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Kein Folientitel

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PSI Experience with Swiss BWRs shows very good agreement with TIP with the SVM ... Steady-State Analysis at TT2 Conditions. Good agreement with PB1 Edit ... – PowerPoint PPT presentation

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Title: Kein Folientitel


1
PAUL SCHERRER INSTITUT
PB2 TTRIP Phase 2 Coupled 3D Kinetics/Core
Thermal-Hydraulic BC Analysis with CORETRAN
H. Ferroukhi, W. Barten, P.Coddington
OECD/NRC BWR Peach Bottom-2 Turbine Trip
Benchmark 2nd Workshop, Villigen,October 2001
2
CONTENTS
PAUL SCHERRER INSTITUT
  • CORETRAN and RETRAN-3D at PSI
  • PB2 TTRIP Phase 2 3-D Kinetics with Core T/H
    Boundary Conditions
  • Steady-State Results
  • Transient Results
  • Summary

3
PAUL SCHERRER INSTITUT
CORETRAN and RETRAN-3D at PSI
  • PSI transient code environment with CORETRAN /
    RETRAN-3D

4
PAUL SCHERRER INSTITUT
PB-2 Phase 2 Objectives at PSI
  • ANALYSIS WITH CORETRAN Coupled 3-D
    Kinetics/Core Thermal-Hydraulic BC Model
  • Steady-state at both TT2 Conditions and HZP
  • Transient Analysis
  • Analysis performed and submitted
  • ANALYSIS WITH RETRAN-3D Coupled 3-D
    Kinetics/Core Thermal-Hydraulic BC Model
  • RETRAN-3D Model needs to be set-up for Phase 3
    but can also be used for Phase 2
  • Model set-up based on CORETRAN
  • Lumped Model necessary in RETRAN-3D (Homogenized
    T/H Feedback Variables !)
  • Steady-State analysis at HZP to verify
    consistency in Neutronic Solution
    CORETRAN-RETRAN-3D
  • Steady-State and Transient Analysis at TT2
    Conditions with 33-T/H Lumped Model
  • Assess differences between CORETRAN and RETRAN-3D
  • Influence of T/H solution and void model
  • Influence of T/H feedback homogenization
  • Analysis with RETRAN 1-D Kinetics
  • Additional exercise if time available
  • Valuable to assess differences 1-D/3-D

5
PAUL SCHERRER INSTITUT
PB2 Phase 2 CORETRAN Model of PB2
  • ANM Neutronic Algorithm (ARROTTA)
  • 6 Equation 2 Fluid T/H Model (VIPRE-02)
  • Full Core Representation
  • 1x1 Neutronic and T/H Radial Mesh
  • Bypass 1 Additional T/H Channel
  • No Bypass Void
  • Detector Model
  • X-S model modified
  • X-S tables read directly
  • Use of provided X-S interpolation routine
  • Xenon densities read as Restart file
  • No Decay Heat Model

6
PAUL SCHERRER INSTITUT
PB2 Phase 2 CORETRAN Steady-State Results
7
PAUL SCHERRER INSTITUT
Note on Spacer Void Model
  • Spacer Void Model (SVM) available in SIMULATE-3
    to treat void accumulation at Spacer Grids
  • PSI Experience with Swiss BWRs shows very good
    agreement with TIP with the SVM
  • Assessment CORETRAN/SIMULATE performed at PSI for
    Swiss LWRs show that the SVM has a
  • Strong impact on the axial power shape in the
    boiling zone
  • Strong impact on the core reactivity (more
    negative void coefficient in boiling zone)

8
PAUL SCHERRER INSTITUT
PB2 Phase 2 CORETRAN Transient Results
  • Analysis 1 Boundary Condition Total Core Flow
    versus Time
  • 6 Eq. NBC
  • FIBWR Flow Split Model in quasi-static mode
  • Pressure-Flow Convergence Problems

Power and LPRM
Core Flow
Pressure
9
PAUL SCHERRER INSTITUT
PB2 Phase 2 CORETRAN Transient Results
  • Analysis 2 Boundary Condition (33 T-H
    Channels) ( Bypass Channel) Flow versus Time
  • No FIBWR Model

No Bypass Correction (Nominal)
With Bypass Correction (BC1)
10
PAUL SCHERRER INSTITUT
PB2 Phase 2 CORETRAN Transient Results
  • Sensitivity Studies Boundary Condition (33 T-H
    Channels) ( Bypass Channel) Flow versus Time
  • Time Step Size
  • SCRAM Signal

Time Step Size
SCRAM Signal
11
PAUL SCHERRER INSTITUT
PB2 Phase 2 Summary
  • CORETRAN Model for PB-2 Exercise 2 Set-Up
  • Steady-State Analysis at TT2 Conditions
  • Good agreement with PB1 Edit
  • Axial Power Shape (Caution on spacer void)
  • Core Average Void Fraction, Average Exit Quality,
    Core Pressure Drop
  • Very High K-eff
  • Transient Results
  • Analysis with total ore flow BC FIBWR flow
    split UNAPPLICABLE
  • Analysis with 33-TH Channel flow BC
  • No Bypass Correction gives slight under
    prediction of power peak (Nominal Case Submitted)
  • Later analysis with Bypass Correction shows
    better agreement with measurements
  • Sensitivity Analysis
  • Large sensitivity on time-step size
  • Small Time-Step size of 1ms selected
  • Choice of SCRAM on 95 power instead of defined
    t0.63 s seems more adequate
  • but leads to earlier and lower power peak
    magnitude
  • Next Step is to perform similar analysis with
    RETRAN-3D before Phase 3

12
PAUL SCHERRER INSTITUT
PAUL SCHERRER INSTITUT
PB2 Phase 2 CORETRAN Bypass Model
  • CORETRAN PB2 Bypass Model
  • Defined Leakage Paths
  • Core Support Plate
  • Control Rod Drive Housing
  • Assembly Lateral Leakage
  • Path a Through Lower Tie Plate Holes (9 in
    FIBWR)
  • Path b between Channel Box and Lower Tie Plate
    (8 in FIBWR)
  • Path c Water Rods
  • All Paths to ONE SINGLE BYPASS T/H CHANNEL
  • Bypass Geometry
  • Assumed Core Shroud Diameter
  • D_CS 5.6 m (220.47 in)
  • Based on EPRI Report NP-563
  • Assumed Assembly Outer Pitch
  • P_OUT 0.1365 m (5.37 in)
  • Bypass Flow Area 7.5 m2 (11570 in2)

1
FIBWR Model
All Leakage Paths defined by Flow-Pressure Drop
Correlations
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