Magnetic Design and Code Benchmarking of the SMC (Short Model Coil) Dipole Magnet
Identifieur interne : 000155 ( PascalFrancis/Checkpoint ); précédent : 000154; suivant : 000156Magnetic Design and Code Benchmarking of the SMC (Short Model Coil) Dipole Magnet
Auteurs : Pierre Manil [France] ; Federico Regis [Suisse] ; James Rochford [Royaume-Uni] ; Paolo Fessia [Suisse] ; Simon Canfer [Royaume-Uni] ; Elwyn Baynham [Royaume-Uni] ; François Nunio [France] ; Gijs De Rijk [Suisse] ; Pierre Vedrine [France]Source :
- IEEE transactions on applied superconductivity [ 1051-8223 ] ; 2010.
Descripteurs français
- Pascal (Inist)
- Codage, Benchmarking, Dipôle, Aimant accélérateur, Europe, Modèle réduit, CERN, Technique poudre dans tube, Toron, Dégradation, Endommagement, Propriété magnétique, Précontrainte, Champ intense, Modèle 3 dimensions, Modèle non linéaire, Méthode paramétrique, Implémentation, Optimisation, Cale espacement, Electroaimant supraconducteur.
- Wicri :
- topic : Codage.
English descriptors
- KwdEn :
- Accelerator magnets, Benchmarking, CERN, Coding, Damaging, Degradation, Dipole, Europe, High field, Implementation, Magnetic properties, Non linear model, Optimization, Parametric method, Powder in tube technique, Prestress, Scale model, Spacer, Strand, Superconducting magnet, Three dimensional model.
Abstract
The Short Model Coil (SMC) working group was set in February 2007 within the Next European Dipole (NED) program, in order to develop a short-scale model of a Nb3Sn dipole magnet. The SMC group comprises four laboratories: CERN/TE-MSC group (CH), CEA/IRFU (FR), RAL (UK) and LBNL (US). The SMC magnet is designed to reach a peak field of about 13 Tesla (T) on conductor, using a 2500 A/mm2 Powder-In-Tube (PIT) strand. The aim of this magnet device is to study the degradation of the magnetic properties of the Nb3Sn cable, by applying different levels of pre-stress. To fully satisfy this purpose, a versatile and easy-to-assemble structure has been realized. The design of the SMC magnet has been developed from an existing dipole magnet, the SD01, designed, built and tested at LBNL with support from CEA. The goal of the magnetic design presented in this paper is to match the high field region with the high stress region, located along the dipole straight section. For this purpose, three-dimensional nonlinear parametric models have been implemented using three codes (CAST3M, ANSYS, and OPERA). This optimization process has been an opportunity to cross-check the codes. The results of this benchmarking are presented here, along with the final design which incorporates the use of end spacers and a surrounding iron structure to deliver a nominal field of 13 T uniformly distributed along the cable straight section.
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sort="Baynham, Elwyn" uniqKey="Baynham E" first="Elwyn" last="Baynham">Elwyn Baynham</name><affiliation wicri:level="1"><inist:fA14 i1="04"><s1>RAL/STFC, Harwell Science and Innovation Campus</s1><s2>Didcot</s2><s3>GBR</s3><sZ>3 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ></inist:fA14><country>Royaume-Uni</country><wicri:noRegion>Didcot</wicri:noRegion></affiliation></author><author><name sortKey="Nunio, Francois" sort="Nunio, Francois" uniqKey="Nunio F" first="François" last="Nunio">François Nunio</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>CEA Saclay/IRFU/SIS</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>7 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Île-de-France</region><settlement type="city">Gif-sur-Yvette</settlement></placeName></affiliation></author><author><name sortKey="De Rijk, Gijs" sort="De Rijk, Gijs" uniqKey="De Rijk G" first="Gijs" last="De Rijk">Gijs De Rijk</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>CERN (European Organization for Nuclear Research)</s1><s3>CHE</s3><sZ>2 aut.</sZ><sZ>4 aut.</sZ><sZ>8 aut.</sZ></inist:fA14><country>Suisse</country><wicri:noRegion>CERN (European Organization for Nuclear Research)</wicri:noRegion></affiliation></author><author><name sortKey="Vedrine, Pierre" sort="Vedrine, Pierre" uniqKey="Vedrine P" first="Pierre" last="Vedrine">Pierre Vedrine</name><affiliation wicri:level="3"><inist:fA14 i1="02"><s1>CEA Saclay/IRFU/SACM</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>9 aut.</sZ></inist:fA14><country>France</country><placeName><region type="region" nuts="2">Île-de-France</region><settlement type="city">Gif-sur-Yvette</settlement></placeName></affiliation></author></analytic><series><title level="j" type="main">IEEE transactions on applied superconductivity</title><title level="j" type="abbreviated">IEEE trans. appl. supercond.</title><idno type="ISSN">1051-8223</idno><imprint><date when="2010">2010</date></imprint></series></biblStruct></sourceDesc><seriesStmt><title level="j" type="main">IEEE transactions on applied superconductivity</title><title level="j" type="abbreviated">IEEE trans. appl. supercond.</title><idno type="ISSN">1051-8223</idno></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Accelerator magnets</term><term>Benchmarking</term><term>CERN</term><term>Coding</term><term>Damaging</term><term>Degradation</term><term>Dipole</term><term>Europe</term><term>High field</term><term>Implementation</term><term>Magnetic properties</term><term>Non linear model</term><term>Optimization</term><term>Parametric method</term><term>Powder in tube technique</term><term>Prestress</term><term>Scale model</term><term>Spacer</term><term>Strand</term><term>Superconducting magnet</term><term>Three dimensional model</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Codage</term><term>Benchmarking</term><term>Dipôle</term><term>Aimant accélérateur</term><term>Europe</term><term>Modèle réduit</term><term>CERN</term><term>Technique poudre dans tube</term><term>Toron</term><term>Dégradation</term><term>Endommagement</term><term>Propriété magnétique</term><term>Précontrainte</term><term>Champ intense</term><term>Modèle 3 dimensions</term><term>Modèle non linéaire</term><term>Méthode paramétrique</term><term>Implémentation</term><term>Optimisation</term><term>Cale espacement</term><term>Electroaimant supraconducteur</term></keywords><keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Codage</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">The Short Model Coil (SMC) working group was set in February 2007 within the Next European Dipole (NED) program, in order to develop a short-scale model of a Nb<sub>3</sub>Sn dipole magnet. The SMC group comprises four laboratories: CERN/TE-MSC group (CH), CEA/IRFU (FR), RAL (UK) and LBNL (US). The SMC magnet is designed to reach a peak field of about 13 Tesla (T) on conductor, using a 2500 A/mm<sup>2</sup> Powder-In-Tube (PIT) strand. The aim of this magnet device is to study the degradation of the magnetic properties of the Nb<sub>3</sub>Sn cable, by applying different levels of pre-stress. To fully satisfy this purpose, a versatile and easy-to-assemble structure has been realized. The design of the SMC magnet has been developed from an existing dipole magnet, the SD01, designed, built and tested at LBNL with support from CEA. The goal of the magnetic design presented in this paper is to match the high field region with the high stress region, located along the dipole straight section. For this purpose, three-dimensional nonlinear parametric models have been implemented using three codes (CAST3M, ANSYS, and OPERA). This optimization process has been an opportunity to cross-check the codes. The results of this benchmarking are presented here, along with the final design which incorporates the use of end spacers and a surrounding iron structure to deliver a nominal field of 13 T uniformly distributed along the cable straight section.</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>1051-8223</s0></fA01><fA03 i2="1"><s0>IEEE trans. appl. supercond.</s0></fA03><fA05><s2>20</s2></fA05><fA06><s2>3</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>Magnetic Design and Code Benchmarking of the SMC (Short Model Coil) Dipole Magnet</s1></fA08><fA09 i1="01" i2="1" l="ENG"><s1>THE TWENTY-FIRST INTERNATIONAL CONFERENCE ON MAGNET TECHNOLOGY, Hefei, Anhui, China, October 18-23, 2009</s1></fA09><fA11 i1="01" i2="1"><s1>MANIL (Pierre)</s1></fA11><fA11 i1="02" i2="1"><s1>REGIS (Federico)</s1></fA11><fA11 i1="03" i2="1"><s1>ROCHFORD (James)</s1></fA11><fA11 i1="04" i2="1"><s1>FESSIA (Paolo)</s1></fA11><fA11 i1="05" i2="1"><s1>CANFER (Simon)</s1></fA11><fA11 i1="06" i2="1"><s1>BAYNHAM (Elwyn)</s1></fA11><fA11 i1="07" i2="1"><s1>NUNIO (François)</s1></fA11><fA11 i1="08" i2="1"><s1>DE RIJK (Gijs)</s1></fA11><fA11 i1="09" i2="1"><s1>VEDRINE (Pierre)</s1></fA11><fA14 i1="01"><s1>CEA Saclay/IRFU/SIS</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>1 aut.</sZ><sZ>7 aut.</sZ></fA14><fA14 i1="02"><s1>CEA Saclay/IRFU/SACM</s1><s2>91191 Gif-sur-Yvette</s2><s3>FRA</s3><sZ>9 aut.</sZ></fA14><fA14 i1="03"><s1>CERN (European Organization for Nuclear Research)</s1><s3>CHE</s3><sZ>2 aut.</sZ><sZ>4 aut.</sZ><sZ>8 aut.</sZ></fA14><fA14 i1="04"><s1>RAL/STFC, Harwell Science and Innovation Campus</s1><s2>Didcot</s2><s3>GBR</s3><sZ>3 aut.</sZ><sZ>5 aut.</sZ><sZ>6 aut.</sZ></fA14><fA18 i1="01" i2="1"><s1>Institute of Electrical and Electronic Engineers (IEEE)</s1><s2>New York, NY</s2><s3>USA</s3><s9>org-cong.</s9></fA18><fA20><s1>184-187</s1></fA20><fA21><s1>2010</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>22424</s2><s5>354000193038910150</s5></fA43><fA44><s0>0000</s0><s1>© 2010 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>13 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>10-0294578</s0></fA47><fA60><s1>P</s1><s2>C</s2></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>IEEE transactions on applied superconductivity</s0></fA64><fA66 i1="01"><s0>USA</s0></fA66><fC01 i1="01" l="ENG"><s0>The Short Model Coil (SMC) working group was set in February 2007 within the Next European Dipole (NED) program, in order to develop a short-scale model of a Nb<sub>3</sub>Sn dipole magnet. The SMC group comprises four laboratories: CERN/TE-MSC group (CH), CEA/IRFU (FR), RAL (UK) and LBNL (US). The SMC magnet is designed to reach a peak field of about 13 Tesla (T) on conductor, using a 2500 A/mm<sup>2</sup> Powder-In-Tube (PIT) strand. The aim of this magnet device is to study the degradation of the magnetic properties of the Nb<sub>3</sub>Sn cable, by applying different levels of pre-stress. To fully satisfy this purpose, a versatile and easy-to-assemble structure has been realized. The design of the SMC magnet has been developed from an existing dipole magnet, the SD01, designed, built and tested at LBNL with support from CEA. The goal of the magnetic design presented in this paper is to match the high field region with the high stress region, located along the dipole straight section. For this purpose, three-dimensional nonlinear parametric models have been implemented using three codes (CAST3M, ANSYS, and OPERA). This optimization process has been an opportunity to cross-check the codes. The results of this benchmarking are presented here, along with the final design which incorporates the use of end spacers and a surrounding iron structure to deliver a nominal field of 13 T uniformly distributed along the cable straight section.</s0></fC01><fC02 i1="01" i2="X"><s0>001D05G01</s0></fC02><fC03 i1="01" i2="X" l="FRE"><s0>Codage</s0><s5>01</s5></fC03><fC03 i1="01" i2="X" l="ENG"><s0>Coding</s0><s5>01</s5></fC03><fC03 i1="01" i2="X" l="SPA"><s0>Codificación</s0><s5>01</s5></fC03><fC03 i1="02" i2="X" l="FRE"><s0>Benchmarking</s0><s5>02</s5></fC03><fC03 i1="02" i2="X" l="ENG"><s0>Benchmarking</s0><s5>02</s5></fC03><fC03 i1="02" i2="X" l="SPA"><s0>Evaluación comparativa</s0><s5>02</s5></fC03><fC03 i1="03" i2="X" l="FRE"><s0>Dipôle</s0><s5>03</s5></fC03><fC03 i1="03" i2="X" l="ENG"><s0>Dipole</s0><s5>03</s5></fC03><fC03 i1="03" i2="X" l="SPA"><s0>Dipolo</s0><s5>03</s5></fC03><fC03 i1="04" i2="3" l="FRE"><s0>Aimant accélérateur</s0><s5>04</s5></fC03><fC03 i1="04" i2="3" l="ENG"><s0>Accelerator magnets</s0><s5>04</s5></fC03><fC03 i1="05" i2="X" l="FRE"><s0>Europe</s0><s2>NG</s2><s5>05</s5></fC03><fC03 i1="05" i2="X" l="ENG"><s0>Europe</s0><s2>NG</s2><s5>05</s5></fC03><fC03 i1="05" i2="X" l="SPA"><s0>Europa</s0><s2>NG</s2><s5>05</s5></fC03><fC03 i1="06" i2="X" l="FRE"><s0>Modèle réduit</s0><s5>06</s5></fC03><fC03 i1="06" i2="X" l="ENG"><s0>Scale model</s0><s5>06</s5></fC03><fC03 i1="06" i2="X" l="SPA"><s0>Modelo reducido</s0><s5>06</s5></fC03><fC03 i1="07" i2="3" l="FRE"><s0>CERN</s0><s5>07</s5></fC03><fC03 i1="07" i2="3" l="ENG"><s0>CERN</s0><s5>07</s5></fC03><fC03 i1="08" i2="X" l="FRE"><s0>Technique poudre dans tube</s0><s5>08</s5></fC03><fC03 i1="08" i2="X" l="ENG"><s0>Powder in tube technique</s0><s5>08</s5></fC03><fC03 i1="08" i2="X" l="SPA"><s0>Tecnica polvo en tubo</s0><s5>08</s5></fC03><fC03 i1="09" i2="X" l="FRE"><s0>Toron</s0><s5>09</s5></fC03><fC03 i1="09" i2="X" l="ENG"><s0>Strand</s0><s5>09</s5></fC03><fC03 i1="09" i2="X" l="SPA"><s0>Bocel</s0><s5>09</s5></fC03><fC03 i1="10" i2="X" l="FRE"><s0>Dégradation</s0><s5>10</s5></fC03><fC03 i1="10" i2="X" l="ENG"><s0>Degradation</s0><s5>10</s5></fC03><fC03 i1="10" i2="X" l="SPA"><s0>Degradación</s0><s5>10</s5></fC03><fC03 i1="11" i2="X" l="FRE"><s0>Endommagement</s0><s5>11</s5></fC03><fC03 i1="11" i2="X" l="ENG"><s0>Damaging</s0><s5>11</s5></fC03><fC03 i1="11" i2="X" l="SPA"><s0>Deterioración</s0><s5>11</s5></fC03><fC03 i1="12" i2="X" l="FRE"><s0>Propriété magnétique</s0><s5>12</s5></fC03><fC03 i1="12" i2="X" l="ENG"><s0>Magnetic properties</s0><s5>12</s5></fC03><fC03 i1="12" i2="X" l="SPA"><s0>Propiedad magnética</s0><s5>12</s5></fC03><fC03 i1="13" i2="X" l="FRE"><s0>Précontrainte</s0><s5>13</s5></fC03><fC03 i1="13" i2="X" l="ENG"><s0>Prestress</s0><s5>13</s5></fC03><fC03 i1="13" i2="X" l="SPA"><s0>Pretensado</s0><s5>13</s5></fC03><fC03 i1="14" i2="X" l="FRE"><s0>Champ intense</s0><s5>14</s5></fC03><fC03 i1="14" i2="X" l="ENG"><s0>High field</s0><s5>14</s5></fC03><fC03 i1="14" i2="X" l="SPA"><s0>Campo intenso</s0><s5>14</s5></fC03><fC03 i1="15" i2="X" l="FRE"><s0>Modèle 3 dimensions</s0><s5>15</s5></fC03><fC03 i1="15" i2="X" l="ENG"><s0>Three dimensional model</s0><s5>15</s5></fC03><fC03 i1="15" i2="X" l="SPA"><s0>Modelo 3 dimensiones</s0><s5>15</s5></fC03><fC03 i1="16" i2="X" l="FRE"><s0>Modèle non linéaire</s0><s5>16</s5></fC03><fC03 i1="16" i2="X" l="ENG"><s0>Non linear model</s0><s5>16</s5></fC03><fC03 i1="16" i2="X" l="SPA"><s0>Modelo no lineal</s0><s5>16</s5></fC03><fC03 i1="17" i2="X" l="FRE"><s0>Méthode paramétrique</s0><s5>17</s5></fC03><fC03 i1="17" i2="X" l="ENG"><s0>Parametric method</s0><s5>17</s5></fC03><fC03 i1="17" i2="X" l="SPA"><s0>Método paramétrico</s0><s5>17</s5></fC03><fC03 i1="18" i2="X" l="FRE"><s0>Implémentation</s0><s5>18</s5></fC03><fC03 i1="18" i2="X" l="ENG"><s0>Implementation</s0><s5>18</s5></fC03><fC03 i1="18" i2="X" l="SPA"><s0>Implementación</s0><s5>18</s5></fC03><fC03 i1="19" i2="X" l="FRE"><s0>Optimisation</s0><s5>19</s5></fC03><fC03 i1="19" i2="X" l="ENG"><s0>Optimization</s0><s5>19</s5></fC03><fC03 i1="19" i2="X" l="SPA"><s0>Optimización</s0><s5>19</s5></fC03><fC03 i1="20" i2="X" l="FRE"><s0>Cale espacement</s0><s5>20</s5></fC03><fC03 i1="20" i2="X" l="ENG"><s0>Spacer</s0><s5>20</s5></fC03><fC03 i1="20" i2="X" l="SPA"><s0>Calce espaciamiento</s0><s5>20</s5></fC03><fC03 i1="21" i2="X" l="FRE"><s0>Electroaimant supraconducteur</s0><s5>21</s5></fC03><fC03 i1="21" i2="X" l="ENG"><s0>Superconducting magnet</s0><s5>21</s5></fC03><fC03 i1="21" i2="X" l="SPA"><s0>Electroimán supraconductor</s0><s5>21</s5></fC03><fN21><s1>186</s1></fN21><fN44 i1="01"><s1>OTO</s1></fN44><fN82><s1>OTO</s1></fN82></pA><pR><fA30 i1="01" i2="1" l="ENG"><s1>International Conference on Magnet Technology (MT)</s1><s2>21</s2><s3>Hefei, Anhui CHN</s3><s4>2009-10-18</s4></fA30></pR></standard></inist><affiliations><list><country><li>France</li><li>Royaume-Uni</li><li>Suisse</li></country><region><li>Île-de-France</li></region><settlement><li>Gif-sur-Yvette</li></settlement></list><tree><country name="France"><region name="Île-de-France"><name sortKey="Manil, Pierre" sort="Manil, Pierre" uniqKey="Manil P" first="Pierre" last="Manil">Pierre Manil</name></region><name sortKey="Nunio, Francois" sort="Nunio, Francois" uniqKey="Nunio F" first="François" last="Nunio">François Nunio</name><name sortKey="Vedrine, Pierre" sort="Vedrine, Pierre" uniqKey="Vedrine P" first="Pierre" last="Vedrine">Pierre Vedrine</name></country><country name="Suisse"><noRegion><name sortKey="Regis, Federico" sort="Regis, Federico" uniqKey="Regis F" first="Federico" last="Regis">Federico Regis</name></noRegion><name sortKey="De Rijk, Gijs" sort="De Rijk, Gijs" uniqKey="De Rijk G" first="Gijs" last="De Rijk">Gijs De Rijk</name><name sortKey="Fessia, Paolo" sort="Fessia, Paolo" uniqKey="Fessia P" first="Paolo" last="Fessia">Paolo Fessia</name></country><country name="Royaume-Uni"><noRegion><name sortKey="Rochford, James" sort="Rochford, James" uniqKey="Rochford J" first="James" last="Rochford">James Rochford</name></noRegion><name sortKey="Baynham, Elwyn" sort="Baynham, Elwyn" uniqKey="Baynham E" first="Elwyn" last="Baynham">Elwyn Baynham</name><name sortKey="Canfer, Simon" sort="Canfer, Simon" uniqKey="Canfer S" first="Simon" last="Canfer">Simon Canfer</name></country></tree></affiliations></record>Pour manipuler ce document sous Unix (Dilib)
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