• Keine Ergebnisse gefunden

criticality calculation in severe accident

N/A
N/A
Protected

Academic year: 2022

Aktie "criticality calculation in severe accident "

Copied!
17
0
0

Wird geladen.... (Jetzt Volltext ansehen)

Volltext

(1)

EMUG meeting – 27 th of April 2018

Helman T. – Fontaine M.-P. – Makine I.

Use of Artificial Neural Network for

criticality calculation in severe accident

(2)

Chapter 1 Context and objectives

Chapter 2 Process overview

Chapter 3 Approach definition

Chapter 4 Modelling of the intact & degraded core

CONTENTS

Chapter 5 Surrogate model (artificial neural network)

Chapter 6 Conclusion & perspectives

(3)

 Context: Calculation of core criticality in severe accident configuration

— Capability to calculate reactivity accidents leading to core damage

— Topic under discussion as severe accident research priority in NUGENIA

— Calculation of Fukushima type sequences (non borated water injected, also foreseen in the SAMG)

— Interest for Gen III reactors foreseen to operate with 100% MOX cores

Criticality in severe accident

Context and objectives

(4)

 Development in Tractebel:

— MELCOR reference code in Tractebel for severe accident calculation includes a point kinetic model (not valid for degraded geometries)

 Development of a surrogate model (Artificial Neural Network) to be included in MELCOR as external reactivity

• Low computational cost compared to coupling with neutron code

• Online ࢑

ࢋࢌࢌ

calculation and feedback on core power

Criticality in severe accident

Context and objectives

(5)

Automatic generation of

MCNP calculations

database Data on

degraded geometry (PSA 2 MELCOR

supporting calculations)

Training of an Artificial Neural

Network (surrogate

model)

Core loading pattern Data on core

content (WIMS &

PANTHER)

Implementation of ANN in MELCOR for

reactivity accident calculation

Criticality in severe accident

Process overview

(6)

 Focus on in-vessel phase and more particularly on idealised TMI-like configuration

— Spherical corium pool in active part of the core

— No relocation of corium in lower plenum considered

— No steel structures

— Infinite water reflector

 Data from MELCOR:

— Fraction of RN released from core (including control rod poison) as a function of core degraded fraction

— Zirconium oxidized fraction as a function of core degraded fraction

Criticality in severe accident

Approach definition and evaluation of input data needed

(7)

Criticality in severe accident

Data for intact core modelling in MCNP

 Data for intact core MCNP input:

1. Core loading pattern:

a) Assemblies types positions b) Control rods positions

c) Number of cycles in core per assembly

2. 12 families of assemblies are defined (assembly type, number of cycles in core)

3. Family burnup as a function of core exposure 4. Different rod types per assembly (depending on

neighbourhood)

5. Composition of fuel rods depending on assembly exposure

MCNP input

MELCOR:

Data on degraded geometry

Burnup of the different assemblies as

a function of core exposure

Rods compositions as a function

of burnup

Number of cycles in core

for each assembly Control rods

positions Assemblies

geometries (position of the

different rod types)

Assemblies types positions

(8)

Criticality in severe accident

Data for intact core modelling in MCNP

MCNP input

MELCOR:

Data on degraded geometry

Burnup of the different assemblies as

a function of core exposure

Rods compositions as a function

of burnup

Number of cycles in core

for each assembly Control rods

positions Assemblies

geometries (position of the

different rod types)

Assemblies types positions

ࢋࢌࢌ obtained:

— BOL, ARO, Bcrit_ARO:

1.00776

— BOL, DBCA, Bcrit_DBCA:

1.00503

 Good starting point

(9)

Data extracted from MELCOR calculation database used for PSA level 2

Criticality in severe accident

MELCOR inputs for degrade geometry modelling in MCNP

(10)

Data extracted from MELCOR calculation database used for PSA level 2

Criticality in severe accident

MELCOR inputs for degrade geometry modelling in MCNP

(11)

Parameter Range

Degradation 0 – 100%

RN Class i released fraction F(Degradation) Fraction of oxidised Zr F(Degradation) Time since SCRAM (depletion) 0 – 10d

Density of corium 7 – 10 g/cm³

Core exposure 0 – 18GWd/tU

Water temperature 100°C – 330°C

Boron concentration 0 – 2800ppm

Core water level 0 – 100%

Criticality in severe accident

Training of ANN – Parameter space

(12)

Criticality in severe accident

Identification of critical zone

 For each parameter, identification of range where ࢑ ࢋࢌࢌ can be higher than 1

(13)

Criticality in severe accident

Training of Artificial Neural Network and first testing

Which parameters are important for ࢑ࢋࢌࢌ ?

 Importance analysis

— Degradation (65%)

— Boron (18%)

— ZrOx (5%)

— BU (3%)

 We take all the parameters !

(14)

Number of data in sample = sufficient ?

 Accuracy = 0.9577 േ 0.02319

 Explained variance score = 0.96146685

 R2 score = 0.96144549

 Mean absolute error = 0.01709

 Mean squared error = 0.0006662

 Median absolute error = 0.0115854

Criticality in severe accident

Training of Artificial Neural Network and first testing

(15)

Criticality in severe accident

Training of Artificial Neural Network and first testing

 Compare ܶ ௠௢ௗஶ ሺߩ ሻ and ܶ ௙௨௘௟ஶ ሺߩ

(16)

Criticality in severe accident

Conclusion

 Need for a high detail modelling of the core to obtain a good starting point

 ANN shows promising results for ࢑ ࢋࢌࢌ evaluation in severe accident configuration:

— Capable of explaining up to 96% of the variance of the ࢑ ࢋࢌࢌ based on input parameters

— Possibility to make ANN more precise in certain zones of the parameters space by increasing number of samples in those zones

— Possibility for feature importance analysis

 Stabilisation temperatures obtained for several reactivity insertion show good agreement with point

kinetic model with measured temperature coefficients for real loading pattern

(17)

Criticality in severe accident

Perspectives

 Perspectives:

— Easy to implement in MELCOR using CFs and existing point kinetic model & low computational cost

 Implementation in MELCOR and test against existing & validated Tractebel models for reactivity insertion accidents without core melting

— Calculation of reactivity accidents with core melting using MELCOR

— Possible extension of approach to other physics e.g. debris bed cooling, MCCI, etc.

Referenzen

ÄHNLICHE DOKUMENTE

In the phenomenological treatment of the elec- troweak Standard Model physical fields are introduced as a consequence of isospin symmetry breaking of a corresponding SU ( 2 )⊗ U ( 1

∙ The secondary circuit input model is limited to heat exchanger connected to the double primary loop on natural circulation.. ∙ Containment and Reactor Hall input models are the

The secondary circuit input model is limited to two SGs connected to the double primary loop on natural circulation.. Secondary coolant in these two SGs is cooled by a

Volatile I released to environment 1345 32 Volatile I suspended in operating rooms 3910 88 Volatile iodine does not pose a problem with proper alkalizing. compared to aerosol

MELCOR 1.8.6 Iodine Pool Model (IPM) has been applied to VVER-440/213 severe accident using a Full Circuit Input Model (FCIM) without IMP and a simplified version called Stand Alone

• Maintain an internal vacuum to avoid excessive convective heat transfer between the Vacuum Vessel (VV) and the Magnet System (MS).. • Vacuum barrier (cryogenic temperatures

 C1-C2: Injection into RPV to terminate/mitigate MCCI inside the reactor cavity (by volume control system, accumulators and/or from SFP), maximizing heat removal from

Design-basis accident source term calculations are used to establish the adequacy of siting for commercial nuclear power plants and to ensure. that adequate radiation protection