May 2-3, 2013
Reliability, Safety and Management Engineering and Software Development Services
Objectives;
Variants of the nodalizations considered;
Conditions and assumptions;
Cases analyzed, initial and boundary conditions;
Important parameters for the sensitivity studies;
Summary results from the sensitivity studies;
Issues identified during the sensitivity studies;
Conclusions;
References.
Main objectives of the presentation are as follows:
o
To discuss the results from sensitivity studies which are performed in order to be analyzed WWER-1000 plant model response during severe accident progression when three different MELCOR 2.1 nodalizations for the core region are used. These three nodalizations are respectively with one, five and thirty hydrodynamic volumes in the reactor core region;
o
To discuss the results from sensitivity studies which are performed in order to be analyzed WWER-1000 plant model response during severe accident progression when two different MELCOR 2.1 nodalizations for the steam generators secondary side are used. These two nodalizations are respectively with one and three hydrodynamic volumes for the
steam generators secondary side;
o
To represent and discuss various MELCOR 2.1 and/or plant model issues which have been identified during the performance of the sensitivity
studies.
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The nodalization schemes for the reactor pressure vessel and reactor
internals, the primary loops and the steam generators secondary side are
shown on Figure 1, Figure 2 and Figure 3 respectively .
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010-020 010-020
010-020
CV013 CV035
CV046
CV032 CV037
CV034 CV055 CV050
CV027
CV054 CV014
CV026
CV025
CV033 CV024
CV053 CV043 CV023
CV056
CV044
CV022 CV012
CV047
CV042 CV016
CV057
CV045 CV017
CV052 CV036
CV015 CVX00
CVX09 (CV110*)
CV040
X=1,2,3,4
035-060 034-060
033-060 032-060
031-060 027-060
057-050
x09-010 (110-010*) 29,440
035-040
CVX09 (CV110*)
16.899
18.519 060-070
070-050
18.419
040-060 24.930
020-040 22.928
020-060
CV020
CV040
CV070
CV050
CV091
CV060 CV010
22.928 047-060
CV032
033-034 031-032 034-035 032-033 035-040
23.728
CV031
CV033
091-092
057-060 047-050
CV034
CV035
CV092
020-031 020-040
26.753
020-032 020-033
020-060
020-034 020-035
050-091 24.647
040-050 040-060 040-050
070-092
037-060
CV010
CV060
CV070
031-050 032-050
020-012 033-050
034-050
16.899 035-050
050-x00
020-022 017-050
24.930
x09-010 (110-010*)
CVX00 29,440
CVX09 (CV110*)
16.899
26.953 26.953
020-032 030-060
18.519
020-040
020-030 060-070
070-050
18.419
060-070
020-042 027-050 24.930
040-050
020-060
040-060
29,440
030-050
CV030
CV020
CV040
020-052
CV070
CV050
CV060 CV010
18.519 030-040
050-x00
x09-010 (110-010*)
22.928
CV020
017-060 037-050
050-x00 CVX00
o Figure 1: Reactor pressure vessel and reactor internals nodalizations (for all the cases 5 radial rings in the COR package are modeled)
x05-x06
x00-x04 25.275
CVx01 CVx05
32,17
x24-x25
x06-x07 x26-x27
x07-x08 x23-x24
22,18 CVx23
x20-x21 CVx02CVx03
x21-x22 x27-x28
109-110*
26.125
23.475
x04-x05
CVx25
CVx08
CVx27
CVx00
24.000 30,128
29.140 x28-x05
20,215 20,215
CVx06
32,17
29.140
CVx04
CVx09
30,128
27,938 27,938
24.325
x25-x05
x01-x02
CVx28
CVx20 x02-x23
CVx26
CVx07 23.900
x08-x09 x02-x26
CVx21 CVx22
CVx24
25.700
20,640 x02-x03
CV110
x22-x05 x02-x20
21,065 23.900
x09-010 (110-010*) 25.700 050-x00
28,0395 28.7565 29.5545
CV050
CV010
CV458 CV458
110-458 109-458
X=1,2,3,4
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o Figure 3: Steam generators secondary side nodalizations
CVX28
CVX24 CVX27
CVX01 CVX22
CVX02
CVX25
FLX03
CVX20 FLX05
FLX04 CVX23
X=5,6,7,8 CVX21
CVX26 Riser
Steam Dome
Downcomer CVX00
CVx12
x00-x10
CVx10
x00-x10
X=5,6,7,8
x10-x12
CVx10 CVx12 x02-x06
29.155 30.380 31.930
35.275
34.695 35.275
30.380
27.930
34.695
31.930
27.930
For the performance of the sensitivity studies, the following conditions and assumptions take place:
o Subversion 5026 of MELCOR 2.1 has been used for the calculations;
o For the flow paths which connect the reactor lower plenum to the reactor core, flow paths inside the core, flow path to the reactor core bypass and the artificial flow paths between the core and the core shroud, the flow blockage option has been activated (FL_BLK). The default value of the minimum
porosity which is used in calculation of the flow resistance is chosen. The exception of that assumption is a case with double ended break of a main circulation pipeline (case 3B from Table 2) for which this coefficient is set to 0.5 in order to avoid failure of MELCOR 2.1;
o No safety systems are available with the exception of the case with reactor pressure vessel bottom break (as initiating event);
o HS degasing option is activated (HS_DG) – for the steel structures inside the vessel;
o No operator actions are considered.
For the purposes of sensitivity studies, the following cases have been selected:
o Total loss of power supply to the unit – For WWER-1000 (V320) this transient is characterized by high primary pressure and relatively slow primary water inventory decrease. Input decks with 1, 5 and 30 volumes in the reactor core are used. One and three volumes for the steam generators secondary side are separately used;
o Double ended break of a main circulation pipeline with DN 2x850 mm (cold leg break) – this case is characterized by the most dynamic change in the primary side parameters and very fast degradation of the core in case of unavailability of safety systems. Input decks with 1, 5 and 30 volumes in the reactor core are used. One volume for the steam generators secondary side is used because the secondary side influence on the severe accident progression for that case is not expected to be significant;
o Reactor pressure vessel partial break with DN 1130 mm (cross section area around 1.0 m2) with active and passive safety systems availability – this case is analyzed in order to assess the core blockage behavior for 1, 5 and 30 volumes in the reactor core region with safety systems availability. One volume for the steam generators secondary side is used, because the secondary side influence on the severe accident progression for that case is not expected to be
significant;
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o Middle LOCA of a cold circulation pipeline (close to the reactor vessel) with DN60 mm – this case is analyzed in order to assess the reactor installation response in case of severe accident progression as a result of middle LOCA.
Input decks with 1, 5 and 30 volumes in the reactor core are used. One and three volumes for the steam generators secondary side are separately used;
o Primary to secondary LOCA with DN 43 mm (PRISE 43 mm) – this case is specifically analyzed in order to be assessed the secondary side influence on the primary parameters in severe accident conditions.
Summary information for the cases which have been selected for the sensitivity studies is presented in Table 1.
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Case Case Case
Case Initial Initial Initial Initial Condition ConditionCondition Condition
Safety systems Safety systems Safety systems Safety systems
availability availabilityavailability
availability VariantVariantVariantVariant
Number of Number of Number of Number of Core/SG Core/SG Core/SG Core/SG volumes volumes volumes volumes
1. Station blackout Nominal Power No
1A 1V/1V
2A 5V/1V
3A 30V/1V
4A 30V/3V
2. LB LOCA with
DN2x850 mm Nominal Power No
1B 1V/1V
2B 5V/1V
3B 30V/1V
3. RPV bottom partial failure with DN 1130
mm
Nominal Power
Yes (one train from each safety
system)
1C 1V/1V
2C 5V/1V
3C 30V/1V
4. MB LOCA with DN60
mm Nominal Power No
1D 1V/1V
2D 5V/1V
3D 30V/1V
4D 30V/3V
5. PRISE with DN43 mm
Nominal Power No 1E 30V/1V
2E 30V/3V
Table 1: Summary information for the cases analyzed
For the sensitivity studies performed, the following parameters during the severe accident progression are analyzed:
o CPU time consumption (tCPU) – up to the moment of vessel breach;
o Total amount of hydrogen generated in the reactor core (COR-DMH2-TOT);
o Onset of gap release (tGR);
o Time when the maximal fuel cladding temperature reaches 1200oC (tCD);
o Onset of reactor core degradation (tDEG);
o Onset of UO2 relocation into the reactor lower plenum (tMUO2);
o Total mass of UO2 relocated into the lower plenum before the vessel breach (MUO2);
o Onset of the reactor pressure vessel breach (tVBR);
o Total amount of molten material ejected to the reactor cavity (COR-MEJEC- TOT);
o Maximal temperature of the hot legs (Thl_max) – important for station
blackout scenarios due to the creep rupture phenomenon (it is assessed 30 min before the vessel breach because HPME/DCH is concurrent to the creep rupture phenomenon);
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CaseCase
CaseCase VariantVariantVariantVariant
Number Number Number Number
of of of of Core/SG Core/SG Core/SG Core/SG volumes volumes volumes volumes
COR COR COR COR---- DMH2DMH2 DMH2DMH2----
TOT TOT TOT TOT [kg][kg][kg]
[kg]
tCPU tCPU tCPU tCPU [h][h]
[h][h]
tStZr tStZrtStZr tStZr [s][s]
[s][s]
tGR tGRtGR tGR [s][s]
[s][s]
tCD tCD tCD tCD [s][s][s]
[s]
tDEG tDEG tDEG tDEG [s][s]
[s][s]
1. Station blackout
1A 1V/1V 582 10.8 10500 10946 12500 15430
2A 5V/1V 912912912912 11.3 11500 11691 15000 24435244352443524435
3A 30V/1V 760 16.9 11000 11347 13000 15844
4A 30V/3V 668 17.5 10500 10727 12500 14997
2. LB LOCA with DN2x850
mm
1B 1V/1V 114 10.1 5 40 160 800
2B 5V/1V 149 10.0 5 45 160 800
3B 30V/1V 131 19.8 5 47 240 720
3. RPV bottom partial failure with DN 1130
mm
1C 1V/1V 95 108 6 48 175 797
2C 5V/1V 208 157 6 48 175 807
3C 30V/1V 2.3 331* 120 278 NONONONO NONONONO 4. MB LOCA
with DN60 mm
1D 1V/1V 273 11.2 2000 1800 2500 2826
2D 5V/1V 263 9.8 2000 2000 2500 3341
3D 30V/1V 295 16.5 2000 2077 2500 3113
4D 30V/3V 246 17.4 2000 2038 2500 3067
5. PRISE with DN43 mm
1E 30V/1V 454 22.3 8000 8417 9500 10576
2E 30V/3V 401 22.9 8000 8242 9500 10271
Table 2: Summary results from the sensitivity studies performed – part 1
*Calculated to the 24-th h (accident progression time) after the accident initiation
Case CaseCase
Case VariantVariantVariantVariant
Number of Number of Number of Number of Core/SG Core/SG Core/SG Core/SG volumes volumesvolumes volumes
tMUO2 tMUO2 tMUO2 tMUO2
[s][s]
[s][s]
MUO2MUO2MUO2 MUO2 [tons]
[tons]
[tons]
[tons]
Thl_max Thl_max Thl_max Thl_max
**
**
**
**
[K]
[K]
[K]
[K]
tVBRtVBR tVBRtVBR [s][s]
[s][s]
CORCOR CORCOR---- MEJEC MEJEC MEJEC MEJEC----
TOT TOTTOT TOT [tons]
[tons]
[tons]
[tons]
1. Station blackout
1A 1V/1V 15684 69 1260126012601260 25236 195 2A 5V/1V 24490244902449024490 52 1428142814281428 25615 218
3A 30V/1V 16389 63 1015 22351 222
4A 30V/3V 15946 53 994 20525 194
2. LB LOCA with DN2x850 mm
1B 1V/1V 1940 77 Not needed 8166 154
2B 5V/1V 2470 74 Not needed 9024 178
3B 30V/1V 2480 78 Not needed 7983 157
3. RPV bottom partial failure with DN 1130
mm
1C 1V/1V 797 83 Not needed 22350223502235022350 144 2C 5V/1V 9208 76 Not needed 40500405004050040500 114 3C 30V/1V NO NO Not needed NONONONO NONONONO
4. MB LOCA with DN60 mm
1D 1V/1V 5704 70 Not needed 12845 186
2D 5V/1V 4290 77 Not needed 14936 173
3D 30V/1V 5923 72 Not needed 12057 156
4D 30V/3V 5506 76 Not needed 13258 162
5. PRISE with 1E 30V/1V 10698 66 Not needed 17972 194
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o Figure 4: Total amount of the hydrogen generated for the in- vessel phase of severe accident (cases A, B,)
0 100 200 300 400 500 600 700 800 900 1000
0 10000 20000 30000 40000 50000 60000
Mass [kg]
Time [s]
COR-DMH2-TOT_1A COR-DMH2-TOT_2A COR-DMH2-TOT_3A COR-DMH2-TOT_4A
0 20 40 60 80 100 120 140 160
0 10000 20000 30000 40000 50000
Mass [kg]
Time [s]
COR-DMH2-TOT_1B COR-DMH2-TOT_2B COR-DMH2-TOT_3B
o Figure 5: Total amount of the hydrogen generated for the in- vessel phase of severe accident (cases D, E)
0 50 100 150 200 250 300
0 20000 40000 60000 80000 100000
Mass [kg]
Time [s]
COR-DMH2-TOT_1D COR-DMH2-TOT_2D COR-DMH2-TOT_3D COR-DMH2-TOT_4D
0 50 100 150 200 250 300 350 400 450 500
0 20000 40000 60000 80000 100000
Mass [kg]
Time [s]
COR-DMH2-TOT_3E COR-DMH2-TOT_4E
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o Figure 6: Total amount of the hydrogen generated – RELAP/SCDAP – Mass (tons) vs. Time (s) [2]
o Figure 7: Maximal gas temperature in the core – station blackout cases
500 1000 1500 2000 2500 3000
10000 12000 14000 16000 18000 20000 22000 24000 26000 28000 30000
Temperature[K]
Time [s]
CFVALU_2357_1V1V CFVALU_2357_5V1V CFVALU_2357_30V1V CFVALU_2357_30V3V
0 500 1000 1500 2000 2500 3000
0 10000 20000 30000 40000 50000 60000
Temperature[K]
Time [s]
CFVALU_2357_1V1V CFVALU_2357_5V1V CFVALU_2357_30V1V CFVALU_2357_30V3V
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o Figure 8: Hot legs gas temperatures (left) and hot legs metal temperature (right)
400 600 800 1000 1200 1400 1600 1800
0 10000 20000 30000 40000 50000 60000
Temperature[K]
Time [s]
CVH-TVAP_400_1V1V CVH-TVAP_400_5V1V CVH-TVAP_400_30V1V
CVH-TVAP_400_30V3V 400
600 800 1000 1200 1400 1600
0 10000 20000 30000 40000 50000 60000
Temperature[K]
Time [s]
HS-TEMP_1V1V HS-TEMP_5V1V HS-TEMP_30V1V HS-TEMP_30V3V
Issue 1: Related to station blackout scenario (5 volumes in the core region):
When nodalization scheme with 5 volumes in the core is used, then the core degradation starts immediately after the vessel breach or very late after that moment which is not physically accurate. This leads to initial ejection of a very small amount of molten material (mainly steel – about 500 kg) and the peak of the molten corium ejection starts about 4000 s after the vessel breach (see COR- MEJEC-TOT_2B_1 on Figure 9). The root cause of that issue might be related to erroneous activation of the lower head mechanical model (by the code or due to user mistakes). It is not clear so far what the exact reason is.
This issue has been overcome by the following ways:
o The lower head mechanical model is switched off by the sensitivity coefficient 1600 (3) which is set to 1.0E10. When the molten core material in the lower plenum reaches around 50-70 tons and there is molten material into the lower plenum region below the barrel perforated bottom (around 2.5 t), then SC
1600 (3) is set back to its default value of 1.0E3. The lower head fails and the molten corium ejection seems to be quite reasonable (see COR-MEJEC-
TOT_2B_2 on Figure 9). For Variant 2A (from Table 2) this approach has been applied;
o Nodalization scheme with 30 hydrodynamic volumes in the core – for that nodalization this issue does not appear at all.
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Depending on the time step this issue might cause additional problems such as:
o Reactor vessel breach with a very small amount of corium ejected – 1.0E-38 kg followed by a large corium ejection several hundred seconds after the vessel breach;
o Generation of error massage: Cavity Overfilled (an attempt to be ejected physically impossible amount of molten material – around 900 tons). This used to happen for the MELCOR 2.1 subversions before subversion 5026 for our WWER-1000 plant model specifically.
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o Figure 9: Mass of molten corium ejected – left hand side (close plan)
0 200 400 600 800 1000 1200 1400 1600 1800 2000
20000 22000 24000 26000 28000 30000
Mass [kg]
Time [s]
COR-MEJEC-TOT_2B_1 COR-MEJEC-TOT_2B_2
0 50000 100000 150000 200000 250000
20000 30000 40000 50000 60000
Mass [kg]
Time [s]
COR-MEJEC-TOT_2B_1 COR-MEJEC-TOT_2B_2
Issue 2: Related to station blackout scenario (5 and 30 volumes in the core region):
When nodalization scheme with 5 or 30 volumes in the core is used, then, at the moment of the reactor pressure vessel breach, the primary pressure oscillation between 14 MPa and 20 MPa occurred (see CVH-P_20_A on Figure 10). It is
followed by a message for lowed head failure due to overpressure. This issue has been overcome by the following ways:
o 500-1000 s before the vessel breach the sensitivity coefficient 1505 (1) was set to 1.0 (core blockage porosity coefficient) (see CVH-P_20_B on Figure 10);
o When 3 volumes for the steam generators are used then this issue does not appear at all.
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o Figure 10: Reactor lower head pressure before and shortly after the vessel breach
13 14 15 16 17 18 19 20
22200 22250 22300 22350 22400
Pressure [MPa]
Time [s]
CVH-P_20_A CVH-P_20_B
Issue 3: Related to LB LOCA with DN 2x850 mm (30 volumes in the core region)
o When nodalization scheme with 30 volumes in the core is used then a very large temperature peak around 10 000 K in a volume from the core region occurs and therefore MELCOR 2.1 fails (see CFVALU_2357_0.05 on Figure 11).
This issue is overcome by setting sensitivity coefficient 1505 (1) to 0.5. Values of that coefficient equal to 0.05 (by default), 0.1 and 0.25 lead to high
temperature peak in the core and code failure.
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o Figure 11: Maximal gas temperatures in the core for Issue 3 (right) – blockage porosity 0.05, 0.25 and 0.5
0 1000 2000 3000 4000 5000 6000 7000 8000 9000 10000 11000
600 800 1000 1200 1400
Temperature[K]
Time [s]
CFVALU_2357_0.05 CFVALU_2357_0.25 CFVALU_2357_0.5
Issue 4: Related to RPV bottom partial failure with DN 1130 mm (all variants);
For that initiating event, quite unexpected results have been obtained. For the variant with 1 and 5 hydrodynamic volumes in the core, the reactor vessel breach occurs about 22350 s and 40500 s after the accident initiation respectively (see Figure 12 (left hand side)). For the case with 30 volumes, core degradation does not occur at all (to ensure that, the calculation is extended to 24h) (see Figure 12 (right hand side)). At that moment, no reasonable explanation for these results has been found.
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o Figure 12: Mass of molten corium ejected (left) and maximal fuel cladding temperature (right) for Issue 4
0 20 40 60 80 100 120 140 160
0 50000 100000 150000 200000 250000 300000
Mass [tons]
Time [s]
COR-MEJEC-TOT_1C COR-MEJEC-TOT_2C
0 500 1000 1500 2000 2500 3000
0 20000 40000 60000 80000 100000
Temperature[K]
Time [s]
CFVALU_9017_1C CFVALU_9017_2C CFVALU_9017_3C
be drawn:
o The general progression of the severe accident for most of the cases considered is reasonable. The exceptions are the cases with RPV bottom break (with DN 1130 mm). The obtained results are quite different and it is difficult to draw a clear
conclusion about them. This causes great uncertainty in the containment event trees development for these cases;
o Most of the issues which have been identified are related to the nodalization schemes with 5 and 30 hydrodynamic volumes into the core region;
o The variants with 1 hydrodynamic volume in the core have not caused any issues and the code run quite stable. This variant leads to the lowest amount of hydrogen
generated for the in-vessel phase of the severe accident in case of station blackout scenario (case 1A). According to the results for the same initiating event which are generated by RELAP/SCDAP, the total amount of hydrogen generated for that phase is around 800 kg (see Figure 6). So the lowest amount of hydrogen for that case may or may not be physically accurate. As it can be seen from Table 2, the COR-DMH2- TOT parameter for cases 2A ÷ 4A is significantly higher than in case 1A which can be explained by the possibility for in-core circulation of water-steam mixture and the different core blockage behavior (more volumes and more flow paths available in the core for 5 and 30 volumes nodalizations). For case 2A, the largest value for the COR- DMH2-TOT parameter comes from the latest core relocation into the lower head and
o For LB LOCA with DN 2x850 mm, MB LOCA with DN 60 mm and PRISE 43 mm, the total amount of hydrogen generated into the core during the in-vessel phase does not differ significantly for the nodallizations with 1, 5 and 30 volumes in the core. Variant 3B is characterized by physically impossible gas temperature behavior in the core when the minimal blockage fraction is less than 0.5;
o For the cases 1A and 1B, the maximal hot legs metal temperatures are significantly higher than in cases 1C and 1D. This result is important when one considers creep rupture phenomenon which is more likely to occur for the hot legs than for the pressurizer surge line or SG tube (in the cases where none of the loop seals is cleared);
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1)
Actualization of PSA level 2 for KNPP (Kozloduy NPP, Bulgaria) units 5 and 6 (full power and shut-down), Risk Engineering Ltd (project is in
progress);
2)
Accident Management Guidelines and Procedures: Improvement of the Emergency Documentation for Ukrainian NPP, Risk Engineering Ltd.
(project is in progress)
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