a brief summary of thermodynamic properties of various ternary systems investigated by emf and...

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A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute of Inorganic Chemistry-Materials Chemistry Währingerstr. 42, A-1090 Vienna, Austria

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Page 1: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

A brief summary of thermodynamic properties of

various ternary systems investigated by EMF and

Calorimetric method

Sabine Knott and Adolf MikulaInstitute of Inorganic Chemistry-Materials Chemistry

Währingerstr. 42, A-1090 Vienna, Austria

Page 2: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Investigated Systems

EMF and Calorimetry

EMF

Calorimetry

AlSnZnAgSnZnCuSnZnBiInZn

BiSnAgBiSnCuInZnPdSnZn

CuInBiInSnCuInSn

AgAuSn AuCuSnAgAlSn 14 binary and ternary systems

Page 3: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

EMF Measurements

Partial Quantities__ΔG = -zFE

= exp (ΔG/RT)

Gibbs Helmholtz Equation•

__ΔH = -z(∂E/∂T)F-zFE__ΔS = z(∂E/∂T)F

STHG

T [K]

850 900 950 1000 1050 1100

EM

F [m

V]

0,0

0,5

1,0

1,5

2,0

2,5

3,0

3,5

4,0

4,5

5,0

FTE

zS

zFEFTE

zH

Page 4: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

EMF Apparatus

Electrodes: Mo or W wire

Quartz container

Valve for evacuation

sample

Liquid electrolyte LiCl/KCl/XCly (X= Al, Zn, Sn), (y=2,3)

Page 5: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

EMF Measurements

Integral Quantities

Gibbs-Duhem Equation x

ΔGEM=(1-xx)[ΔGE

M,x=0+∫dxx]y/z 0

__ΔGE

x = RT lnx

= lnx / (1-xx)2

21 )( x

x

x

H

Page 6: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Drop Calorimetry

SetaramMicrocalorimeter

200-1000°C, automatic sample device (max. 30 drops/measurement) controller/data aquisition with LabView, evaluation with HiQCalibration with NIST-sapphire

Page 7: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Calorimetry

HSignal = ni. (Hsample,FT-Hsample,DT) + HReaction

__

ΔHi = (HSignal/ni) – (Hsample,FT-Hsample,DT)

ΔHMIX =Hbin + ΣHReaction /(n+Σni)

Page 8: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Redlich Kister Muggianu Polynom

CCBABCBAACBACBAji ij

ijijimix xMxMxMxxxxxLxxH )(::

)(::

)(::

)(: )( 210

Isoenthalpy lines of the ternary Cu-In-Sn systemat 1073 K

Lν i,j binary interaction parameter

M ternary interaction parameter

Page 9: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Pd─Sn─Zn

Sn0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0

Zn

0,0

0,1

0,2

0,3

0,4

0,5

0,6

0,7

0,8

0,9

1,0

Pd

0,0

0,1

0,2

0,3

0,4

0,5

0,6

0,7

0,8

0,9

1,0

Page 10: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Bi─In─Zn

In0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0

Zn

0,0

0,1

0,2

0,3

0,4

0,5

0,6

0,7

0,8

0,9

1,0

Bi

0,0

0,1

0,2

0,3

0,4

0,5

0,6

0,7

0,8

0,9

1,0

Calorimetry, 500°C EMF, 600°C

Page 11: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Bi─In─Zn

Bi:In=1:1

xZn

0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0

H (

J/m

ol)

-3000

-2000

-1000

0

1000

2000

3000

4000

5000

EMFCalorimetry

Enthalpy of mixing measured by EMF and Calorimetry

Y Djaballah, L Bennour, F Bouharkat and A Belgacem-BouzidaModelling Simul. Mater. Sci. Eng. 13 (2005) 361–369

Page 12: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

BiInZn

at.%Zn

0 20 40 60 80 100

EM

K (

mV

)0

20

40

60

80

BiIn21BiIn21 (600°C)

Calorimetric measurementEMF measurement

Page 13: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Bi─In─Zn

Y Djaballah, L Bennour, F Bouharkat and A Belgacem-BouzidaModelling Simul. Mater. Sci. Eng. 13 (2005) 361–369

Page 14: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Ternary AgAuSn System

• Verschiedene Modelle:

• Extrapolationsmodelle nach Toop, Muggianu und Kohler

• Chou Modell

0.0 0.2 0.4 0.6 0.8 1.0-14000

-12000

-10000

-8000

-6000

-4000

-2000

0

2000

4000HM, J/mol

xAu

section with Sn:Ag 1:1 1:9 3:7 7:3 9:1

Ag:Sn=1:1

xAu

0,0 0,1 0,2 0,3 0,4 0,5 0,6 H

(J/

mol

)

-12000

-10000

-8000

-6000

-4000

-2000

0

exp. 1023 KKohlerMuggianuToop

Dragana Živković, Dragan Manasijević, Živan Živković, J. of the University of Chemical Technology and Metallurgy, (2004) 39(1), 63-76

Z.Li, M.Dallegri, S.Knott, ccepted for publication in J. of Alloys and Compounds

Page 15: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Ag-Bi-Sn vertical cross section Ag:Bi = 1:1

Δ-heating curve-cooling curve

Calcs based on [01Oht]Calcs based on [94Kat]

Page 16: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Cu-In

xIn

0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0

H [J

/mo

l]

-8000

-6000

-4000

-2000

0

Kang, 973 KHultgren, 1073 KItagaki, 1373 K

xIn

0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0

H [

J/m

ol]

-8000

-6000

-4000

-2000

0

973 K1073 K1073 K1173 K1273 K

973K

1073K, 1373K

xIn

0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0

H [J

/mo

l]

-8000

-6000

-4000

-2000

0

Kang, 973 KHultgren, 1073 KItagaki, 1373 K973 K1073 K1073 K1173 K1273 K

Page 17: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

CuInSn

Phase Diagram at different temperaturesLiu et al., J. Electronic Materials, 30(9), 2001, 1093

Experimental Procedure: Calorimetric Measurements at 1073 K and 973 K

Page 18: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Comparison Cu-In-Sn Kalorimetrie vs. Knudsen

A. Popovic, L. Bencze,International Journal of Mass Spectrometry 255 (2006) 41–49

Page 19: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Wetting angles

Systems: CuInSn, 5 at.%Cu

AgCuSn

0

20

40

60

80

100

120

We

ttin

g A

ng

le (

°)

Sn-

0.5A

g4C

uS

n-2A

g1.5

Cu

Sn-

2Ag0

.5C

uS

n-2.

5Ag0

.9C

uS

n-3A

g4C

uS

n-3A

g0.5

Cu

Sn-

3.2A

g0.8

Cu

Sn-

3.4A

g0.9

Cu

Sn-

03.5

Ag2

Cu

Sn-

3.5A

g0.7

Cu

Sn-

3.6A

g1C

uS

n-3.

8Ag2

.3C

uS

n-3.

8Ag0

.7C

uS

n-3.

9Ag0

.6C

uS

n-4A

g1C

uS

n-4A

g0.5

Cu

Sn-

4.7A

g1.7

Cu

Alloy

Cu Substrate

Ni Substrate

17 different alloysCopper and Nickel substrateCollophonium flux

Page 20: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Acknowledgements

• Dr. Zuoan Li

• FWF P16491–N11

• FWF P19469–N19

• COST 531

Page 21: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute

Thank you for your attention

Page 22: A brief summary of thermodynamic properties of various ternary systems investigated by EMF and Calorimetric method Sabine Knott and Adolf Mikula Institute