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Program - Brookhaven National Laboratory

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incident energies.<br />

[1] Yu. Malyshkin et al., ”Modeling spallation reactions in tungsten and uranium targets with the Geant4<br />

toolkit”, Proc. Third International Workshop on Compound Nuclear Reactions and Related Topics, vol.<br />

21 of EPJ Web of Conferences, p. 10006 (2012) [2] Yu. Malyshkin et al., ”Neutron production and energy<br />

deposition in fissile spallation targets studied with Geant4 toolkit” (to be submitted) [3] J. Apostolakis<br />

et al. (Geant4 Collaboration), ”Geometry and physics of the Geant4 toolkit for high and medium energy<br />

applications”, Radiat. Phys. Chem., 78, p. 859 (2009)<br />

PR 81<br />

A New Formulation for the Doppler Broadening Function Relaxing the Approximations of<br />

Beth-Plackzec<br />

Daniel A. P. Palma, Comissão Nacional de Energia Nuclear - CNEN. Felipe C. Paiva, Fernando C. Silva,<br />

Aquilino S. Martinez, <strong>Program</strong>a de Engenharia Nuclear - COPPE/UFRJ.<br />

In all nuclear reactors some neutrons can be absorbed in the resonance region and, in the design of these<br />

reactors, an accurate treatment of the resonant absorptions is essential. Apart from that, the resonant<br />

absorption varies with fuel temperature, due to the Doppler broadening of the resonances. The thermal<br />

agitation movement of the reactor core is adequately represented in microscopic cross-section of the<br />

neutron-core interaction through the Doppler broadening function. This function is calculated numerically<br />

in modern systems for the calculation of macro-group constants, necessary to determine the power distribution<br />

of a nuclear reactor. It can also be applied to the calculation of self-shielding factors to correct the<br />

measurements of the microscopic cross-sections through the activation technique and used for the approximate<br />

calculations of the resonance integrals in heterogeneous fuel cells. In these types of application we<br />

can point the need to develop precise analytical approximations for the Doppler broadening function to be<br />

used in the calculation codes that calculates the values of this function. However, the Doppler broadening<br />

function is based on a series of approximations proposed by Beth-Plackzec. In this work a relaxation of<br />

these approximations is proposed, generating an additional term in the form of an integral. Analytical<br />

solutions of this additional term are discussed. The results obtained showed that the new term is important<br />

for high temperatures, typical in the centreline of fuel rods operating in nuclear power plants.<br />

PR 82<br />

Reaction Data Assimilation Phase 1: Model Based Files and Parameter Covariances<br />

A. Palumbo, S. Hoblit, M. Herman, G. P. A. Nobre,, <strong>National</strong> Nuclear Data Center, <strong>Brookhaven</strong> <strong>National</strong><br />

<strong>Laboratory</strong>. M. Sin, Dept. of Atomic and Nuclear Physics, University of Bucharest. R. Capote, IAEA. G.<br />

Palmiotti, M. Salvatores, INL.<br />

Assimilation is a refinement of the usual data adjustment procedure. It links results of integral experiments<br />

to the parameters of nuclear reaction theory, so that it is the reaction model parameters that are<br />

adjusted rather than energy-averaged group cross sections. This novel approach should make adjustment<br />

independent from the target application and should account for the physics constraints imposed by the<br />

nuclear reaction models, differential, and integral measurements. The resulting covariances should reflect<br />

our cumulative knowledge leading to the reduction of the uncertainty margins in the final data. Cross<br />

sections and covariances for the model parameters for 239,242Pu, and 235,238U nuclei fully based on the<br />

EMPIRE-3.1 code [1] calculations were produced (starting with values from the RIPL database [2]). The<br />

Kalman filter technique was used for adjusting selected input model parameters to reproduce differential<br />

303

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