ThermodynamicsThermodynamicsand and ...tofa2010/Apresentacoes_TOFA2010/O50... · Bi–Sn alloys are...
Transcript of ThermodynamicsThermodynamicsand and ...tofa2010/Apresentacoes_TOFA2010/O50... · Bi–Sn alloys are...
ThermodynamicsThermodynamics and and thermophysicalthermophysical propertiespropertiesofof liquidliquid BiBi--OO--SnSn alloysalloys
Donatella Giuranno, Enrica Ricci, Rada Novakovic, Elisabetta Arato
National Research Council Istitute for Energetics and Interphases
Via de Marini, 6 – 16149 Genoa, Italy
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
IntroductionIntroduction
MotivationMotivation
Bi–Sn alloys are regarded as one of the alternatives to toxic lead-containing solders, as made and as constituent of ternary alloys.
The surface properties and wetting characteristics of Bi-Sn, as otherslead-free solders, are presently subjected to very intensive studies.
The presence of oxides on the surface of solder alloys is of criticalimportance because it affects the formation of an otherwise goodsolder joint by degrading joint wettability and solderability.
Therefore, knowledge of surface oxidation and relatedmechanisms is a key issue in the optimisation of the welding
�Oxidation reactions under steady state conditions: evaporation of oxides and diffusion phenomena are takeninto account.
IdeaIdea
ToolsTools
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
mechanisms is a key issue in the optimisation of the weldingprocess.
into account.
�Surface tension as sensitive parameter to reveal oxidationprocesses undergoing at the liquid metal surfaces
�A fluid-dynamic model on the oxygen transport to evaluate:
� degree of contamination of the surface � mechanism of the gas mass-transfer at the liquid metal-
gas interface.
�Dynamic surface tension: influence of operative conditions (Temperature, Ptot, PO2, time).
ToolsTools
xKPPP sOx
sOO ∆+Κ+= '
22
*
Effective pressure
�Diffusion in gas phase under different regimes
Saturation pressure
O2
Oxide evaporation
Oxide
Mass transport in the liquid phase
Pure metals: The Effective Oxidation Pressure Pure metals: The Effective Oxidation Pressure
1,E+02
1,E+05
OxidationOxidation
E. Arato, E. Ricci, D. Giuranno, P. Costa, J. Cryst. Growth 293 (1) (2006)
under different regimes� Knudsen Ptot ≤ 1 Pa� Fick Ptot ≤ 105 Pa
�Oxidation phenomena:- predominant the most volatile oxide and the most stable oxide
� Reaction domains:- at gas-liquid interface - inside the gaseous layer
�Oxide condens/evapor�Metal condens/evapor
�Diffusion in liquid phase
The presence of volatile oxides can contribute to mantain the surface underoxygen-free conditions
sOxPΚ
1,E-25
1,E-22
1,E-19
1,E-16
1,E-13
1,E-10
1,E-07
1,E-04
1,E-01
1,E+02
600 650 700 750 800 850 900 950 1000
Temperature [K]
PO
2 [Pa]
sOP
2
xK ∆'
OxidationOxidation
sOxKP
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
� The imposed temperature is lowered / increased under well controlled PO2
(modulation of the temperature � modulation of the saturation level)
� Evidence of oxygen tensioactive effect ( “inversion points” ) from dynamicsurface tension measurements
By increasing and decreasing the temperaturefor several hours, “inversions” of the
540 1000
AA BBdγ/dT>0
Dynamic Surface Tension MeasurementsDynamic Surface Tension MeasurementsE. Ricci, E. Arato, A. Passerone, P. Costa, Adv. Colloid Interface Sci. 117 (1–3) (2005) 15.
for several hours, “inversions” of thetemperature coefficient are observed.
AA and BB points correspond respectively to the beginning and to the end of the oxygen tensioactive effect
→ the transition between oxidation and deoxidation regime occurs
500
510
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0 1 2 3 4Time [h]
Su
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e te
nsi
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[m
N/m
]
500
600
700
800
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Tem
per
atu
re [
K]
Surface Tension Temperature [K]
dγ/dT<0 dγ/dT<0
AA BB
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
Flow-meterHV
pump
GAS mixing chamber
Feed GAS
Exhausted gas
ASTRAview
Oxygen sensor “ PO outlet’’
CCD Light
SAMPLE
Oxygen sensor “ PO2 sample”
Oxygen sensor “ PO2 chamber’’
Thermocouple
Oxygen sensor “ PO2 outlet’’
Oxygen sensor “ PO2 inlet’’
Pt-heating elementStainless steel chamber
Alumina tube
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
Knudsen regime: Ptot ≤ 10-4 Pa
8 ▪10-7 Pa ≤ PO2 ≤ 1 ▪10-5 Pa
Dynamic Surface Tension Dynamic Surface Tension
L. Fiori, E. Ricci, E. Arato, Acta Mater. 51 (2003) 2873.
Effective Oxidation Pressure Effective Oxidation Pressure
O2 transport in liquid phase
PO2 eff
PO2 sat
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
Effective Effective OxidationOxidation Pressure: Pressure: PurePure metalsmetals
PO2 eff SnOSnSn isis the “the “lessless” ” oxidisableoxidisable
PO2sat SnO2
PO2sat Bi2O3
M1
O2
Oxide
M2
O2
Oxide
M1XM2Y
� Liquid phase = ideal solution
� Two possible evaporating and stable oxide species
Binary Alloys: The Effective Oxidation Pressure Binary Alloys: The Effective Oxidation Pressure E. Arato, E. Ricci, P. Costa, Surf. Sci. 602 (1) (2008) 349. E. Arato, E. Ricci, P. Costa, Surf. Sci. 602 (1) (2008) 349.
� Two possible evaporating and stable oxide species
� Ideal mixture of oxides
12 MMCs
Oxs
Ox PPf =Volatility ratio
12
22
MMAs
Os
O PPf =Oxidability ratio
),,/(2
212
*CAMiMjMiMiMM ffxxPPP s
Oxs
OO Φ+Κ+=−
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
),,/(2
212
*CAMiMjMiMiMM ffxxPPP s
Oxs
OO Φ+Κ+=−
212
*MMOP −
M121
2
*MMOP −
M1
Binary Alloys: The Effective Oxidation Pressure Binary Alloys: The Effective Oxidation Pressure
the behaviour of the alloy towards oxidation tends to be similar to the component
which forms the most volatile oxide (the “less oxidisable “)
the existence of at least a volatile oxide prevents the surface oxidation even if the
the behaviour of the alloy towards oxidation tends to be similar to the component
which forms the most volatile oxide (the “less oxidisable “)
the existence of at least a volatile oxide prevents the surface oxidation even if the
212
*MMOP −
M2
];min[ 2212121
221
2
***MMMMMMMM OOO PPP −−− =
the existence of at least a volatile oxide prevents the surface oxidation even if the
corresponding metal is present in low percentages.
the existence of at least a volatile oxide prevents the surface oxidation even if the
corresponding metal is present in low percentages.
BiBi--SnSn: : DynamicDynamic surfacesurface tensiontension measurementsmeasurements
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
EffectiveEffective OxidationOxidation PressurePressure
Bi30Sn70
Knudsen regime: Ptot ≤ 1 Pa
8 ▪10-14 Pa ≤ PO2 ≤ 2 ▪10-2 Pa
Bi43Sn57
Bi85Sn15
10-11 10-7 10-4 10-210-9
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
10-910-12 10-4
saturationBi O2 tensioactive effect
Bi: Bi: DynamicDynamic surfacesurface tensiontension measurementsmeasurements
EffectiveEffective OxidationOxidation PressurePressure ofof BiBi--OO--SnSn: T = 650 K: T = 650 K
PO Bi-O-Sn
),(),,/(2
212
*ji
sOx
sOO CAMiMjMiMiMM ffxxPPP ΨΨΨ+Φ+Κ+=−
Ψi =f(xsO2, Ps
ox,CL, transport coefficients, diffusivities)
PO2 eff Bi-O-Sn
PO2 sat Bi-O-Sn
ConclusionsConclusions�The experimental results obtained on the oxidation of Bi-Sn system in theliquid phase, agree very well with the predictions: the less oxidizable element(Sn) governs the behavior of the alloy towards oxidation.
�In many instances the existence of a volatile oxide (SnO) prevents thesurface oxidation even if the corresponding metal is present in low percentages:confirmed up to Bi95Sn5.
�If the evaporation of oxides from the surface is taken into consideration aswell as diffusion phenomena, the prediction of the real effective oxidationpressure is well comparable with experimental findings.
�Experimental and theoretical investigation of Bi-Sn oxidation tendencyunder Fick regime.
�Comparison between the results obtained by fluid-dynamic approach and theprediction of oxidation by applying thermodynamic models.
�Surface tension measurements and related temperature coefficients on Bi-Snliquid system under equilibrium conditions as a function of oxygen partialpressure.
Next stepsNext steps
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
Thank youfor your attention!for your attention!
TOFA 2010 TOFA 2010 -- Discussion Meeting on Thermodynamics of Alloys Discussion Meeting on Thermodynamics of Alloys -- September 12September 12--16, 2010, Porto (Portugal)16, 2010, Porto (Portugal)
EffectiveEffective OxidationOxidation PressurePressure ofof BiBi4343SnSn5757
T=T= 550550÷÷650 K650 K
Effective Oxidation Pressure of PbEffective Oxidation Pressure of Pb--OO--BiBi
390
410
430
450
470
Su
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e te
nsi
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[m
N/m
]
700
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900
1000
Tem
per
atu
re [
K]
Fick regimeFick regimePPtottot = 10= 1055 PaPaPOPO22 ≅≅≅≅≅≅≅≅1010--22 PaPa
370
390
410
Su
rfac
e te
nsi
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[m
N/m
]
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900
1000
Tem
per
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re [
K]
400
420 1000
350
370
54 57 60 63 66 69 72
time [h]
Su
rfac
e te
nsi
on
[m
N/m
]
500
600
Surface Tension
T [K]
BiBi--95at%Pb95at%Pb
310
330
350
370
0 2 4 6 8 10 12 14 16 18
time [h]
Su
rfac
e te
nsi
on
[m
N/m
]
400
500
600
700
Tem
per
atu
re [
K]
Surface Tension
T [K]
BiBi--44.1at%Pb44.1at%Pb
300
320
340
360
380
400
0 5 10 15 20
time [h]
Su
rfac
e te
nsi
on
[m
N/m
]
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600
700
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Tem
per
atu
re [
K]
Surface Tension
T [K]BiBi--18at%Pb18at%Pb
Effective Oxidation Pressure of PbEffective Oxidation Pressure of Pb--OO--BiBi
1,E-07
1,E-05
1,E-03
1,E-01
1,E+01
[P
a]
PO Pb-O-Bi1,E-07
1,E-05
1,E-03
1,E-01
1,E+01
[P
a]
PO2 eff Pb-O-Bi
1,E-07
1,E-05
1,E-03
1,E-01
1,E+01
[P
a]
PO2 eff Pb-O-Bi
),(),,/(2
212
*ji
sOx
sOO CAMiMjMiMiMM ffxxPPP ΨΨΨ+Φ+Κ+=−
1,E-15
1,E-13
1,E-11
1,E-09
1,E-07
0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0
X Bi
PO
2 [P
a]
PO2 eff Pb-O-Bi
PO2 sat Pb-O-Bi
1,E-15
1,E-13
1,E-11
1,E-09
1,E-07
0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0
X Bi
PO
2 [P
a]
PO2 sat Pb-O-Bi
$
$ Hasouna et al. 1991
1,E-15
1,E-13
1,E-11
1,E-09
1,E-07
0,0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1,0
X Bi
PO
2 [P
a]
PO2 sat Pb-O-BiT = 762 K
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Time [h]
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Tem
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In65Sn35
EffectiveEffective OxidationOxidation PressurePressure::
InIn--OO--SnSn
1,0E-15
1,0E-12
1,0E-09
1,0E-06
1,0E-03
1,0E+00
0 0,1 0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9 1
XSn
Pef
f [P
a]
In2O3 SnO2
In2O SnOIn-O-Sn
∆G In2O3 < ∆G SnO2
PS In2O > PS SnO
Volatility ratio ~ 102
Oxidizability ratio ~ 10-3
600 K
EffectiveEffective OxidationOxidation PressurePressure
CuCu--OO--SnSn
500
505
510
515
520
525
530
0 2 4 6 8 10 12 14 16 18 20 22
Time[h]
surf
ace
ten
sio
n[m
N/m
]
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600
700
800
900
1000
Tem
per
atu
re[K
]
Cu5Sn95
∆G SnO2 < ∆G Cu2O
PS SnO > PS Cu2O> PS CuO
Volatility ratio ~ 107
Oxidizability ratio ~ 10-9
1.E-05
1.E-04
1.E-03
1.E-02
1.E-01
1.E+00
0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
XCu
PO
2 e
ff / P
a
Cu-O-Sn1050 K