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NE 452552 Nuclear Reactor Analysis II

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Title: NE 452552 Nuclear Reactor Analysis II


1
NE 452/552Nuclear Reactor Analysis II
  • Lecture 8Group collapse
  • Intro to MULTIFLUX

2
What is a group collapse?
  • Often times, we may need to take data from a
    dataset calculated with a fine group structure
    (many energy groups) and use it in a multigroup
    model with fewer groups, or a coarse group
    structure.
  • To do this, the data must be group collapsed.

3
What is the principle behind the group collapse?
  • The basic idea comes from the definition of the
    multigroup cross-section set. Suppose we have
    the following energy range with four fine
    groups and two coarse groups

1
2
I
Coarse groups
Fine groups
3
II
4
4
How do we perform the collapse?
  • The reaction rates in the single coarse fast
    group must equal the sum of the reaction rates in
    the three fine fast groupsNow, the flux in
    the single coarse fast group is the integral of
    the flux (or, more correctly, the spectrum) over
    the energy range

5
So, this gives us equations for most of the
coarse group cross-sections
  • Absorption can be found by
  • We can also do the diffusion coefficient and
    nu-sigma-f terms this way.
  • What about the removal term? Well, removal has
    two pieces

6
The removal cross-section...
  • We already know how to do the absorption term.
    What about the downscatter term?
  • We again need to set the reaction rates in coarse
    and fine group structures equal to each
    otherGraphically, this means

7
The slowing cross-section
  • So, the slowing cross-section is collapsed
    using
  • Then our removal cross-section is found by

8
So, this tells us how to perform the group
collapse, if we have the fluxes...
  • So how do we calculate the fluxes?
  • We first write the multigroup diffusion equations
    for the fine energy group structure

9
Calculating the fluxes...
  • Now, we can proceed in two ways
  • Assume an infinite medium
  • Assume a finite medium and associated buckling
  • Going with the infinite medium approach, our
    equations become

10
Calculating the fluxes...
  • Now, since we are solving an eigenvalue problem,
    we have the freedom to choose a normalization for
    the fluxes. We choose the most convenient
    normalization we can
  • Our flux equations then become very simple

11
O.k. Lets talk about the MULTIFLUX code.
  • What is MULTIFLUX?
  • 2-d (xy geometry), multigroup diffusion code, for
    solving reactor flux and power profile problems
  • Up to nine material types
  • Either vacuum or reflecting boundary conditions
  • Iterates using Inverse Power Iteration
  • Uses a finite-difference technique to solve for
    fluxes at the center of each node (cell, zone)
  • Written by a graduate student of Alan Robinsons
  • Nodes are assumed to be square

12
MULTIFLUX, cont
  • Where is MULTIFLUX?
  • /usr/local/neapps/bin/multiflux_c_sun on the Sun
    machines...
  • How do I run it?
  • Check to see that you are in the nuclear group by
    typing id.If nuclear does not show up, let me
    know.
  • Next, copy the sample input file to your home
    directorycp /usr/local/classes/past/classes_wint
    er2002/ne/ne452/multiflux_c/multiflux_sample .
  • Now, type the following commandmultiflux_c lt
    multiflux_sample gtoutputfilewhere outputfile is
    a filename of your choice
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