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Geometrical shape and self-shielding effect of burnable poison particles on pin-in block type HTGR neutronic performance

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초록

In our previous works, two different spherical burnable poison particles (BPPs) as B4C and Gd2O3 in pin-in block type HTGR core had utilized to suppress the excess reactivity and to control long-term reactivity during the burnup period. In the present work, we performed the neutronic analysis of a prismatic HTGR operating at 850 ◦C with thermal power of 100 MW containing spherical and cylindrical BPPs and then studied the self-shielding effect of BPPs and shape effect. The calculations were performed when the surface area (1) or volume (2) of cylindrical BPPs equals to that of the spherical BPPs. The calculations showed that the neutronic parameters were slightly better for the second case than the first one, such as the excess reactivity of the reactor core at the beginning of the cycle were more suppressed, the core lifetime were more extended, and the fuel-burning were more efficiently. The neutron spectrum in each region of the cylindrical BBPs slightly differs than that of the spherical BPPs. Therefore, the self-shielding effect of BPPs on reactor core performance depends on the particle’s geometrical shape.

Abstract

In our previous works, two different spherical burnable poison particles (BPPs) as B4C and Gd2O3 in pin-in block type HTGR core had utilized to suppress the excess reactivity and to control long-term reactivity during the burnup period. In the present work, we performed the neutronic analysis of a prismatic HTGR operating at 850 ◦C with thermal power of 100 MW containing spherical and cylindrical BPPs and then studied the self-shielding effect of BPPs and shape effect. The calculations were performed when the surface area (1) or volume (2) of cylindrical BPPs equals to that of the spherical BPPs. The calculations showed that the neutronic parameters were slightly better for the second case than the first one, such as the excess reactivity of the reactor core at the beginning of the cycle were more suppressed, the core lifetime were more extended, and the fuel-burning were more efficiently. The neutron spectrum in each region of the cylindrical BBPs slightly differs than that of the spherical BPPs. Therefore, the self-shielding effect of BPPs on reactor core performance depends on the particle’s geometrical shape.

참고문헌 (12)

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  3. Toru Obara, "Flattening of burnup reactivity in long-life prismatic HTGR by particle type burnable poisons", Ann. Nucl. Energy, 57, pp.216~220 (2013)
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  8. Т. Jamiyansuren, "The effect of shape of the burnable poison particles on prismatic HTGR core", Scientific Transaction of the National University of Mongolia, 31(536), pp.77~83 (2020)
  9. MVP, "GMVP II: General-Purpose Monte Carlo Code for Neutron and Photon Transport Calculations Based on Continuous Energy and Multigroup Methods", Y. Nagaya, 2005, JAERI-1348
  10. K. Okumura, "MVP-BURN User’s Manual", Atomic Energy Agency, ~ (2005)
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  12. John R. Lamarsh, "Introduction to Nuclear Engineering"

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