ASTEC validation on PANDA tests A. BENTAIB, A. BLEYER Institut de Radioprotection et de Sûreté...
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Transcript of ASTEC validation on PANDA tests A. BENTAIB, A. BLEYER Institut de Radioprotection et de Sûreté...
ASTEC validation
on PANDA tests
A. BENTAIB , A. BLEYERInstitut de Radioprotection et
de Sûreté NucléaireBP 17, 92262 Fontenay aux
Roses Cedex, FRANCE
B. ATANASOVAINRNE-BAS
Tzarigradsko shossee 72, 1784 Sofia, BULGARIA
Nesseber september 2010 2/26
Motivation
Conclusions & perspectives
Outline
PANDA T9, T9bis and T25 analysis
Nesseber september 2010 3/26
3 barriers between radioactive materials and
environment (« Defense in depth » principle) :
• Combustible clads
• Primary Circuit
• Containment
Volume : 50000 to 80000 m3 depending of the type
Length scale : some cm to several meters
Double concrete containment or simple concrete containment with liner (steel or composite)
H2 risk issues: Pressurized Water Reactors
Nesseber september 2010 4/26
Severe Accident:
A severe accident is characterized by a reactor core uncovery leading to
core degradation and Fission Products release into the containment
atmosphere (loss of the two first barriers)
H2 Risk Issues: Pressurized Water Reactors
Four main Phases :
• Loss of Fuel coolant phase in the primary circuit
• Core uncovery and core degradation phases
• Core melt-throughand reactor core vessel
failure
• Core concrete interaction and base mat
penetration
Nesseber september 2010 5/26
• the composition of the gaseous mixture inside the containment at each location and at each time (Distribution)
• the effect of the mitigation means as spray, catalytic recombiners (Mitigation)
• an estimation of the possible ignition of the gaseous mixture (Flammability limits)
• an evaluation the propensity of a premixed flame to propagate inside the containment (Flame acceleration criteria)
• the pressure and temperature loads due to combustion events inside the containment (Combustion)
Hydrogen Risk evaluation for PWR: Needs
Nesseber september 2010 6/26
IRSN/GRS cooperation since 1996 for development of an integral code for LWR (present/future PWR, BWR, VVER) source term severe accident (SA) calculation
Main objectives: o Applications to PSA2, including uncertainty analysis,o Accident management studies, o Investigations of NPP behaviour in SA cond., including source term
evaluation, o Support and interpretation of experiments,o Basis for a better understanding of SA physical phenomena.
Main requirements:o Comprehensive coverage of phenomena, account for their interactions.o "Reasonable" calculation time (fast-running code) < 12h CPU for one day
of accident simulated, o Accounting for safety systems and their availability (SAM),o High level of model validation,o Modularity, flexibility, user-friendliness, easy model incorporation.
=> ASTEC aim : becoming the european reference code for Severe Accidents
ASTEC : Accident Source Term Evaluation Code
Nesseber september 2010 7/26
TOSQAN (IRSN) ThAI (BT) MISTRA (CEA) PANDA (PSI)
Example of experimental programs in support of ASTEC validation
Addressed phenomena : Condensation, Gas and Thermal stratification , stratification break-up, Spray effect, Scaling effect
7 m3 60 m3 100 m3 480 m3
Nesseber september 2010 8/26
PANDA facility
SETH configuration :Dimensions : Height 8 m, diameter 3.957 m, volume about 180 m³Materials: Steel walls
instrumentation: more than 275 TC and 47 sampling points for MS measurements
Operated by Paul Scherrer Institute (Switzerland)
Nesseber september 2010 9/26
Experiments
Steam/gasvent
Steam/gas vent
Test 13 Test 14
Steam injection into DW1: DW1 and DW2 initially filled with air or steam/air mixture
DW1 DW2DW1 DW2
4 m
6 m
Steam/gasvent
Test 11
DW1 DW2
1.8 m
Steaminjection140 °C, 1 m/s
Init. cond. Air 108 °C 1.3 bar
Init. cond. Air 108 °C 1.3 bar
Steaminjection140 °C, 1 m/s
Steaminjection140 °C, 1 m/s
Steam/gas vent
Test 10
DW1 DW2
1.8 m
Init. cond. Air 108 °C 1.3 bar
Steam/gasvent
Tests 9, 16, 17
DW1 DW2
1.8 m
Steaminjection140 °C
Exitvelocity:
: 1 m/s: 3 m/s: 5 m/s
Test 9Test 16Test 17
Init. cond. Air 108 °C 1.3 bar
Steaminjection108 °C, 1 m/s
Steam/gasvent
Test 9bis
DW1 DW2
1.8 m
Init. cond. Air 76 °C 1.3 bar
Steam/gasvent
Test 12
DW1 DW24 m
Init. cond. Air 108 °C 1.3 bar
Steaminjection140 °C, 1 m/s
Steaminjection140 °C
Exitvelocity 1 m/s
Init. cond. Steam/ 50% Air 108 °C 1.3 bar
Steam/gasvent
Steam/gas vent
Test 13 Test 14
Steam injection into DW1: DW1 and DW2 initially filled with air or steam/air mixture
DW1 DW2DW1 DW2
4 m
6 m
Steam/gasvent
Test 11
DW1 DW2
1.8 m
Steaminjection140 °C, 1 m/s
Init. cond. Air 108 °C 1.3 bar
Init. cond. Air 108 °C 1.3 bar
Steaminjection140 °C, 1 m/s
Steaminjection140 °C, 1 m/s
Steam/gas vent
Test 10
DW1 DW2
1.8 m
Init. cond. Air 108 °C 1.3 bar
Steam/gasvent
Tests 9, 16, 17
DW1 DW2
1.8 m
Steaminjection140 °C
Exitvelocity:
: 1 m/s: 3 m/s: 5 m/s
Test 9Test 16Test 17
Init. cond. Air 108 °C 1.3 bar
Steaminjection108 °C, 1 m/s
Steam/gasvent
Test 9bis
DW1 DW2
1.8 m
Init. cond. Air 76 °C 1.3 bar
Steam/gasvent
Test 12
DW1 DW24 m
Init. cond. Air 108 °C 1.3 bar
Steaminjection140 °C, 1 m/s
Steaminjection140 °C
Exitvelocity 1 m/s
Init. cond. Steam/ 50% Air 108 °C 1.3 bar
Main addressed phenomena
- Steam and non-condensable gases mixing behavior- Thermal stratification phenomena- Characteristic of gas transportation between compartments- Steam condensation on the walls- Injection location effect
Nesseber september 2010 10/26
PANDA nodalizationnear wall injection configuration
2.15 m
0 m
1.47 m
0.81 m
2.85 m
3.31 m
3.78 m
4.65 m
5.3 m
6.47 m
8 m
DW1 DW2
A040
A114L
B040
B114L
A181L
A250L
A308L
A355L
A421L
A498L
A589L
A725
A589P
A498P
A421P
A355P
PIPE
A589R
A498R
A421R
A355R
A308R
A250R
A181R
A114R
B725P B725
B589P B589L B589R
B498P B498L B498R
B421L B421R
B355L B355R
B308L B308R
B250L B250R
B181L B181R
B114R
C355
C308
C355
C308
50 zones
10 vertical levels
Zones connected by
flowpaths with area
according geometry
Structures: heat exchange
with atmosphere,
condensation, heat capacity,
heat losses to environment
Nesseber september 2010 11/26
In the early phase the amount of steam is for both tests comparable over the Vessel 1 height
Test 9 and Test 9bis analysis
steam concentration profil
0
1
2
3
4
5
6
7
8
9
0,00E+00 1,00E+01 2,00E+01 3,00E+01 4,00E+01 5,00E+01 6,00E+01
steam concentration
hei
ght
(m)
Test9bis-1400s
test9bis-3400s
test9bis-5500s
test9-1400s
test9-3400s
test9-5500s
expT9b-1400s
expT9b-3400s
exp9b-5500s
expT9-1400s
expT9-3400s
expT9-5500s
Later on, due to the on-set of condensation in Test 9bis the steam concentration at the top of vessel increases faster in Test 9
Due to the evaporation of condensate water, steam concentration in lower becomes higher in test9bis
Nesseber september 2010 12/26
Test 9bis: steam concentration (DW1)
DW1
0,0
0,1
0,1
0,2
0,2
0,3
0,3
0,4
0,4
0,5
0,5
0 1000 2000 3000 4000 5000 6000
Time(s)
Ste
am
mass f
racti
on
Astec -0.53
Astec-7.48
Exp-7.48
Exp._0.53 m
Evolution of Gas temperature (top and bottom of DW1)
70
72
74
76
78
80
82
84
0 1000 2000 3000 4000 5000 6000 7000 8000 9000
time (s)
tem
pera
ture
(°C)
Exp.-DW1-7,48m
Exp.-DW1-1,076m
Astec-A114R
Astec-A725
the condensate water drained to the lower part of DW1 leads to a sharp decrease of gas temperature at 4000 seconds. Afterwards and due to the difference between gas and wall temperature, steam evaporation occurs and generates an increase of gas temperature and steam concentration in the bottom of DW1
Nesseber september 2010 13/26
Thermal stratification in DW1
Gas Temperature profile DW1 half radius
0
2
4
6
8
70,00 72,00 74,00 76,00 78,00 80,00 82,00 84,00 86,00 88,00 90,00
Temperature (°C)
Ele
vat
ion
(m
)
Exp.-1000s
Astec-1000s
Exp.-4000s
Astec-4000s
Exp.-7000s
Astec-7000s
Gas Temperature profile DW1 half radius
0
2
4
6
8
102 103 104 105 106 107 108 109 110 111 112 113
Temperature (°C)
Ele
vat
ion
(m
)
Exp.-1000s
Astec-1000s
Exp.-2000s
Astec-2000
Exp.-3000s
Astec-3000s
Exp.-7000s
Astec-7000s
Until 3000 s, the increase of gas temperature is comparable for both tests
For test 9bis and after 3000 s, steam condensation induces a strong heat transfer and an increase of wall and gas temperature
Nesseber september 2010 14/26
Thermal stratification in DW2
Nesseber september 2010 15/26
time evolution of steam concentration in IP
0,0
0,1
0,2
0,3
0,4
0,5
0 1000 2000 3000 4000 5000 6000 7000 8000
Time (s)
Ste
am
mo
lar
fracti
on
ASTEC-T9bis
Exp-T9bis
ASTEC-T9
Exp-T9
Steam transport in IP
steam is transported mainly in the top of the interconnecting pipe The on-set of condensation in Test 9bis determines similar observation as in Vessel 1
Nesseber september 2010 16/26
Steam transport to DW2
DW2
0,0
0,2
0,4
0,6
0,8
1,0
0 1000 2000 3000 4000 5000
Time (s)
Ste
am v
olu
me
frac
tio
n
Exp. z=0,538m
Exp. z=7.478m
Astec-(6,47m-8m)
Astec (0-0,81m)
Steam volume fraction:DW2
0,00E+00
1,00E-01
2,00E-01
3,00E-01
4,00E-01
5,00E-01
6,00E-01
0,00E+00 1,00E+03 2,00E+03 3,00E+03 4,00E+03 5,00E+03 6,00E+03 7,00E+03 8,00E+03 9,00E+03
time (s)
stea
m v
olum
e fr
acti
on
Astec-bottom
Astec-top
Exp-0.538m
Exp-7.748m
Sharp steam stratification is observed during the overall test period, between the regions above and under the interconnecting pipe height
The on-set of condensation in Test 9bis determines similar observation as in Vessel 1
Nesseber september 2010 17/26
Steam concentration at venting location
0,0
0,2
0,4
0,6
0,8
1,0
0 1000 2000 3000 4000 5000 6000 7000
time (s)
Ste
am v
olu
me
frac
tio
n
ASTEC-T9bis
Exp-T9bis
Astec-T9
Exp-T9
Steam at the venting locationUntil 3000 s, steam concentration at venting location is compared for both tests
After 3000 s, The on-set of condensation in Test 9bis determines similar observation as in Vessel 1, Vessel 2 and IP.
Nesseber september 2010 18/26
PANDA nodalizationcentral injection configuration
ww
53 zones with 12 vertical levels
Zones connected by flowpaths with area according
geometry
Structures: heat exchange with atmosphere,
condensation, heat capacity, heat losses to
environment
Nesseber september 2010 19/26
Predicted pressure, gas composition and temperature in the vent are in good agreement with data
Test 25 analysis : pressure time evolution
Nesseber september 2010 20/26
Test 25 analysis: 1st Phase (time <815s)
Nesseber september 2010 21/26
Test 25 analysis 1st Phase (2215<time <2815s)
Nesseber september 2010 22/26
Test 25 analysis 1st Phase (4415<time <7015s)
Nesseber september 2010 23/26
Test 25 analysis 2nd Phase (7415<time <14215s)
Nesseber september 2010 24/26
Conclusions
Results on gas temperature and gas concentration obtained with the ASTEC code for both tests T9, T9bis and Test25 are in good agreement with the experimental data:
gas mixing and stratification above and under the height of the DW interconnecting pipe have been well reproduced by the code.
the steam condensation effect on the thermal and the concentration front propagation in the two drywells and the interconnecting pipe have been well predicted by the calculation
Nesseber september 2010 25/26
Conclusions
The Astec validation process will continue by considering well instrumented experiments to check the effect of facility scaleand to prepare rules and recommendations to best use of LP codes for reactor applications
Nesseber september 2010 26/26
Thank you for your attention