“Benefits and Challenges of Fast Reactors of the SMR Type”...IAEA TM on “Benefits and...
Transcript of “Benefits and Challenges of Fast Reactors of the SMR Type”...IAEA TM on “Benefits and...
ALFRED PROTECTED LOSS OF FLOW
ACCIDENT EXPERIMENT IN CIRCE FACILITY
MARIANO TARANTINO
DANIELE MARTELLI
FABIO GIANNETTI
PIERDOMENICO LORUSSO
VINCENZO NARCISI
GIANFRANCO CARUSO
IAEA TM on
“Benefits and Challenges of Fast Reactors of the SMR Type”
Politecnico di Milano, Department of Energy
via Lambruschini 4/a,
20156 Milano, Italy
September 24-27, 2019
ANTONIO NAVIGLIO
ULISSE PASQUALI
MICHELE FRIGNANI
ALESSANDRO ALEMBERTI
CONTENTS
• Framework of the activity
• Objectives of the activity
• Outline of CIRCE facility
• Experimental test description
• RELAP5-3D© nodalization
• Numerical results and comparison with experimental data
• Summary
IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
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FRAMEWORK OF THE ACTIVITIES
FALCON (Fostering ALFRED CONstruction), an international consortium under
the leadership of Ansaldo Nucleare with ENEA (IT) and ICN (RO), is pursuing the
re-design of the LFR-DEMO in addition to the definition of an R&D and licensing
roadmap.
ALFRED is considered also the prototype of a viable competitive LFR commercial
unit in the SMR segment, by 2035-2040.
Among these organizations, CIRTEN (IT) and Servizi di Ricerche e Sviluppo
(SRS, IT) takes part as Supporting Organization to FALCON to enhance the R&D
activities devoted to ALFRED.
In this frame an R&D activity has been carried out at the CR ENEA Brasimone,
aiming at investigating the thermal-hydraulic behavior
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INTRODUCTION
• R&D activities carried out at the ENEA Brasimone Research Centre for
characterising SGBT performance in steady-state and transient conditions and
the pool thermal hydraulics phenomena
• A mock-up of 7 BTs 1:1 in length for ALFRED SG designed, assembled and
implemented in HERO test section for the CIRCE facility at ENEA CR
Brasimone
• An Experimental Test consisting of Protected Loss of Flow Accident (PLOFA)
transitions will be carried out in the framework of the European Project
HORIZON2020 SESAME (Simulations and Experiments for the Safety
Assessment of MEtal cooled reactors).
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OBJECTIVES OF THE ACTIVITY
❑ to compare best-estimate TH-SYS code calculations to
experimental data, thus, to validate RELAP5-3D© system code
in simulating liquid metal pool type FR designs
❑ to assess the reliability of SYS-TH multiD components in
modeling transient in LM pool FR
❑ to identify and, as far as possible, to quantify the code
limitations and the source of uncertainties in simulating
postulated accidents occurring in heavy liquid metal FR designs
❑ to improve the understanding of the TH processes and
phenomena observed in LOFA test
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Type”, Milan, June 24-27,2019
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Separator
HERO-SGBT
Riser
Fitting
volume
Fuel Pin
Simulator
Dead
Volume
S100
Main Vessel
CIRCE-HERO OVERVIEW
6
• Primary circuit
o Feeding conduit
o Fuel Pin Simulator: 37 electrically heatedpins; 800 kW nominal thermal power
o Fitting volume: large not insulated volume
o Riser: double wall with air gap insulatedpipe. A nozzle installed at the inlet sectionallows the argon injection for the LBEcirculation enhancement
o Separator: expansion volume where theseparation of the two phases occurs
o SG: 7 double wall bayonet tubes (6 m ofactive length) equipped with leakagemonitoring system
• Instrumentationo 39 thermocouples (TCs) monitoring
different FPS sub-channels
o 42 TCs installed in the SG
o 119 monitoring the LBE temperature alongthe whole height of the pool
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Type”, Milan, June 24-27,2019
HERO
Steam Generator
Riser
Fuel Pin
Simulator
Dead
Volume
Fitting
Volume
Feeding
Conduit
S100
Main Vessel
CIRCE
Parameters
Value
S100 OD [mm] 1200
S100 height
[mm]
8500
Max LBE
Inventory [kg]
90000
Temperature
Range [°C]
200-
500
Operating
Pressure [kPa]
15(g)
ALFRED RELEVANCE
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HERO
Steam Generator
Riser
Fuel Pin
Simulator
Dead
Volume
Fitting
Volume
Feeding
Conduit
Hot
pool
RISER
Cold
pool
CORE
CIRCE-HERO SECONDARY CIRCUIT LAYOUT
PCPC
PC
TFM
TFM
TFM
TFM
T0TFM
T3TFM
T2TFM
PC
Differential pressure transmitter
Relative pressure transmitter
DEMI
plastic line
accumulator
PUMP
HVW1
TCL1-1
¾'' BWG 16 tube
PCL1-1
HEATER
MA
NIF
OLD
7 DWBTs
PCL2-1
PCL3-1
TCL3-3
RVW2
TCH-T2
TCH-T1
TCH-T3
1" (FC)
BYPASS LINEF
USFMF
CFM
TCT2-I
T1 T2 T3 T0 T4 T5 T6
TCT3-I
TCT0-I
TCT4-I
TCT5-I
TCT6-I
TCT1-I
1" (FC)
3" (FC)
¾'' BWG 16 tube¾'' BWG 16 tube
¾''
BW
G 1
6 t
ub
e
HVW2
RVW1
T0-I
40 bar
LINE 1
LINE 2
LINE 3
LINE 4
ΔP
T0
T5-I
TCL2-2
TCL2-1
½'' BWG 18 tube
2.½'' sch. 80
TCL4-1
PCL3-2
TCL3-4
TCL3-2
TCL3-1
TCH-A1
TCH-W
TCH-A2
Steam 400°C, ̴180 bar
0.047 kg/s
TCH-T2
TCH-T6
TCH-T5
TCH-T3
TCH-T4
TCH-A1
TCH-A2
TCH-W
TCH-T1
HEATER
TCH-T4
TCH-T5
TCH-T6
PVW1
TCTCM
-3
COLD
HOT
M-2
TCM-1
V1
V2
V3
Low flow BYPASS LINE(V3 closed)
SCHL
ACC
PCLH
He 5 bar
HC
environment
TCH-T7
TCH-T7
+
-
SVW1
V8
V5
V4
H2O liquid 335°C, ̴184 bar
0.047 kg/sv=1.9 m/s
(slave tube)
H2O liquid 335°C, ̴184 bar
0.047 kg/sv=0.9 m/s
H2O liquid 335°C, ̴184 bar
0.331 kg/sv=2.6 m/s
H2O liquid 20°C, ̴184 bar
0.331 kg/sv=1.7 m/s
½''BWG 18 tube
¾'' BWG 16 tube
V6
HVW3
V7
CVW
VL
F
F
F
RIBArgon
Compressors
Ar
Ar
ΔP
T5ΔP
T3ΔP
T1T1 T4 T5 T6
T3-I
T1-I
FLT90
Flow meter Thermocouples
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Secondary Side Steady State Conditions: water @ 335ºC at SGBT inlet and @172 bar at SGBT
outlet, water mass flow rate 0.33 kg/s.
Secondary system composed of:
• a demineraliser;
• an alternative pump with an
accumulator and a check valve;
• a helical heating system (HEATER)
• a MANIFOLD with seven outlet ½''
tubes connected to the BTs of SGBT;
• a 3'' discharge line equipped with a
regulation valve V3, operated for
maintaining upstream about 172 bar;
• a 3/4'' bypass line equipped with the
regulation valve V2;
• a helium line, for pressurizing the
outer gap of bayonet tubes at about
10 bar.
V1
V2
V3
HEATER
MANIFOLD
BT INLETS
HELIUM
CHAMBER
STEAM
CHAMBER
Feedwater Inlet
Steam Outlet
Inlet
Outlet
CIRCE-HERO LAYOUT
CIRCE-HERO Secondary Side
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TEST #1 description
Parameter Unit Before Transient After Transient
FPS Power [kW] 352 20
Argon Flow Rate [Nl/s] 2.75 0
H2O mass flow rate [kg/s] 0.274 0.095
H2O T inlet SG [°C] ~336 ~336
IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
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PLOFA scenario is reproduced
• FPS power according to a characteristic heat decay curve,
• Loss of the primary pumping system simulated by reducing the
argon flow rate from 2.75 Nl/s to 0 in 10 s
• Loss of the primary heat sink simulated reducing the SG
feedwater to 30% of the nominal value in 2 s
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0
1
2
3
4
0
100
200
300
400
0 5 10 15 20 25 30
Flo
w R
ate
[Nl/
s]
Pow
er [
kW]
Time [min]
FPS Power Argon Flow Rate
0
1000
2000
3000
4000
5000
0 5 10 15 20 25 30
Flo
w R
ate
[cc/
min
]
Time [min]
TFM-T4 TFM-T5 TFM-T6
IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
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0
10
20
30
40
50
0 5 10 15 20 25 30
Mas
s Fl
ow R
ate
[kg/
s]
Time [min]
LBE Mass Flow Rate
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• LBE mass flow rate initial value ~34 kg/s subjected to a sudden
decrease due to the argon flow rate reduction
• minimum of 2 kg/s immediately after the gas transition
• final value of about 6 kg/s when the Natural Circulation (NC) regime is
established
PLOFA EXPERIMENT
Experimental Results
400
430
460
490
520
0 5 10 15 20 25 30
Tem
per
atu
re [ C
]
Time [min]
T-FPS-31 (inlet) T-FPS-32 (inlet)T-FPS-33 (inlet) T-FPS-37 (outlet)T-FPS-38 (outlet) T-FPS-39 (outlet)
430
460
490
520
550
0 5 10 15 20 25 30
Tem
per
atu
re [ C
]
Time [min]
T-FPS-16 T-FPS-18 T-FPS-19
T-FPS-20 T-FPS-22
PLOFA EXPERIMENT
Experimental Results
FPS Temperature
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The LBE in the top part of the riser and
inside the separator does not suffer
immediately the effects of the transient, due
to the sudden reduction of the LBE mass
flow rate, which delays the rise of the
coolant, and its temperature decreases
slowly.
This results in an inversion of the
temperatures in the rising leg, in which the
LBE on the top remains hotter than the
coolant flowing up from the FPS.
320
340
360
380
400
420
440
460
0 5 10 15 20 25 30
Tem
pera
ture
[ C
]
Time [min]
TC-T0-I TC-T1-I TC-T2-I TC-T3-I
TC-T4-I TC-T5-I TC-T6-I TC-C0-070
TC-C1-070 TC-C3-070 TC-C4-070
360
380
400
420
440
460
480
500
0 5 10 15 20 25 30
Tem
pera
ture
[ C
]
Time [min]
TC-SG-01 (inlet) TC-SG-02 (inlet)TC-SG-03 (inlet) TC-01-L00 (outlet)TC-07-L00 (outlet) TC-09-L00 (outlet)
LBE, inlet and outlet
320
340
360
380
400
420
440
460
0 5 10 15 20 25 30
Tem
pera
ture
[ C
]
Time [min]
TC-T0-I TC-T1-I TC-T2-I TC-T3-I
TC-T4-I TC-T5-I TC-T6-I TC-C0-070
TC-C1-070 TC-C3-070 TC-C4-070
360
380
400
420
440
460
480
500
0 5 10 15 20 25 30
Tem
pera
ture
[ C
]
Time [min]
TC-SG-01 (inlet) TC-SG-02 (inlet)TC-SG-03 (inlet) TC-01-L00 (outlet)TC-07-L00 (outlet) TC-09-L00 (outlet)
SGBTs temperatures
IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
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320
340
360
380
400
420
440
460
0 5 10 15 20 25 30
Tem
pera
ture
[ C
]
Time [min]
TC-T0-I TC-T1-I TC-T2-I TC-T3-I
TC-T4-I TC-T5-I TC-T6-I TC-C0-070
TC-C1-070 TC-C3-070 TC-C4-070
360
380
400
420
440
460
480
500
0 5 10 15 20 25 30
Tem
pera
ture
[ C
]
Time [min]
TC-SG-01 (inlet) TC-SG-02 (inlet)TC-SG-03 (inlet) TC-01-L00 (outlet)TC-07-L00 (outlet) TC-09-L00 (outlet)
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Water, inlet and outlet
LBE, inlet and outlet
PLOFA EXPERIMENT
Experimental Results
400
420
440
460
480
500
0 1200 2400 3600 4800 6000 7200
Tem
per
ature
[ C
]
Length [mm]
Before Transient
After Transient
Thermal stratification
IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
1426/09/2019
The relevant stratification phenomenon occurs at the SG outlet level. This
is due to the heat losses between the hot leg and the main pool that warms
the upper part of the pool. Downstream the SG outlet, the cold fluid exiting
the heat exchanger cools the lower pool, causing the characteristic thermal
stratification
RELAP5-3D MODELLING (1)
Correlations:
• Ushakov* for HTC evaluation in
bundle geometries
• Seban-Shimazaki for HTC
evaluation in non-bundle geometries
• Rehme for local pressure drop
coefficients Re-dependent
The nodalization scheme has been developed using RELAP5-3D© ver. 4.3.4 (R5-3D)
1D MODELMULTI-D COMPONENTMono-dimensional model:
• Primary flow path
• Sub-channel analysis of the FPS
• SGBTs secondary side
MULTI DIMENSIONAL
COMPONENT:
• CIRCE pool
• Calibrated porosity factors
• 3D momentum equations
+
26/09/2019IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
QUANTITY Value
HYDR volumes 3594
HYDR junctions 8322
HEAT structures mesh points 24263
15
RELAP5-3D MODELLING (2)
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• 72 parallel pipes divided into 15 control volumes
• 1536 cross junctions to reproduce mass transfer
between adjacent sub-channels
• 5760 heat structure active nodes suppling the
thermal power to the sub-channels
• 1728 heat structure passive nodes simulating the
heat losses through the hexagonal shell
• 3456 heat structure passive nodes, assuming a
“fake” material with negligible heat capacity and
LBE thermal conductivity, to simulate the heat
conduction through adjacent sub-channels
• Calibrated fouling factor is applied to the HTC of
the active heat structure to correct Westinghouse
correlation according with Ushakov correlation
FPS SUB-CHANNEL ANALYSIS
• FPS is equipped with several TCs to measured the LBE temperature across the HS.
• The model is obtained to compare the temperature in the exact position of the TCs.
The grids are simulated with pressure loss coefficients, dependent on the flow
conditions and evaluated with Rheme correlation.
26/09/2019IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
Full power calculation: main results
IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
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Parameter Unit Experiment Uncertainty R5-3D Error
LBE MFR kg/s 34.0 10 - 25% 31.7 -6.7%
Av. FPS inlet T K 420.0 2.0 418.4 -1.6
Av. FPS outlet T K 493.5 2.0 495.0 1.5
Av- SG inlet T K 480.0 5.0 485.1 5.1
Av. SG outlet T K 403.7 8.0 413.9 10.2
TFM-T4 kg/s 0.036 0.0044 0.039 0.003
TFM-T5 kg/s 0.033 0.0044 0.039 0.006
TFM-T6 kg/s 0.035 0.0044 0.034 -0.001
TC-C0-O70 K 387.9 2.0 387.9 0.0
TC-C1-O70 K 353.0 2.0 353.9 0.9
TC-C3-O70 K 376.1 2.0 366.1 -10.0
TC-C4-O70 K 365.4 2.0 366.1 0.7
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RELAP5-3D POST-TEST ANALYSIS
Simulation Results
• SHORT TERM:
o Good matching between experiment and
calculation
o Delay of the MFR decrease at SG inlet
• LONG TERM:
• good prediction of the natural circulation
with a little underprediction in the central
part of the test
• SHORT TERM:
• matching of the prompt temperature
decrease (Tmin = 439 °C)
• 100 ≤ t ≤ 110 s: small obsillations in
reverse flow → Tpeak at FPS inlet (not
clearly acquired by TCs) and quick T
increase at the outlet (good prediction
of the Tmax)
• LONG TERM: slight error prediction in Tout
LBE mass flow rate FPS temperature
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Type”, Milan, June 24-27,2019
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FPS
temperatures
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Type”, Milan, June 24-27,2019
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RELAP5-3D POST-TEST ANALYSIS
SGBTs temperatures
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• 0 ≤ t ≤ 100 s: good prediction by R5-3D
• 100 s ≤ t ≤ END:
o ΔT overestimation by R5-3D
o Uncertainties related to powder performances
• 0 ≤ t ≤ 100 s: good prediction by R5-3D
• 100 s ≤ t ≤ END:
o ΔT overestimation by R5-3D
o Uncertainties related to powder performances
LBE temperature Steam outlet temperature
Pool thermal stratification
IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
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SOT conditions (0s)
EOT conditions (1800s)
Conclusion
26/09/2019IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
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• The CIRCE-HERO PLOFA experiment #1 provided a useful data for the
analysis in support to the HLM safety demonstration and for the
validation of the TH transient analysis codes.
• The comparison of the experimental data and the numerical results
(obtained with R5-3D) make know a good agreement.
• Multi-dimensional component offers a very fine prediction of the thermal
stratification inside the pool with a large part of the values within the
experimental error bars
• The prediction in natural circulation is good for the mass flow rate and
the FPS inlet and outlet temperatures, but in this test is present an
overestimation of the temperatures in the HERO TS both in the primary
and secondary side in the central part of the transient, with a good long-
term prediction. This needs additional analysis to investigate the HERO
behavior at low mass flow rate for the secondary side
26/09/2019IAEA TM on “Benefits and Challenges of Fast Reactors of the SMR
Type”, Milan, June 24-27,2019
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THANK YOU
FOR
YOUR ATTENTION