The Interaction Force Between a Permanent Magnet and a Superconducting Ring
The interaction force between a small magnet and a superconducting ring in assumptions of the Meissner state was analyzed using the dipole-dipole interaction model. Two configurations were evaluated: the vertical configuration when the magnetic moment lies parallel to the symmetry axis of the ring a...
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| Veröffentlicht in: | IEEE transactions on applied superconductivity 2007-09, Vol.17 (3), p.3814-3818 |
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| container_end_page | 3818 |
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| container_issue | 3 |
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| container_title | IEEE transactions on applied superconductivity |
| container_volume | 17 |
| creator | Alzoubi, F.Y. Alqadi, M.K. Al-Khateeb, H.M. Ayoub, N.Y. |
| description | The interaction force between a small magnet and a superconducting ring in assumptions of the Meissner state was analyzed using the dipole-dipole interaction model. Two configurations were evaluated: the vertical configuration when the magnetic moment lies parallel to the symmetry axis of the ring and the horizontal when it is perpendicular. The levitation force on the magnet increases by decreasing the distance from the center of the ring up to a maximum value and then decreases down to zero when the magnet is exactly at the center of the ring. The levitation force when the magnet is in the horizontal configuration is mostly higher than that when it is in the vertical configuration. Simulation results were compared with experimental results reported in literature. |
| doi_str_mv | 10.1109/TASC.2007.902108 |
| format | Article |
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Two configurations were evaluated: the vertical configuration when the magnetic moment lies parallel to the symmetry axis of the ring and the horizontal when it is perpendicular. The levitation force on the magnet increases by decreasing the distance from the center of the ring up to a maximum value and then decreases down to zero when the magnet is exactly at the center of the ring. The levitation force when the magnet is in the horizontal configuration is mostly higher than that when it is in the vertical configuration. Simulation results were compared with experimental results reported in literature.</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2007.902108</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Applied sciences ; Electronics ; Exact sciences and technology ; Flux pinning ; High temperature superconductors ; Horizontal ; Levitation ; Levitation force ; Magnetic analysis ; Magnetic fields ; Magnetic flux ; Magnetic levitation ; Magnetic moment ; Meissner state ; Permanent magnets ; Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices ; Simulation ; Superconducting devices ; Superconducting magnetic energy storage ; Superconducting magnets ; superconducting ring ; Superconductivity ; Symmetry ; Type II superconductors</subject><ispartof>IEEE transactions on applied superconductivity, 2007-09, Vol.17 (3), p.3814-3818</ispartof><rights>2007 INIST-CNRS</rights><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. 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Two configurations were evaluated: the vertical configuration when the magnetic moment lies parallel to the symmetry axis of the ring and the horizontal when it is perpendicular. The levitation force on the magnet increases by decreasing the distance from the center of the ring up to a maximum value and then decreases down to zero when the magnet is exactly at the center of the ring. The levitation force when the magnet is in the horizontal configuration is mostly higher than that when it is in the vertical configuration. Simulation results were compared with experimental results reported in literature.</description><subject>Applied sciences</subject><subject>Electronics</subject><subject>Exact sciences and technology</subject><subject>Flux pinning</subject><subject>High temperature superconductors</subject><subject>Horizontal</subject><subject>Levitation</subject><subject>Levitation force</subject><subject>Magnetic analysis</subject><subject>Magnetic fields</subject><subject>Magnetic flux</subject><subject>Magnetic levitation</subject><subject>Magnetic moment</subject><subject>Meissner state</subject><subject>Permanent magnets</subject><subject>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</subject><subject>Simulation</subject><subject>Superconducting devices</subject><subject>Superconducting magnetic energy storage</subject><subject>Superconducting magnets</subject><subject>superconducting ring</subject><subject>Superconductivity</subject><subject>Symmetry</subject><subject>Type II superconductors</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2007</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNqFkU1P3DAQhqMKpPLRe6VeIiTglGX8MY59hBVQBKhV2Z4tx5lA0K6z2Imq_vt6taiVOJTLzGjmeUdjv0XxmcGMMTBni_OH-YwD1DMDnIH-UOwxRF1xZLiTa0BWac7Fx2I_pWcAJrXEveJ28UTlTRgpOj_2QyivhuipvKDxF1EoXfmd4soFCmN57x4DjaULbW4_TGuKfgjtlGXhsfyRw2Gx27llok-v-aD4eXW5mH-t7r5d38zP7yovGY6VNxzRa1XLjjdeKmx4JzVRh4CKVIsC0Pm6aZgxRvLWaKmIMy9b4ZoaSBwUp9u96zi8TJRGu-qTp-Uy3zlMyRoQSmom8V1SayPqWiLP5Ml_SSGlUjWvM3j0Bnwephjye61h-X-5ApEh2EI-DilF6uw69isXf1sGdmOX3dhlN3bZrV1Zcvy61yXvll10wffpn86AMihZ5r5suZ6I_o4lN9owJf4AZr2bPA</recordid><startdate>20070901</startdate><enddate>20070901</enddate><creator>Alzoubi, F.Y.</creator><creator>Alqadi, M.K.</creator><creator>Al-Khateeb, H.M.</creator><creator>Ayoub, N.Y.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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Microelectronics. Optoelectronics. Solid state devices</topic><topic>Simulation</topic><topic>Superconducting devices</topic><topic>Superconducting magnetic energy storage</topic><topic>Superconducting magnets</topic><topic>superconducting ring</topic><topic>Superconductivity</topic><topic>Symmetry</topic><topic>Type II superconductors</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Alzoubi, F.Y.</creatorcontrib><creatorcontrib>Alqadi, M.K.</creatorcontrib><creatorcontrib>Al-Khateeb, H.M.</creatorcontrib><creatorcontrib>Ayoub, N.Y.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><jtitle>IEEE transactions on applied superconductivity</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Alzoubi, F.Y.</au><au>Alqadi, M.K.</au><au>Al-Khateeb, H.M.</au><au>Ayoub, N.Y.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The Interaction Force Between a Permanent Magnet and a Superconducting Ring</atitle><jtitle>IEEE transactions on applied superconductivity</jtitle><stitle>TASC</stitle><date>2007-09-01</date><risdate>2007</risdate><volume>17</volume><issue>3</issue><spage>3814</spage><epage>3818</epage><pages>3814-3818</pages><issn>1051-8223</issn><eissn>1558-2515</eissn><coden>ITASE9</coden><abstract>The interaction force between a small magnet and a superconducting ring in assumptions of the Meissner state was analyzed using the dipole-dipole interaction model. Two configurations were evaluated: the vertical configuration when the magnetic moment lies parallel to the symmetry axis of the ring and the horizontal when it is perpendicular. The levitation force on the magnet increases by decreasing the distance from the center of the ring up to a maximum value and then decreases down to zero when the magnet is exactly at the center of the ring. The levitation force when the magnet is in the horizontal configuration is mostly higher than that when it is in the vertical configuration. Simulation results were compared with experimental results reported in literature.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/TASC.2007.902108</doi><tpages>5</tpages></addata></record> |
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| identifier | ISSN: 1051-8223 |
| ispartof | IEEE transactions on applied superconductivity, 2007-09, Vol.17 (3), p.3814-3818 |
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| language | eng |
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| source | IEEE Electronic Library (IEL) |
| subjects | Applied sciences Electronics Exact sciences and technology Flux pinning High temperature superconductors Horizontal Levitation Levitation force Magnetic analysis Magnetic fields Magnetic flux Magnetic levitation Magnetic moment Meissner state Permanent magnets Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices Simulation Superconducting devices Superconducting magnetic energy storage Superconducting magnets superconducting ring Superconductivity Symmetry Type II superconductors |
| title | The Interaction Force Between a Permanent Magnet and a Superconducting Ring |
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