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Prof. dr. ir. ing. René Boonen
The formation of hydrogen flakes during fabrication of the reactor pressure vessel. dr. ir. Jan Peirs Prof. dr. ir. ing. René Boonen 13/04/2018 INRAG Fachtagung
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Overview Location and distribution of flakes Hypothesis of Electrabel
Overview Location and distribution of flakes Hypothesis of Electrabel Test hypothesis: calculate hydrogen balance
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Reactor vessel construction
3 Reactor vessel construction
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4 Distribution of flakes around the circumference of the Doel3 lower shell 7200 flakes 25.8 / L 11600 flakes 41.6 / L
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Size distribution of the flakes
5 Size distribution of the flakes
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Hypothesis of Electrabel
Hypothesis of Electrabel Cracks formed during production During transformation from gamma to alfa phase, the segregation zones become supersaturated in hydrogen which will recombine to hydrogen gas H2 at trapping sites in the metal, building up an internal pressure. Pressure -> cracks Cracks already present at start-up of the reactor Reactor vessel is stable, flakes do not grow => safe
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Test Electrabel hypothesis: hydrogen balance
7 Test Electrabel hypothesis: hydrogen balance Amount of hydrogen available during production ? Amount of hydrogen required to create present measured amount of cracks ? if(available hydrogen < required for cracks) then hypothesis = false
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Available hydrogen measured (in liquid state)
8 Available hydrogen measured (in liquid state)
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Crack formation: calculation
Crack formation: calculation p Calculation based on equilibrium at final state of flake KIC & a -> -> FEM -> volume of flake under pressure -> volume of H2 p = KIc : critical stress intensity factor (material parameter) : bulk stress or internal pressure in flake a: radius of flake
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Determination of the critical stress intensity factor
10 Determination of the critical stress intensity factor Use KIC of the lower shelf of the ASME curve 40 MPa/m Minimum amount of required H2 In reality: even more H2 required (conservative approach)
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Volume of flake under internal H2 pressure
11 FEM analysis Volume of flake under internal H2 pressure
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Crack formation: volume
Crack formation: volume Crack grows Equilibrium, crack stops growing H2 has disappeared, crack closes again } dV x p
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Total H2 volume for 11600 flakes
13 Total H2 volume for flakes
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Hydrogen balance Full shell ( 4 m, H=2,5 m, d=0,2 m)
14 Hydrogen balance Full shell ( 4 m, H=2,5 m, d=0,2 m) Available: 383 L H2 Required: 375 L H2 No H2 should escape through the walls High density zone with 41 flakes / L Available: 61 mL / L Required: 1373 mL / L Factor 22 short
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Conclusion Our calculations show that there is not sufficient hydrogen available during production to form all the flakes. Only limited number of flakes can be explained by this mechanism Hypothesis of Electrabel does not explain flakes.
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Apparently, Electrabel has not investigated the volumetric hydrogen balance.
Electrabel should recalculate the hydrogen balance using their extensive dataset which they have at their disposal.
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Einladung Part 2 of this study: Prof. dr.-ing. René Boonen
Einladung Part 2 of this study: Prof. dr.-ing. René Boonen Saturday 10:45 “Ungelöste Probleme der Materialstruktur des Reaktordruckbehälters von Tihange 2“ Extended calculation for different KIC at room temperature Upper and lower shells
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Breukmechanica - Scheuren hebben energie nodig om te groeien.
19 Breukmechanica - Scheuren hebben energie nodig om te groeien. - 4 soorten energie: - elastische energie (leverancier) - plastische energie - oppervlakte-energie (scheurgroei) - kinetische energie (materiaalverplaatsing, kraakgeluid) -Scheuren groeien onder cyclische belasting.
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20 Breukmechanica Scheurvormen Stress Intensity Factor SIF:
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Breukmechanica RT Curve bepaald door trekproeven en kerfslagproeven
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22 Breukmechanica
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Oplosbaarheid waterstof in staal
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