lbe-water interaction in lifus v facility under different operating conditions
DESCRIPTION
LBE-Water interaction in LIFUS V facility under different operating conditions. A. Ciampichetti, D. Bernardi - ENEA T. Cadiou - CEA N. Forgione – Università di Pisa D. Pellini - KIT International DEMETRA Workshop Berlin, March 4th, 2010. Introduction. - PowerPoint PPT PresentationTRANSCRIPT
LBE-Water interaction in LIFUS V facility under different operating
conditions
A. Ciampichetti, D. Bernardi - ENEAT. Cadiou - CEAN. Forgione – Università di PisaD. Pellini - KIT
International DEMETRA WorkshopBerlin, March 4th, 2010
Introduction
The XT-ADS and EFIT reactors’ heat exchangers / steam generator modules are designed to be placed in direct contact with the heavy liquid metal in the main vessel. Since the likelihood of a pipe break is not negligible, the interaction between the secondary coolant and LBE represents an important concern for such a configuration. In fact, the consequences might have a strong impact on safety, design and maintenance of these reactors.
Consequences• The peculiarities of the heavy liquid metals (such as high thermal conductivity,
high density and low surface tension) determine their gift to interact with water energetically, thus producing vapour at high pressure.
• The interaction leads to pressures waves propagation which might damage the surrounding structures, causing an escalation of the accident.
• The seriousness of the consequences is determined by the injection pressure and flow rate, the vapour production rate and the intervention of safeguards.
Description of work
An experimental study focused on LBE/water interaction aimed at assessing physical effects and possible consequences relating to this kind of interaction has been performing in ENEA through LIFUS 5 plant. The main parameters for carrying out the experiments have been selected taking into account the XT-ADS primary heat exchanger design and the indications obtained from the pre-test activity performed with SIMMER code.
The parameters considered have been:- system geometry;- lead temperature;- temperature and pressure of the water The modelling activity with SIMMER code have been performing in CEA and
University of Pisa.
LIFUS 5 Facility
The main LIFUS 5 components are:• the reaction vessel S1, containing at the bottom the water injection device. Its
volume is 100 l• the expansion vessel S5, connected to S1 through four tubes. Its volume is 10 l• the pressurised water vessel S2 • the safety vessel S3• the liquid metal storage vessel S4• Instrumentation: S1 is equipped with water-cooled high precision piezometric
pressure transducers, which allow to achieve very low time constants. A number of K-type thermocouples are also present. A fast DAQ system with a dedicated software acquires the main test parameters in different positions of the system.
LIFUS 5 has been designed to simulate LOCA accidents and to operate in a wide range of conditions (pressure up to 200 bar, initial LM temperature up to 500 °C)
LIFUS 5 Facility
Experimental campaigns
Three experimental campaigns for DEMETRA have been completed and the last one will be completed in March 2010.
Test n.1 Test n.2 Test ELSY Test n.3 Test n.4
LBE temperature 350 °C 350 °C 400 °C 350 °C 350 °C
Water injection pressure
70 bar 6 bar 185 bar 40 bar 40 bar
Water temperature 235 °C 130 °C 300 °C 235 °C 235 °C
Free volume/ LBE volume
5% 20% 20% S1 completely
filled 20%
Water injector device penetration
in the melt 80 mm 80 mm 5 mm 5 mm 5 mm
Reaction system Initial one Modifications on S5 and WI
Possibility to discharge in S3
Possibility to discharge in S3
Possibility to discharge in S3
Time schedule Completed Completed Completed Completed March 2010
Test n.1: experimental results
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Time [ms]
Pre
ssu
re [
bar
]
Pressure evolutions in the
reaction-expansion vessel
First phase: the pressure reaches a maximum of about 65 bar.Second phase: pressure decreases in S1 because of the free flow of gases into S5 is not balanced by an equivalent injection of water.Third phase: there is a further pressure increase in both S1 and S5 due to the further water vaporization. A maximum value of about 80 bar has been reached.Fourth phase: pressure become stable at 70 bar due to the reverse flow-rate.
• Liquid metal temperature: 350 °C
• Water injection pressure: 70 bar
• Water temperature: 235 °C (sub-cooling of 50 °C)
• Test performed with the expansion vessel S5
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360
0 500 1000 1500 2000 2500 3000 3500 4000
Time [ms]
Tem
per
atu
re [
°C]
Top
Middle
Bottom
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300
320
340
360
0 1000 2000 3000 4000 5000 6000 7000 8000
Time [ms]
Tem
pera
ture
[°C
]
Test n.1: modelling
SIMMER model of LIFUS5
March 5, 9 2007 9Forschungszentrum Karlsruhe
SIMMER results (pressure)
Pressure à t=0.2 sInitial state
Reaction vessel
Expansion tube
March 5, 9 2007 10Forschungszentrum Karlsruhe
SIMMER results (Pressure)
Pressure à t=0.5 sPressure à t=0.4 s
Pressure evolutions in the interaction vessel (S1) and expansion vessel (S5)
June 21, 22 2006 6ROSSENDORF
Expansion volume
Interaction tank
J = 1,64
Expansion vessel
Expansion tubes
connected to the different
zones
U tubes bundle
Injector
I = 1, 20Boundary conditions at inlet injector Porous wall
LIFUS modeling with SIMMER
S1
S5
Test n.2: experimental results
Pressure evolution detected in gas phase followed the same trend as in LBE but the first sharp peak was not present.
• Liquid metal temperature: 350 °C
• Water injection pressure: 6 bar
• Water temperature: 130 °C (sub-cooling of 28 °C)
• Test performed without the expansion vessel S5
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7
0 500 1000 1500 2000 2500 3000 3500 4000
Time [ms]
Pre
ssu
re [
bar]
LM
Gas
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400
0 1000 2000 3000 4000 5000 6000 7000 8000
Time [ms]
Tem
per
atu
re [
°C] Top
Middle
Bottom
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350
0 2000 4000 6000 8000 10000 12000 14000 16000
Time [ms]
Te
mp
era
ture
[°C
]
TC10
TC11
Tc12
Temperature evolution detected in three vertical positions.
Test n.2: modelling /1
Test n.2: modelling /2
SIMMER III domains developed by PISA University
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2.0E+05
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6.0E+05
8.0E+05
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0 2 4 6 8 10Time [s]
Pre
ssu
re [
Pa]
CM1
CM2
Experimental
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2.0E+05
4.0E+05
6.0E+05
8.0E+05
1.0E+06
0 2 4 6 8 10Time [s]
Pre
ssu
re [
Pa]
CM1
CM2
Experimental
Comparison between SIMMER simulations and
experimental results
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360
0 2 4 6 8 10Time [s]
Tem
per
atu
re [°
C]
TC18 Bottom- tube n.3
CM2
Pressure evolution
Temperature evolution
University of Pisa
Experimental and SIMMER results of Test n.2 were used to support the assessment of the accidental scenario of “heat exchanger tube rupture” considered as reference accident in the safety analysis of the ICE activity.
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7
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Time [ms]
Pre
ssur
e [b
ar]
LM
Gas
Test n.2: experimental results
SIMMER domain for Test n.2
Safety activity for ICE /1
ICE simulations with SIMMER have shown that a double rupture of a HX tube produces a fast pressurisation of CIRCE main vessel that strongly overcomes the design value.
Double breakage - Argon Zone
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4.0E+05
6.0E+05
8.0E+05
1.0E+06
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0 2 4 6 8 10Time [s]
Pres
sure
[Pa
]
Injection depht : 900 mm
Injection depht : 450 mm
Injection depht : 100 mm
Double Rupture – Argon RegionDouble breakage - Argon Zone
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0 2 4 6 8 10Time [s]
Pres
sure
[Pa
]
Injection depht : 900 mm
Injection depht : 450 mm
Injection depht : 100 mm
Double Rupture – Argon Region
ICE design team has
developed another
solution for the HX
based on the adoption
of water at 1 bar and
double wall tubes
Dead volume
Cylindricalskirt
Dead volume
Cylindricalskirt
Primary coolant Heat Exchanger
(old solution)
Heat Exchanger
(new solution)
Fluid LBE Water Boiling Water
Temperature
in-out 400 – 300 °C 115 – 150 °C 60°C – 100°C
Pressure 1.2 bar (cover
gas) 6 bar
2.5 bar (liquid side)
1 bar (steam side)
Flow rate 55.2 kg/s 5.5 kg/s 0.6-0.8 kg/s
Velocity 0.2 m/s 1.3 m/s 0.5 m/s (liquid)
Material T91 AISI 304
Tubes
- Triangular assembly - “U” shape - Diameter and thickness: 26.7 / 2.9 - Length: 895 mm - Number: 13
- Bayonet double wall (helium gap)
- Diameter 1”, ¾”, ½” - Length: 5000 mm - Number: 91
Safety activity for ICE /2University of
Pisa
In order to simulate the possibility to discharge the vapour/liquid metal mixture outside the steam generator module during a tube rupture accident, the reaction system of Lifus5 facility has been modified. A discharge line directly connecting the reaction vessel S1 with the safety vessel S3 has been designed and constructed.
Modification of LIFUS5
S2
LIFUS5: old and new configuration
Test n.3: experimental results /1
Pressure evolution detected by the different transducers placed in S1
• Liquid metal temperature: 350 °C
• Water injection pressure: 40 bar
• Water temperature: 235 °C (sub-cooling of 15 °C)
• Possibility to discharge in S3
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25
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Time [ms]
Pre
ss
ure
[b
ar]
PT in S1
Test n.3: experimental results /2
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5
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15
20
25
0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000
Time [ms]
Pre
ss
ure
[b
ar]
PT in the flange of S1
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5
10
15
20
25
0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000
Time [ms]
Pre
ssu
re [
ba
r]
PT close to the water injector
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0 1000 2000 3000 4000 5000 6000 7000 8000 9000
Time [ms]
Tem
per
atu
re [
°C]
Top
Middle
Bottom
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0 500 1000 1500 2000 2500 3000 3500 4000 4500 5000
Time [ms]
Tem
per
atu
re [
°C]
TC closest to the water injector
TC in the discharge line
Pressure
Temperature
PT close to the water injector PT in the flange of S1
TCs in front of the water injector
Features of the domainSimplified geometry: cylindrical coordinates (r-z) with 30 radial and 39 axial meshes.In LIFUS 5 there is a strong asymmetry in the geometry
Assumptions1. The overall volume of the main elements is
conserved 2. The injector and vent pipe are placed coaxially
with the reaction vessel S13. The flow area of the various pipes is conserved
Test n.3: modelling /1
In the reaction vessel S1, U tubes are represented by 12 “no calculation” regions
The strong asymmetry due to U tube shape and position cannot be adequately accounted for
U tubes are simulated through annular elements which conserve the overall volume
SIMMER III Model (2D): GeometrySIMMER III Model (2D): Geometry
University of Pisa
Test n.3: modelling /2
Comparison between calculated and experimental pressure in S1 vessel
SIMMER III overestimates the maximum value of the pressure in the reaction vessel S1 even though the trend is in agreement especially for the pressurization
0.0
0.5
1.0
1.5
2.0
2.5
0.0 0.5 1.0 1.5 2.0 2.5 3.0
Time [s]
Pres
sure
[MPa
]
Experimental
SIMMER III calculations
Comparison between calculated and experimental
temperature in LBE region: top thermocouple
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Time [s]
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ture
[°C
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Experimental
SIMMER III calculations
University of Pisa
SIMMER IV Model (3D): GeometrySIMMER IV Model (3D): Geometry
• 3-D model of LIFUS 5 facility performed with SIMMER IV code
• Simplified geometry: Cartesian coordinates (x-y-z) with 20 meshes along x, 15 along y and 18 along z
• The correct position of the water injector and of the vent tube is preserved
Test n.3: modelling /3 University of Pisa
Test n.3: modelling /4
The 3D version of the code is able to evaluate the first pressure peak associated with the impact between the water jet and the “rigid surface” of the liquid metal.
A better agreement concerning the maximum values reached with respect to SIMMER III results even though some discrepancies still remain.
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Time [s]
Pres
sure
[M
Pa]
Experimental
SIMMER IV calculations
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2.5
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Time [s]
Pres
sure
[MPa
]
ExperimentalSIMMER III calculationsSIMMER IV calculations
University of Pisa
Test n.3: modelling /5
TestTotal mass of injected water
[kg]
SIMMER III 1.66
SIMMER IV 1.13
Experimental data 1.60
Mass Flow Rate: Comparison between SIMMER III and SIMMER IV calculation results
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Time [s]
Mas
s Fl
ow R
ate
[kg/
s]
SIMMER III calculations
SIMMER IV calculations
University of Pisa
Possible consequences
The pressure evolution detected during Test n.3 has shown a first sharp peak and a following slower pressurisation of the system. In reactor scale the latter event can be avoided using adequate countermeasures (e.g. rupture disks, stop and check valves on the steam generator tubes). The first sharp peak reached about 15 bar in the pressure transducer closest to the water injector and smaller values in the other pressure sensors. This peak is originated from the impact of the water jet on the liquid metal and it could be a threat for the integrity of the surrounding tubes. Further tests are necessary to investigate this issue.
Conclusions
Experimental results concerning the simulation of water large leaks in LBE have been obtained under different operating conditions. Maximum pressure values higher than the water injection pressure have been detected during Test n.1 and 2.
The experimental results provided helpful data to prove the capability of the SIMMER code to simulate such an accident. SIMMER III was able to reproduce the interaction between a water jet and LBE, even though the 2D feature of the code has represented a limitation in reproducing the LIFUS 5 results. A new activity with SIMMER IV (3D) has been recently launched and is giving promising results.
Test n.2 was used to support the safety analysis of ICE. In this case simulations showed that a double rupture in the LBE–pressurized water shell heat exchanger leads to a fast pressurisation of CIRCE main vessel that strongly overcomes the design value. Considering this warning, the ICE design team has adopted another solution with water at atmospheric pressure.
LIFUS 5 has been modified in order to simulate the possibility of discharging the vapour/liquid metal mixture outside the steam generator module during a tube rupture accident as it might happen in lead cooled reactors. After that, Test n.3 was carried out in the operating conditions fixed for the heat exchanger of XT-ADS.
Test n.3 has shown a first sharp pressure peak and a following slower pressurisation of the system. In reactor scale, the first peak could be dangerous for the surrounding structures while the following pressurisation can be avoided with adequate safeguards.