safety of nuclear reactors...accident (2/2) university of fukui • ct d dt ltcomputer codes are...
TRANSCRIPT
University of Fukui
Safety of Nuclear Reactors
Professor H. MOCHIZUKINuclear Reactor Thermal Hydraulics DivisionNuclear Reactor Thermal Hydraulics Division
Research Institute of Nuclear Engineeringf
1
University of Fukui
Accident (1/2)University of Fukui
• Design Basis Accident: DBA• Assumption of simultaneous double ended break
• Installation of Engineered Safety FeaturesEmergency Core Cooling System: ECCSg y g yAccumulated Pressurized Coolant Injection System: APCIyLow Pressure Coolant Injection System: LPCIHigh Pressure Coolant Injection System: HPCIg j y
2
Accident (2/2)University of Fukui
C t d d t l t• Computer codes are used to evaluate temperature behavior of fuel bundle.
• Computer codes should be validated.• Blow-down and ECC injection tests haveBlow down and ECC injection tests have
been conducted using mock-ups.RELAP5/mod3 and TRAC code are• RELAP5/mod3 and TRAC code are developed and validated.
3
ECCSUniversity of Fukui
Control Rod Drive
Turbine
Containment Air Cooling SystemRod Drive Relief
valve
Feed Water System Sea water
Shield Cooling SystemDump valve
Residual Heat Removal System (RHR)
g yHigh Pressure Coolant Injection System (HPCI)
Low Pressure Coolant Injection System (LPCI)
ve
Containment SprayS t
(APCI)
Byp
ass
valv
Heavy Water CoolingSystem
Reactor AuxiliaryComponent CoolingW S
Reactor Core Isolation Cooling System(RCIC)
SystemCondensate Tank
4Main System Diagram of Fugen
Water SystemReactor AuxiliaryComponent CoolingSea-Water System
(RCIC)
Blow-down experimentUniversity of Fukui
5
6MW ATR Safety Experimental FacilityUniversity of Fukui
y p y
Outlet pipes(74mmID, 10.5mL, 2 deg.)( , , g )
P,T
P
TPressure transducerThermocouple
P T
EL 11.5EL 9.7EL 9.51
Downcomer(
EL: Elevation in mID: Inner diameterL : Length from a component
to the next arrow.P,T
P,T Steam drum(1525mmID,4.46mL)
High power
EL 5.97EL 7.0
EL 8.45Shield plug
(275.7mmID,6.8mL)
Low powerheaters
Main steamisolation valve
P,T
P,T
P TWater drum
High powerheater3.7mL, 6MW
EL 2.27
EL 4.5
3.7mL, 200kWP,T (387mmID,3.9mL)
(186mmID, 24.6mL)
EL 1.64
EL 2 3Inlet ppes(62.3mmID,12mL) EL0.9
Check valves
Turbine flow meter
Connecting pipe
EL 0.4
EL 2.3
6
Pump
Fig. 6 Schematic of Safety Experiment Loop (SEL)
Connecting pipe(186mmID, 15.6mL)
Water level behavior after a main steam pipe break
University of Fukuip p
Drum
0
0.2
12
15Drum water level
m)
vel (
m) D/P
-0.2 9
er le
vel (
m
wat
er lw
v
D i ill ti d t b k
Drum water level increase duringdowncomer water level decrease
0 6
-0.4
3
6Dowmcomer water level
um w
ate
ncom
er wDevice oscillation due to break
D/P
-0.8
-0.6
0
3
0 10 20 30 40 50
Dr
Dow
n Reactor core
0 10 20 30 40 50Time (sec)
100 mm break at main steam pipeBreak
7
Beak
Simulated fuel bundleUniversity of Fukui
Location of maximum axial peaking
Local peaking is high for the outer rods due to the
47.30
52.01
49.55
54.49
51.81
56.07
39.63
Unit in mm
Outer
Power of clusterat each zone(kW/m)
axial peakingneutronic characteristics
Tie rod14.5 OD
29.72
27.04
18.92
33.12 34.6936.26
25.23
36.04 Middle
InnerHeater pin14.5 OD
Spacer TieGadlinia pin
493 740 740 1234 493V IV III II I plate
Gadlinia pin14.5 OD
405 460 360 260 260 260 260 260 260 260 280 320 400
T
T T T TT T T T
1020 Active heated length : 3700 mm
Cross sectional view of 36-heater bundleBottom
Top
T Thermocouple position
8
Fig. 7 Power distribution of 36-rod high power heater
Thermocouple positionsUniversity of Fukui
p pH19-1
0°
Section 1
E8 1D34-1
F17 1
D36-4Section 4
D20-4
F34-4 B18-4
D8 4
A21-4C7-4
C19-4
A17 4
C35-4
0°
DT-1270° 90°
G22-1E8-1
H1-1
F17-1
A4-1
D14-1A31-1
A11-1C25-1
GT-4
G4-4
270° 90°
D16-4C1-4
H5-4
B22-4
B10-4
F14-4B30-4
A3-4 H24-4
H12-4
D8-4
H32-4G23-4D2-4
A9-4F6-4E33-4
A17-4
E25-4G11-4
E13-4
G31-4
C15-4
180° 180°0°
E28-1 D28-4
F26-4
B20-2
Section 2
D18-2H34-2
B36-2 D19-5Section 5D35-5
D7 5 B21 5
A19-2
A7-2 C21-2
A35-2
C27-4A29-4
A20-5
C18 5G34-5
A36-5
0°
E1-2
F12 2
270° 90°
D22-2
B2-2F32-2
B8-2
B16-2
E1-2
H14-2
D10-2F24-2
G6-2
90°HT-5270°
F33-5B17-5
D7-5 B21-5
B9-5F6-5
D15-5H31-5 H4-5 B3-5
H11-5
A2-5H23-5
A7 2 C21 2
A1-2C9-2
E23-2
C17-2G35-2
F5-2
C3-2
E11-2
A15-2E31-2
G13 2
C22-5D1-5
A8-5
E5-5E32-5A16-5
C18-5G34-5
E24-5
C10-5
G14-5
B19-3Section 3
B35-3
180°0°
F12-2D30-2
B28-2 H26-2
E20-6
0°
Section 6H35-6
180°
F13-5
B29-5F25-5
D27-5
G13-2
C29-2
G25-2
A27-2
C20-3C36-3
E12-5
G26-5A28-5
C30-5
FT-3270° 90°
D21-3
H33-3 H6-3
D17-3
G5-3
D9-3
F23-3C2-3
B15-3F31-3 D3-3
F11 3
B7-3
AT-6270° 90°G10-6
B32-6E16-6
F3-6
C6-6
H7-6
A23-6
E14 3
F4-3A10-3
G32-3
C16-3
A22-3B1-3
C8-3E34-3 A18-3
G24-3
9
H13-3
D29-3
F11-3H25-3
B27-3
Fig. 8 Thermocouple positions on high power heater rods
C13-6
F29-6 D26-6
E14-3
E26-3C28-3
G12-3A30-3
180° 180°
Cladding temperature measured in a same cross section of heater bundle
University of Fukui
500Data at section-II
300
400
500
。
0
100
200
0 10 20 30 40 50 60Time (sec)
Fig. 14 Experimental cladding temperature for 150 mmdowncomer break
10
Calculation model of pipe break experimentUniversity of Fukui
p p p
Main steamisolationvalveMain steam pipe
Outlet pipesSteam drum
Upper shield
Powerdi t ib ti200kW
Max. 6 MW1 ch. Downcomer
Break
0.8
1.15
1.10
distribution200kW5 ch.
Waterdrum
Checkvalves
Pump
1.05
0.6
Inlet pipes
pLowerextension
AccumlatedPressure Coolant
11Fig. 9 Nodalization scheme for ATR Safety Experiment Loop
essu e Coo a tInjection system
Comparison between experimental result and simulation
University of Fukui
20
and simulation
10
15
20Calculatin
Experiment
-5
0
5
0 10 20 30 40 50 60Time (sec)
5
500
600Calculation Section-II
200
300
400
500
。
Experiment
0
100
200
0 10 20 30 40 50 60
12
Time (sec)Fig.16 Behavior of cladding temperature after 100 mm downcomer break
Improvement of blow-down analysis by applying statistical method
University of Fukui
600
pp y gDowncomer 100 mm break
500
550 Calculation
Experiment
350
400
450
ture (℃
)
250
300
350
Temperat
150
200
250
ScramECCS operation
1000 5 10 15 20 25 30 35 40 45 50
Time (sec)
13
( )
Improvement of blow-down analysis by applying statistical method
University of Fukui
500
Calculation
Downcomer 150 mm break
pp y g
400
450 Experiment
300
350
ture
(℃)
250
300
Tem
pera
t
150
200
100
150
0 5 10 15 20 25 30 35 40 45 50
14
Time (sec)
Application of stochastic method to FBR analysis
University of Fukui
7 8 9
Air cooler[31]
[32]
[33][15]
[14]to turbine
[19]
13
[48]
14[37]
[38][20]
[36] A-loopB-loop15
y
[13]
[47]15
10-2
1
5
6
-1
[28]
[29]
[30]
Upper plenum
[17]
turbine
Pump
3
[18]
[46][48]
1816
-3
[22]1
16
14
Evaporator Super-heater
[1]~[7]
12
[8] IHXHigh-pressureplenum
[16]
[34][35]11
[10]
[11]
[12]
[9]
3
[42]
18
[39] [40]
17[21]
[41]to B-loopC-loop From B&C loops
42 Low-pressure
plenum
Pump[24]
[23]
19
[49]
1922
-4
2021[ ]
[43][25]
[41]
to C-loop
C loop p
14 16Low-pressure turbine
Low-pressure side
16
p
19
24
[44] [45]
[27]
-1Deaerator
1 14
Link 1-Link 6: 1st to 6th layer (Inner driver)Link 7: 7th & 8th layer (Outer driver)Link 8: 9th to 11th layer (Blanket)Link 9: Center CRLink 10: CRs
[44] [45]
23[26]
2 3020
#2#3#4#5
25
#1
1
13
1Feedwater
Condenser
15
Link 10: CRsLink 11: Bypass
Feedwaterpump
High-pressure feedwater heaters Low-pressure feedwater heaters
Application of stochastic method to FBRUniversity of Fukui
℃) Method:
Plant parameters are
Pe number: 1000
mpe
ratu
re (
Measured at Monju
Analysis
Plant parameters are investigated by 10,000 trials of the Monte-Carlo calculation for 43 factorsqu
ency
(-)
Tem
Time (sec)
calculation for 43 factors which can affect on the plenum temperature.
Freq
℃)
( )
Result:The measured temperature
Statistics if measured Nu number Evolution of plenum temperature during turbine trip
quen
cy(-)
erat
ure (℃ Measured at Monju
Analysis
The measured temperature transient has been included in the group of calculated curves Most non safety
Freq
Tem
p curves. Most non-safety side value could be evaluated taking into account various statistical
16
Cool-down velocity of plenum temperature (℃/s)
Time (sec)account various statistical errors.
[1] N. Kikuchi and H. Mochizuki, Application of statistical method for FBR plant transient computation, FR’13, Paris (2013-March)
Severe accidentUniversity of Fukui
17
Heat transfer of melted fuel to materialUniversity of Fukui
18
Heat transfer between melted jet and materials
University of Fukui
104
1000
10
Nu = 0 0033 Re Pr
100NaCl-Sn 10 1100NaCl-Sn 20 900NaCl-Sn 20 1000/P
r j
Material, Dj(mm), T
j(oC)
Num
= 0.0033 RejPr
j
1
10 NaCl-Sn 20 1100NaCl-Sn 30 900NaCl-Sn 30 1000NaCl-Sn 30 1100
Nu m
/
Num = 0.00123 Re
j Pr
j
0.1
1Al2O3-SS 10 2200Al2O3-SS 10 2300Al2O3-SS 10 2300
j j
103 104 105 106Re
jComparison of Nusselt number between present data and data fromSaito et al.1) and Mochizuki2).1)Saito et al Nuclear Engineering and Design 132 (1991)
19
1)Saito, et al., Nuclear Engineering and Design, 132 (1991)2)Mochizuki, Accident Management and Simulation Symposium, Jackson Hole, (1997).
Fuel melt experiment using BTF in CanadaUniversity of Fukui
20
Fuel melt experiment using CABRIUniversity of Fukui
p g
21
Source term analysis codesUniversity of Fukui
General codes
NRC codes ORIGEN-2, MARCH-2, MERGE, CORSOR, TRAP-MELT, CORCON, VANESA NAUA 4 SPARC ICEDFVANESA, NAUA-4, SPARC, ICEDF
IDCOR codes MAAP, FPRAT, RETAIN
NRC code (2nd Gen.) MELCOR( )Precise analysis
d
Core melt SCDAP, ELOCA, MELPROG, SIMMER
Debris-concrete reaction CORCONcodes
Hydrogen burning HECTOR, CSQ Sandia, HMS BURN
FP discharge FASTGRASS, VICTORIA
FP behavior in heat transport system
TRAP-MELT
FP discharge during debris- VANESAFP discharge during debris-concrete reaction
VANESA
FP behavior in containment CONTAIN, NAUA, QUICK, MAROS, CORRAL II
22
CORRAL-II
CONATIN codeUniversity of Fukui
(13) AirContainment spray In case of containment bypass
(11)(14)
Air
ypContainmentrecirculation
system
(10)
(12)
Stack
Annulus
system
(7)(8)
(9)(10) Stack
(5)(6)
(7)(8) Filter Blower
Water flow
(1)(2)(3)
(4)(5)( )
Gas flow
23
( )(2)
Steam release pool
Fluid- structure interaction analysis during hydrogen detonation
University of Fukuiy g
24
University of Fukui
Analysis of Chernobyl AccidentInvestigation of Root Cause- Investigation of Root Cause -
25
Schematic of Chernobyl NPPUniversity of Fukui
1. Core2. Fuel channels3. Outlet pipes4. Drum separator5 St h d
9. Inlet pipes10. Fuel failure detection equipment11 Top shield
Electrical power 1,000 MWThermal power 3,200 MWCoolant flow rate 37,500 t/hSteam flow rate 5,400 t/h (Turbine)5. Steam header
6. Downcomers7. MCP8. Distribution group headers
11. Top shield12. Side shield13. Bottom shield14. Spent fuel storage15. Fuel reload machine16 Crane
,Steam flow rate 400 t/h (Reheater) Pressure in DS 7 MPaInlet coolant temp. 270 0COutlet coolant temp. 284 0CFuel 1.8%UO2Number of fuel channels 1,693
16. Crane
26
Elevation PlanUniversity of Fukui
27
Above the Core of Ignarina NPPUniversity of Fukui
28
Core and Re-fueling MachineUniversity of Fukui
29
Control RoomUniversity of Fukui
30
Configuration of inlet valveUniversity of Fukui
1
2
3 41. Isolation and flow control valve2.Ball-type flow meter 3.Inlet pipe4 Distribution group header
31
4.Distribution group header
Drum SeparatorUniversity of Fukui
32
Configuration of Fuel Channnel
University of Fukui
S.S.
Position: -0.018m
-8.283 (-8.335)
Diffusion welding
Zr-2.5%Nb Roll region
Electron beem welding (EBW)
200
mm
-8.483
Effective
Spacers
-8.969 Zr-2.5%Nb
core regionFuel assembly
Connecting rod
-12.451
14 192
-15.933
80
-14.192
Diffusion welding
(-16.478) EBW -16.433
(-16.588)S.S.
72
77 -16.633
33
-16.671 Welding
Heat Removal by ModerationUniversity of Fukui
P t b G hit iPressure tube Graphite ring Maximum graphite temperature is 720℃at rated power
φ88mmφ114mmφ91mm Heat generated in graphite
blocks is removed by coolant
p
Graphiteblocks
φφ111mm
Gap of 1.5mmCoolant
34
RBMK & VVERUniversity of Fukui
Finland
Russia
Lith iLithuania
Germany
Ukraine
35
Objective of the ExperimentUniversity of Fukui
• Power generation after the reactor scram for several tens of seconds in order to supply power to main components.
• There is enough amount of vapor in drum• There is enough amount of vapor in drum separators to generate electricity.
• But they closed the isolation valve.• They tried to generate power by the inertia• They tried to generate power by the inertia
of the turbine system.
36
Report in Dec. 1986University of Fukui
37
Trend of the Reactor PowerUniversity of Fukui
3500 Power excursion
2500
3000(M
W)
excursion
1500
2000
al P
ower
500
1000
Ther
ma
Scheduled power level for experiment20-30% of rated power
200MW0
00 00 00 00 00 00 04 40
30MW
sec
200MW
25:00
:00:00
25:01
:00:00
25:13
:05:00
25:23
:10:00
26:00
:28:00
26:01
:00:00
26:01
:23:04
26:01
:23:40 sec
minhourday
38
2 2 2 2 2 2 2 2 day
Time Chart Presented by USSRUniversity of Fukui
y
再循環流量Recirculation flowrate
給水流量 蒸気ドラム圧力出力Feedwater flowrate PowerDS pressure給水流量 蒸気ドラム圧力DS pressure
39
安全棒挿入開始Safety rod insertion
Result in the Past Analysis (1/2)University of Fukui
• T. Wakabayashi, H. Mochizuki, et al., Analysis of the Chernobyl Reactor Accident (I) Nuclear and Thermal Hydraulic Characteristics and Follow-up Calculation of the Accident, J. Atomic Energy Society of Japan, 28, 12 (1986), pp.1153-1164.
• T. Wakabayashi, H. Mochizuki, et al., Analysis of the Chernobyl Reactor Accident (I) Nuclear and Thermal Hydraulic Characteristics and Follow-up Calculation of the Accident NuclearThermal Hydraulic Characteristics and Follow-up Calculation of the Accident, Nuclear Engineering and Design, 103, (1987), pp.151-164.
• Requirement from the Nuclear Safety Committee in Japan
Recirculation flow rate
Water level
Drum pressure
Feed water
Water level
Neutron flux
40
Result in the Past Analysis (2/2)University of Fukui
Power at 48,000 MWTiming of peak
diff t
P j t b f th
was different. Why???
Power just before the accident was twice as large as the report. Why???
Power at 200 MW
Why???
???
Result of FATRAC
41
code is transferred, and initial steady calculation was conducted.
Possible Trigger of the AccidentUniversity of Fukui
• Positive scram due to flaw of scram rods• Pump cavitation• Pump coast down• Pump coast-down• Opening of turbine bypass valve
(6.96MPa)
42
Calculation Model by NETFLOW++ CodeUniversity of Fukui
y
7 MPaMain steam pipe
7 MPa
-1-21
EL:33.65-21
[11]Drum separators2 for one loopL: 30mID: 2.6mt: 0.105 m
Feed water for one DSWf =115 t/h, 140 oC(1453 t/h, 177-190 oC)
Fuel channelOD 0 088
Feed water pipe
Suction header
200 (3200) MWt[8]DowncomersOD: 0.325 mID: 0.295 mL: 23 - 33.5 mN: 12 (for each DS)
OD: 0.088 mID: 0.080mN: 1661ch. Outlet pipe
L: 12.7 - 23mOD: 0.076mID : 0.068m
8.2 m Flow control valve
EL:25.6m
Check valve
Suction header
EL:21.3EL:20.0
EL:14.852[10]
91
OD: 1.020mID: 0.9mL: 21m
Cooling pump :2 for one DSH: 200 m1000 rpm
Distribution group headersOD: 0.325mID: 0.295mL: 24mN: 16
1
EL: 12.15
Flow meterCheck valve
EL:11.8EL:11.6
[1]EL:5.9
EL:7.6
96
3
1000 rpm5500 kWGD2=1500 kg m25250 t/h ×2(8000 m3/h for one pump)
Pressure headerOD: 1.040mID: 0.9mL: 18.5m
EL: 9.60.080.088 95
EL: 0
Check valveTh ttli l ti l
[ ]
[2]
[9]
[3]
93
[4][5][6][7]
1121314151617192
OD: 0.828mID: 0.752mL= 36m
OD: 0.828mID 0 752
Feeder pipesL: 22.5 - 32.5 mOD: 0.057 mID : 0.050 mEL: 6.3
EL: 9.3
0.091
0.111
Graphite ring
0.02
94
43
Throttling-regulating valveL= 36m ID: 0.752mL= 34m
Graphite ring
Fuel channel
Trigger of the AccidentUniversity of Fukui
gg• Positive scram
P.S.W. Chan and A.R. DasterNuclear Science and EngineeringNuclear Science and Engineering,103, 289-293 (1989).
Andriushchenko, N.N. et al., Simulation of reactivity and neutron fields change, Int. Conf. of Nuclear Accident and the Future of Energy, P i F (1991)Paris, France, (1991).
44
Trigger of the Accident (cont.)University of Fukui
Scram rod (24rods)inserted by AZ-5 button
1.0Negative reactivity
8.0 5.0 Graphite block
1.5 Positive reactivityG hit di lGraphite displacer
Fuel 2×3.5mWater Column
45
Simulation from 1:19:00 to First PeakUniversity of Fukui
Data acquired by SKALA
10 400Flowrate (m3/s) DS water level (mm)F d t fl t (k / ) g/
s)
9
10
200
400( )P (MPa)Flowrate (calc.)Pressure (calc.)
Feed water flowrate (kg/s)Reactor power (calc.)DS water level (calc.)
MP
a)
flow
rate
(k
8 0
Pre
ssur
e (
edw
ater
f
7 -200
(m3 /s
), P
(mm
), Fe
6 -400
Flow
rate
ater
leve
l
Close stop valve:Turbine trip
5 -6000 60 120 180 240 300 DS
wa
Time (sec) Push AZ-5 button
Turbine trip
1:19:00
46
Trend of parameters for one loop from 1:19:00 on 26 April 1986
Behavior of Steam QualityUniversity of Fukui
0.05
0 03
0.04 TopCenter
ty, x
(-) Turbine trip
RCP trip
0.02
0.03
stea
m q
ualit
0
0.01
equi
libriu
m s
Two-phase
-0.01
Ther
mal
e
Water
-0.020 50 100 150 200 250 300
Tim e (sec) Push AZ-5 button
47
Void CharacteristicUniversity of Fukui
1
0.8-)
Void fraction
0.6Measuredon
, α (-
Pressure 7MPa 2Void fraction increase
0.4Correlation
id fracti
Void fraction
0.2
Vo
Void fraction increase
00 0.2 0.4 0.6 0.8 1
48
Thermal equilibrium steam quality, x (-)
Nuclear CharacteristicsUniversity of Fukui
Doppler Void
-1 10-5
-8 10-6
0.0004
0.0005
pp
-1.2 10-5
1 10
Δk/k/℃ 0.0003
k/k/%Void
-1.6 10-5
-1.4 10-5
Δ
0.0001
0.0002Δk
-1.8 10-5
0 500 1000 1500 2000 2500
T (℃)
00 20 40 60 80 100
Void fraction (%)
49
Peak Power and its ReactivityUniversity of Fukui
y
3.5 105
Power reported by USSR (MW)
3
T t l
5
2.5 105
3 105Power reported by USSR (MW)NETFLOW
)
1
2TotalScram (input)DopplerVoid
$)
5
1.5 105
2 105
Pow
er (M
W)
-1
0
Rea
ctiv
ity ($
0
5 104
1 105
-2Push AZ-5 button
0270 275 280 285 290
Time (sec)
-3270 275 280 285 290
Time (sec)1:23:30
50
Relationship between Peak Powerand Peak Positive Reactivity
University of Fukuiy
100
ers
full
pow
e
10
ak m
ultip
les
1pow
er p
ea
1
alue
of f
irst
0.10.75 0.8 0.85 0.9 0.95
Peak
va
51
Peak positive reactivity ($)
Just after the AccidentUniversity of Fukui
52
Control Room and Corium beneath the CoreUniversity of Fukui
53
University of Fukui
54
Before earthquake (14:46) & After Tsunami(15:45) at Fukushima-1 on 11 Mar. 2011
University of Fukui(15:45) at Fukushima 1 on 11 Mar. 2011
B f thBefore the earthquake
After the Tsunami
Area damaged by the Tsunami
Seawater pumps
Intake of seawater Heavy-oilpumps seawater Heavy-oil
tanks
55
Severe accident at Fukushima-1After Tsunami
University of FukuiAfter Tsunami
Operators injected water into the reactorcore by RCIC. After the loss-off-all-AC-
Fuel pool
core by RCIC. After the loss off all ACpower, water injection was impossible. Damaged
by Tsunami
DC powerOff-site powerContainment
vessel○
○
原子炉圧力容器
vessel
×Loss of off-site power
ECCS
○
Diesel generators
×RCIC pump
Stack
g
××
×pu p
56
Suppression poolSeawater pumps
Cooling pump for suppression pool
Hand calculation to estimate uncoveryUniversity of Fukui
y
• Assumption: Reactor diameter=4m, water level from top of f l 4fuel=4m
• Water inventory ≒ 50t/• Latent heat at 7MPa≒1500kJ/kg
• Initial heat generation rate of Unit-1(460,000kW)≒460 000/0 3 ≒ 1 500 000kW (70% f h t i l d t≒460,000/0.3 ≒ 1,500,000kW (70% of heat is released to seawater)Decay heat ratio at around 1000 sec ≒ 2%Decay heat ratio at around 1000 sec.≒ 2%Heat generation rate by decay heat≒1500000×0.02=30,000kW
• Mass evaporated for 1000 sec. : M(kg)M=30,000×1000÷1500
57
=20000kg=20t
Real water level and detected water levelUniversity of Fukui
Low pressure(Spent fuel pool)
High pressure (Core)Volume of steam ( p p )
Volume of steam expands 1600 times of water at 0.1 MPa.
expands 21 times of water at 7 MPa.
ExperimentExperiment
VV
Cv
V燃料 Mochizuki, H. et al., Core coolability of an ATR by heavy water moderator om situation beyo9nd design basis accidents, Nuclear Engineering and Design,
58
燃料
, g g g ,144 (1993), pp293-303.
Natural circulation after the loss of AC power and sea water pump
University of Fukuip p
Secondary sodium
Primary T bi G t
Super heater(SH)
Primarysodium
Primary pump
Air cooler(AC)
Turbine Generator
Condenser
Secondary pump
Evaporator(EV)
Sea water cooler
IHXCore Feed water pump
59[1] H. Mochizuki, Plant Behavior of a Fast Breeder Reactor under Loss of AC Power for Long Period, Nuclear Engineering and Design, 245, (2012), pp.19-27.
Analytical Model of Whole Heat Transport SystemsUniversity of Fukui
7 8 9
Air cooler[31]
[32]
[33][15]
Link 1-Link 6: 1st to 6th layer (Inner driver)Link 7: 7th & 8th layer (Outer driver)Link 8: 9th to 11th layer (Blanket)
1314[37]
[38][20]
[36] A-loopB-loop15
[13]
[47]15
10-2
16
-1
[29]
[30]
Upper plenum
[33]
[17]
[14]to turbine
Pump
Link 9: Center CRLink 10: CRsLink 11: Bypass
[18]
[19]
[46][48]
1816
-3
[ ][ ]
[22]1
16
14
Evaporator
Super-heater[1]~[7]
12
5
[8] IHX
[28]
[ ]
High- [16]
[34][35]11
[10]
[11]
[9]
3
[18]
18
[39] [40]17[21]
[22]
4[ ] [ ]
pressureplenum
Pump
[12]
[24]
192021[42]
[43][25]
[41]to B-loop
to C-loop
C-loop From B&C loops
14 16
42
Low-pressure
Low-pressure side
Low-pressureplenum
[23][49]
1922
-4
[27]
turbine
1
16
14
24
[44] [45]23[26]
#2#3#4#5 #1
13-1Deaerat
or Condenser
60
2 3020 251 1Feedwater pump
High-pressure feedwater heaters Low-pressure feedwater heaters
Station Blackout Event of “Monju”University of Fukui
700 500Inner core Ch.1 outletInner core Ch.2 outletInner core Ch 3 outlet
Inner core Ch.6 outletOuter core outletBlanket outlet
500
600
300
400Inner core Ch.3 outletInner core Ch.4 outletInner core Ch.5 outlet
Blanket outletUpper plenumHigh pressure plenum
te (k
g/s)
atur
e (o C
)
700 500300
400
100
200
A loopB loop
Flow
rat
Tem
pera
600 400
Inner core Ch.1 outletInner core Ch.2 outletInner core Ch.3 outletInner core Ch.4 outletInner core Ch.5 outlet
Inner core Ch.6 outletOuter core outletBlanket outletUpper plenumHigh pressure plenum
s)o C)
200 00 1000 2000 3000 4000 5000
C loop
Time (sec)
400
500
200
300A loopB loopC loop
Flow
rate
(kg/
s
Tem
pera
ture
(o
200
300
0
100
0 1 2 3 4 5 6 7
61
0 1 2 3 4 5 6 7Time (day)
Station Blackout at 1000 sec.University of Fukui
1000 500Inner core Ch.1 outletInner core Ch 2 outlet
Inner core Ch.6 outletOuter core outlet
800
900
400
Inner core Ch.2 outletInner core Ch.3 outletInner core Ch.4 outletInner core Ch.5 outlet
Outer core outletBlanket outletUpper plenumHigh pressure plenum
600
700 300A loopB loopC loop at
e (k
g/s)
ratu
re (o C
)
500 200
C loop
Flow
ra
Tem
per
300
400100
200 00 1000 2000 3000 4000 5000
Time (sec)
62