EP2599134A1 - Hochtemperatur-supraleiter-magnetsystem - Google Patents
Hochtemperatur-supraleiter-magnetsystemInfo
- Publication number
- EP2599134A1 EP2599134A1 EP10743028.2A EP10743028A EP2599134A1 EP 2599134 A1 EP2599134 A1 EP 2599134A1 EP 10743028 A EP10743028 A EP 10743028A EP 2599134 A1 EP2599134 A1 EP 2599134A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- hts
- magnet system
- winding
- wound
- poles
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 239000002887 superconductor Substances 0.000 title claims abstract description 6
- 238000004804 winding Methods 0.000 claims abstract description 43
- 238000003780 insertion Methods 0.000 claims abstract description 18
- 230000037431 insertion Effects 0.000 claims abstract description 18
- 230000005469 synchrotron radiation Effects 0.000 claims abstract description 6
- 239000004020 conductor Substances 0.000 claims description 7
- 238000001816 cooling Methods 0.000 abstract description 12
- 238000000034 method Methods 0.000 abstract description 6
- 239000002245 particle Substances 0.000 abstract description 3
- 239000003574 free electron Substances 0.000 abstract description 2
- 230000004907 flux Effects 0.000 description 4
- 230000005855 radiation Effects 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- 229910000831 Steel Inorganic materials 0.000 description 2
- 230000001427 coherent effect Effects 0.000 description 2
- 238000010894 electron beam technology Methods 0.000 description 2
- 238000002474 experimental method Methods 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 239000010959 steel Substances 0.000 description 2
- 101000848724 Homo sapiens Rap guanine nucleotide exchange factor 3 Proteins 0.000 description 1
- 102100034584 Rap guanine nucleotide exchange factor 3 Human genes 0.000 description 1
- 238000012790 confirmation Methods 0.000 description 1
- 238000005520 cutting process Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 230000000737 periodic effect Effects 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 230000002269 spontaneous effect Effects 0.000 description 1
- 238000003860 storage Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/06—Coils, e.g. winding, insulating, terminating or casing arrangements therefor
-
- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21K—TECHNIQUES FOR HANDLING PARTICLES OR IONISING RADIATION NOT OTHERWISE PROVIDED FOR; IRRADIATION DEVICES; GAMMA RAY OR X-RAY MICROSCOPES
- G21K1/00—Arrangements for handling particles or ionising radiation, e.g. focusing or moderating
- G21K1/08—Deviation, concentration or focusing of the beam by electric or magnetic means
- G21K1/093—Deviation, concentration or focusing of the beam by electric or magnetic means by magnetic means
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05G—X-RAY TECHNIQUE
- H05G2/00—Apparatus or processes specially adapted for producing X-rays, not involving X-ray tubes, e.g. involving generation of a plasma
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H7/00—Details of devices of the types covered by groups H05H9/00, H05H11/00, H05H13/00
- H05H7/04—Magnet systems, e.g. undulators, wigglers; Energisation thereof
Definitions
- the invention relates to a high-temperature superconductor (HTS) magnet system, preferably for an insertion device for generating a high-intensity synchrotron radiation according to the features of the first claim.
- HTS high-temperature superconductor
- the device is not limited to this use, but can also be used for all other suitable applications, such as in an electromagnetic bearing.
- Undulators and wigglers are made of permanent magnets and electromagnets.
- a winding body for an electromagnetic undulator is described in DE 10 2007 010 414 A1.
- two yokes are aligned with each other so that they are symmetrical to the beam axis of the electron beam and generate the desired field.
- the use of permanent magnets for undulators and wigglers goes back to the first prototypes.
- electromagnets the magnetic flux is directed through the poles, by energizing the adjacent coils in opposite directions. Compared to
- Electromagnets are permanent magnetic undulators the most common solution, but limited in their maximum field.
- superconducting insertion devices achieve higher magnetic fields and thus allow a higher electron flow and / or higher photon energies than the permanent magnetic systems, which is desired for future experiments.
- SCU superconducting insertion devices
- LTS low-temperature superconductors
- the coils are usually wound together from as possible a continuous conductor with only a few interruptions. This means a lot of effort for the winding process, since the coils must be wound in each case in different directions to produce the alternating magnetic field.
- these LTS coils which are therefore also protected from the outside by cold shields, must be cooled to cryogenic temperatures of about 4 K, typically with cryocoolers. They form with everything that has the lowest temperature in the cryostat, the so-called "cold mass.”
- Cryo-coolers are refrigerators with a closed cooling circuit, by which the cryogenic temperatures can be reached and by which a bath cooling with liquid helium can be bypassed Use of the magnet greatly simplified.
- a problem related to the solution for superconducting insertion devices is the handling of the generated by the wave motion of the electron beam
- the total amount of heat of a beam of a third generation synchrotron source can be determined by "Heat load issues of superconducting undulator operated at TPS storage ring", JC Jan, CS Hwang and PH Lin, NSRRC, Hsinchu, Taiwan “Proceedings EPAC 2008” and "Measurements of the beam heat load in the cold bore superconductive undulator installed at ANKA ", S. Casalbuoni, A. Gray, M. Hagelstein, R. Rossmanith, Anlagenstechnik Düsseldorf, Germany, F. Zimmermann, CERN, Geneva, Switzerland, B. Kostka, E Maschkina, E. Steffens, University of Er Weg, Germany A. Bernhard, D. Wollmann, T. Baumbach, University of Düsseldorf, Germany, Proceedings PAC 2007 over 10W.
- the cooling system of the magnet which must be kept at a temperature of 4.2K at all times in order to operate, is typically disconnected from the jet pipe cooling system to minimize the number of cryocoolers.
- This solution makes it possible to keep the jet pipe at a higher temperature compared to the magnet, so that the cryocoolers still sufficient cooling capacity is available to the
- HTS high-temperature superconductor
- the solution according to the invention provides a bobbin, the cylindrical, oval, rectangular, quadrangular, as a block consisting of plates u. a. m. can be executed.
- a bobbin On the lateral surface of the bobbin coaxial poles are arranged, which may have different shapes similar to the bobbin. Windings are arranged between the poles, the winding being an HTS conducting band.
- Low-temperature superconducting wire as used in standard magnet systems for insertion devices, solved by a HTS guide band.
- the HTS conduction band becomes superconducting even at the temperature of liquid nitrogen (77 K), and when operating at lower temperatures, the performance parameters of the conductor can increase significantly.
- the conductor can not be wound up as desired due to its geometry and other mechanical properties.
- HTS conductor strips are connected to one another by means of a connecting part such that an opposite current flow (FIGS. 2 and 4) is produced in the connected coils in order to produce the desired magnetic field configuration.
- the conductive band preferably has a rectangular or similar cross-section.
- the proposed solution requires two findings: a new winding scheme to generate the required magnetic field configuration and the use of HTS guide band for the magnet system, such as undulators, wigglers and insertion devices.
- FIG. 1 shows the basic principle of an undulator with an electron 1 on the
- Radiation axis 2 wherein above and below the radiation axis 2 north and south poles 4 of the magnetic field are arranged.
- the device shown as a cut-out, generates a periodically alternating magnetic field on the beam axis 2, the period length being precisely defined. As the electrons 1 pass the field, they are forced by this field configuration onto an oscillating trajectory 3 and emit so
- FIG. 2 shows the detail of two winding bodies 6 of a magnet system with the functional principle of an insertion device with oppositely energized magnetic coils 9, 1 whose magnetic flux 10, 12 is amplified in the poles 9, 11.
- the winding body 6 with magnetic coils (poles) 9, 1 1 are arranged opposite one another, wherein the beam axis 2 passes between the winding body 6 with poles 9.1 1.
- the generated by the magnetic coils 9.1 1 magnetic flux 10, 12 generates a magnetic field for each of the largest
- Magnetic field vector 7 between the bobbins 6 was located.
- FIG. 3 shows the schematic representation of a superconducting insertion device with the cryocooler 8 on the steel tube 14 through which the jet axis 2 passes.
- Cryostat 15, the undulator magnet 17 consisting of the upper and the lower yoke and the cold mass 18 are also shown in the figure.
- Figure 4 shows a schematic representation of the partial section A-A of the bobbin 6 of Figure 5 with elevations, wherein HTS winding packages 13 in individual layers 23, 24 consisting of HTS guide strip 23 and insulating film 24 are arranged one above the other. These layers represent the field-generating magnetic coils with different energization, in which the
- the connecting piece 16, 20 is arranged between the coils above and below, so that a current flow can take place.
- FIG. 5 shows the winding body 6 for the solution according to the invention in a view with several continuous poles 22 with the cutting profile A-A. Between the continuous poles 22, the connecting piece 20 can be seen at the beginning of the winding in a recess on the pole 21, wherein the connecting piece 20 connects two HTS-Leitb selected 23 together to form a pair, under which an insulating film 24 is located. Between the respective pairs 23, 24, a pole 21 is arranged with a recess.
- the new winding scheme shown and described in FIG. 4 allows all coils to be wound in the same direction as that shown in FIG.
- the alternating magnetic field structure typical of an undulator or winding is created by properly interconnecting the coils so as to control the current flow, as shown in Figure 4, to produce an opposite current flow.
- the bare HTS conductive strip 23 is wound parallel to the winding body 6 simultaneously with an insulating tape 24.
- the Winding two Leitb sections 23 are soldered to a HTS plate 20 so as to connect them electrically.
- the wafer is glued to the winding core 6 so as to be during the
- the two conductors 23 are simultaneously wound parallel to each other and with the insulating films 24.
- the leader tape is fixed and cut to wind two new spools.
- the Polerhöhungen 21 of the bobbin 6 have recesses where one of the lower connectors 20 must be, and continuous Polerhöhungen 22, where the winding segments 25 are electrically connected to each other via a top-mounted connector.
- FIG. 6 shows how the two coils are connected to the two preceding ones to produce the electrical flux as shown in FIG. This procedure greatly simplifies the winding process and due to the modular arrangement can
- the scheme can be applied to any possible configuration of an HTS magnet system of an insertion device, and is therefore also suitable for use in so-called free electron lasers and other particle accelerator based light sources.
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Optics & Photonics (AREA)
- Plasma & Fusion (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Power Engineering (AREA)
- General Engineering & Computer Science (AREA)
- High Energy & Nuclear Physics (AREA)
- Particle Accelerators (AREA)
Abstract
Description
Claims
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
PCT/EP2010/004656 WO2012013205A1 (de) | 2010-07-30 | 2010-07-30 | Hochtemperatur-supraleiter-magnetsystem |
Publications (2)
Publication Number | Publication Date |
---|---|
EP2599134A1 true EP2599134A1 (de) | 2013-06-05 |
EP2599134B1 EP2599134B1 (de) | 2015-01-21 |
Family
ID=43728756
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP10743028.2A Active EP2599134B1 (de) | 2010-07-30 | 2010-07-30 | Hochtemperatur-supraleiter-magnetsystem |
Country Status (5)
Country | Link |
---|---|
US (1) | US8849364B2 (de) |
EP (1) | EP2599134B1 (de) |
DK (1) | DK2599134T3 (de) |
ES (1) | ES2533225T3 (de) |
WO (1) | WO2012013205A1 (de) |
Families Citing this family (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB201217782D0 (en) * | 2012-10-04 | 2012-11-14 | Tesla Engineering Ltd | Magnet apparatus |
GB201515978D0 (en) | 2015-09-09 | 2015-10-21 | Tokamak Energy Ltd | HTS magnet sections |
DE102015223991A1 (de) * | 2015-12-02 | 2017-06-08 | Bruker Biospin Ag | Magnetspulenanordnung mit anisotropem Supraleiter und Verfahren zu deren Auslegung |
US10249420B2 (en) | 2015-12-08 | 2019-04-02 | Uchicago Argonne, Llc | Continuous winding magnets using thin film conductors without resistive joints |
US10646723B2 (en) * | 2016-08-04 | 2020-05-12 | The Johns Hopkins University | Device for magnetic stimulation of the vestibular system |
US10062486B1 (en) * | 2017-02-08 | 2018-08-28 | U.S. Department Of Energy | High performance superconducting undulator |
US10485089B2 (en) * | 2017-09-07 | 2019-11-19 | National Synchrotron Radiation Research Center | Helical permanent magnet structure and undulator using the same |
HRP20230164T1 (hr) * | 2018-10-15 | 2023-03-31 | Tokamak Energy Ltd | Superprovodni magnet visoke temperature |
US11600416B1 (en) | 2021-08-16 | 2023-03-07 | National Synchrotron Radiation Research Center | Cryogen-free high-temperature superconductor undulator structure and method for manufacturing the same |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102007010414A1 (de) | 2007-03-01 | 2008-09-04 | Babcock Noell Gmbh | Wickelkörper für elektromagnetische Undulatoren |
-
2010
- 2010-07-30 DK DK10743028.2T patent/DK2599134T3/da active
- 2010-07-30 EP EP10743028.2A patent/EP2599134B1/de active Active
- 2010-07-30 ES ES10743028.2T patent/ES2533225T3/es active Active
- 2010-07-30 WO PCT/EP2010/004656 patent/WO2012013205A1/de active Application Filing
- 2010-07-30 US US13/812,915 patent/US8849364B2/en active Active
Non-Patent Citations (1)
Title |
---|
See references of WO2012013205A1 * |
Also Published As
Publication number | Publication date |
---|---|
US20130130914A1 (en) | 2013-05-23 |
WO2012013205A1 (de) | 2012-02-02 |
ES2533225T3 (es) | 2015-04-08 |
EP2599134B1 (de) | 2015-01-21 |
US8849364B2 (en) | 2014-09-30 |
DK2599134T3 (da) | 2015-04-13 |
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