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Gadolinium-doped polymeric as a shielding material for X-ray
A relatively new polymeric base compounds (CnH2n) had been proposed as a shielding material for 150 keV photon for an X-ray laboratory. When doped with 8 % gadolinium (Gd), a thickness of 2 cm shielding compound (6 g cm −3 ) could attenuate more than 90 % of the incident photons with an average dose...
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Published in: | IOP conference series. Materials Science and Engineering 2021-03, Vol.1106 (1), p.12010 |
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description | A relatively new polymeric base compounds (CnH2n) had been proposed as a shielding material for 150 keV photon for an X-ray laboratory. When doped with 8 % gadolinium (Gd), a thickness of 2 cm shielding compound (6 g cm
−3
) could attenuate more than 90 % of the incident photons with an average dose rate reduction of more than 88 % for 150 keV incident photon. While considering the transmitted photons after the shielding, it is necessary to account for reflected photons and its dose contribution. The reflected photons and ambient dose equivalent were calculated for single-photon energy of 150 keV and an X-ray of 150 kVp. The shielding compound was successfully attenuated most of the incident photon energies particularly below 90 keV. In both cases of photon sources, two significant reflected photon peaks at ~40 and 50 keV were observed as a result of Gd characteristic X-rays. A Compton scattered photon at energy of 95 keV appeared as a result of large scattering angle within 130° -140° for 150 keV incident photons. Thus it is necessary to add a thin inner layer at the source-facing side of the shielding compound to shield the radiation workers and patient inside the X-ray room during the X-ray procedure. An iron layer with thickness of 0.5 cm was adequate to shield almost completely the reflected photons and ambient dose for X-ray 150 kVp source |
doi_str_mv | 10.1088/1757-899X/1106/1/012010 |
format | article |
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−3
) could attenuate more than 90 % of the incident photons with an average dose rate reduction of more than 88 % for 150 keV incident photon. While considering the transmitted photons after the shielding, it is necessary to account for reflected photons and its dose contribution. The reflected photons and ambient dose equivalent were calculated for single-photon energy of 150 keV and an X-ray of 150 kVp. The shielding compound was successfully attenuated most of the incident photon energies particularly below 90 keV. In both cases of photon sources, two significant reflected photon peaks at ~40 and 50 keV were observed as a result of Gd characteristic X-rays. A Compton scattered photon at energy of 95 keV appeared as a result of large scattering angle within 130° -140° for 150 keV incident photons. Thus it is necessary to add a thin inner layer at the source-facing side of the shielding compound to shield the radiation workers and patient inside the X-ray room during the X-ray procedure. An iron layer with thickness of 0.5 cm was adequate to shield almost completely the reflected photons and ambient dose for X-ray 150 kVp source</description><identifier>ISSN: 1757-8981</identifier><identifier>EISSN: 1757-899X</identifier><identifier>DOI: 10.1088/1757-899X/1106/1/012010</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><subject>Dosage ; Elastic scattering ; Gadolinium ; Photons ; Radiation shielding ; Scattering angle ; Thickness ; X-rays</subject><ispartof>IOP conference series. Materials Science and Engineering, 2021-03, Vol.1106 (1), p.12010</ispartof><rights>2021. This work is published under http://creativecommons.org/licenses/by/3.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1790-c3962f27579bfa3c32fbf244b88a1b2cc9a28805cc2b580ee72db2ca994b9b1b3</citedby><cites>FETCH-LOGICAL-c1790-c3962f27579bfa3c32fbf244b88a1b2cc9a28805cc2b580ee72db2ca994b9b1b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.proquest.com/docview/2512294561?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>314,776,780,25732,27903,27904,36991,44569</link.rule.ids></links><search><creatorcontrib>Tajudin, S M</creatorcontrib><creatorcontrib>Aminordin Sabri, A H</creatorcontrib><creatorcontrib>Abdul Aziz, M Z</creatorcontrib><creatorcontrib>Tabbakh, F</creatorcontrib><title>Gadolinium-doped polymeric as a shielding material for X-ray</title><title>IOP conference series. Materials Science and Engineering</title><description>A relatively new polymeric base compounds (CnH2n) had been proposed as a shielding material for 150 keV photon for an X-ray laboratory. When doped with 8 % gadolinium (Gd), a thickness of 2 cm shielding compound (6 g cm
−3
) could attenuate more than 90 % of the incident photons with an average dose rate reduction of more than 88 % for 150 keV incident photon. While considering the transmitted photons after the shielding, it is necessary to account for reflected photons and its dose contribution. The reflected photons and ambient dose equivalent were calculated for single-photon energy of 150 keV and an X-ray of 150 kVp. The shielding compound was successfully attenuated most of the incident photon energies particularly below 90 keV. In both cases of photon sources, two significant reflected photon peaks at ~40 and 50 keV were observed as a result of Gd characteristic X-rays. A Compton scattered photon at energy of 95 keV appeared as a result of large scattering angle within 130° -140° for 150 keV incident photons. Thus it is necessary to add a thin inner layer at the source-facing side of the shielding compound to shield the radiation workers and patient inside the X-ray room during the X-ray procedure. An iron layer with thickness of 0.5 cm was adequate to shield almost completely the reflected photons and ambient dose for X-ray 150 kVp source</description><subject>Dosage</subject><subject>Elastic scattering</subject><subject>Gadolinium</subject><subject>Photons</subject><subject>Radiation shielding</subject><subject>Scattering angle</subject><subject>Thickness</subject><subject>X-rays</subject><issn>1757-8981</issn><issn>1757-899X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNo9kE9LxDAQxYMouK5-BgOea2fSfwl4kUVXYcGLwt5Ckibapd3UZHvot7elsqcZ3jzePH6E3CM8InCeYlVUCRdinyJCmWIKyADhgqzOl8vzzvGa3MR4ACirPIcVedqq2rfNsRm6pPa9rWnv27GzoTFURapo_GlsWzfHb9qp0ySrljof6D4JarwlV0610d79zzX5en353Lwlu4_t--Z5lxisBCQmEyVzbGogtFOZyZjTjuW55lyhZsYIxTiHwhimCw7WVqyeZCVEroVGna3Jw5LbB_872HiSBz-E4_RSsgIZE3lR4uSqFpcJPsZgnexD06kwSgQ5o5IzBDkDkTMqiXJBlf0BPPxb5Q</recordid><startdate>20210301</startdate><enddate>20210301</enddate><creator>Tajudin, S M</creator><creator>Aminordin Sabri, A H</creator><creator>Abdul Aziz, M Z</creator><creator>Tabbakh, F</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>KB.</scope><scope>L6V</scope><scope>M7S</scope><scope>PDBOC</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope></search><sort><creationdate>20210301</creationdate><title>Gadolinium-doped polymeric as a shielding material for X-ray</title><author>Tajudin, S M ; Aminordin Sabri, A H ; Abdul Aziz, M Z ; Tabbakh, F</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1790-c3962f27579bfa3c32fbf244b88a1b2cc9a28805cc2b580ee72db2ca994b9b1b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Dosage</topic><topic>Elastic scattering</topic><topic>Gadolinium</topic><topic>Photons</topic><topic>Radiation shielding</topic><topic>Scattering angle</topic><topic>Thickness</topic><topic>X-rays</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tajudin, S M</creatorcontrib><creatorcontrib>Aminordin Sabri, A H</creatorcontrib><creatorcontrib>Abdul Aziz, M Z</creatorcontrib><creatorcontrib>Tabbakh, F</creatorcontrib><collection>CrossRef</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central</collection><collection>SciTech Premium Collection</collection><collection>Materials Science Database</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Materials Science Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering collection</collection><jtitle>IOP conference series. Materials Science and Engineering</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tajudin, S M</au><au>Aminordin Sabri, A H</au><au>Abdul Aziz, M Z</au><au>Tabbakh, F</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Gadolinium-doped polymeric as a shielding material for X-ray</atitle><jtitle>IOP conference series. Materials Science and Engineering</jtitle><date>2021-03-01</date><risdate>2021</risdate><volume>1106</volume><issue>1</issue><spage>12010</spage><pages>12010-</pages><issn>1757-8981</issn><eissn>1757-899X</eissn><abstract>A relatively new polymeric base compounds (CnH2n) had been proposed as a shielding material for 150 keV photon for an X-ray laboratory. When doped with 8 % gadolinium (Gd), a thickness of 2 cm shielding compound (6 g cm
−3
) could attenuate more than 90 % of the incident photons with an average dose rate reduction of more than 88 % for 150 keV incident photon. While considering the transmitted photons after the shielding, it is necessary to account for reflected photons and its dose contribution. The reflected photons and ambient dose equivalent were calculated for single-photon energy of 150 keV and an X-ray of 150 kVp. The shielding compound was successfully attenuated most of the incident photon energies particularly below 90 keV. In both cases of photon sources, two significant reflected photon peaks at ~40 and 50 keV were observed as a result of Gd characteristic X-rays. A Compton scattered photon at energy of 95 keV appeared as a result of large scattering angle within 130° -140° for 150 keV incident photons. Thus it is necessary to add a thin inner layer at the source-facing side of the shielding compound to shield the radiation workers and patient inside the X-ray room during the X-ray procedure. An iron layer with thickness of 0.5 cm was adequate to shield almost completely the reflected photons and ambient dose for X-ray 150 kVp source</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/1757-899X/1106/1/012010</doi><oa>free_for_read</oa></addata></record> |
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subjects | Dosage Elastic scattering Gadolinium Photons Radiation shielding Scattering angle Thickness X-rays |
title | Gadolinium-doped polymeric as a shielding material for X-ray |
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