- CACL2. FE- C- B. FE- ZN-
255........................ZN- SN. ZN- IN. ZN-
255................................ZN- SN. ZN- 255....................................... ZN-
. . . . 239
c;:.;;;. cu:.;;:. 254 CU:.G;;.C;:‘;N;.C;:.GA;.C;:‘A;:::244
NI- SI- B- CR- FE, AL- FE, NI- AL. W- NI- CU. M..261 SN- SE. PD- TI. PD- B. GA- TL. BINARY ALLOYS WI..261
AL. AU- GA, MONTE CARLO FOR CONFIGURATIONAL ENT..261
GA, . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...255 IN. ZN- GA, . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . ...255
SN. ZN- IN. ZN- GA. . . . . . . . . . . . . . . . . . . . . . . . . . . ...255
261..- CR- C. FE- PD. METALLIC GLASSES CU- ZR. EKVI DATA BASE. FIRST PRINCIPLES CALCULATIONS. ..261
261..T CAPACITY. CO- GA- IN LIOUID ALLOYS, ZR- C. HF- C. TI- C. AL(XIGA(YIINil-YISB. SURFACE P..261
261 AL203. TIO2- SIO?. TIO?- Y203. HFO?- ZRO?- CAO. HFOZ- Y203- MGD. HF02- SIO2- Y203. HF02-..261
261 .03- SIO2. TIC2- AL203- MGO. BAD- UO2- 2R02- M002. MICROALLOYED STEELS: DUPLEX PRECIPITATE..26!
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