zirconium hydride precipitation and dissolution kinetics in ......zirconium / zirconium hydride...
TRANSCRIPT
-
Zirconium hydride precipitation and dissolutionkinetics in zirconium alloys
E. Lacroix1,2, P.-C. Simon2, A. T. Motta2 and J. D. Almer3
1
1: Framatome, Lynchburg, VA, USA2: Pennsylvania State University, PA, USA3: Argonne National Laboratory, Lemont, IL, USA
19th International Symposium on Zirconium in the Nuclear Industry
Manchester, UK, May 22nd, 2019
-
• Background
• Experiments
• Model development
• Conclusions
Outline
2
– Hydride hysteresis understanding
– How can hydrogen behavior be studied?
– How can we incorporate the experimental
data obtained to create the HNGD model
-
Background:Hydride hysteresis understanding
3
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
Zirconium / zirconium hydride hysteresis
4
0
50
100
150
200
250
0 50 100 150 200 250 300 350 400 450
Hyd
roge
n c
on
ten
t in
so
lid s
olu
tio
n (
wt.
pp
m)
Temperature (°C)
Hydride precipitation behavior by region
TSSD
TSSP
Precipitation
Dissolution
if hydrides are present
PrecipitationHydride nucleation and growth
E. Lacroix, A. T. Motta, J.D. Almer "Experimental determination of zirconium hydride precipitation and dissolution in zirconium alloy", Journal of Nuclear Materials, 509 (2018) 162-167.
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
z
5
Terminal solid solubility for precipitation and dissolution
E. Lacroix, A. T. Motta, J.D. Almer "Experimental determination of zirconium hydride precipitation and dissolution in zirconium alloy", Journal of Nuclear Materials, 509 (2018) 162-167.
603 wt.ppm
400 wt.ppm
541 wt.ppm
-
z
6
hydrides
Dissolved Hydrogen
Dissolution Temperature
E. Lacroix, A. T. Motta, J.D. Almer "Experimental determination of zirconium hydride precipitation and dissolution in zirconium alloy", Journal of Nuclear Materials, 509 (2018) 162-167.
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
7
Dissolved hydrogen
Precipitation Temperature
hydrides
E. Lacroix, A. T. Motta, J.D. Almer "Experimental determination of zirconium hydride precipitation and dissolution in zirconium alloy", Journal of Nuclear Materials, 509 (2018) 162-167.
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
How was the hydride
behavior studied?
8
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
Experimental Setup at Beamline 1 at APS
Load Frame
Clam shell
furnaceSample
9
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
z
Diffraction patterns
10
Peak intensityPeak position
Peak width
volume fractionStress
Size of the crystal size
Integration of diffraction data
Raw data
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
Differential Scanning Calorimetry(DSC)
CoolingSystem
Heating system and sample holder
11
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
Nucleation and Dissolution
kinetics measurement using
Synchrotron X-ray diffraction
12
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
Nucleation and Dissolution kinetics:hypothesis
13
• First order kinetics in the form:
𝑑𝐶𝑆𝑆𝑑𝑡
= −𝐾 ⋅ 𝐶𝑆𝑆 − 𝐶𝑒𝑞
• Differentiating:
𝐾 = −Δ𝐶𝑆𝑆
(𝐶𝑆𝑆−𝐶𝑒𝑞)Δ𝑡
• K is the kinetic constant, following an Arrhenius law:
𝐾 = 𝐾0 ⋅ exp −𝐸𝑝𝑘𝐵𝑇
𝐶𝑆𝑆 is the hydrogen content in solid solution (wt.ppm)𝐶𝑒𝑞 is the hydrogen content in solid solution at equilibrium (wt.ppm)
𝐾0 is the pre-exponential factor (𝑠−1)𝐸𝑝 is the activation energy of the process (eV/atom)
𝑘𝐵 is the Boltzmann constant𝑇 is the temperature (K)
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
Studying hydrogen behavior in Zr
14
• I: 𝑇𝑆𝑆P, 𝑇𝑆𝑆𝐷 (dynamic)
• II: 𝑇𝑆𝑆D (equilibrium)
• III: Dissolution rateNucleation rate
Conclu
sio
ns
Model
Experim
ents
Backgro
und
𝐾 = −Δ𝐶𝑆𝑆
(𝐶𝑆𝑆−𝐶𝑒𝑞)Δ𝑡
-
Studying hydrogen behavior in Zr
15
• Nucleation Kinetics
•𝑑𝐶𝑆𝑆
𝑑𝑡= −𝐾𝑁(𝐶𝑆𝑆 − 𝑇𝑆𝑆𝑃)
• 𝐾𝑁 =−Δ𝐶𝑆𝑆
Δ𝑡 𝐶𝑆𝑆−𝑇𝑆𝑆𝑃
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
Studying hydrogen behavior in Zr
16
• Dissolution Kinetics
•𝑑𝐶𝑆𝑆
𝑑𝑡= −𝐾𝐷(𝐶𝑆𝑆 − 𝑇𝑆𝑆𝐷)
• 𝐾𝐷 =−Δ𝐶𝑆𝑆
Δ𝑡 𝐶𝑆𝑆−𝑇𝑆𝑆𝐷
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
Growth kinetics measurement
using DSC
17
Conclu
sio
ns
Model
Experim
ents
Backgro
und
-
Differential Scanning Calorimetry
18
Conclu
sio
ns
Model
Experim
ent
Backgro
und
350 ℃320 ℃305 ℃300 ℃290 ℃280 ℃
𝑥(𝑡) =Δ𝐻 𝑡
Δ𝐻𝑡𝑜𝑡=
𝐶𝑃𝑃(𝑡)
𝐶0 − 𝑇𝑆𝑆𝐷(𝑡)
𝑥 = 1 − exp − 𝐾𝐺𝑡𝑝
Growth Kinetics Parameter
Depends on the growth
regime
𝐾𝐺 = 𝐾𝐺0 ⋅ exp −
𝐸𝐺𝑘𝐵𝑇
Avrami Parameter
Dimensionality of the growth.
• 2.5 for platelets
• 3 for spheres, 1 for
needles
ASTM standard E2070
-
19
Conclu
sio
ns
Model
Experim
ent
Backgro
und
Differential Scanning Calorimetry
99%(𝑥, 𝑡)
(𝑥, 𝑡)
(𝑥, 𝑡)
ASTM standard E2070
-
20
Conclu
sio
ns
Model
Experim
ent
Backgro
und
Time Temperature Transformation diagram
Tem
per
atu
re
Time to reach 99% of reaction
Diffusion reaction, 𝐾𝐺𝑅
Phase transformation reaction, 𝐾𝐺𝐷
𝑇𝑑
1
𝐾=
1
𝐾𝐺𝐷 +
1
𝐾𝐺𝑅
-
21
Conclu
sio
ns
Model
Experim
ent
Backgro
undExperiment repeated to obtain TTT
-
Model development
22
Conclu
sio
ns
Model
Experim
ent
Backgro
und
-
23
Conclu
sio
ns
Model
Experim
ent
Backgro
und
Model Summary
0
50
100
150
200
250
0 50 100 150 200 250 300 350 400 450
Hyd
roge
n c
on
ten
t in
so
lid s
olu
tio
n (
wt.
pp
m)
Temperature (°C)
Hydride precipitation behavior by region
TSSD
TSSP
Dissolution
if hydrides are present
Hydride nucleation and growth
𝑥 = exp −𝐾𝐷𝑡
Nucleation: 𝑥 = 1 − exp(−KNt)
Growth: 𝑥 = 1 − exp − 𝐾𝐺𝑡𝑝
-
24
Conclu
sio
ns
Model
Experim
ent
Backgro
und
Model Results
-
25
Conclu
sio
ns
Model
Experim
ent
Backgro
und
Synchrotron Experiment Simulation
E. Lacroix, A. T. Motta, J.D. Almer "Experimental determination of zirconium hydride precipitation and dissolution in zirconium alloy", Journal of Nuclear Materials, 509 (2018) 162-167.
-
z Hold time: 41 days
26
157⁰C 454⁰C
1”
64 wt.ppm of Hydrogen
Conclu
sio
ns
Model
Experim
ent
Backgro
und
A. Sawatzky, Hydrogen in Zircaloy-2: its distribution and heat of transport, Journal of Nuclear Materials 2 (1960) 321{328.
-
Conclusions
▪ Synchrotron X-ray diffraction was successfully used to
measure nucleation, and dissolution kinetics of hydrides.
▪ DSC was successfully used to measure hydride growth
kinetics and to obtain a Time-Temperature-Transformation
diagram for hydride precipitation.
▪ A hydrogen precipitation and dissolution model was created
based on a new approach and showed good agreement with
experimental data.
27
Conclu
sio
ns
Model
Experim
ent
Backgro
und
-
Acknowledgement
▪ DOE-NEUP
▪ Argonne National Laboratory
▪ Penn State Nanofab
▪ Penn State MCL
28
-
Questions
-
Furnace
Roughing Pump
Diffusion Pump
Gas tankControl Volume
Vacuum chamber
1. Remove oxide from sample using an acid solution
2. Deposit Nickel to prevent further oxidation
3. Introduce hydrogen using gaseous charging method
30
Introducing Hydrogen in the zirconium metal
Conclu
sio
ns
Model
Experim
ent
Backgro
und
-
sugar
1. T0 = Room temperature (RT)
2. T1 > Room temperature → less solid sugar in the water→ more dissolved sugar
3. T2 > T1 → Dissolution Temperature→ Only dissolved sugar
4. T3 < T2 → Precipitation Temperature→ first occurrence of solid sugar
5. T3 hold → Growth of sugar crystals
6. T4 = Room temperatureT
time
T1
T2 T3
32
T4
-
z
33
157⁰C 454⁰C
1”
64 wt.ppm of Hydrogen
-
Differential Scanning Calorimetry
34
• Low temperature to measure only diffusion-driven process
•1
𝐾𝐺=
1
𝐾𝐺𝐷 +
1
𝐾𝐺𝑅
• High temperature was implemented using free energy curves
-
z
35
Terminal solid solubility for precipitation and dissolution
E. Lacroix, A. T. Motta, J.D. Almer "Experimental determination of zirconium hydride precipitation and dissolution in zirconium alloy", Journal of Nuclear Materials, 509 (2018) 162-167.
603 wt.ppm
400 wt.ppm
541 wt.ppm
✓ Show that hydrogen continues to precipitate
below TSSP
-
z
36
Terminal solid solubility measurement using DSC
300
Temp
H content
TDTP
K. Une and S. Ishimoto, “Dissolution and precipitation behavior of hydrides in Zircaloy-2 and high Fe Zircaloy,” Journal of Nuclear
Materials, vol. 322, pp. 66–72, 2003.
K. Colas, A. Motta, D. M.R., and J. Almer, “Mechanisms of hydride reorientation in Zircaloy-4 studied in situ,” Zirconium in the Nuclear Industry: 17th International Symposium, vol. ASTM STP 1543, pp. 1107–1137, 2014.
TSSPTSSD
0
100
200
300
400
500
600
100 200 300 400 500 600
CS
S(w
t.p
pm
)
Temperature (°C)
TSSP (APS) [5]
TSSD (APS) [5]
TSSP (DSC) [3]
TSSD (DSC) [3]
✓ Show that the TSSP is the nucleation temperature
-
Studying hydrogen behavior in Zr
37
• Sample A: 0 MPa• Sample B: 200 MPa