Critical experiments are used for validation of reactor physics codes, in particular, to determine the biases and uncertainties in code predictions. To reflect all conditions present in operating reactors, plans for such experiments often require tests involving irradiated fuel. However, it is impractical to use actual irradiated fuel in critical experiments due to hazards associated with handling and transporting the fuel. To overcome this limitation, a simulated irradiated fuel, whose composition mimics the neutronic behavior of the truly irradiated fuel (TRUFUEL), can be used in a critical experiment. Here, we present an optimization method in which the composition of simulated irradiated fuel for the Canadian supercritical water-cooled reactor (SCWR) concept at midburnup ( (IHM)) is varied until the integral indices , , and are maximized between the true and simulated irradiated fuel. In the optimization, the simulated irradiated fuel composition is simplified so that only the major actinides (, , and ) remain, while the absorbing fission products are replaced by dysprosia and zirconia. In this method, the integral indices , , and are maximized while the buckling, and the relative ring-averaged pin fission powers are constrained, within a certain tolerance, to their reference lattice values. Using this method, maximized integral similarity indices of , , and have been obtained.
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April 2016
Research-Article
Methodology to Design Simulated Irradiated Fuel by Maximizing Integral Indices (ck, E, G)
Jason R. Sharpe,
Jason R. Sharpe
1
Department of Engineering Physics,
e-mail: sharpejr@mcmaster.ca
McMaster University
, Hamilton, ON L8S 4L8
, Canada
e-mail: sharpejr@mcmaster.ca
1Corresponding author.
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Adriaan Buijs,
Adriaan Buijs
Department of Engineering Physics,
e-mail: buijsa@mcmaster.ca
McMaster University
, Hamilton, ON L8S 4L8
, Canada
e-mail: buijsa@mcmaster.ca
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Jeremy Pencer
Jeremy Pencer
Computational Physics Branch, Canadian Nuclear Laboratories,
Engineering Physics,
e-mail: jeremy.pencer@cnl.ca
Engineering Physics,
McMaster University
, Deep River, ON K0J 1P0
, Canada
e-mail: jeremy.pencer@cnl.ca
Search for other works by this author on:
Jason R. Sharpe
Department of Engineering Physics,
e-mail: sharpejr@mcmaster.ca
McMaster University
, Hamilton, ON L8S 4L8
, Canada
e-mail: sharpejr@mcmaster.ca
Adriaan Buijs
Department of Engineering Physics,
e-mail: buijsa@mcmaster.ca
McMaster University
, Hamilton, ON L8S 4L8
, Canada
e-mail: buijsa@mcmaster.ca
Jeremy Pencer
Computational Physics Branch, Canadian Nuclear Laboratories,
Engineering Physics,
e-mail: jeremy.pencer@cnl.ca
Engineering Physics,
McMaster University
, Deep River, ON K0J 1P0
, Canada
e-mail: jeremy.pencer@cnl.ca
1Corresponding author.
Manuscript received May 8, 2015; final manuscript received July 8, 2015; published online February 29, 2016. Assoc. Editor: Thomas Schulenberg.
ASME J of Nuclear Rad Sci. Apr 2016, 2(2): 021017 (7 pages)
Published Online: February 29, 2016
Article history
Received:
May 8, 2015
Revision Received:
July 8, 2015
Accepted:
July 13, 2015
Citation
Sharpe, J. R., Buijs, A., and Pencer, J. (February 29, 2016). "Methodology to Design Simulated Irradiated Fuel by Maximizing Integral Indices (ck, E, G)." ASME. ASME J of Nuclear Rad Sci. April 2016; 2(2): 021017. https://doi.org/10.1115/1.4031074
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