{"id":20440,"date":"2025-05-19T15:26:19","date_gmt":"2025-05-19T13:26:19","guid":{"rendered":"https:\/\/lncmi.cnrs.fr\/?page_id=20440"},"modified":"2025-05-19T15:29:47","modified_gmt":"2025-05-19T13:29:47","slug":"static-fields-more-details","status":"publish","type":"page","link":"https:\/\/lncmi.cnrs.fr\/en\/static-fields\/static-fields-more-details\/","title":{"rendered":"Static fields – more details"},"content":{"rendered":"

[et_pb_section fb_built=”1″ _builder_version=”4.25.1″ _module_preset=”default” width=”99.8%” locked=”off” global_colors_info=”{}”][et_pb_row module_id=”aimants” _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”][dsm_text_divider header=”MORE DETAILS – The hybrid electromagnet” _builder_version=”4.27.4″ _module_preset=”default” hover_enabled=”0″ global_colors_info=”{}” sticky_enabled=”0″][\/dsm_text_divider][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=”4.27.4″ _module_preset=”default” hover_enabled=”0″ module_alignment_tablet=”center” module_alignment_phone=”center” module_alignment_last_edited=”on|phone” global_colors_info=”{}” custom_padding=”0px||2px|||” module_alignment=”center” sticky_enabled=”0″][et_pb_column type=”4_4″ _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”][et_pb_text content_tablet=”” content_phone=”” content_last_edited=”on|phone” _builder_version=”4.27.4″ _module_preset=”default” text_font_size=”12px” hover_enabled=”0″ text_text_color_tablet=”” text_text_color_phone=”” text_text_color_last_edited=”on|phone” text_orientation_tablet=”” text_orientation_phone=”center” text_orientation_last_edited=”on|phone” global_colors_info=”{}” sticky_enabled=”0″]<\/p>\n

<\/strong>Contact\u00a0: <\/strong>pierre.pugnat@lncmi.cnrs.fr<\/a><\/p>\n

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Fig. 3:<\/strong> Overview of the Grenoble hybrid electromagnet equipment and its integration into the LNCMI.<\/p>\n

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 <\/p>\n\n\n\n\n\n\n\n\n
Magnetic field\u00a0 (T)<\/strong><\/td>\nRoom temperature diam. bore (mm)<\/strong><\/td>\nCoils<\/strong><\/td>\nApproximate Power (MW)<\/strong><\/td>\n<\/tr>\n
43<\/td>\n34<\/td>\n1 polyhelix, 2 Bitter, supercond.<\/td>\n24<\/td>\n<\/tr>\n
40<\/td>\n50<\/td>\n1 polyhelix, 2 Bitter, supercond.<\/td>\n24<\/td>\n<\/tr>\n
27<\/td>\n170<\/td>\n1 polyhelix, 2 Bitter, supercond.<\/td>\n18<\/td>\n<\/tr>\n
17.5<\/td>\n375<\/td>\n2 Bitter, supercond.<\/td>\n12<\/td>\n<\/tr>\n
9<\/td>\n810<\/td>\nSuperconding coil alone<\/td>\n0.4<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

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Table 1: Magnetic field and flux configurations of the Grenoble hybrid magnet. To minimize risks, these magnetic field values will be achieved gradually.<\/p>\n

[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”][et_pb_column type=”4_4″ _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”][et_pb_accordion _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”][et_pb_accordion_item title=”References” open=”on” _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}”]<\/p>\n

[1] https:\/\/scitechdaily.com\/chinas-42-tesla-magnet-shatters-previous-u-s-record\/<\/a><\/p>\n

[2] G. Claudet et al.<\/em>, \u201cThe design and operation of a refrigerator system using superfluid helium\u00a0\u201d, Proceedings of the 5th<\/sup> international cryogenic engineering conference (ICEC-5), Kyoto, 1974, p. 265-267.<\/p>\n

[3] L. Ronayette et al.<\/em>, \u201cCryogenic system for the 43 T Hybrid Magnet at LNCMI Grenoble: from the needs to the commissioning\u201d, IOP Conf. Series: Materials Science and Engineering, vol. 171, 012107 (2017), DOI 10.1088\/1757-899X\/171\/1\/012107<\/p>\n

[4] P. Pugnat et al.<\/em>, \u201c43+T Grenoble Hybrid Magnet: From Final Assembly to Commissioning of the Superconducting Outsert \u201d, IEEE Transactions on Applied Superconductivity, vol. 32, no. 6, pp. 1-7, Sept. 2022, doi: 10.1109\/TASC.2022.3151838<\/p>\n

[5] P. Pugnat et al.<\/em>, \u201cCommissioning Tests of the 43+T Grenoble Hybrid Magnet\u201d, IEEE Transactions on Applied Superconductivity, vol. 34, no. 5, pp. 1-5, Aug. 2024, Art no. 4300305, doi: 10.1109\/TASC.2023.3341864<\/p>\n

[6] https:\/\/www.alpes.cnrs.fr\/fr\/laimant-hybride-du-lncmi-atteint-42-tesla<\/a><\/p>\n

[7] P. Pugnat et al.<\/em>,\u201cGrAHal-CAPP for axion dark matter search with unprecedented sensitivity in the 1-3 \u00b5eV mass range\u201d, Front. Phys., Sec. High-Energy and Astroparticle Physics, Volume 12 \u2013 2024 | doi: 10.3389\/fphy.2024.1358810<\/p>\n

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Pugnat et al.<\/em>, \u201cCommissioning Tests of the 43+T Grenoble Hybrid Magnet\u201d, IEEE Transactions on Applied Superconductivity, vol. 34, no. 5, pp. 1-5, Aug. 2024, Art no. 4300305, doi: 10.1109\/TASC.2023.3341864<\/p>\n

Pugnat et al.<\/em>, \u201c43+T Grenoble Hybrid Magnet: From Final Assembly to Commissioning of the Superconducting Outsert \u201d, IEEE Transactions on Applied Superconductivity, vol. 32, no. 6, pp. 1-7, Sept. 2022, doi: 10.1109\/TASC.2022.3151838<\/p>\n

Pugnat et al.<\/em>, \u201cFrom Manufacture to Assembly of the 43 T Grenoble Hybrid Magnet \u201d, IEEE Transactions on Applied Superconductivity, vol. 30, no. 4, pp. 1-5, June 2020, doi: 10.1109\/TASC.2020.2972509<\/p>\n

J. Schneider-Muntau et al.<\/em>, \u201cUltimate Forces of the Grenoble Hybrid Magnet\u201d, IEEE Trans. Appl. Supercond., vol. 28, no. 3, pp. 1-6, April 2018, doi: 10.1109\/TASC.2017.2783345<\/p>\n

Pugnat et al.<\/em>, \u201cProgress in the Construction of the 43 T Hybrid Magnet at LNCMI-Grenoble \u201d, IEEE Transactions on Applied Superconductivity, vol. 28, no. 3, pp. 1-7, April 2018, doi: 10.1109\/TASC.2017.2780820<\/p>\n

Pugnat et al.<\/em>, \u201cIn-House Industrial Production of the Superconducting Conductor for the 43 T Hybrid Magnet of LNCMI-Grenoble\u201d, IEEE Transactions on Applied Superconductivity, vol. 28, no. 4, pp. 1-5, June 2018, doi: 10.1109\/TASC.2018.2797548<\/p>\n

Ronayette et al.<\/em>, \u201cCryogenic system for the 43 T Hybrid Magnet at LNCMI Grenoble: from the needs to the commissioning\u201d, IOP Conf. Series: Materials Science and Engineering, vol. 171, 012107 (2017), DOI 10.1088\/1757-899X\/171\/1\/012107<\/p>\n

Fazilleau et al.<\/em>, \u201cRole and Impact of the Eddy Current Shield in the LNCMI-G Hybrid Magnet\u201d, IEEE Transactions on Applied Superconductivity, vol. 26, no. 4, pp. 1-5, June 2016, doi: 10.1109\/TASC.2016.2525018<\/p>\n

Pes et al.<\/em>, \u201cTwo-Dimensional and Three-Dimensional Mechanical Analysis of the Superconducting Outsert of the LNCMI Hybrid Magnet\u201d, IEEE Transactions on Applied Superconductivity, vol. 26, no. 4, pp. 1-5, June 2016, doi: 10.1109\/TASC.2016.2518747<\/p>\n

Manil et al.<\/em>, \u201cDynamical response of a hybrid magnet structure featuring eddy current shield during transient failure mode\u201d, IEEE Transactions on Applied Superconductivity, vol. 24, no. 3, pp. 1-6, June 2014, doi: 10.1109\/TASC.2013.2286351<\/p>\n

Hervieu et al.<\/em>, \u201cCryogenic design of the 43 T LNCMI Grenoble hybrid magnet\u201d, Physics Procedia, Volume 67, Pages 692\u2013697 (2015), https:\/\/doi.org\/10.1016\/j.phpro.2015.06.117<\/a><\/p>\n

Pfister et al.<\/em>, \u201cA New Test Station to Measure the Critical Current of Superconducting Strands\u201d, IEEE Transactions on Applied Superconductivity, vol. 22, no. 3, pp. 9500504-9500504, June 2012, doi: 10.1109\/TASC.2011.2178581<\/p>\n

Pugnat et al.<\/em>, \u201cStudy and Development of the Superconducting Conductor for the Grenoble Hybrid Magnet\u201d, IEEE Transactions on Applied Superconductivity, vol. 22, no. 3, pp. 6001604-6001604, June 2012, doi: 10.1109\/TASC.2011.2180882<\/p>\n

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Abir1<\/sup>, R. Barbier1<\/sup>, C. Berriaud2,<\/sup>*, R. Berthier2<\/sup>, F. Debray1<\/sup>, T. Disparti1<\/sup>, P. Fazilleau2<\/sup>, P. Graffin2<\/sup>, C. Grandcl\u00e9ment1<\/sup>, B. Hervieu2,<\/sup>*, F. P. Juster2<\/sup>, M. Kamke1<\/sup>, S. Kr\u00e4mer1<\/sup>, Y. Krupko1<\/sup>, P. Manil2<\/sup>, J. Allard2<\/sup>, F. Molini\u00e92<\/sup>, H. Neyrial2<\/sup>, K. Paillot1<\/sup>, M. Pelloux1<\/sup>, C. Pes2<\/sup>, R. Pfister1<\/sup>, L. Ronayette1,<\/sup>**, C. Trophime1<\/sup>, J. M. Tudela1<\/sup>, E. Verney1<\/sup>, E. Yildiz1<\/sup>, et P. Pugnat1,<\/sup>***<\/p>\n

Ex CDDs Projet1<\/sup> : Z. Ben Mimoun, T. Boujet, N. Bournaud-Mournetas, G. Caplane, P. Harnoux, C. Peroni, et M. Pissard, H. Xiao<\/p>\n

1 <\/sup>LNCMI, EMFL, CNRS, Universit\u00e9 Grenoble Alpes, 38042 Grenoble Cedex 9, France<\/p>\n

2<\/sup> CEA Paris-Saclay, IRFU, 91191 Gif-sur-Yvette Cedex, France<\/p>\n

 <\/p>\n

* Chefs de Projet CEA<\/em><\/p>\n

** Adjoint au chef du Projet<\/em><\/p>\n

*** Chef du Projet<\/em><\/p>\n

[\/et_pb_accordion_item][et_pb_accordion_item title=”Special Scientific & Technical Advisor” _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}” open=”off”]<\/p>\n

\u2013 Hans Scheider-Muntau, CS&T, Former Director of Magnet Science and Technology, National High Magnetic Field Laboratory, Tallahassee, US<\/p>\n

[\/et_pb_accordion_item][et_pb_accordion_item title=”International Advisory Committee of Scientific & Technical Experts” _builder_version=”4.27.4″ _module_preset=”default” global_colors_info=”{}” open=”off”]<\/p>\n

\u2013 Hans Scheider-Muntau (CS&T, Former Director of Magnet Science and Technology at NHMFL)<\/p>\n

\u2013 A. Siemko (Former Deputy Director of TE Department at CERN )<\/p>\n

\u2013 A. Herv\u00e9 (University of Wisconsin, Former Technical Coordinator of CMS at CERN)<\/p>\n

\u2013 K. Brodsinski (Former Project Leader for the LHC cryogeny operation at CERN)<\/p>\n

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 <\/p>\n

Funding<\/h3>\n

This project has been funded by CNRS, Universit\u00e9 Grenoble-Alpes and the French Ministry of Education and Research as part of the \u201cInvestissements pour l’avenir\u201d Equipex LaSUP (Large Superconducting User Platform), the European Regional Development Fund (ERDF) and the Rh\u00f4ne-Alpes region.<\/p>\n

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MORE DETAILS - The hybrid electromagnet<\/span><\/h3>\n\t\t\t\t
<\/div>\n\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t<\/div>Contact\u00a0: pierre.pugnat@lncmi.cnrs.frFig. 3: Overview of the Grenoble hybrid electromagnet equipment and its integration into the LNCMI.  Magnetic field\u00a0 (T) […]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":15238,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_et_pb_use_builder":"on","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"folder":[184],"class_list":["post-20440","page","type-page","status-publish","hentry"],"jetpack_sharing_enabled":true,"_links":{"self":[{"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/20440","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/comments?post=20440"}],"version-history":[{"count":0,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/20440\/revisions"}],"up":[{"embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/15238"}],"wp:attachment":[{"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/media?parent=20440"}],"wp:term":[{"taxonomy":"folder","embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/folder?post=20440"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}