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        <identifier>oai:kyutech.repo.nii.ac.jp:00006048</identifier>
        <datestamp>2025-04-15T01:47:00Z</datestamp>
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          <dc:title>Study of the Effects of Heat Load, Ablator Density and Backup Structure upon the Thermal Protection Performance of Heat Shield Systems Consisting of Phenolic Carbon Ablators</dc:title>
          <dc:creator>Kato, Sumio</dc:creator>
          <dc:creator>24782</dc:creator>
          <dc:creator>Matsuda, Shoichi</dc:creator>
          <dc:creator>24783</dc:creator>
          <dc:creator>Okuyama, Keiichi</dc:creator>
          <dc:creator>24784</dc:creator>
          <dc:creator>Gibo, Kenta</dc:creator>
          <dc:creator>24785</dc:creator>
          <dc:creator>Oya, Hiroaki</dc:creator>
          <dc:creator>24786</dc:creator>
          <dc:creator>Watanabe, Akihiro</dc:creator>
          <dc:creator>24787</dc:creator>
          <dc:creator>Shimada, Naoyuki</dc:creator>
          <dc:creator>24788</dc:creator>
          <dc:creator>Sakai, Shunsuke</dc:creator>
          <dc:creator>24789</dc:creator>
          <dc:subject>Ablator</dc:subject>
          <dc:subject>Heat Shield System</dc:subject>
          <dc:subject>Re-Entry Capsule</dc:subject>
          <dc:subject>Ablation Analysis</dc:subject>
          <dc:description>The effects of heat load, ablator density, and backup structure, etc. upon the heat shield performance of the lightweight phenolic carbon ablators named LATS were investigated using a one-dimensional ablation analysis code. The ablator density was assumed to be from about 260 to 1000 kg/m3. Heat flux time histories of a rectangular pattern were assumed, where cases of constant heating duration time and constant accumulated heat load (up to 600 MJ/m2) were considered. The heating level was assumed to be from 1 to 10 MW/m2, which means that the ablator surface is in the region of diffusion control oxidation/sublimation. The materials of the backup wall are assumed to be aluminum, stainless steel and high density CFRP. Main findings are: (1) For a low heat flux q with the same heating duration time tq, the necessary thickness, with which the maximum back surface temperature equals to the pre-determined allowable temperature, is nearly constant as the density ρv changes. On the other hand, the necessary thickness increases largely when q is larger and ρv is smaller. The ablator necessary mass increases with the increase of ρv and q for the same tq. (2) When a backup wall is attached, the necessary thickness decreases and the necessary mass including the wall mass increases. (3) For a constant accumulated heat load, necessary thickness and mass decrease for a higher heat flux q especially when ρv is high. (4) A lower density ablator with a CFRP backup wall gives the lightest mass of the heat shield system for most of the parameter range among the three wall materials. (5) For a high heat flux, selection of a lower density ablator gives a larger necessary thickness.</dc:description>
          <dc:description>30th International Symposium on Space Technology and Science (ISTS), July 4th-July 10th, 2015, Kobe-Hyogo, Japan</dc:description>
          <dc:description>conference paper</dc:description>
          <dc:publisher>日本航空宇宙学会</dc:publisher>
          <dc:date>2016-12-02</dc:date>
          <dc:type>VoR</dc:type>
          <dc:format>application/pdf</dc:format>
          <dc:identifier>Transactions of the Japan Society for Aeronautical and Space Sciences, Aerospace Technology Japan</dc:identifier>
          <dc:identifier>ists30</dc:identifier>
          <dc:identifier>14</dc:identifier>
          <dc:identifier>Pe_95</dc:identifier>
          <dc:identifier>Pe_104</dc:identifier>
          <dc:identifier>1884-0485</dc:identifier>
          <dc:identifier>https://kyutech.repo.nii.ac.jp/record/6048/files/LaSEINE-2016_11.pdf</dc:identifier>
          <dc:identifier>http://hdl.handle.net/10228/00007258</dc:identifier>
          <dc:identifier>https://kyutech.repo.nii.ac.jp/records/6048</dc:identifier>
          <dc:language>eng</dc:language>
          <dc:relation>https://doi.org/10.2322/tastj.14.Pe_95</dc:relation>
          <dc:rights>Copyright (c) 2016 by the Japan Society for Aeronautical and Space Sciences and ISTS.</dc:rights>
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