turmet - vtt.fi puoliväliseminaari... · 27.10.2017 3 turmet: a change in scope §the funding for...
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TEKNOLOGIAN TUTKIMUSKESKUS VTT OY
TURMETTurvallisuusperustelun metodiikansystematisointi
KYT2018 Puoliväliseminaari 7.4.2017Suvi Karvonen
227.10.2017 2
TURMET – Systemizing Safety Case Methodology
§ Safety Case is the basis and documentation of the safety of thechosen repository design§ In practice Safety Case often evolves through several iterations
and in tandem with the design, instead of guiding it§ Many components of the Safety Case commonly aren’t derived in
a systematic manner when they perhaps could be§ The original idea of TURMET was to answer this question of how
to create a Safety Case “from scratch”§ Most focus was on using mathematical analysis to create a tool for
scenario analysis and selection
327.10.2017 3
TURMET: A Change in Scope
§ The funding for most KYT projects was significanly cut for thefirst two years of the programme, including TURMET: theoriginal scope of the project became impossible to achieve§ Feedback from the programme had consistently been that the
most interesting part of the project was our scenario analysismodel§ It was decided to focus on scenario analysing while the
oroginally planned systemic approach to safety casemethodology had to be cut§ As a result TURMET has been focusing on scenario analysis in
2016-2017
427.10.2017 4
TURMET – Systemizing Safety Case Methodology
§ Website: http://www.vtt.fi/sites/turmet§ 2015 – Literature reviews & concept model
§ Literature Review on Safety Case & Scenario Analysis§ Scenario Analysis and the Conceptual Model
§ 2016 – more focus on Scenario Analysis§ Development of the scenario model§ Publication to be submitted to Risk Analysis
§ 2017§ Finishing scenario model§ Expert judgement tools
§ 2018§ Analysis of scenario model results§ Safety Case methodology
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Literature Review on Safety Case
§ Topics§ Safety Case definition, requirements and purpose§ Examples of Safety Cases§ Practical experiences of Safety Case through interviews and
published reports§ Authors: Suvi Karvonen and Jutta Peura, VTT
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Literature review on Scenario Analysis
§ Scenario Analysis for theSafety Assessment of NuclearWaste Repositories§ Purposes and structure of the
review:§ Key characteristics of
Scenario Analysis§ Challenges in Scenario
Analysis§ Publication submitted to Risk
Analysis, under review
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A model for Scenario Analysis
§ A model for Scenario Analysis is under development, in order toaddress the following challenges:§ Build a System Model of the disposal system, in which to display
all FEPs and their interactions§ Ensure comprehensiveness - due to computation times,
laboratory costs etc. it is not practicable to analyze allscenarios - which scenarios to analyze for still coming toconclusions on safety§ Characterize epistemic uncertainties – e.g. giving Kd a
range or distribution instead of a single value in uncertaincases
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System Model
§ An Influence diagram displaysall FEPs and their interactions
§ A Bayesian network is themathematical model embeddedinto the Influence diagram
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Bayesian network: FEPs
§ FEPs are modeled as stochastic variables assuming discretestates§ Safety is assessed at the radiological consequence at the end of the
Bayesian network (e.g. Radionuclide discharge)
FEP u.m. StatesIce sheet km 0 0.5 2
Saline water upconing - None Medium Intense
Fracture displacement cm 0 5 300
Corrodants concentration g/l 0 35 70
Near-field flow l/y 0 100 1,000
Buffer flow l/y 0 100 1,000
Canister breach mm 0 1 950
Radionuclide discharge - Negligible Below limit Above limit
FEP u.m. StatesIce sheet km 0 0.5 2
Saline water upconing - None Medium Intense
Fracture displacement cm 0 5 300
Corrodants concentration g/l 0 35 70
Near-field flow l/y 0 100 1,000
Buffer flow l/y 0 100 1,000
Canister breach mm 0 1 950
Radionuclide discharge - Negligible Below limit Above limit
Radiologicalconsequence
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§ Interactions are modeled as conditional probabilities between aFEP and its predecessors§ Conditional probability tables (CPTs)
Fracturedisplacement
[cm]
Near-fieldflow[l/y]
Chlorideconcentration
[mm]
Buffer flow [l/y]
0 100 1,000
0 0 0 0.64 0.32 0.045 0 0 0.25 0.50 0.25
300 0 0 0.04 0.32 0.64. . . . . . . . . . . . . . . . . .0 0 35 0.93 0.06 05 0 35 0.66 0.31 0.03
. . . . . . . . . . . . . . . . . .5 1,000 70 0.25 0.50 0.25
300 1,000 70 0.04 0.32 0.64
Bayesian network: interactions
( )lg
Bshearyl
B ClqcmdqP 35,0,5100 ====
Sem
i-ran
dom
ly-g
ener
ated
data
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Bayesian network: scenarios
§ A scenario is a combination of FEP states
§ Specifically, a combination of states of allFEPs but the radiological consequence
§ Each scenario results in a differentprobability distribution over the states of theradiological consequence
§ The probability of large radiologicalconsequences can be calculated byaccounting for all the scenarios
§ Safety can be assessed by comparing thisprobability against a maximum acceptablelevel
( ) ( )[ ] ( )[ ]å ÕÎ Î
-- ×=Ss
s ssAk
rrlimitabove
kks
rlimitabove
vcvcpk
E.g. the probability ofunacceptable radionuclide
discharge is 49%
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Challenges in modeling the interactions
§ How to obtain the conditional probabilities, that is, how to fill in theconditional probability tables?§ Historical data, but also:
Experts’ beliefs+ Can be elicited in reasonable
times− Involve epistemic uncertainties
Radionuclide-transport code(model verification still ongoing)
Simulations+ Provide more precise predictions (initial
assumption: determinisitc)− Are resource-intensive (time, costs)
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Experts’ beliefs
§ For each FEP, multiple experts (e.g. three)§ Each expert provides his/her conditional probability table about the
FEP at hand§ For aggregating the beliefs, weight zik can be assigned to expert k at
FEP i§ Values of the weights should be fixed such that the estimated
probability of large consequences is the most conservative§ This is done through multilinear optimization (see next slide)
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Simulations
§ Each simulation provides a deterministic prediction§ Before any simulation is run, the conditional probability table is empty and the
probability of unacceptable radionuclide discharges is interval-valued§ Simulations are resource-intensive, calling for prioritization of simulations§ This is done through an iterative algorithm, selecting the next simulation
until a conclusive probability interval is obtained
Near-fieldflow [l/y]
Bufferflow [l/y]
Canisterbreach [mm]
Radionuclide discharge [-]
Negligible Belowlimit
Abovelimit
0 0 0 1 0 010 0 0 1 0 0
1,000 0 0 1 0 00 10 0 1 0 0
. . . . . . . . . . . . . . . . . .1,000 10 950 0 0 1
0 1,000 950 0 1 010 1,000 950 0 0 1
1,000 1,000 950 0 0 1
Sim
ulat
ions
Near-fieldflow [l/y]
Bufferflow [l/y]
Canisterbreach [mm]
Radionuclide discharge [-]
Negligible Belowlimit
Abovelimit
0 0 0 - - -10 0 0 - - -
1,000 0 0 - - -0 10 0 - - -
. . . . . . . . . . . . . . . . . .1,000 10 950 - - -
0 1,000 950 - - -10 1,000 950 - - -
1,000 1,000 950 - - -
0 1 2 3 40
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Threshold
0 1 2 3 40
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Threshold
Non-conclusive and conclusive interval-valuedprobabilities of unacceptable radionuclide discharges
1627.10.2017 16
§ The bounds of the interval are conservative estimates
Near-fieldflow [l/y]
Bufferflow [l/y]
Canisterbreach [mm]
Radionuclide discharge [-]
Negligible Belowlimit
Abovelimit
0 0 1 - - -10 0 1 - - -
1,000 0 1 - - -0 10 1 - - -
10 10 1 - - -1,000 10 1 - - -
0 1,000 1 - - -10 1,000 1 - - -
1,000 1,000 1 - - -0 0 950 - - -
10 0 950 - - -1,000 0 950 - - -
0 10 950 - - -10 10 950 - - -
1,000 10 950 - - -0 1,000 950 - - -
10 1,000 950 - - -1,000 1,000 950 - - -
Simulations
0 1 2 3 40
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Iterations (number of simulations run)
Pro
babi
lity
ofla
rge
cons
eque
nces
p abov
elim
it
11
11
11
11
0 1 2 3 40
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Iterations (number of simulations run)
Pro
babi
lity
ofla
rge
cons
eque
nces
p abov
elim
it
0 1 2 3 40
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Iterations (number of simulations run)
Pro
babi
lity
ofla
rge
cons
eque
nces
p abov
elim
it
0 1 2 3 40
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Iterations (number of simulations run)
Pro
babi
lity
ofla
rge
cons
eque
nces
p abov
elim
it
0 1 2 3 40
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Iterations (number of simulations run)
Pro
babi
lity
ofla
rge
cons
eque
nces
p abov
elim
it
Interval-valued probability of unacceptableradionuclide discharges
1727.10.2017 17
Next steps 2017-2018 for TURMET
§ Scenario Modeling (2017-)§ More realistic numbers for physical interactions and parameters§ Implementation of time-dependence§ Post-processing to identify the causes of unacceptable radionuclide
releases§ Visualization and analysis of results
§ Safety Case Methodology (2018-)§ Implementing the scenario analysis results into safety case methodology
framework
1827.10.2017 18
Contact Information
§ Suvi Karvonen; [email protected]§ Edoardo Tosoni; [email protected]§ Prof. Ahti Salo; [email protected]
http://www.vtt.fi/sites/turmet