2014
DOI: 10.1016/j.nucengdes.2013.11.060
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Stochastic arranging of CFPs in HTTR and criticality benchmark considering different modeling of CFPs

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Cited by 5 publications
(2 citation statements)
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“…Subsequently, the calculated values were then used as the input parameter for neutronic steady‐state calculation via the MCNPX 2.7 code 41 . It has been widely used to simulate and analyze the HTR core, including fuel burnup, in detail with a less simplified geometry model 42‐45 . Besides, this specific code could also simulate the stochastic arrangement of TRISO particles in the HTR compact fuel.…”
Section: Methodsmentioning
confidence: 99%
“…Subsequently, the calculated values were then used as the input parameter for neutronic steady‐state calculation via the MCNPX 2.7 code 41 . It has been widely used to simulate and analyze the HTR core, including fuel burnup, in detail with a less simplified geometry model 42‐45 . Besides, this specific code could also simulate the stochastic arrangement of TRISO particles in the HTR compact fuel.…”
Section: Methodsmentioning
confidence: 99%
“…Monte Carlo code such as the Monte Carlo N‐Particle Transport (MCNP) is widely accepted as one of the advanced 3D neutronic design tools to simulate complicated reactor cores. The MCNP code, in fact, had been used to model and simulate the simplified HTR core 99,102‐104 . The code can even randomly arrange TRISO particles in the HTR fuel compact.…”
Section: Duplex Fuel Design For Htrmentioning
confidence: 99%