1998
DOI: 10.1016/s0921-4534(97)01773-5
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AC transport current losses of multifilamentary Bi(2223) tapes with varying filament geometries

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1998
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Cited by 46 publications
(34 citation statements)
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“…With these, a direct prove on the magneto-coupling physical mechanism that gives place to the field deformations inside SC-SFM heterostructures, these being observed by magneto optical imaging techniques 39,41,43,69 , has been provided. Likewise, the cause of the intriguing increment in the AC-losses in SC-SFM heterostructures [36][37][38] , is explained as result of the found magneto-steady coupling between the SC and the SFM sheath. Thus, we have proven that the sole coupling between the SC and a SFM sheath is capable to produce a slight rise in the AC-losses at the SC material, even when the SFM does not add any electrical nor magnetic losses to the system.…”
Section: Discussionmentioning
confidence: 99%
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“…With these, a direct prove on the magneto-coupling physical mechanism that gives place to the field deformations inside SC-SFM heterostructures, these being observed by magneto optical imaging techniques 39,41,43,69 , has been provided. Likewise, the cause of the intriguing increment in the AC-losses in SC-SFM heterostructures [36][37][38] , is explained as result of the found magneto-steady coupling between the SC and the SFM sheath. Thus, we have proven that the sole coupling between the SC and a SFM sheath is capable to produce a slight rise in the AC-losses at the SC material, even when the SFM does not add any electrical nor magnetic losses to the system.…”
Section: Discussionmentioning
confidence: 99%
“…5. In this sense, we have arrived to a fully analytical solution for the magnetic vector potential and the distribution of the magnetic field inside the SC core of a cylindrical SC-SFM metastructure, it subjected to an AC transport current and under self-field conditions, allowing to demonstrate the physics origin of the deformations of the magnetic field inside the SC observed by magneto optical imaging techniques 39,41,43,69 , and the intriguing increment in the AC-losses as result of the magneto-steady coupling between the SC and the SFM sheath [36][37][38] . The time interval between columns is ∆t = (π/4)ω −1 , such that the dynamics shown between the second column (ωt = 3 * π/2) and last column (ωt = π/2) represents the minimum hysteresis period for the calculation of AC Losses, in accordance with the distribution of profiles of current density shown in Fig.…”
Section: Multipole Expansion Of the Critical State Model In Sc-sfm Romentioning
confidence: 99%
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“…Firstly, demonstrating that the origin of the deformations of the magnetic field inside SC-SFM wires reported by MOI techniques [ 39 , 41 , 43 , 80 ] is a direct consequence of the magneto-steady coupling between the SC and the SFM sheath. Secondly, with our extended CST it will be proven that a straightforward explanation of the intriguing increment in the AC-losses of SC-SFM metastructures [ 36 , 37 , 38 ] can be achieved without the ansatz of overcritical currents.…”
Section: Multipole Expansion Of the Cst In Rounded Sc-sfm Heterostructuresmentioning
confidence: 99%
“…However, a direct involvement of the inductive coupling elements between the profiles of current density in SC wires and finite SFM sheaths is still to be achieved, such that the understanding of the actual physical mechanism that couples their macroscopic magnetic features is not hindered. In fact, a theoretical explanation for the increment of the AC losses in monocore SC-SFM heterostructures at self-field conditions, that is, under applied transport current but no external magnetic field, has not been reached for even the simplest configuration of an SC-SFM wire of a cylindrical cross section, a problem that has remained open for about two decades [ 36 , 37 , 38 ].…”
Section: Introductionmentioning
confidence: 99%