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Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
1 WSE 12.1_Bl23 rev 2, 2017-04-24
WAAP-11382
Test-Reactor Study of the Effect of Zirconia Coating
of Inconel Spacer Cells on Shadow Corrosion
Clara Anghel
Magnus Limbäck
Gunnar Westin
Terje Tverberg
Björn Andersson
Michael Leideborg
Jonathan Wright
2
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Overview
• Shadow corrosion: Background
• Remedies
• Materials and Coating Methods
• In-reactor testing
• Results and Discussions
• Summary
• References
3
Westinghouse Electric Sweden AB. All Rights Reserved.Westinghouse Non-Proprietary Class 3
WAAP-11382
Shadow corrosion: Background
▪ It is well known since many years
▪ It is an enhanced local corrosion that occurs mostly in BWRs on zirconium-based
alloys which are in contact or in close proximity to another more noble metal or alloy.
It is a generic phenomena that is normally
harmless
Cha
tela
inA
et a
l., A
NS
20
00
Shadow of a control rod handle on a
Zircaloy-2 fuel channel2 Cycles, 25 MWd/kgU
No Crud high visibility
4
Westinghouse Electric Sweden AB. All Rights Reserved.Westinghouse Non-Proprietary Class 3
WAAP-11382
Corrosion of Zr-based alloys in BWRs
Shadow corrosion
ESSC
Zr-based alloys: BWR corrosion mechanisms
Source: R. Adamson & P. Rudling, 2013
5
Westinghouse Electric Sweden AB. All Rights Reserved.Westinghouse Non-Proprietary Class 3
WAAP-11382
Shadow corrosion of Zr-based alloys in BWRs
• There is a trend for saturation
of the oxide thickness with
fluence or burnup.
• Generally, shadow corrosion
do not cause fuel performance
problems.
• The upper curve is a special
case of shadow corrosion
called Enhanced Spacer
Shadow Corrosion, ESSC, that
caused fuel failures in the past.
Normal
Shadow
corrosion
Shadow corrosion data from various BWR fuel vendors
claddings. Source: R. Adamson & P. Rudling, 2013
6
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Galvanic corrosion mechanism
Aim: To reduce the shadow corrosion development on Zry-2
by coating of Inconel X-750 spacer cells with ZrO2
An
od
e
(-)
Cathode
(+)
e-
Source: M. Ullberg et al, SKI report 2004:28
E1 (Inconel) E2 (Zircaloy)
Typical remedies for the galvanic corrosion process
• Disconnect the electrical joint between the dissimilar metals (using and
insulator) - difficult to maintain the insulator properties in reactor
• Coatings: coat either the anode or the cathode to generate a decrease in the
corrosion potential between the two metals
7
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Coating Inconel X-750 Spacer cells
Method 1 – thin coatings Method 2 – thick coatings
Cleaning Inconel X-750 spacer
cells in acetone and deionized
water; drying at 150C
Tap coating with 0.2M Zr(OPrn)4
alkoxide solution, coating rate
∼0.6 cm/min
Hydrolysis in air for 10min, heat
treatment in air at 100 °C, 1h
and at 500°C for 1h.
Dense homogeneous thin
films of ZrO2: 100 nm; 200 nm
Repeat 3 or 5 times (0.4M Zr(OPrn)4)
Produce the base coating using
Coating method 1
Tap coating with ZrO2 -nanoparticle
containing containing PEG and
DEG, coating rate ∼1.8 cm/min
Dried in air for 10min, heat
treatment in air at 100 °C, 15 min.
Repeat up to 6 times
Heat treatment at 500°C for 1h.
Thick films of ZrO2: 300 nm; 600 nm;
1.2 µm; 2.4 µm; 4.5 µm; 9 µm
PEG – Polyethyleneglycol
DEG - Diethyleneglycol
Treatment with a dilute alkoxide
solution from Method 1.
8
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
SpecimensTotal thickness of the coating
[µm]
W3A02M 0.1
W5A04M 0.2
W3A10 0.3
W3A20 0.6
W3A40 1.2
W3A80 2.4
W3A150 4.5
W3A300 9.0
Coated Inconel X-750 Spacer cell specimens
9
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Inconel X-750 Spacer cell specimens
Un-coated spacer
cell specimen
Spacer cell specimen
W3A02M
Spacer cell specimen
W3A20
Coating thickness 100 nm Coating thickness 600 nm
TRITON11 is a trademark or registered trademark of Westinghouse Electric Company LLC, its affiliates and/or its subsidiaries
in the United States of America and may be registered in other countries throughout the world. All rights reserved.
Unauthorized use is strictly prohibited. Other names may be trademarks of their respective owners.
Spacer cells that are used in the SVEA-96 Optima3 10x10 fuel design and in
the TRITON11 11x11 fuel design, includes sleeve-type cells with four long
linear supports (contact lines)
10
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Irradiation in Halden
Standard fully re-crystallized LK3 Zircaloy-2 instrumentation
tube equipped with spacer cells
11
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Irradiation in Halden
Fast neutron fluence (>1 MeV) for the 21 spacer
cell specimens
Temp.
[°C]
Pressure
[MPa]
Water Flow
[kg/s]
Duration
[FPD]
Fast Neutron
Flux
[n/cm2/s]
278 - 288 7.1 - 7.3 0.6 – 0.7 1490.09 –
0.16·1014
PeriodConductivity
[µS/cm]
O2
[ppb]
H2
[ppb]
1st cycle Loop 4)
(July – Oct 2005) 0.1 250 - 300 50 - 100
2nd cycle (Loop 10)
(Jan – March 2006) 0.3 - 0.5 250 - 300 50 - 100
12
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
In-reactor testingSpacer cell specimens
Specimen No. Specimen IDAxial pos.
[m]
Coating thickness Fluence Flux
[µm] [1021 n/cm2] [1014 n/cm2/s]
21 Standard5 1.450 0 0.121 1.101
20 W3A02M 1.395 0.1 0.130 1.169
19 W5A04M 1.370 0.2 0.134 1.200
18 W3A20 1.345 0.6 0.138 1.231
17 W3A150 1.320 4.5 0.142 1.261
16 Standard4 1.295 0 0.146 1.290
15 W3A40 1.270 1.2 0.150 1.318
14 W3A10 1.245 0.3 0.154 1.345
13 W3A80 1.220 2.4 0.157 1.369
12 W5A04M 1.195 0.2 0.160 1.391
11 Standard3 1.150 0 0.165 1.423
10 W3A300 1.125 9.0 0.167 1.437
9 W3A02M 1.100 0.1 0.168 1.447
8 W3A150 1.075 4.5 0.169 1.454
7 W3A20 1.050 0.6 0.170 1.460
6 Standard2 1.000 0 0.171 1.465
5 W3A300 0.950 9.0 0.171 1.461
4 W3A40 0.925 1.2 0.170 1.455
3 W3A10 0.900 0.3 0.169 1.446
2 W3A80 0.875 2.4 0.168 1.434
1 Standard1 0.850 0 0.166 1.420
13
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Post Irradiation Examination of the Zircaloy-2 tube
• Visual inspection
• Oxide thickness measurements:
– Axially at 9 different orientations: 0, 20, 40, 90, 130, 230, 270,
320 and 360
– Circumferentially in the shadow area of the spacer cell specimens
measured from 0 to 360 orientation, with steps of about 0.35 and
axially every 1 mm
The oxide measurement system: Fischer developed probe and a Fisherscope Eddy 560C-S desktop
instrument. The instrument uses the eddy current lift-off principle where changes to the probe impedance (and
corresponding instrument signal) are proportional to oxide thickness. The instrument was calibrated before and
after the measurements using standard foils of known thickness on an un-irradiated reference cladding tube of
the same design as the test tube. The accuracy of the oxide thickness measurement equipment is ±2 µm.
14
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Results of the oxide thickness measurements
• Shadow corrosion occurred on the
cladding tube under all spacer cell
specimens
• The thickness of the oxide formed
in the shadow area was strongly
affected by the thickness of the
ZrO2 coating on the Inconel X-750
spacer cells.
• Small effects were observed for
coating thicknesses below 2.5 μm
• Coating thicknesses of 4.5 and
9 μm reduced the shadow
corrosion with 26 to 42%.
15
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Contour plots of the oxide thickness in the spacer
shadow area
Significant improvement provided by
the 4.5 µm ZrO2 spacer cell coating
Area under the un-coated
spacer cell Standard2
Area under the spacer cell specimen W3A150
with a coating of 4.5 µm
16
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Oxide thickness axial variation measured on the Zircaloy-2
instrumentation tube at an orientation of 40
Direct contact spacer cell – Zry-2 tube4
.5 µ
m
4.5
µm
9 µ
m
9 µ
m
Sta
nd
ard Sta
nd
ard
Sta
nd
ard
Sta
nd
ard
Sta
nd
ard
17
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Oxide thickness axial variation measured on the Zircaloy-2
instrumentation tube at an orientation of 270
No effect of flux level above threshold level
non-contact mode
9 µ
m
9 µ
m
4.5
µm
4.5
µm
Sta
nd
ard
Sta
nd
ard
Sta
nd
ard
Sta
nd
ard
Sta
nd
ard
18
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
Summary
• Good in-reactor performance of the coatings produced on the Inconel X-750 spacer cells
• Shadow corrosion occured under all the spacer cell specimens
• The thickness of the oxide formed on the Zircaloy-2 tubing in the shadow area was strongly affected by the thickness of the ZrO2 coating on the Inconel X-750 spacer cells:
– Small effects were observed for coating thicknesses below 2.5 μm
– Coating thicknesses of 4.5 and 9 μm reduced the shadow corrosion with 26 to 42%.
• No effect of flux level above threshold level on the shadow corrosion performance
• The results confirm the electrochemical nature of the shadow corrosion and galvanic corrosion mechanism as a driver for the oxide growth in the shadow area of the spacer cells.
19
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
References
Andersson B., Limbäck M., Wikmark G., Hauso E., Johnsen T., Ballinger R.G. and Nystrand A.C., ”Test
Reactor Studies of the Shadow Corrosion Phenomenon”, Zirconium in the Nuclear Industry: Thirteenth
International Symposium, Annecy, France, June 10-14, 2001, Moan G.D. and Rudling P. (Eds.), STP1423,
ISBN: 0-8031-2895-9; ISSN: 1050-7558
Adamson R.B. & Rudling P., ”Properties of zirconium alloys and their applications in light water reactors
(LWRs)”, in “Materials Ageing and Degradation in Light Water Reactors: Mechanisms and Management”,
©Woodhead Publishing Limited, 2013, DOI : 10.1533/9780857097453.2.151.
Châtelain A., Anderson B., Ballinger R.G.,Wikmark G., ”Enhanced Corrosion of Zirconium-Base Alloys in
Proximity to Other Metals: The Shadow Effect”, International Topical Meeting on Light Water Reactor Fuel
Performance, Park City, UT, USA, 2000.
Châtelain A. R., ”Enhanced corrosion of zirconium-based alloys in proximity to other metals: the "shadow
effect”, MS thesis, Massachusetts Institute of Technology. Dept. of Nuclear Engineering, 2000.
Zwicky H-U., Lohner H., Andersson B., Wiktor C-G., Harbottle J.: “Enhanced Spacer Shadow Corrosion
on SVEA Fuel Assemblies in the Leibstadt Nuclear Power Plant”. ANS Topical Meeting on LWR Fuel
Performance, Park City, Utah, April 10-13, 2000.
20
Westinghouse Non-Proprietary Class 3 Westinghouse Electric Sweden AB. All Rights Reserved.
WAAP-11382
References
Lysell G., Nystrand A.-C. & Ullberg M.,” Shadow corrosion mechanism of Zircaloy”, Proceedings of the 14th
International Symposium on Zirconium in the Nuclear Industry, Stockholm, Sweden, June 13-17, 2004, pg.
445.
Treeman N. M.,”Electrochemical study of corrosion phenomena in zirconium alloys”, MS thesis,
Massachusetts Institute of Technology. Dept. of Nuclear Engineering, 2005.
Kim Y.-J. et al., “Photoelectrochemical Investigation of Radiation Enhanced Shadow Corrosion
Phenomenon”, 16th Int. Symposium on Zirconium in the Nuclear Industry, Chendu, China, May 9-13, 2010.
Ramasubramanian N., Shadow corrosion, Journal of nuclear materials 328, p. 249-252 (2004)
Ullberg M. et.al, SKI Report 2004:28, Shadow Corrosion Mechanism of Zircaloy (2004)
Lemaignan C., Impact of β- radiolysis and transient products on irradiation-enhanced corrosion of
Zirconium alloys, Journal of Nuclear Materials 187, p. 122-130 (1992)
Kucuk A. & Cheng B., Laboratory Investigation on Shadow Corrosion Phenomenon, EPRI 1021032 (2010)
Edsinger K., Enhanced Spacer Shadow Corrosion (ESSC) of BWR Fuel at Kernkraftwerk Leibstadt, (KKL),
EPRI, Palo Alto, CA, and Kernkraftwerk Leibstadt AG, Leibstadt Switzerland, Technical Report 1009736
(2004)