Rubber based neutron shielding material simulation using MCNP5
Rubber-Based Neutron Shielding Material Simulation using MCNP5. The natural rubber-based neutron radiation shielding was simulated using MCNP5 computer code. The attenuation curves of natural rubber, rubber-neoprene, rubber-silicone, natural rubber+5% Vol. Gd2O2S composite, natural rubber+25% Vol. B...
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creator | Panitra, M. M. Aziz, F. Rivai, A. K. Sukaryo, S. G. Fisli, A. Sudirman Parikin |
description | Rubber-Based Neutron Shielding Material Simulation using MCNP5. The natural rubber-based neutron radiation shielding was simulated using MCNP5 computer code. The attenuation curves of natural rubber, rubber-neoprene, rubber-silicone, natural rubber+5% Vol. Gd2O2S composite, natural rubber+25% Vol. Borax, natural rubber+ 5% Vol. B4C, natural rubber+5% Vol. Li2O and natural rubber+5% Vol. Gd2O2S composite+Pb layer were made. The half-value layer (HVL) of each shielding was also calculated for both fast and thermal neutron. For the thermal neutron, the smallest HVL was obtained by using a composite of natural rubber+5% Vol. Gd2O2S i.e. 0.23 cm and the biggest was obtained for natural rubber+25% Vol. Borax i.e. 0.92 cm. on the other hand, for fast neutron, the smallest HVL was obtained for the shielding of Natural Rubber+5% Vol Gd2O2S i.e. 0.7 cm and Natural Rubber+25% Vol. Borax i.e. 1.23 cm. Photon was induced when thermal neutrons pass through the shielding of Natural Rubber+5% Vol Gd2O2S due to the (nth,ψ) |
doi_str_mv | 10.1063/5.0066597 |
format | Conference Proceeding |
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M. ; Aziz, F. ; Rivai, A. K. ; Sukaryo, S. G. ; Fisli, A. ; Sudirman ; Parikin</creator><contributor>Sugono, Irawan ; Mulyani, Emy ; Mujamilah ; Taufik ; Rifai, Muhammad ; Santoso, Muhayatun</contributor><creatorcontrib>Panitra, M. M. ; Aziz, F. ; Rivai, A. K. ; Sukaryo, S. G. ; Fisli, A. ; Sudirman ; Parikin ; Sugono, Irawan ; Mulyani, Emy ; Mujamilah ; Taufik ; Rifai, Muhammad ; Santoso, Muhayatun</creatorcontrib><description>Rubber-Based Neutron Shielding Material Simulation using MCNP5. The natural rubber-based neutron radiation shielding was simulated using MCNP5 computer code. The attenuation curves of natural rubber, rubber-neoprene, rubber-silicone, natural rubber+5% Vol. Gd2O2S composite, natural rubber+25% Vol. Borax, natural rubber+ 5% Vol. B4C, natural rubber+5% Vol. Li2O and natural rubber+5% Vol. Gd2O2S composite+Pb layer were made. The half-value layer (HVL) of each shielding was also calculated for both fast and thermal neutron. For the thermal neutron, the smallest HVL was obtained by using a composite of natural rubber+5% Vol. Gd2O2S i.e. 0.23 cm and the biggest was obtained for natural rubber+25% Vol. Borax i.e. 0.92 cm. on the other hand, for fast neutron, the smallest HVL was obtained for the shielding of Natural Rubber+5% Vol Gd2O2S i.e. 0.7 cm and Natural Rubber+25% Vol. Borax i.e. 1.23 cm. Photon was induced when thermal neutrons pass through the shielding of Natural Rubber+5% Vol Gd2O2S due to the (nth,ψ)</description><identifier>ISSN: 0094-243X</identifier><identifier>EISSN: 1551-7616</identifier><identifier>DOI: 10.1063/5.0066597</identifier><identifier>CODEN: APCPCS</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Attenuation ; Borax ; Boron carbide ; Fast neutrons ; Lithium oxides ; Natural rubber ; Neoprene ; Neutrons ; Radiation shielding ; Rubber ; Simulation ; Thermal neutrons</subject><ispartof>AIP conference proceedings, 2021, Vol.2381 (1)</ispartof><rights>Author(s)</rights><rights>2021 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/acp/article-lookup/doi/10.1063/5.0066597$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>309,310,314,776,780,785,786,790,4498,23909,23910,25118,27901,27902,76127</link.rule.ids></links><search><contributor>Sugono, Irawan</contributor><contributor>Mulyani, Emy</contributor><contributor>Mujamilah</contributor><contributor>Taufik</contributor><contributor>Rifai, Muhammad</contributor><contributor>Santoso, Muhayatun</contributor><creatorcontrib>Panitra, M. M.</creatorcontrib><creatorcontrib>Aziz, F.</creatorcontrib><creatorcontrib>Rivai, A. K.</creatorcontrib><creatorcontrib>Sukaryo, S. G.</creatorcontrib><creatorcontrib>Fisli, A.</creatorcontrib><creatorcontrib>Sudirman</creatorcontrib><creatorcontrib>Parikin</creatorcontrib><title>Rubber based neutron shielding material simulation using MCNP5</title><title>AIP conference proceedings</title><description>Rubber-Based Neutron Shielding Material Simulation using MCNP5. The natural rubber-based neutron radiation shielding was simulated using MCNP5 computer code. The attenuation curves of natural rubber, rubber-neoprene, rubber-silicone, natural rubber+5% Vol. Gd2O2S composite, natural rubber+25% Vol. Borax, natural rubber+ 5% Vol. B4C, natural rubber+5% Vol. Li2O and natural rubber+5% Vol. Gd2O2S composite+Pb layer were made. The half-value layer (HVL) of each shielding was also calculated for both fast and thermal neutron. For the thermal neutron, the smallest HVL was obtained by using a composite of natural rubber+5% Vol. Gd2O2S i.e. 0.23 cm and the biggest was obtained for natural rubber+25% Vol. Borax i.e. 0.92 cm. on the other hand, for fast neutron, the smallest HVL was obtained for the shielding of Natural Rubber+5% Vol Gd2O2S i.e. 0.7 cm and Natural Rubber+25% Vol. Borax i.e. 1.23 cm. Photon was induced when thermal neutrons pass through the shielding of Natural Rubber+5% Vol Gd2O2S due to the (nth,ψ)</description><subject>Attenuation</subject><subject>Borax</subject><subject>Boron carbide</subject><subject>Fast neutrons</subject><subject>Lithium oxides</subject><subject>Natural rubber</subject><subject>Neoprene</subject><subject>Neutrons</subject><subject>Radiation shielding</subject><subject>Rubber</subject><subject>Simulation</subject><subject>Thermal neutrons</subject><issn>0094-243X</issn><issn>1551-7616</issn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2021</creationdate><recordtype>conference_proceeding</recordtype><recordid>eNp9kFtLxDAQhYMoWFcf_AcF34Suuad5EWRxVVgviIJvYdqmmqU3k1bw35t1F3zzaWC-MzNnDkKnBM8JluxCzDGWUmi1hxIiBMmUJHIfJRhrnlHO3g7RUQhrjKlWKk_Q5fNUFNanBQRbpZ2dRt93afhwtqlc9562MFrvoEmDa6cGRhfpFDbkfvHwJI7RQQ1NsCe7OkOvy-uXxW22ery5W1ytsoFiprI8Z6qUklZKQgkYcFFxJgByqLWgXEc7wAsQuOIRqdgBCmWdW6ClLYuazdDZdu_g-8_JhtGs-8l38aShQscXCdcsqs63qlC68derGbxrwX-br94bYXbZmKGq_xMTbDZh_g2wH8QcZdY</recordid><startdate>20211111</startdate><enddate>20211111</enddate><creator>Panitra, M. M.</creator><creator>Aziz, F.</creator><creator>Rivai, A. K.</creator><creator>Sukaryo, S. G.</creator><creator>Fisli, A.</creator><creator>Sudirman</creator><creator>Parikin</creator><general>American Institute of Physics</general><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20211111</creationdate><title>Rubber based neutron shielding material simulation using MCNP5</title><author>Panitra, M. M. ; Aziz, F. ; Rivai, A. K. ; Sukaryo, S. G. ; Fisli, A. ; Sudirman ; Parikin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p2037-8837c662d76aca0a0bd435aa8af95249002a4ba50d40bd7249a2acf8ea2cecbf3</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Attenuation</topic><topic>Borax</topic><topic>Boron carbide</topic><topic>Fast neutrons</topic><topic>Lithium oxides</topic><topic>Natural rubber</topic><topic>Neoprene</topic><topic>Neutrons</topic><topic>Radiation shielding</topic><topic>Rubber</topic><topic>Simulation</topic><topic>Thermal neutrons</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Panitra, M. M.</creatorcontrib><creatorcontrib>Aziz, F.</creatorcontrib><creatorcontrib>Rivai, A. K.</creatorcontrib><creatorcontrib>Sukaryo, S. G.</creatorcontrib><creatorcontrib>Fisli, A.</creatorcontrib><creatorcontrib>Sudirman</creatorcontrib><creatorcontrib>Parikin</creatorcontrib><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Panitra, M. M.</au><au>Aziz, F.</au><au>Rivai, A. K.</au><au>Sukaryo, S. G.</au><au>Fisli, A.</au><au>Sudirman</au><au>Parikin</au><au>Sugono, Irawan</au><au>Mulyani, Emy</au><au>Mujamilah</au><au>Taufik</au><au>Rifai, Muhammad</au><au>Santoso, Muhayatun</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Rubber based neutron shielding material simulation using MCNP5</atitle><btitle>AIP conference proceedings</btitle><date>2021-11-11</date><risdate>2021</risdate><volume>2381</volume><issue>1</issue><issn>0094-243X</issn><eissn>1551-7616</eissn><coden>APCPCS</coden><abstract>Rubber-Based Neutron Shielding Material Simulation using MCNP5. The natural rubber-based neutron radiation shielding was simulated using MCNP5 computer code. The attenuation curves of natural rubber, rubber-neoprene, rubber-silicone, natural rubber+5% Vol. Gd2O2S composite, natural rubber+25% Vol. Borax, natural rubber+ 5% Vol. B4C, natural rubber+5% Vol. Li2O and natural rubber+5% Vol. Gd2O2S composite+Pb layer were made. The half-value layer (HVL) of each shielding was also calculated for both fast and thermal neutron. For the thermal neutron, the smallest HVL was obtained by using a composite of natural rubber+5% Vol. Gd2O2S i.e. 0.23 cm and the biggest was obtained for natural rubber+25% Vol. Borax i.e. 0.92 cm. on the other hand, for fast neutron, the smallest HVL was obtained for the shielding of Natural Rubber+5% Vol Gd2O2S i.e. 0.7 cm and Natural Rubber+25% Vol. Borax i.e. 1.23 cm. Photon was induced when thermal neutrons pass through the shielding of Natural Rubber+5% Vol Gd2O2S due to the (nth,ψ)</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0066597</doi><tpages>11</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Attenuation Borax Boron carbide Fast neutrons Lithium oxides Natural rubber Neoprene Neutrons Radiation shielding Rubber Simulation Thermal neutrons |
title | Rubber based neutron shielding material simulation using MCNP5 |
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