2000
DOI: 10.1007/bf02673316
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HTGR nuclear fuel based on plutonium oxide microspheres

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Cited by 2 publications
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“…Thus, buffer layer thicknesses less than 20 µm are too small to extinguish the kinetic energy of the recoil nuclei; the result is an unfavorable over-irradiation of the inner surface of the pyrocarbon layer, giving rise to anisotropic radiation-induced size changes in it [16]. In most requirements for HTGR fuel, it is assumed that the density of the pyrocarbon buffer layer must be ≤1.1 g/cm 3 [3][4][5][6]. Other requirements are not imposed.…”
Section: Of Htgr Fuel Elementsmentioning
confidence: 99%
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“…Thus, buffer layer thicknesses less than 20 µm are too small to extinguish the kinetic energy of the recoil nuclei; the result is an unfavorable over-irradiation of the inner surface of the pyrocarbon layer, giving rise to anisotropic radiation-induced size changes in it [16]. In most requirements for HTGR fuel, it is assumed that the density of the pyrocarbon buffer layer must be ≤1.1 g/cm 3 [3][4][5][6]. Other requirements are not imposed.…”
Section: Of Htgr Fuel Elementsmentioning
confidence: 99%
“…For pyrocarbon density 1.8-2 g/cm 3 (this is density of the inner and outer pyrocarbon layers [5,6]), the fibrous component comprises the dominating fraction. The boundaries of contiguity of the secondary supermolecular formations, formed on the basis of such components, are quite arbitrary.…”
Section: Of Htgr Fuel Elementsmentioning
confidence: 99%
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