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Comparison of Sensitivity Analysis Techniques in Monte

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Title: Comparison of Sensitivity Analysis Techniques in Monte


1
Comparison of Sensitivity Analysis Techniques in
MonteĀ Carlo Codes for Multi-Region Criticality
Calculations
  • Bradley T. Rearden
  • Douglas E. Peplow
  • Oak Ridge National Laboratory

2
Sensitivity and Uncertainty Analysis Techniques
  • New techniques recently developed at ORNL to
    determine applicability of critical experiments
    for criticality code validation.
  • Use energy-dependent sensitivity coefficients and
    cross section covariance data to assess
    similarity of systems.

3
Sensitivity Methods in Monte Carlo Codes
  • Differential Sampling
  • Calculates the derivatives of the response with
    respect to some parameter at the same time the
    response is calculated.
  • First, second, third, etc. and cross derivatives
    can be computed.
  • Available in MCNP and can be used for fixed
    source or criticality problems.
  • MCNP manual cautions The track length estimate
    of keff in KCODE criticality calculations assumes
    the fundamental eigenvector (fission
    distribution) is unchanged in the perturbed
    configuration.
  • This means that the source dependence on the
    parameter of interest is not taken into account
    by the differential sampling, which could lead to
    incorrect values of the derivatives if that
    source dependence is large.

4
Sensitivity Methods in Monte Carlo Codes
  • Perturbation Theory
  • Independent forward and adjoint calculations
  • Group-wise fluxes are computed and folded with
    cross-section data to produce sensitivity
    coefficients.
  • Only valid for small perturbations with linear
    response.
  • Employed inSEN3 analysis sequence using KENO V.a
    in SCALE.

5
GODIVA Sphere
  • 8.7414 cm bare HEU metal
  • 18.74 g/cm3
  • 93.71 235U, and 5.27 238U, 1.02 234U
  • ENDF/B-V data were used in both codes to ensure
    consistency

6
Sensitivity Calculations
  • Sensitivity of keff to fuel density was
    investigated.
  • Over entire system
  • Only in outer 2-cm thick shell
  • Code generated sensitivity coefficients
  • Direct Recalculation
  • /- 10 in MCNP
  • /- 5 in KENO V.a

7
Sensitivity Results
  • Reasonable results for both codes for whole
    system.
  • MCNP over-predicts outer shell by 40.

8
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9
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10
Explanation
  • Differential Sampling
  • When density of whole system is perturbed,
    uniform change in source distribution.
  • Only outer 2-cm thick shell is perturbed,
    non-uniform change in source distribution.
  • Perturbation Theory
  • Forward fluxes are weighted with adjoint flux or
    importance function

11
Possible Solution for Differential Operator
  • Fixed source problem where source is function of
    material density, accumulator stores sum of the
    relative derivatives of interaction
    probabilities, Pij
  • To include effect of source that is proportional
    to density (Scr), start accumulator with
    derivative of source with respect to density

12
Application to Criticality Problems
  • Must be extended from generation to generation.
  • Effect of each energy-dependent cross-section of
    interest would have to be taken into account.
  • Would provide powerful tool for analysts with
    ability to predict non-linear response to
    perturbations.
  • For now, perturbation theory provides adequate
    results for criticality applications.

13
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