AVKOK Neutrondetection based monitoring of void effects in boiling water reactors - PowerPoint PPT Presentation

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AVKOK Neutrondetection based monitoring of void effects in boiling water reactors

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Channel bow. Channel bow (2 mm) Void change and burn up. 0-50 MWd/KgU ... flux, but not on the fast flux, hence it may be possible to detect channel bow. ... – PowerPoint PPT presentation

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Title: AVKOK Neutrondetection based monitoring of void effects in boiling water reactors


1
AVKOKNeutron-detection based monitoring of void
effects in boiling water reactors
  • John Loberg

2
Parameter Study
  • All simulations are performed at Vattenfall
    Bränsle, using Casmo4 Extended version.

3
Background
  • Experimental in-core determination of the void.
  • Validation of codes, safety.
  • Ratio of thermal and fast neutrons depends on the
    void
  • Increased void More fast neutrons,
    less thermal
  • The ratio decreases!
  • Decreased void Less fast neutrons, more
    thermal
  • The ratio increases!
  • The thermal neutron flux is already monitored in
    reactors
  • today by fission chambers based on 235U (Power
    Range Monitors).
  • The fast neutron flux could be monitored by
    fission chambers
  • based upon 238U.

4
Thermal neutrons
Fast (MeV) neutrons
0.625 eV
1.353 MeV
5
  • BWR detectors F3
  • 4 nodes with PRM detectors
  • 37 detectors in each node


4
3
2
1
6
Range of detector
Thermal diffusion length L 2,7
cm Slowing-down length 5
cm Migration length
L
f
7
There is a correlation!
8
Calculations in Casmo 4E
First 1x1 cases
  • Atrium 10B
  • Areva
  • 10x10
  • Forsmark 3
  • Input file specifies
  • Exact geometry
  • Material compositions of each fuel pin
  • BWR or PWR
  • Temperatures, void

9
CASMO
  • Calculates resonance and macroscopic cross
    sections in 70 energy groups for the problem,
    i.e. geometry, temperatures, densities etc., from
    neutron data libraries
  • Divides every fuel pin in to microregions and
    calculates individual spectra for all microgroups
  • Microscopic calculation is then condensed to 2D
    macrogroup calculation in 40 energy groups
  • ..which gives the neutron spectra for the energy
    condensation of cross sectios for the transport
    calculation performed in 8 energy groups
  • Output is cross sections and group constants in 2
    energy groups for nodal codes like POLCA and
    SIMULATE

D1,D2,S1, S2
s1 s70
Sn1 ...Sn40
10
Infinite lattice calculation ?
Mirror Boundary condition
11
Neutron flux distribution, void 0-90
MeV neutron flux
Thermal neutron flux
12
Not only the void has influence on the neutron
flux
  • Burnable absorbers
  • Control rods
  • Channel bow
  • Burn up
  • And more

13
Control rod
Reference
Channel bow
Burnable absorbers
14
Results
15
Channel bow
16
Channel bow (2 mm)
17
Void change and burn up 0-50 MWd/KgU
Axial
Radial
18
Some (humble) observations so far
  • Even though different factors offset the ratio up
    or down, the slope of the ratio remains fairly
    constant, 2 , in the void range 0-90.
  • E.g. if the void changes 10 the prediction will
    be (10 0.2)
  • A small change in position of the box will have
    significant influence on the thermal neutron
    flux, but not on the fast flux, hence it may be
    possible to detect channel bow.

19
Present work
  • MxN ¼ -core Forsmark 3
  • Time consuming
  • Also 3x3 from this ¼ -core for closer study of
    crd and depletion effects

20
Future
  • Investigate more ! Geometry changes, power
    measurements, void determination, depletion
  • Build a prototype detector for validation of
    results
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