results of the quench-loca experimental program at kit · quench-l0 july 22, 2010 zry-4 2.5 1350...
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Institute for Applied Materials IAM-AWP; Program NUSAFE
www.kit.eduKIT – The Research University in the Helmholtz Association
Results of the QUENCH-LOCA Experimental Program at KIT
J. Stuckert, M. Grosse, M. Steinbrück, M. Walter, A. Wensauer
ASTM B10 2019
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Maintain coolable core geometry
Keep fuel inside cladding
Prevent cladding breaking
Maintain residual ductility in cladding
Limit oxidation (combined with hydrogen uptake during operation)
Limit hydriding after burst - under consideration
Oxidation limits
Keep equivalent cladding reacted below 17% → ECRBJ < 17%
Keep oxidation temperature below 1200°C → PCT < 1200°C
Keep hydriding below ? → ECR = ECR(H)
Present Regulatory Limit
for LOCA (international)
GRS
GRS
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steamoxidation
of inner
cladding
surface
Zr+2H2O=
ZrO2+2H2↑
Kr (He)
Secondary hydriding of cladding
Sequence of phenomena during LOCA:
➢ cladding ballooning and burst, relief of inner rod pressure
➢ steam penetration through the burst opening, steam
propagation inside the gap between cladding and pellet
➢ oxidation of inner cladding surface with hydrogen release
➢ absorption of hydrogen by cladding at the boundary of
inner oxidised area at temperatures above the phase
transition α → (α+β) in Zr alloy
➢ local embrittlement of cladding near to burst opening
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Higher burn-up: increased oxidation during normal operation
and pertaining hydrogen uptake
Secondary hydriding of cladding after burst
Application of new cladding alloys
Evidence of core coolability
Contribution to modification of current LOCA embrittlement
criteria (1200°C, 17% ECRBJ) with consideration of cladding
hydrogenation
Objective for QUENCH-LOCA bundle tests at KIT
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TestType of
cladding tubes
Max heat-up rate, K/s
Max T on the end of heat-
up, K
Duration of inner clad.
oxidation at T > 1123 K, s
Secondary cladding
hydro-genation
Post-test fracture due
to second. hydro-
genation
CommissioningQUENCH-L0July 22, 2010
Zry-4 2.5 1350 110 yes yes
ReferenceQUENCH-L1Feb. 02, 2012
Zry-4 7 1373 105 yes no
QUENCH-L2July 30, 2013
M5® 8 1373 88 yes no
QUENCH-L3HTMarch 21, 2014
Opt. ZIRLO™ 8 1623 252 yes yes
QUENCH-L4July 30, 2014
Pre-hydr. M5®
(100 wppm H)8 1385 100 yes yes
QUENCH-L3March 17, 2015
Opt. ZIRLO™ 8 1346 84 yes no
QUENCH-L5Feb. 17, 2016
Pre-hydr. opt. ZIRLO™
(300 wppm H)8 1257 45 no -
QUENCH-LOCA Test Matrix 2010 – 2016:
boundary conditions and results
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Hardware elements
QUENCH facility:
test section with flow lines
Rod pressurization from bottom
of each rod
TC fastening at the test rod
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Cross-sections of the QUENCH-L2 … -L5 bundles
All rods are filled with Kr with p=55 bar at Tpct=800 K.
QL-2, QL-4 QL-3, QL-3HT, QL-5
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400
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-50 0 50 100 150 200 250 300
Te
mp
eratu
re
, K
El.
po
wer, kW
; p
ressu
re, b
ar
Time, s
el. power
p first burst
p last burst
QL4_950mm (TFS7/13i)
QL2_950mm (TFS7/13i)
water 100 g/ssteam 150 C, 20 g/ssteam 190 C, 2 g/s
Ar 190 C, 6 g/s
Test progresses
M5: QL-2, QL-4 Opt. ZIRLO: QL-3, QL-5
inner pressure drop
due to burst3 test stages: 1) transient 8 K/s,
2) cooldown in steam, 3) quench
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-250
-50
150
350
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950
1150
1350
500 600 700 800 900 100011001200
Ele
vati
on
, m
m
Temperature, K
QL2 rod 7 48 s
QL4 rod 7 48 s
-250
-50
150
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500 600 700 800 900 100011001200
Ele
va
tio
n,
mm
Temperature, K
QL2 rod 7 76 s
QL4 rod 7 76 s
-250
-50
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Ele
va
tio
n,
mm
Temperature, K
QL3 rod7 48s
QL5 rod7 51s
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-50
150
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750
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1350
500 600 700 800 900 100011001200
Ele
va
tio
n,
mm
Temperature, K
QL3 rod7 76s
QL5 rod7 75s
Axial temperature profiles on first cladding burst and end of transient
QL-2 and QL-4 bundles
(M5):
QL-3 and QL-5 bundles
(ZIRLO):
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Post-test views of different bundles in the burst region
QL-1, view at 180° QL-2, view at 270°QL-4 bundle
(typical view for QL-3, -4, -5 bundles)Increased bending of QL-0, QL-1, QL-2 and QL-3HT rods
due to limited axial heater expansion
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QL-2, at corner rod A QL-3, at corner rod A
QL-4, at corner rod C QL-5, at corner rod C
Videoscope observations with camera
inserted from the bundle bottom at positions of corner rods
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Ele
vatio
n,
mm
Rod number
internal rods
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vatio
n,
mm
Rod number
internal rods
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Ele
vatio
n,
mm
Rod number
inner rods outer rods
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1010
1 2 3 4 5 6 7 8 9 101112131415161718192021
Ele
vatio
n,
mm
Rod number
inner rods outer rods
QL-2 (M5®) QL-4 (hydrogenated M5®) QL-5 (hydrogenated
opt. ZIRLO)QL-3 (opt. ZIRLO)
Radial and axial positions of burst openings
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0
100
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825 850 875 900 925 950 975 1000 1025
Wa
ll t
hic
kn
es
s, µ
m
Bundle elevation, mm
63°
153°
243° burst angle
333°
vsound=4717 m/s
Ultrasound measurements: typical cladding wall thinning
below and above the burst opening (rod #1, QUENCH-L5)
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Surface cracks (inside oxide)
formed during ballooning
around burst opening
QL-5, rod #1 burst opening top,
≈ 20 cracks/mmburst opening side,
≈ 20 cracks/mm
4 mm above opening tip,
≈ 40 cracks/mm
ZrO2
α-
Zr(O)
QL-3, rod #5: cross section
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Test
average burst
time,
inner rods, s
average burst
time,
outer rods, s
average burst
temperature,
inner rods, °C
average burst
temperature,
outer rods, °C
QL-0 (Zry-4, 2.6 K/s) 124 ± 10 159 ± 9 903 ± 26 897 ± 31
QL-1 (Zry-4, 7 K/s) 58 ± 2 75 ± 7 855 ± 31 858 ± 30
QL-2 (M5®, 8 K/s) 52 ± 2 65 ± 3 875 ± 22 860 ± 27
QL-3 (ZIRLO, 8 K/s) 52 ± 2 63 ± 4 843 ± 13 845 ± 39
QL-3HT (ZIRLO, 7.5 K/s) 54 ± 3 70 ± 7 854 ± 42 854 ± 54
QL-4 (hydr. M5®, 8 K/s) 51 ± 3 62 ± 4 835± 13 833 ± 32
QL-5 (hydr. ZIRLO, 8 K/s) 54 ± 2 68 ± 4 792 ± 19 820 ± 42
Burst time and burst temperature
Burst temperature of hydrogenated claddings is about 25 … 50 K lower in comparison to fresh claddings
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Testmax burst width,
mm
burst length, mm burst area, mm²
QL0 (Zry-4, 2.6 K/s),
bended rodsn. a. 12.7 ± 3.3 33.5 ± 21.1
QL1 (Zry-4, 7 K/s), strong
bended rods3.9 ± 2.6 14.5 ± 6.7 44.7 ± 49.2
QL2 (M5®, 8 K/s),
bended rods3.1 ± 1.2 13.5 ± 4.0 29.0 ± 22.9
QL3 (ZIRLO, 8 K/s) 3.9 ± 0.9 14.4 ± 2.2 31.0 ± 11.8
QL3HT (ZIRLO, 7.5 K/s),
strong bended rodsn. a. 19.3 ± 7.3 n. a.
QL4 (hydr. M5®, 8 K/s) 3.3 ± 0.7 13.1 ± 2.0 24.1 ± 7.4
QL5 (hydr. ZIRLO, 8 K/s) 3.8 ± 0.6 14.3 ± 1.8 29.9 ± 8.8
Average geometrical parameters of burst openings
Relatively small opening width: only pellet fragments with size ⪅3.5 mm can be released
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fewer oxidised spots at pellet-cladding contact
burst opening
Videoscope observation of contact between pellet and
cladding at inner cladding surface below burst opening
QL-2,
clad #8
QL-4, endoscopy of rod #1 QL-3, endoscopy of rod #5 QL-5, endoscopy of rod #3
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0 25 50 75 100 125 150
Te
mp
era
ture
, K
Time, s
QL5_TFS 7/13i
QL5_TFS 7/13
77
Dependence of radial temperature difference
from position of contact between pellet and cladding
QL-3 bundle:
large circumferential gradient (100 K)
QL-5 bundle:
moderate circumferential gradient (50 K)
Superposition of two temperatures gradients:
global bundle gradient (from shroud to central rod) and local gradient inside rod
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5
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Tem
pe
ratu
re, K
Str
ain
, %
Elevation, mm
QL2: circumferentialstrain of rod #1, shifted+45 mmQL4: circumferentialstrain of rod #1
QL4: T of rod #7 atburst time of rod #1
300
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5
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Tem
pe
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re, K
Str
ain
, %
Elevation, mm
QL3: circumferentialstrain of rod# 1(shifted +17 mm)QL5: circumferentialstrain of rod #1
QL5: T of rod #7 atburst time of rod #1
Results of laser profilometry: typical axial distributions
of the circumferential strain of claddings
➢ additional ballooning peaks (alongside the main burst peak) formed during heat-up
➢ circumferential strain values in ballooning regions outside of burst opening are noticeably higher for the pre-
hydrogenated claddings: cladding starts to creep earlier due to α→β transformation around dissolving hydrides
relative
low strain
maximum
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900
905
910
915
920
925
0 3 6 9 12
mm
µm
ZrO2
a-Zr(O)
Axial distribution of inner oxidation
within the region of secondary hydrogenation
metallographic
measurements along
longitudinal cut thick oxide
near to
burst opening
thin oxide
far from
burst opening
QL-1, rod #6
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ASTM B10, Manchester
Strong secondary hydriding for QUENCH-L0 with long transient:
hydrogen bands around burst location
(with quantitative results of n0-tomography)
rods #7 and #14:
tube ruptures during
tensile testing
at room temperature
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QL-0 (Zry-4): microhardness peaks at hydrogen bands
170
190
210
230
250
270
290
310
330
350
370
910 920 930 940 950 960 970 980 990 1000 1010
Elevation, mm
Hard
ne
ss
, V
ick
ers
rod #3; tburst=119 s; Tburst=820°C; Aburst=40 mm2 rod #8; tburst=122 s; Tburst=820°C; Aburst=60 mm2
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Neutron tomography: reconstruction of hydrogen distribution
and determination of hydrogen concentration
QL-3, clad #6, n0 3D image
n0 3D cross section,
axial thickness 40 µm
(voxel size)
mean CH = 475 ± 5 wppm,
local max CH = 1430 ± 70 wppm
mean CH = 278 ± 15 wppm,
local max CH = 1450 ± 100 wppm
light spots → max CH
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Neutron tomography: axial distribution of hydrogen
(mean and max values for each elevation)
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rod # QL-0 QL-1 QL-2 QL-3 QL-3HT QL-4 (H 100) QL-5 (H 300)
1 1393 490 640 390
2 980 260 240 1930 330
3 845 260 180 2000 165 345
4 505 1940
5 366 200 238
6 225 475 273
7 363 220 327
8 307 180
9 311 190 371 285
10 165 236
11
12
13 25 940
14 35 230
16 55 510
17
18 104
19
20 25
21 160 293
Axial maxima of the mean value of the hydrogen concentration (wppm)
(results of n0 tomography)
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{111}γ
{0
02
}γ
{2
00
}γ
{2
02
}γ
{2
20
}γ
{1
13
}γ
{311}γ
{2
22
}γ
{4
00
}γ
{1
11
}δ
{200}δ
{2
20
}δ
{3
11
}δ
{2
22
}δ
{4
00
}δ
{1
01
}ε
{1
10
}ε
{0
02
}ε
{2
00
}ε
{1
12
}ε
{2
11
}ε
{2
02
}ε
{1
03
}ε
{2
20
}ε
{1
00
}α
-Zr
{0
02
}α
-Zr
{1
01
}α
-Zr
{1
02
}α
-Zr
{1
10
}α
-Zr
{1
03
}α
-Zr
{2
00
}α
-Zr {
11
2}α
-Zr
{2
01
}α
-Zr
{0
04
}α
-Zr
{2
02
}α
-Zr
{1
04
}α
-Zr
{110}β
-Zr
{200}β
-Zr
{2
11}β
-Zr
{2
20}β
-Zr
0
20
40
60
80
100
30 40 50 60 70 80
Inte
nsit
y, %
Angle 2θ,
QL4 rod#5 161°
ZrH γ-hydride
ZrH1.66 δ-hydride
ZrH2 ε-hydride
α-Zr
M5 as-received 0 wppm H
β-Zr #34-0657
QUENCH-L4, rod #5: XRD analysis
indication of γ-hydrides
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ASTM B10, Manchester
δ-ZrH1.66
δ- and γ-
hydrides
EBSD analysis of cladding region inside hydrogen band
(QL-4, central rod)
hydride clusters near to boundaries of the region
of coalesced grains with the same spatial orientation
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#1 #2 #3 #5 #6 #7 #8 #9
QUENCH-L4: tensile tests at RT with inner rods,
fractures at hydrogen-bands (3 rods) and due to necking (5 rods)
n0-tomogr.
after
tensile test:
fracture
at H-spot
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Tensile test results: typical cladding fracture types
QL-4, clad #1
hydrogen
embrittlement
𝑪𝑯𝒎𝒂𝒙>1500 wppm
QL-3, clad #6 QL-3, clad #21 QL-4, clad #12 QL-3, clad #12
necking
far away from
burst regionstress concentration at the edges of burst opening
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Fracture surface: brittle and ductile regions
due to different hydrogen content
QL-4, clad #9 QL-4, clad #10
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Summary and conclusions
➢Seven QUENCH-LOCA bundle tests with different cladding materials (Zry-4, M5®, opt.
ZIRLO™) were performed according to a temperature/time-scenario typical for a LBLOCA in a
German PWR. For two tests (QUENCH-L4 and -L5) pre-hydrogenated claddings (with 100 and
300 wppm H for M5® and Opt. ZIRLO™, correspondingly) were used.
➢Generally, a peak cladding temperature of about 1080 °C was reached. The circumferential
temperature gradient was between 30 and 70 K on the burst onset (reason for not symmetric
ballooning with not significant strain).
➢The detailed profilometry of the whole length of the rods showed formation of not only main
ballooning area (with burst) but also, for several rods of each bundle, additional two or three
ballooning regions.
➢The influence of type of the fresh cladding material on the burst temperature is not very
remarkable: 865 ± 34 °C for M5, 857 ± 30 °C for Zry-4, 844 ± 30 °C for opt. ZIRLO.
➢For pre-hydrogenated claddings the cladding burst occurred at temperatures about 30 K lower
in comparison to as-delivered claddings. The reason of this difference could be a shift of the
phase transformation (α ↔ α+β) to lower temperature for the pre-hydrogenated claddings.
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Summary and conclusions (cont.)
➢Cladding wall thinning from 725 to 350 µm due to ballooning was observed at the burst side
along 50 mm below and above burst opening.
➢Oxide layer formed after the burst at the inner cladding surface around the burst opening with a
thickness of about 15 µm decreasing to 3 µm at a distance of about 20 mm from the burst
opening.
➢Hydrogen enrichments of a quite complex 3D form were observed for inner rods having seen
peak cladding temperatures of more than 1200 K.
➢Neutron tomography analysis showed the maximum hydrogen concentrations inside the
hydrogen bands less of 1000 wppm (averaged through the cladding cross section).
➢EBSD analysis showed that the zirconium δ- and γ-hydrides with µm-sizes are distributed as
compact clusters in the matrix intra- as well inter-granular.
➢During quenching, following the high-temperature test stages, no fragmentation of claddings
was observed (residual strengths and ductility were sufficient).
➢Tensile tests at room temperature evidenced fracture at hydrogen bands for several inner
rods with local hydrogen concentrations about 1500 wppm and more. Claddings with lower
hydrogen concentrations fractured due to stress concentration at burst opening edges. Other
tensile tested claddings failed after necking far away from burst region.
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Thank you for your attention
http://www.iam.kit.edu/awp/666.php
http://quench.forschung.kit.edu/
Acknowledgment
The QUENCH-LOCA experiments are supported and partly sponsored by the
association of the German utilities (VGB). The M5® claddings and Zircaloy-4
spacer material were provided by AREVA. The opt. ZIRLO™ claddings and
spacer material were provided by WESTINGHOUSE.
The author would like to thank Mr. C. Rössger, Mr. J. Moch, Ms. J. Laier and
Ms. U. Peters for intensive work during test preparation and post-test
investigations, Mr. M. Große for neutron tomography, Dr. M. Steinbrück and
Ms. U. Stegmaier for mass spectrometry, Dr. A. Pshenichnikov for the EBSD
analysis, Dr. H. Leiste for the X-ray diffractometry measurements.