o54-surface tension and density of liquid ag-cu alloys
TRANSCRIPT
Surface tension and density of liquid Ag -Cu alloys
Foundry
Research
Institute
of liquid Ag -Cu alloys
Przemyslaw Fima1,2 and Natalia Sobczak1
1 - Center for High Temperature Studies, Foundry Research Institute, Krakow
2 - Institute of Metallurgy and Materials Science PAS, Krakow
E-mail: [email protected]
• Introduction
• Results for pure Ag
• Results for Ag-Cu alloys
– Density and molar volume
Presentation plan
– Surface tension
– Modelling of the surface tension
• Summary
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Ag-Cu system:
• A subsystem of ternary andmulticomponent solders
– Ag-Cu-Sn – Ag-Cu-Sn-In
Introduction
• A braze alloy for joining of metals and ceramics
– Ag-Cu– Ag-Cu-Ti
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
www.nims.go.jp/cmsc/pst/database/agelem/agcu/
• Investigated by a few groups:– relatively good agreement of density data– some differences in surface tension data
Introduction
Author (Year) DensitySurface tension
Krause et al. (1929) + +
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Krause et al. (1929) + +
Bricard et al. (1973) +
Sebo et al. (1977) + +
Lee et al. (2004) +
Novakovic et al. (2005) +
Kucharski et al. (2006) + +
Brillo et al. (2006) +
Experimental procedure
• Materials: Ag (5N), X(Cu): 0.3; 0.4; 0.5
• Sessile drop method
• Ar (6N) protective gas
• 1098 – 1573 K, temperature • 1098 – 1573 K, temperature decreasing stepwise
• Hold time 10 min
• Surface tension calculated with AstraView®, developed by CNR-IENI, Genoa, Italy N. Sobczak et al. Mater Sci Eng A495 (2008) 43
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Surface tension measurement
-0.5
-0.45
-0.4
-0.35
-0.3
-0.25
-0.2
-0.15
-0.1
-0.05
0-0.4 -0.3 -0.2 -0.1 0 0.1 0.2 0.3 0.4
1. capture the image2. change the image into
a set of coordinates3. fit the solution of Laplace
equation to coordinates
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Rotenberg et al., J Colloid Interf Sci 93 (1983) 16 9
Ag (pure) - density
ρL (g· cm-3)
ρT (g·cm-3 K-1)
Method Atmosphere Temperature
(K) Year
9.237 -0.00065 A – 1273 – 1473 1929 9.28 -0.0009 A – 1234 – 1573 1951 9.302 -0.000959 A N2 1234 – 1573 1953 9.348 -0.0011 MBP H2 1323 – 1423 1960 9.346 -0.0009067 A – 1234 – 2450 1962 9.337 -0.00105 MBP Ar 1234 – 1673 1964 9.36 -0.00108 MBP Ar 1273 – 1473 1969 9.36 -0.00108 MBP Ar 1273 – 1473 1969 9.301 -0.00105 SD Ar 1253 – 1381 1971 9.32 -0.00097 A N2 + 10% H2 1234 – 1773 1972 9.321 -0.0009787 A – 1234 – 1400 1975 9.31 -0.00078 SD Ar, H2 1234 – 1873 1989 9.346 -0.000911 MBP Ar + 10% H2 1273 – 1473 2003 9.304 -0.00071 SD Ar 1273 – 1523 2005 9.15 -0.00074 EML He + 8% H2 1250 – 1380 2006 9.288 -0.001175 SD Ar 1273 – 1573 2010
A – Archimedean principle, EML – electromagnetic levi tation, MBP – maximum bubble pressure, SD – sessile drop meth od
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Ag (pure) - density
9,1
9,2
9,3
9,4
Den
sity
, g c
m-3
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
8,8
8,9
9,0
9,1
1200 1250 1300 1350 1400 1450 1500 1550 1600
Den
sity
, g c
m
Temperature, K
Brillo et al. (EML)
Gasior et al. (MBP)
Kucharski et al. (SD)
This work (SD)
Ag (pure) – surface tensionρL
(mN· m-1) σT
(mN·m-1 K-1) Method Atmosphere
Temperature (K)
Year
946.0 -0.4 SD Vac. 1248 - 1298 1953 884.9 -0.17 MBP - 1273 - 1473 1958 898.4 -0.135 MBP - 1273 - 1473 1958 900.4 -0.1883 MBP H2 1273 - 1523 1960 913.0 -0.155 MBP H2 1273 - 1473 1964 921.3 -0.174 MBP - 1800 - 2330 1968 957.5 -0.14 SD Vac. 1246 - 1346 1970 910.7 -0.117 SD Ar 1253 - 1381 1971 910.7 -0.117 SD Ar 1253 - 1381 1971 926.0 -0.15 SD He 1234 - 1573 1972 890.0 -0.16 SD He 1253 - 1373 1982 910.0 -0.17 SD Ar, H2 1270 - 1860 1986 924.0 -0.19 EML Ar, H2 1273 - 1383 1986 898.3 -0.1905 MBP Ar + 10% H2 1273 - 1473 2003 925.6 -0.228 SD Ar + 10% H2 1269 - 1473 2004 914.0 -0.15020 SD Ar 1234 - 1473 2005 912.3 -0.204 SD Ar 1273 – 1523 2005 984 -0.298 EML Ar + 5% H2 1234 – 1734 2008
919.8 -0.176 SD Ar 1273 – 1573 2010
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Ag (pure) – surface tension
890
900
910
920
930
Sur
face
tens
ion,
mN
m-1
840
850
860
870
880
1200 1250 1300 1350 1400 1450 1500 1550 1600
Temperature, K
Sur
face
tens
ion,
mN
m
Mills and Su (review)
This work (SD)
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Ag-Cu alloys - density
8.8
8.9
9
9.1
9.2
9.3
Den
sity
, g c
m-3
8.2
8.3
8.4
8.5
8.6
8.7
1000 1100 1200 1300 1400 1500 1600
Temperature, K
Den
sity
, g c
m
Ag (pure)X(Cu) = 0.3X(Cu) = 0.4X(Cu) = 0.5
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Ag-Cu alloys – molar volume
10
10.5
11
11.5
12
Mol
ar v
olum
e, c
m3
mol
-1
7.5
8
8.5
9
9.5
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
X(Cu)
Mol
ar v
olum
e, c
m
Krause and Sauerwald (A)Sebo et al. (SD)Brillo et al. (EML)Kucharski et al. (SD)This work (SD)
1373 K
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Ag-Cu alloys – surface tension
920
940
960
980
1000
Sur
face
tens
ion,
mN
m-1
840
860
880
900
920
1000 1100 1200 1300 1400 1500 1600
Tempeature, K
Sur
face
tens
ion,
mN
m
Ag (pure)X(Cu) = 0.3X(Cu) = 0.4X(Cu) = 0.5
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
• The Butler equation
• The partial Gibbs free energy of the component i
Modelling of the surface tension
( )Exi
sExi
ii
si
ii GG
Ax
x
A
RT −−+= )()( 1
lnσσ
• The partial Gibbs free energy of the component i
• Parameters L from COST 531 thermodynamic database
( ) ( ) ( ) ( ) ( ) ( )( )[ ]...53 2102 +−−+−+= −−− ijijjiijjijijExi xxxxLxxLLxG
Exi
sExi GG ⋅= β)(
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Modelling of the surface tension
1200
1300
1400
1500
Sur
face
tens
ion,
mN
m-1
Sebo et al. (SD)Kucharski et al. (SD)Krause et al. (MBP)Bricard et al. (SD)Lee et al. (SD)Novakovic et al. (SD)
1373 K
800
900
1000
1100
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1X(Cu)
Sur
face
tens
ion,
mN
m
This work (SD)
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Modelling of the surface tension
0.5
0.6
0.7
0.8
0.9
1
X(A
g) in
the
surf
ace
laye
r
0
0.1
0.2
0.3
0.4
0.5
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
X(Ag) in the bulk
X(A
g) in
the
surf
ace
laye
r
1373 K1573 K
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
• Our data for pure Ag agree well with literature dat a
• Density of Ag-Cu alloys decreases with increasing t emperature and with increasing concentration of Cu
• Molar volume shows additive behavior in the whole r ange of Ag-Cu compositions
• Surface tension decreases with temperature and incr eases with Cu content, a small change of slope is observed
Summary
content, a small change of slope is observed
• There is a good agreement of experimental data with surface tension calculated with the Butler equation
• Surface layer of Ag-Cu solution is enriched with si lver
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
P. Fima, N. Sobczak (2010) Int J Thermophys, doi: 10.1007/s10765-010-0798-5
This work was financially supported by the Ministry of Science and Higher Education of Poland under the project no .
PBZ/MNiSW/07/2006/56, in the years 2007 – 2010
Thank you for your attention!
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Ag-Cu alloys – surface tension
-0.1
-0.05
0
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
X(Cu)
-0.3
-0.25
-0.2
-0.15
dσσ σσ/
dT
This workKucharski et al.Novakovic et al.
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
Modelling of the surface tension
1100
1200
1300
1400
Sur
face
tens
ion,
mN
m-1 beta = 1
beta = 0
1373 K
800
900
1000
1100
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1X(Cu)
Sur
face
tens
ion,
mN
m
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
• …
….
TOFA 2010, Discussion meeting on thermodynamics of alloys, 12-16.09.2010, Porto
( ) Czhgrr
+−=
+ ρσ
21
11