People | Locations | Statistics |
---|---|---|
Naji, M. |
| |
Motta, Antonella |
| |
Aletan, Dirar |
| |
Mohamed, Tarek |
| |
Ertürk, Emre |
| |
Taccardi, Nicola |
| |
Kononenko, Denys |
| |
Petrov, R. H. | Madrid |
|
Alshaaer, Mazen | Brussels |
|
Bih, L. |
| |
Casati, R. |
| |
Muller, Hermance |
| |
Kočí, Jan | Prague |
|
Šuljagić, Marija |
| |
Kalteremidou, Kalliopi-Artemi | Brussels |
|
Azam, Siraj |
| |
Ospanova, Alyiya |
| |
Blanpain, Bart |
| |
Ali, M. A. |
| |
Popa, V. |
| |
Rančić, M. |
| |
Ollier, Nadège |
| |
Azevedo, Nuno Monteiro |
| |
Landes, Michael |
| |
Rignanese, Gian-Marco |
|
Berger, Kévin
Université de Lorraine
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (46/46 displayed)
- 2022Microstructural Parameters for Modelling of Superconducting Foamscitations
- 2021Preparation of superconducting Iron-selenide using Spark Plasma Sintering ; Synthèse de Fer-Sélénium (FeSe) supraconducteur par Frittage Flash
- 2021Magnetic phases in superconducting, polycrystalline bulk FeSe samples
- 2021Magnetic phases in superconducting, polycrystalline bulk FeSe samplescitations
- 2021Experimental Study on Flux Trapping and Flux Jump on Pulsed-Field Magnetization Process for Mg-B Trapped-Field Magnet
- 2021Review on the Use of Superconducting Bulks for Magnetic Screening in Electrical Machines for Aircraft Applicationscitations
- 2020On the origin of the sharp, low-field pinning force peaks in MgB2 superconductorscitations
- 2020Magnetic phases in superconducting, polycrystalline bulk FeSe samples
- 2019Electron Irradiation of Polycrystalline Bulk FeSe Superconductors
- 2019Electron Irradiation of Polycrystalline Bulk FeSe Superconductors
- 2019Investigation of flux jumps during Pulsed Field Magnetization in various MgB2 bulks
- 2019Superconducting cryo-magnets processed by Spark Plasma Sintering and Texturingcitations
- 2019Exploring the flux pinning performance of bulk FeSe by electron irradiation
- 2019Exploring the flux pinning performance of bulk FeSe by electron irradiation
- 2019Exploring the potential of FeSe bulk superconductors
- 2018Hybrid analytical and integral methods for simulating HTS materials
- 2018Eddy current modeling in linear and nonlinear multifilamentary composite materialscitations
- 2018Superconducting cryo-magnets processed by Spark Plasma Sintering and Texturing
- 2018Distribution of current density, temperature and mechanical deformation in YBCO bulks under Field-Cooling magnetizationcitations
- 2017Electromagnetic field modeling in HTS composite tapes in the frequency domain
- 2017A novel route to prepare bulk superconductors: Spark Plasma Sintering and Texturing
- 2017Dependence of the trapped magnetic flux density of YBCO pellets on mechanical stress
- 2017A novel route to prepare bulk superconductors : Spark Plasma Sintering and Texturing
- 2017Bulk superconducting cryo-magnets processed by Spark Plasma Sintering/Texturing
- 2017Eddy current modeling in composite materials: CFRPs and multifilamentary HTS tapes
- 2016Trapped Magnetic Field Experiments and Characterization of Large-Sized Bulk MgB2 Samples
- 2016Design of a Vector Magnet Generating up to 3 T with 3 Axis Orientation
- 2016Recent development of superconducting cryomagnets by Spark plasma Sintering
- 2016Modelling of HTS bulk during Pulsed Field Magnetization within an iron core using analytical and integral methods
- 2016Design of a Vector Magnet Generating up to 3 T with 3 Axis Orientation
- 2016Eddy current modeling in multifilementary superconductive tapes submitted to external time varying magnetic field
- 2015Design of a Low-Temperature Superconducting coils system generating up to 3 T in a 10 cm bore diameter with 3 axis orientations
- 2015Analytical modelling of superconductors in electrical engineering applications
- 2015Design of a Low-Temperature Superconducting coils system generating up to 3 T in a 10 cm bore diameter with 3 axis orientations
- 2015Conception d'un aimant vectoriel supraconducteur produisant 3 T dans une sphère de diamètre 100 mm
- 2015Design of a vector magnet generating up to 3 T with 3 axis orientation
- 2014Critical current density determination of superconducting material
- 2012Modeling of a 3D superconducting inductor structure using analytical formulae
- 2011Magnetic shielding performances of YBCO superconductors : applications to multiple bulks and thin films
- 2011Preliminary study of 3D modeling of superconductors using analytical formulae
- 2011Determination of superconducting material critical current density from magnetic field diffusion measurement
- 2011Magnetic shielding performances of YBCO superconductors: applications to multiple bulks and thin films
- 2008Self Field Effect Compensation in an HTS Tubecitations
- 2007Influence of Temperature and/or Field Dependences of the E−J Power Law on Trapped Magnetic Field in Bulk YBaCuOcitations
- 2006Influence of Jc(B) on the full penetration current of superconducting tubecitations
- 2005Pulse field magnetization of high-temperature superconductor bulk parts considering thermal effects
Places of action
Organizations | Location | People |
---|
conferencepaper
Magnetic shielding performances of YBCO superconductors : applications to multiple bulks and thin films
Abstract
International audience ; HTS bulks present a high critical current density which can either be used as strong magnets or perfect magnetic shields. Previous works showed that BSCCO bulks can screen magnetic fields up to 0.1 T. For large scale applications like electrical machines, stronger magnetic field is usually needed. In so doing, (RE)BCO materials are more suitable since they can shield much higher magnetic fields (typically around 0.5T at 77 K). Another key issue concerns the size of the bulks. Nowadays, it is possible to manufacture 150-mm diameter class cylindrical YBCO bulk. In order to get larger magnetic shielding areas, multiple bulk superconductors should be arrayed and stacked in layers. Thin films can also be deposited to get very large screening areas. The paper presents experimental results on screening performances of layered YBCO pellets as well as thin films. The experiments are carried out at 77 K under external magnetic fields of 150 mT. Different topologies are considered as follows: - Single layer configuration with 9 square pellets, - Double layer configuration with respectively 9 and 4 square pellets, - One layer of YBCO thin film. It is shown that the double layer configuration improves the shielding performances. Other results and discussions will be given in the full presentation.