Safety Issues for High Temperature Gas...
Transcript of Safety Issues for High Temperature Gas...
Safety Issues for High Temperature Gas Reactors
Andrew C. KadakProfessor of the Practice
Major Questions That NeedGood Technical Answers
• Fuel Performance– Normal operational performance– Transient performance
• Ejected Rod (maximum energy insertion capability)• Reactivity insertions (seismic, water)
– Accident Performance– Weak fuel issues– Mechanistic source term for high burn-up fuel– Fuel fabrication quality assurance
• Risk Dominant Accident Sequences– Establish risk informed design to identify risk
dominant accident sequences to be analyzed.– Use either IAEA1 or NRC2 risk informed
approach to establish safety requirements of plant.
– Use of safety goal as a design guide– Application of risk informed “Defense in
Depth”– Scope of risk analysis may be easier due to
inherent robustness of basic design.1. “Development of Technology Neutral Safety Requirements for Innovative Reactors”, IAEA
TECDOC Draft Dec. 20042. “Regulatory Structure for New Plant Licensing, Part 1: Technology Neutral Framework, Dec.
2004, Draft, US NRC.
Consequences
FInitiating Event/Y
Lev. 1Lev. 2
Lev. 3
Lev. 4
Lev. 5
10-2
10-6
10-7
Failure of Level 1Initiating Event
Minimal emergencyactions beyonddefined distancefrom the plant
No off-site actionsbeyond defineddistance from theplant
Off-site Actions
NOTE 2: Dosesare derived fromIAEA-SS No 115
5 mSv/a(For 1 year periodfollowing the accident)
5 mSv/a(For 1 year periodfollowing the accident)
5 mSv/a1 mSv/a (average 5 y)
1 mSv/a(10 µ Sv/a–target)
Doses to thepublic
NOTE 1: Dosesfor NO, AOO, ACare derived fromIAEA-SS No 115
500 mSv (limit)(This value derivedfrom Finnishregulation)
50mSv/a (Could beexceeded for rearrecovery events)
50 mSv/a20 mSv/a (average 5 y)(5 mSv/a target)
50 mSv/aALARA(5 mSv/a target)
Doses toOperators
Severe plantconditions* (SSPC)
Accident conditions(AC)
AnticipatedOperationalOccurrences (AOO)
NormalOperations(NO)
Plant conditions
Consequences
AOO
AC
SPC
Challenges
DESIGN BASIS
* Severe challenge to the Fission Products Confinement Function
Risk Informed Safety Profile
LEVELS OF DEFENCE IN DEPTH (From INSAG-10)
Control, limiting and protection systemsLevel 2 Control of deviations from normal operation and detection of failures and other surveillance features
ObjectiveLevels ofdefence
Essential means
Level 1 Prevention of deviations from normal operation and failures
Conservative design and high quality inconstruction and operation
Level 3 Control of accident conditionswithin the design basis
Engineered safety features and accidentprocedures
Level 4 Control of severe plant conditions Complementary measures and accidentmanagement
Level 5 Mitigation of radiological consequencesof significant releases of radioactivematerials
Off-site emergency response
Acceptablefailures of the
Level of Defence(events/year)
< 10-2
10-2- 10-6
10-6- 10-7
< 10-7
• Expected Significant Accident Sequences– Air Ingress– Water Ingress (reactivity insertion)– Seismic Events (reactivity insertion)– Loss of Load– Rod Ejection (more significant in block reactors)– Failure of reactor cavity cooling system– Recuperator By-pass events (overcooling)– Graphite dust, plate-out, lift off– Impact of Terrorism– Identification of “cliff edge” effects
Knowledge Required• Improved understanding of core behavior • Improved understanding of heat transfer in core and vessel
- pebble and block - bypass flows• Materials behavior at high temperature in helium (plus
contaminants) including radiation effects and chemical attack on graphite
• Blow down loads and timing of accident event sequences.• Behavior of fuel, fission product release behavior in
reactor building and structures under accident conditions.• Development and validation of computer codes used in the
analysis• Validation of passive performance of safety systems -
natural circulation - heat conduction and convection.
Issues
• Fuel Temperature limits (1600 C ?)• Regulatory Credit for Basic Design
Strengths • Need new risk informed licensing process
to allow credit for innovative systems.
Containment • Based on design and accident analysis of source
term and sequences - a containment of radioactive materials strategy is developed to assure that safety goals are met.– Full pressure containment– Confinement - low pressure - not pressure tight– Dynamic containment/confinement (time
dependent)– Performance is quite different than water
reactors.
Classification of Safety “Systems”
• Ideally safety system classification should be done on importance to safety function in a risk informed manner.
• Some “systems” are not components but parameters in analysis for passive performance (ex. emissivity of reactor vessel).
Expectations• Water Ingress - generally understood and can be
limited by amount of water ingress - some German experience at AVR
• Seismic - reactivity simulations can assess reactivity impact.
• Rod ejection - more significant for block reactors but fuel energy limits like for LWRs can be established for rod worths.
• Testing on heat transfer and flow can be verified by South African tests and Chinese pebble bed reactor including reactor cavity cooling systems.
• Fuel behavior data to be provided by past German and focused South African and US testing programs
Challenges• Verification of high temperature material
behavior (fuel, graphite, metals, carbides)• Validation of analysis tools• Air ingress
– Most visible concern among the public– Most significant in terms of potential offsite
consequences– Can not be eliminated by “design”
Air Ingress Status• Most “eliminate” connecting “vessel”
failure as too low a probability event (10-8).• Break sizes limited to largest connecting
“pipe”.• Two breaks (top and bottom) considered
unlikely but are analyzed (chimney effect)• Graphite corrosion behavior not well
modeled in existing codes.• CFD analysis and confirmatory experiments
needed.
Air Ingress Tests
• Japanese series on prismatic configuration– Diffusion– Natural Circulation– Corrosion (multi-component)
• German NACOK tests - pebble bed– Natural circulation– Corrosion
• MIT CFD (Fluent Methodology Development)
Experimental Apparatus - Japanese
C4
270
Nitrogen
Helium
Valves
C3
C1
C2
H4
H3
H2
H1
Figure 16: Apparatus for Isothermal andNon-Isothermal experiments
Figure 17: Structured mesh
Isothermal Experiment
0.00
0.20
0.40
0.60
0.80
0 50 100 150 200 250 300Time (min)
Mol
e fra
ctio
n
H-1 & C-1(Calculation)H-2 & C2 (Calculation)H-3 & C3 (Calculation)H-4 & C4 (Calculation)H-1 & C-1(Experiment)H-2 & C2 (Experiment)H-3 & C3 (Experiment)H-4 & C4 (Experiment)
Figure 18: Mole fraction of N2 for the isothermal experiment
Thermal Experiment
Figure 19: The contour of the temperature bound4ary condition
Pure Helium in top pipe,
pure Nitrogen in the
bottom tank
N2 Mole fractions are
monitored in 8 points• Hot leg heated• Diffusion Coefficients as a
function of temperature
Thermal Experiment
0
0.2
0.4
0.6
0.8
1
0 50 100 150 200
Time (min)
Mol
e fra
ctio
n of
N2
H-1(FLUENT)C-1(FLUENT)H-1(Experiment)C-1(Experiment)
Figure 20: Comparison of mole fraction of N2 at Positions H-1 and C-1
0
0.2
0.4
0.6
0.8
1
0 50 100 150 200
Time(min)
Mol
e Fr
actio
n
H2(Experiment)C2(Experiment)H-2(FLUENT)C-2(FLUENT)
Figure 21: Comparison of mole fraction of N2 at Positions H-2 and C-2
Thermal Experiment (Cont.)
0
0.2
0.4
0.6
0.8
1
0 50 100 150 200 250
Time(min)
Mol
e Fr
actio
n of
N2
H4(Exp)C4(Exp)
H-4(Calc)C-4(Calc)
Figure 22: Comparison of mole fraction of N2 at Positions H-1 and C-1
-0.15
-0.10
-0.05
0.00
0.05
0.10
0.15
0.20
0.25
0 2 4 6
Time (Second)
Velo
city
(m/s
econ
d)
Figure 23: The vibration after the opening of the valves.
Multi-Component Experiment
2
1
3
4
Heated Graphite
Air
Helium
Graphite InsertedMultiple gases: O2, CO, CO2, N2, He, H2OMole fraction at 3 points are measuredMuch higher calculation requirementsDiffusion Coefficients
Figure 34: Apparatus for multi-Component experiment of JAERI
Multi-Component Experiment(Cont.)
0.00
0.03
0.06
0.09
0.12
0.15
0.18
0.21
0 20 40 60 80 100 120 140
Time(min)
Mol
e Fr
actio
n
O2(Experiment)O2(Calculation)CO(Experiment)CO(Calculation)CO2(Experiment)CO2(Calculation)
Figure 36: Mole Fraction at Point-1 (80% Diffusion Coff.)
Multi-Component Experiment(Cont.)
Figure 37: Mole Fraction at Point-3
0.00
0.04
0.08
0.12
0.16
0.20
0.24
0 20 40 60 80 100 120 140Time(min)
Mol
e Fr
actio
n
O2(Experiment)O2(Calculation)CO(Experiment)CO(Calculation)
CO2(Experiment)CO2(Calculation)
Multi-Component Experiment(Cont.)
Figure 38: Mole Fraction at Point-4
0.00
0.05
0.10
0.15
0.20
0.25
0 20 40 60 80 100 120 140Time (min)
Mol
e Fr
actio
n
O2(Experiment)O2(Calculation)CO(Experiment)CO(Calculation)CO2(Experiment)CO2(Calculation)
NACOK Natural Convection Experiments
Figure 39: NACOK Experiment
Boundary Conditions
Figure 41: Temperature Profile for one experiment
The Mass Flow Rates
Figure 42: Mass Flow Rates for the NACOK Experiment
0.0E+00
1.0E-03
2.0E-03
3.0E-03
4.0E-03
100 300 500 700 900 1100
Temperature of the Pebble Bed (C)
Mas
s Fl
ow R
ate
(kg/
s
5.0E-03
)
T_R=200 DC(Exp.)T_R=400 DC(Exp.)T_R=600 DC(Exp.)T_R=800 DC(Exp.)T_R=200 DC(FLUENT)T_R=400 DC(FLUENT)T_R=600 DC(FLUENT)T_R=800 DC(FLUENT)
Future NACOK Tests
• Blind Benchmark using MIT methodology to reproduce recent tests.
• Update models• Expectation to have a validated model to be
used with system codes such as RELAP and INL Melcor.
Air Ingress Mitigation
• Air ingress mitigation strategies need to be developed– Realistic understanding of failures and repairs– Must be integrated with “containment” strategy
to limit air ingress– Short and long term solution needed
Overall Safety Performance Demonstration and Validation
• China’s HTR-10 provides an excellent test bed for validation of fundamentals of reactor performance and safety.
• Japan’s HTTR provides a similar platform for block reactors.
• Germany’s NACOK facility vital for understanding of air ingress events for both types.
• PBMR’s Helium Test Facility, Heat Transfer Test Facility, Fuel Irradiation Tests, PCU Test Model.
• Needed - open sharing of important technical details to allow for validation and common understanding.
Chinese HTR-10 Safety Demonstration
• Loss of flow test– Shut off circulator– Restrict Control Rods from Shutting down
reactor– Isolate Steam Generator - no direct core heat
removal only but vessel conduction to reactor cavity
Video of Similar Test
Loss of Cooling Test
Power
Loss of Cooling Test
Power
Summary• Safety advantages of High Temperature
Reactors are a significant advantage.• Air ingress most challenging to address• Fuel performance needs to be demonstrated in
operational, transient and accident conditions.• Validation of analysis codes is important• Materials issues may limit maximum operating
temperatures and lifetimes of some components.
• International cooperation is essential on key safety issues.