US20040256922A1 - Device for supplying electric power to a superconductor - Google Patents

Device for supplying electric power to a superconductor Download PDF

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US20040256922A1
US20040256922A1 US10/846,361 US84636104A US2004256922A1 US 20040256922 A1 US20040256922 A1 US 20040256922A1 US 84636104 A US84636104 A US 84636104A US 2004256922 A1 US2004256922 A1 US 2004256922A1
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transformer
winding
secondary winding
primary winding
superconductor
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US10/846,361
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Florian Steinmeyer
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Siemens AG
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Siemens AG
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Publication of US20040256922A1 publication Critical patent/US20040256922A1/en
Priority to US11/423,186 priority Critical patent/US7355307B2/en
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K55/00Dynamo-electric machines having windings operating at cryogenic temperatures
    • H02K55/02Dynamo-electric machines having windings operating at cryogenic temperatures of the synchronous type
    • H02K55/04Dynamo-electric machines having windings operating at cryogenic temperatures of the synchronous type with rotating field windings
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Definitions

  • the present invention relates to a device for supplying to electric power to a superconductor, in particular to a superconducting winding, which can be cooled to a predetermined temperature for achieving superconductivity.
  • a superconducting rotor with a superconducting winding for an electric motor is known, for example, from U.S. Pat. No. 5,482,919 A.
  • the superconducting winding is cooled by a cooling system to a sufficiently low temperature, so that the coil becomes superconducting.
  • a high-temperature superconducting material HTSC
  • the coil can be cooled by a cooling system that employs the Gifford-McMahon cycle or the Stirling cycle process for cooling.
  • An AC current is supplied to the superconducting coil via brush rings.
  • the brushes can wear down which adversely affects the life expectancy of the motor, and the brush rings can introduce excessive heat into the cooled region.
  • the current is supplied through a current supply line that is cooled only by thermal conduction, approximately 45 W/kA are introduced into the cooled region at a temperature of between 20 K and 40 K. At least 27 W of thermal energy are introduced by the two required current supply lines at a typical operating current in the superconductor of, for example, 300 A. This approximately equals the total cooling power of a conventional high-efficiency Gifford-McMahon cooler (approximately 25 W at 20 K).
  • the operating temperature of the coil increases with the heat loss introduced by the current supply lines. This reduces the critical current of the superconductor and hence also the magnetic field strength attained by the coil. This limits the current that can be efficiently supplied to the motor and makes the operation of the motor less cost-effective.
  • the device described herein is designed to supply power to a superconductor, in particular a superconducting winding of an electric motor with a superconducting rotor.
  • At least one transformer is used to transmit energy between a source of electric energy and the superconductor.
  • the transformer transmits the electric energy to the superconductor without the use of brushes that can wear out.
  • the transformer(s) can also significantly reduce heat transfer into the cooled superconductor.
  • a device for supplying electric energy to at least one superconductor, wherein the superconductor is cooled in a cooled region to at least one predetermined temperature for achieving superconductivity includes at least one electric energy source and a transformer for transferring electric energy between the at least one energy source and the superconductor.
  • the transformer has a primary winding electrically connected with the energy source and a secondary winding electrically connected with the superconductor. At least the secondary winding of the transformer is arranged within the cooled region.
  • a device for supplying electric energy to at least one superconductor, wherein the superconductor is cooled in a cooled region to at least one predetermined temperature for achieving superconductivity includes at least one electric energy source and a first transformer and a second transformer. Each transformer has a primary winding and a secondary winding for transferring electric energy between the energy source and the superconductor.
  • the primary winding of the first transformer is electrically connected with the energy source and the secondary winding of the second transformer is electrically connected with the superconductor. At least the primary winding of the first transformer is arranged outside the cooled region.
  • the transformer or transformers transform an AC voltage applied to the primary winding into an AC voltage in the secondary winding.
  • the magnitude of the AC voltage in the secondary winding of the transformer or the second transformer can be smaller or greater than, or equal to, the magnitude of the AC voltage in the primary winding of the transformer.
  • the secondary winding of the transformer can rotate relative to the primary winding and particularly together with the superconductor.
  • the primary winding and the secondary winding of the transformer and also of the second transformer can be spaced apart by an air gap, or alternatively by a layer of an electrically insulating material arranged between the primary winding and the secondary winding.
  • the primary winding of the transformer can be arranged outside the cooled region.
  • the primary and/or secondary winding of the first transformer and/or of the second transformer can also be arranged outside the cooled region.
  • the primary winding and/or the secondary winding of the second transformer can also be arranged inside the cooled region.
  • the superconductor can rotate with respect to the motor stator.
  • the secondary winding of one of the first and second transformers can also rotate relative to the primary winding of that first or second transformer and also together with the superconductor.
  • At least one rectifier or MOSFET can be electrically connected before the superconductor.
  • the rectifier or MOSFET can be telemetrically controlled.
  • the transformer can be operated at high frequencies to increase its efficiency.
  • the primary winding and the secondary winding of the transformer and/or of the second transformer can be arranged axially side-by-side or radially stacked on top of one another.
  • the primary winding and the secondary winding of the transformer can be arranged at, on, or in a common magnetic flux-conducting body.
  • the primary winding of the transformer can be arranged at, on, or in a first magnetic flux-conducting body
  • the secondary winding of the transformer can be arranged at, on, or in a second separate magnetic flux-conducting body.
  • the primary winding and the secondary winding of at least one of the first and second transformers can be arranged at, on, or in a common magnetic flux-conducting body.
  • the primary winding and the secondary winding of the first transformer can be arranged at, on, or in a first magnetic flux-conducting body
  • the primary winding and the secondary winding of the second transformer can be arranged at, on, or in a second magnetic flux-conducting body.
  • a superconductor constructed in the manner described above can rotate and hence form a superconducting rotor coil in an electric motor.
  • the primary winding of the transformer can be stationary relative to the superconductor, while the secondary winding of the transformer can rotate together with the superconducting rotor coil.
  • FIG. 1 shows a cross-section of a first embodiment of a synchronous motor with a superconducting rotor coil with two transformers
  • FIG. 2 shows a cross-section of a second embodiment of a synchronous motor with a superconducting rotor coil with two transformers
  • FIG. 3 shows a cross-section of a third embodiment of a synchronous motor with a superconducting rotor coil with two transformers
  • FIG. 4 shows a cross-section of a fourth embodiment of a synchronous motor with a superconducting rotor coil with one transformers
  • FIG. 5 shows schematically a diagram with the time dependence of the current in the rotor coil.
  • the electric motor 1 with a superconducting rotor coil (winding) 2 .
  • the rotor coil 2 must be cooled to enable superconductivity in the coil 2 .
  • the electric motor 1 includes a cooled region 9 which is indicated in FIG. 1 by dash-dotted lines and is located inside a cryogenic vessel 13 .
  • the region 9 is cooled by a cooling system that operates according to the Gifford-McMahon cycle or the Stirling cycle.
  • the rotor coil 2 is preferably made of a high-temperature superconducting material (HTSC) having superconducting transition temperature above 35 K.
  • HTSC high-temperature superconducting material
  • Power to the rotor coil 2 is supplied by an electric energy source 3 , which can be a stationary power supply 15 .
  • a first transformer 4 is provided for transmitting the electric energy to the rotor coil 2 .
  • the first transformer 4 has a primary winding 5 axially spaced by an air gap 7 from a secondary winding 6 . While the primary winding 5 is stationary, the secondary winding 6 is connected with the schematically indicated rotor 16 for rotation therewith.
  • the shaft 14 of rotor 16 is supported in bearings (not shown).
  • the primary winding 5 of the transformer 4 is electrically connected with the energy source 3 .
  • the energy source 3 produces an AC voltage U 1 , i.e., a temporally changing voltage of alternating polarity, which is applied to the primary winding 5 of the transformer 4 .
  • the AC voltage U 1 is electrically coupled via the air gap 7 to the secondary winding 6 of the transformer 4 and transformed.
  • the transformed output voltage of the secondary winding referred to as U 2 , is also an AC voltage.
  • the ratio U 2 /U 1 of the two AC voltages U 2 and U 1 can be set by selecting number of turns in the primary winding 5 and/or the secondary winding 6 .
  • the two windings 5 and 6 of the first transformer 4 are located outside the cooled region 9 , i.e. essentially at ambient temperature T u .
  • a second transformer 8 is connected downstream of the first transformer 4 and, in particular, to the secondary winding 6 of the first transformer 4 .
  • the second transformer 8 is connected to and supplies electric energy to the rotor coil 2 .
  • the second transformer 8 is located in the cooled region 9 having a temperature T s that supports superconductivity of the rotor coil 2 .
  • the primary winding 80 of the second transformer 8 is electrically connected with the secondary winding 6 of the first transformer 4 via a high-current wire (current supply line) 68 .
  • the center tap of the secondary winding 81 of the transformer 8 is electrically connected with the rotor coil 2 , as shown in FIG. 1.
  • the supply voltage generated at the secondary coil 81 of the second transformer 8 is also an AC voltage and shown as U 3 .
  • the AC voltage U 1 supplied by power supply 15 is stepped up by the transformer 4 to a significantly higher voltage U 2 .
  • the transformation ratio can be at least 2, in particular at least 5, or can be greater than 10.
  • Both transformers 4 and 8 operate at high frequencies.
  • the operating frequencies are typically in a range between 100 Hz and 1 MHz, but can also be smaller or greater.
  • Each of the transformers 4 and 8 has a transformation ratio which can be selected over a wide range.
  • the energy from the electric energy source 3 is preferably supplied into the “cold region”, i.e., from the first transformer 4 to the second transformer 8 , at a higher voltage U 2 and a smaller current via the electric connection, i.e. the current supply line 68 .
  • the electric energy is transformed in the second transformer 8 to a smaller voltage U 3 and a correspondingly higher current. Accordingly, the second transformer 8 can be used to bring the current in the circuit of the superconductor 2 to the required level by stepping down the voltage U 2 to the smaller voltage U 3 . Only small thermal losses are observed in the cooled region 9 which is at cryogenic temperatures.
  • the current for operating the superconducting coil 2 is subsequently rectified in a rectifier—depicted in FIG. 1 in form of a circuit with two MOSFET switches.
  • the MOSFET gates have to be controlled by a voltage with the proper phase, which is achieved by using a controller 16 that rotates together with the rotor.
  • the controller 16 is controlled in a non-contacting manner by schematically indicated telemetry 17 .
  • This can be accomplished, for example, by infrared transmission, via a fiber-optic brush ring, or by radio waves.
  • the telemetry 17 is typically required anyway for monitoring the operating temperature and voltage of the rotor coil 2 . If necessary, the transformer 4 can also supply the energy for powering the controller 16 or the telemetry 17 .
  • FIGS. 2, 3 and 4 show alternative embodiments of the electric motor 1 .
  • the primary winding 5 and the secondary winding 6 of the transformer in FIG. 1 are arranged side-by-side in the axial direction of shaft 14
  • the two windings 5 , 6 are stacked radially in the embodiment shown in FIG. 2.
  • the air gap 7 is here shaped as a hollow cylinder. Otherwise, the configuration of the electric motor 1 is substantially identical to that of FIG. 1.
  • FIG. 3 shows an electric motor 1 wherein the primary winding 5 of the transformer 4 is arranged in an annular recess of a common magnetic flux-conducting element (yoke) 65 that holds the primary winding 5 and the secondary winding 6 .
  • yoke common magnetic flux-conducting element
  • the flux-conducting yoke 65 of the transformer 4 can be constructed of laminated ferrite sheets (transformer sheets) to prevent eddy currents.
  • laminated ferrite sheets transformer sheets
  • FIG. 4 shows another embodiment of the electric motor 1 which has only a single transformer—namely the transformer 4 —for supplying power to the rotor coil 2 ; the second transformer 8 used in the embodiments described above with reference to FIGS. 1, 2 and 3 , has been eliminated.
  • the stationery primary winding 5 of the transformer 4 is here located in a “warm region”, i.e., essentially at ambient temperature T u .
  • the rotating secondary winding 6 is arranged in the “cold region”, i.e., at the superconducting temperature T s .
  • a wall 12 made of a non-conducting material fills the gap between the two windings 5 , 6 .
  • Suitable non-conducting materials are, in particular, glass fiber reinforced plastics.
  • the wall 12 can here be, for example, a portion of the wall of the cryogenic vessel 13 .
  • the embodiment of FIG. 4 results in a particularly simple configuration.
  • FIG. 5 shows schematically a diagram of the current I flowing in the rotor coil 2 as a function of time t. Three operating regions are illustrated:
  • the magnetic field is rapidly built up in coil 2 by rapidly increasing the current in the coil 2 (charging phase 18 , MOSFETs 10 in FIG. 1 in charging configuration).
  • the gate supply of the rectifier bridge in the charging circuit is synchronized, with the power supply operating at a high voltage and/or high frequency to guarantee a high energy transfer rate.
  • discharge phase 20 MOSFETs 10 in discharge configuration
  • the phase of the MOSFET synchronization is shifted by 180°. Again, high voltages and/or high frequencies are selected for rapid discharge.
  • MOSFETs are advantageous because high voltages and frequencies can be implemented, allowing a rapid adjustment to changing operating conditions.
  • Protective diodes can be used to protect the windings should a faulty synchronization occur.
  • the coil is discharged according to the transformer-rectifier principle with cold MOSFET switches.
  • the proposed device of the invention eliminates brushes which reduced wear on the motor parts during operation.
  • the motor is also very compact and can therefore have a high power density.
  • the current supply line introduces only a small amount of heat into the cooled region, which helps maintain the superconducting properties of the coil and a high magnetic field in the rotor coil.

Abstract

A device for supplying electric energy to at least one superconductor, with the superconductor being cooled in a cooled region to at least one predetermined temperature for achieving superconductivity, includes at least one electric energy source, and a transformer for transferring electric energy between the at least one energy source and the superconductor. The transformer has a primary winding electrically connected with the energy source and a secondary winding electrically connected with the superconductor, wherein at least the secondary winding of the transformer is arranged within the cooled region.

Description

    CROSS-REFERENCES TO RELATED APPLICATIONS
  • This application is a continuation of prior filed copending PCT International application no. PCT/DE02/04071, filed Oct. 31, 2002, which designated the United States and on which priority is claimed under 35 U.S.C. §120, the disclosure of which is hereby incorporated by reference. [0001]
  • This application claims the priority of German Patent Application, Serial No. 101 56 212.8, filed Nov. 15, 2001, pursuant to 35 U.S.C. 119(a)-(d), the disclosure of which is incorporated herein by reference.[0002]
  • BACKGROUND OF THE INVENTION
  • The present invention relates to a device for supplying to electric power to a superconductor, in particular to a superconducting winding, which can be cooled to a predetermined temperature for achieving superconductivity. [0003]
  • A superconducting rotor with a superconducting winding for an electric motor is known, for example, from U.S. Pat. No. 5,482,919 A. The superconducting winding is cooled by a cooling system to a sufficiently low temperature, so that the coil becomes superconducting. Preferably, a high-temperature superconducting material (HTSC) is used with a superconducting transition temperature above approximately 35 K. The coil can be cooled by a cooling system that employs the Gifford-McMahon cycle or the Stirling cycle process for cooling. [0004]
  • An AC current is supplied to the superconducting coil via brush rings. However, the brushes can wear down which adversely affects the life expectancy of the motor, and the brush rings can introduce excessive heat into the cooled region. For example, when the current is supplied through a current supply line that is cooled only by thermal conduction, approximately 45 W/kA are introduced into the cooled region at a temperature of between 20 K and 40 K. At least 27 W of thermal energy are introduced by the two required current supply lines at a typical operating current in the superconductor of, for example, 300 A. This approximately equals the total cooling power of a conventional high-efficiency Gifford-McMahon cooler (approximately 25 W at 20 K). The operating temperature of the coil increases with the heat loss introduced by the current supply lines. This reduces the critical current of the superconductor and hence also the magnetic field strength attained by the coil. This limits the current that can be efficiently supplied to the motor and makes the operation of the motor less cost-effective. [0005]
  • It would therefore be desirable to provide a device for supplying electric power to a superconductor, in particular to a superconducting winding of a motor, to obviate prior art shortcomings and to operate efficiently and economically. It would also be desirable to minimize heat transfer via the current supply lines, so that the superconductive properties of the superconductor and hence the magnetic field strength of the superconducting winding or coil can be maintained. [0006]
  • SUMMARY OF THE INVENTION
  • The device described herein is designed to supply power to a superconductor, in particular a superconducting winding of an electric motor with a superconducting rotor. At least one transformer is used to transmit energy between a source of electric energy and the superconductor. The transformer transmits the electric energy to the superconductor without the use of brushes that can wear out. The transformer(s) can also significantly reduce heat transfer into the cooled superconductor. [0007]
  • According to one aspect of the invention, a device for supplying electric energy to at least one superconductor, wherein the superconductor is cooled in a cooled region to at least one predetermined temperature for achieving superconductivity, includes at least one electric energy source and a transformer for transferring electric energy between the at least one energy source and the superconductor. The transformer has a primary winding electrically connected with the energy source and a secondary winding electrically connected with the superconductor. At least the secondary winding of the transformer is arranged within the cooled region. [0008]
  • According to another aspect of the invention, a device for supplying electric energy to at least one superconductor, wherein the superconductor is cooled in a cooled region to at least one predetermined temperature for achieving superconductivity, includes at least one electric energy source and a first transformer and a second transformer. Each transformer has a primary winding and a secondary winding for transferring electric energy between the energy source and the superconductor. The primary winding of the first transformer is electrically connected with the energy source and the secondary winding of the second transformer is electrically connected with the superconductor. At least the primary winding of the first transformer is arranged outside the cooled region. [0009]
  • Advantageously, the transformer or transformers transform an AC voltage applied to the primary winding into an AC voltage in the secondary winding. The magnitude of the AC voltage in the secondary winding of the transformer or the second transformer can be smaller or greater than, or equal to, the magnitude of the AC voltage in the primary winding of the transformer. When using two transformers, an AC voltage applied to the primary winding of the second transformer, which is connected with the secondary winding of the first transformer, is transformed into an AC voltage of the secondary winding of the second transformer that is provided to the superconductor. [0010]
  • In one advantageous embodiment, the secondary winding of the transformer can rotate relative to the primary winding and particularly together with the superconductor. The primary winding and the secondary winding of the transformer and also of the second transformer can be spaced apart by an air gap, or alternatively by a layer of an electrically insulating material arranged between the primary winding and the secondary winding. [0011]
  • According to another advantageous embodiment, the primary winding of the transformer can be arranged outside the cooled region. When two transformers are used, the primary and/or secondary winding of the first transformer and/or of the second transformer can also be arranged outside the cooled region. Alternatively or in addition, the primary winding and/or the secondary winding of the second transformer can also be arranged inside the cooled region. [0012]
  • Advantageously, the superconductor can rotate with respect to the motor stator. Moreover, the secondary winding of one of the first and second transformers can also rotate relative to the primary winding of that first or second transformer and also together with the superconductor. [0013]
  • According to yet another advantageous embodiment, at least one rectifier or MOSFET can be electrically connected before the superconductor. The rectifier or MOSFET can be telemetrically controlled. Advantageously, the transformer can be operated at high frequencies to increase its efficiency. The primary winding and the secondary winding of the transformer and/or of the second transformer can be arranged axially side-by-side or radially stacked on top of one another. [0014]
  • According to another advantageous embodiment, the primary winding and the secondary winding of the transformer can be arranged at, on, or in a common magnetic flux-conducting body. Alternatively, the primary winding of the transformer can be arranged at, on, or in a first magnetic flux-conducting body, and the secondary winding of the transformer can be arranged at, on, or in a second separate magnetic flux-conducting body. When two transformers are employed, the primary winding and the secondary winding of at least one of the first and second transformers can be arranged at, on, or in a common magnetic flux-conducting body. Or the primary winding and the secondary winding of the first transformer can be arranged at, on, or in a first magnetic flux-conducting body, and the primary winding and the secondary winding of the second transformer can be arranged at, on, or in a second magnetic flux-conducting body. [0015]
  • According to another aspect of the invention, a superconductor constructed in the manner described above can rotate and hence form a superconducting rotor coil in an electric motor. In this case, the primary winding of the transformer can be stationary relative to the superconductor, while the secondary winding of the transformer can rotate together with the superconducting rotor coil.[0016]
  • BRIEF DESCRIPTION OF THE DRAWING
  • Other features and advantages of the present invention will be more readily apparent upon reading the following description of currently preferred exemplified embodiments of the invention with reference to the accompanying drawing, in which: [0017]
  • FIG. 1 shows a cross-section of a first embodiment of a synchronous motor with a superconducting rotor coil with two transformers; [0018]
  • FIG. 2 shows a cross-section of a second embodiment of a synchronous motor with a superconducting rotor coil with two transformers; [0019]
  • FIG. 3 shows a cross-section of a third embodiment of a synchronous motor with a superconducting rotor coil with two transformers; [0020]
  • FIG. 4 shows a cross-section of a fourth embodiment of a synchronous motor with a superconducting rotor coil with one transformers; and [0021]
  • FIG. 5 shows schematically a diagram with the time dependence of the current in the rotor coil.[0022]
  • DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS
  • Throughout all the Figures, same or corresponding elements are generally indicated by same reference numerals. These depicted embodiments are to be understood as illustrative of the invention and not as limiting in any way. It should also be understood that the drawings are not necessarily to scale and that the embodiments are sometimes illustrated by graphic symbols, phantom lines, diagrammatic representations and fragmentary views. In certain instances, details which are not necessary for an understanding of the present invention or which render other details difficult to perceive may have been omitted. [0023]
  • Turning now to the drawing, and in particular to FIG. 1, there is shown an [0024] electric motor 1 with a superconducting rotor coil (winding) 2. The rotor coil 2 must be cooled to enable superconductivity in the coil 2. For this purpose, the electric motor 1 includes a cooled region 9 which is indicated in FIG. 1 by dash-dotted lines and is located inside a cryogenic vessel 13. The region 9 is cooled by a cooling system that operates according to the Gifford-McMahon cycle or the Stirling cycle. The rotor coil 2 is preferably made of a high-temperature superconducting material (HTSC) having superconducting transition temperature above 35 K.
  • Power to the [0025] rotor coil 2 is supplied by an electric energy source 3, which can be a stationary power supply 15. A first transformer 4 is provided for transmitting the electric energy to the rotor coil 2. The first transformer 4 has a primary winding 5 axially spaced by an air gap 7 from a secondary winding 6. While the primary winding 5 is stationary, the secondary winding 6 is connected with the schematically indicated rotor 16 for rotation therewith. The shaft 14 of rotor 16 is supported in bearings (not shown).
  • The primary winding [0026] 5 of the transformer 4 is electrically connected with the energy source 3. The energy source 3 produces an AC voltage U1, i.e., a temporally changing voltage of alternating polarity, which is applied to the primary winding 5 of the transformer 4. The AC voltage U1 is electrically coupled via the air gap 7 to the secondary winding 6 of the transformer 4 and transformed. The transformed output voltage of the secondary winding, referred to as U2, is also an AC voltage. While the frequency of the AC voltage U2 is generally the same as a frequency of the original AC voltage U1 the ratio U2/U1 of the two AC voltages U2 and U1, also referred to as transformer ratio or voltage transformation ratio, can be set by selecting number of turns in the primary winding 5 and/or the secondary winding 6.
  • As seen from FIG. 1, the two [0027] windings 5 and 6 of the first transformer 4 are located outside the cooled region 9, i.e. essentially at ambient temperature Tu.
  • A [0028] second transformer 8 is connected downstream of the first transformer 4 and, in particular, to the secondary winding 6 of the first transformer 4. The second transformer 8 is connected to and supplies electric energy to the rotor coil 2. The second transformer 8 is located in the cooled region 9 having a temperature Ts that supports superconductivity of the rotor coil 2. The primary winding 80 of the second transformer 8 is electrically connected with the secondary winding 6 of the first transformer 4 via a high-current wire (current supply line) 68. The center tap of the secondary winding 81 of the transformer 8, on the other hand, is electrically connected with the rotor coil 2, as shown in FIG. 1. The supply voltage generated at the secondary coil 81 of the second transformer 8 is also an AC voltage and shown as U3.
  • In order to reduce the heat flow from the secondary winding [0029] 6 of the transformer 4, that is located in the warm region, into the cooled region 9 through the high-current wire (current supply line) 68, the AC voltage U1 supplied by power supply 15 is stepped up by the transformer 4 to a significantly higher voltage U2. The transformation ratio can be at least 2, in particular at least 5, or can be greater than 10. As a result of the higher voltage U2, the current in the current line 68 is reduced while delivering the same electric power. Accordingly, the cross-section of the current line 68 can be significantly reduced without increasing the heat dissipation, which would otherwise result from the increased power supply line resistance.
  • Both [0030] transformers 4 and 8 operate at high frequencies. The operating frequencies are typically in a range between 100 Hz and 1 MHz, but can also be smaller or greater.
  • Each of the [0031] transformers 4 and 8 has a transformation ratio which can be selected over a wide range.
  • The energy from the electric energy source [0032] 3 is preferably supplied into the “cold region”, i.e., from the first transformer 4 to the second transformer 8, at a higher voltage U2 and a smaller current via the electric connection, i.e. the current supply line 68.
  • The electric energy is transformed in the [0033] second transformer 8 to a smaller voltage U3 and a correspondingly higher current. Accordingly, the second transformer 8 can be used to bring the current in the circuit of the superconductor 2 to the required level by stepping down the voltage U2 to the smaller voltage U3. Only small thermal losses are observed in the cooled region 9 which is at cryogenic temperatures.
  • The current for operating the [0034] superconducting coil 2 is subsequently rectified in a rectifier—depicted in FIG. 1 in form of a circuit with two MOSFET switches. To operate the rectifier 10, the MOSFET gates have to be controlled by a voltage with the proper phase, which is achieved by using a controller 16 that rotates together with the rotor.
  • The [0035] controller 16 is controlled in a non-contacting manner by schematically indicated telemetry 17. This can be accomplished, for example, by infrared transmission, via a fiber-optic brush ring, or by radio waves. The telemetry 17 is typically required anyway for monitoring the operating temperature and voltage of the rotor coil 2. If necessary, the transformer 4 can also supply the energy for powering the controller 16 or the telemetry 17.
  • FIGS. 2, 3 and [0036] 4 show alternative embodiments of the electric motor 1. For example, while the primary winding 5 and the secondary winding 6 of the transformer in FIG. 1 are arranged side-by-side in the axial direction of shaft 14, the two windings 5, 6 are stacked radially in the embodiment shown in FIG. 2. The air gap 7 is here shaped as a hollow cylinder. Otherwise, the configuration of the electric motor 1 is substantially identical to that of FIG. 1.
  • FIG. 3 shows an [0037] electric motor 1 wherein the primary winding 5 of the transformer 4 is arranged in an annular recess of a common magnetic flux-conducting element (yoke) 65 that holds the primary winding 5 and the secondary winding 6.
  • In this case, like in the other embodiments described above, the flux-conducting [0038] yoke 65 of the transformer 4 can be constructed of laminated ferrite sheets (transformer sheets) to prevent eddy currents. Those skilled in the art will appreciate that at higher operating frequencies, in particular in the MHz range, energy can be transferred inductively from the stationery section to the rotating section through the opposing windings 5, 6 without the use of transformer sheets.
  • FIG. 4 shows another embodiment of the [0039] electric motor 1 which has only a single transformer—namely the transformer 4—for supplying power to the rotor coil 2; the second transformer 8 used in the embodiments described above with reference to FIGS. 1, 2 and 3, has been eliminated.
  • The stationery primary winding [0040] 5 of the transformer 4 is here located in a “warm region”, i.e., essentially at ambient temperature Tu. The rotating secondary winding 6 is arranged in the “cold region”, i.e., at the superconducting temperature Ts.
  • A [0041] wall 12 made of a non-conducting material fills the gap between the two windings 5, 6. Suitable non-conducting materials are, in particular, glass fiber reinforced plastics. Although the gap between the windings 5, 6 may here be wider than in the embodiments described above with reference to FIGS. 1, 2, and 3, respectively, this does not adversely affect the performance when the transformer is operated at high frequencies. The wall 12 can here be, for example, a portion of the wall of the cryogenic vessel 13. The embodiment of FIG. 4 results in a particularly simple configuration.
  • FIG. 5 shows schematically a diagram of the current I flowing in the [0042] rotor coil 2 as a function of time t. Three operating regions are illustrated:
  • The magnetic field is rapidly built up in [0043] coil 2 by rapidly increasing the current in the coil 2 (charging phase 18, MOSFETs 10 in FIG. 1 in charging configuration). The gate supply of the rectifier bridge in the charging circuit is synchronized, with the power supply operating at a high voltage and/or high frequency to guarantee a high energy transfer rate.
  • During operation (holding [0044] phase 19, MOSFETs 10 in charging configuration), only the very small losses of the HTSC rotor coil have to be replenished. Small voltages and/or low frequencies are sufficient.
  • For discharging ([0045] discharge phase 20, MOSFETs 10 in discharge configuration), the phase of the MOSFET synchronization is shifted by 180°. Again, high voltages and/or high frequencies are selected for rapid discharge.
  • The use of MOSFETs is advantageous because high voltages and frequencies can be implemented, allowing a rapid adjustment to changing operating conditions. Protective diodes can be used to protect the windings should a faulty synchronization occur. [0046]
  • The coil is discharged according to the transformer-rectifier principle with cold MOSFET switches. [0047]
  • With the afore-described embodiments, energy can advantageously be transferred independent of the rotation speed, which is different from induction machines where the rotor voltage depends on the rotation speed. [0048]
  • The proposed device of the invention eliminates brushes which reduced wear on the motor parts during operation. The motor is also very compact and can therefore have a high power density. Moreover, the current supply line introduces only a small amount of heat into the cooled region, which helps maintain the superconducting properties of the coil and a high magnetic field in the rotor coil. [0049]
  • While the invention has been illustrated and described in connection with currently preferred embodiments shown and described in detail, it is not intended to be limited to the details shown since various modifications and structural changes may be made without departing in any way from the spirit of the present invention. The embodiments were chosen and described in order to best explain the principles of the invention and practical application to thereby enable a person skilled in the art to best utilize the invention and various embodiments with various modifications as are suited to the particular use contemplated. [0050]
  • What is claimed as new and desired to be protected by Letters Patent is set forth in the appended claims and includes equivalents of the elements recited therein: [0051]

Claims (59)

What is claimed is:
1. A device for supplying electric energy to at least one superconductor, said superconductor being cooled in a cooled region to at least one predetermined temperature for achieving superconductivity, comprising:
at least one electric energy source,
a transformer for transferring electric energy between the at least one energy source and the superconductor, said transformer having a primary winding electrically connected with the energy source and a secondary winding electrically connected with the superconductor,
wherein at least the secondary winding of the transformer is arranged within the cooled region.
2. The device of claim 1, wherein the secondary winding of the transformer is rotatable relative to the primary winding and rotates in unison with the superconductor.
3. The device of claim 1, wherein the primary winding and the secondary winding of the transformer are spaced apart by an air gap.
4. The device of claim 1, wherein a layer of an electrically insulating material is arranged between the primary winding and the secondary winding of the transformer.
5. The device of claim 1, wherein a layer of a heat-insulating material is arranged between the primary winding and the secondary winding of the transformer.
6. The device of claim 1, wherein the primary winding of the transformer is arranged outside the cooled region.
7. The device of claim 2, wherein the primary winding of the transformer is arranged outside the cooled region.
8. The device of claim 1, wherein the transformer transforms an AC voltage applied to the primary winding into an AC voltage in the secondary winding.
9. The device of claim 8, wherein a magnitude of the AC voltage in the secondary winding of the transformer is smaller than a magnitude of the AC voltage in the primary winding of the transformer.
10. The device of claim 8, wherein a magnitude of the AC voltage in the secondary winding of the transformer is greater than a magnitude of the AC voltage in the primary winding of the transformer.
11. A device for supplying electric energy to at least one superconductor which is cooled in a cooled region to at least one predetermined temperature for achieving superconductivity, said device comprising:
at least one electric energy source
a first transformer and a second transformer, each transformer having a primary winding and a secondary winding for transferring electric energy between the at least one energy source and the superconductor;
wherein the primary winding of the first transformer is electrically connected with the energy source, and the secondary winding of the second transformer is electrically connected with the superconductor; and
wherein at least the primary winding of the first transformer is arranged outside the cooled region.
12. The device of claim 11, wherein the secondary winding of the first transformer is arranged outside the cooled region.
13. The device of claim 12, wherein the primary winding of the second transformer is arranged outside the cooled region.
14. The device of claim 13, wherein the secondary winding of the second transformer is arranged outside the cooled region.
15. The device of claim 11, wherein the secondary winding of the second transformer is arranged outside the cooled region.
16. The device of claim 12, wherein the secondary winding of the second transformer is also arranged outside the cooled region.
17. The device of claim 13, wherein the secondary winding of the second transformer is also arranged outside the cooled region.
18. The device of claim 11, wherein the primary winding of the second transformer is also arranged inside the cooled region.
19. The device of claim 12, wherein the primary winding of the second transformer is also arranged inside the cooled region.
20. The device of claim 18, wherein the secondary winding of the first transformer is also arranged inside the cooled region.
21. The device of claim 1, wherein the superconductor is rotatable.
22. The device of claim 2, wherein the superconductor is rotatable.
23. The device of claim 11, wherein the superconductor is rotatable.
24. The device of claim 12, wherein the superconductor is rotatable.
25. The device of claim 13, wherein the superconductor is rotatable.
26. The device of claim 21, wherein the secondary winding of one of the first and second transformers is rotatable relative to the primary winding of that first or second transformer and also rotates with the superconductor.
27. The device of claim 24, wherein the secondary winding of one of the first and second transformers is rotatable relative to the primary winding of that first or second transformer and also rotates with the superconductor.
28. The device of claim 25, wherein the secondary winding of one of the first and second transformers is rotatable relative to the primary winding of that first or second transformer and also rotates with the superconductor.
29. The device of claim 11, wherein the primary winding and the secondary winding of the second transformer are spaced apart by an air gap.
30. The device of claim 11, wherein a layer of an electrically insulating material is arranged between the primary winding and the secondary winding of the second transformer.
31. The device of claim 11, wherein a layer of a heat-insulating material is arranged between the primary winding and the secondary winding of the second transformer.
32. The device of claim 11, wherein each of the first and second transformers transforms an AC voltage applied to the primary winding of the corresponding first or second transformer into an AC voltage in the secondary winding of the corresponding first or second transformer.
33. The device of claim 32, wherein a magnitude of the AC voltage in the secondary winding of at least one of the transformers is smaller than the AC voltage in the primary winding of the at least one transformer.
34. The device of claim 32, wherein a magnitude of the AC voltage in the secondary winding of at least one of the transformers is greater than the AC voltage in the primary winding of the at least one transformer.
35. The device of claim 11, wherein an AC voltage applied to the primary winding of the second transformer, which is connected with the secondary winding of the first transformer, is transformed into an AC voltage of the secondary winding of the second transformer that is provided to the superconductor.
36. The device of claim 35, wherein a magnitude of the AC voltage at the secondary winding of the second transformer is smaller than a magnitude of the AC voltage at the primary winding of the second transformer.
37. The device of claim 35, wherein a magnitude of the AC voltage at the secondary winding of the second transformer is greater than a magnitude of the AC voltage at the primary winding of the second transformer.
38. The device of claim 1, wherein at least one rectifier is electrically connected upstream of the superconductor.
39. The device of claim 38, wherein the rectifier is telemetrically controlled.
40. The device of claim 1, wherein at least one MOSFET switch is electrically connected upstream of the superconductor.
41. The device of claim 1, wherein the transformer is operated at high frequencies.
42. The device of claim 1, wherein the primary winding and the secondary winding of the transformer are arranged axially side-by-side.
43. The device of claim 1, wherein the primary winding and the secondary 3inding of the transformer are radially stacked on top of one another.
44. The device of claim 1, wherein the primary winding and the secondary winding of the transformer are arranged at, on, or in a common magnetic flux-conducting body.
45. The device of claim 1, wherein the primary winding of the transformer is arranged at, on, or in a first magnetic flux-conducting body, and the secondary winding of the transformer is arranged at, on, or in a second magnetic flux-conducting body.
46. The device of claim 11, wherein at least one rectifier is electrically 6onnected upstream of the superconductor.
47. The device of claim 46, wherein the rectifier is telemetrically controlled.
48. The device of claim 11, wherein at least one MOSFET switch is electrically connected upstream of the superconductor.
49. The device of claim 11, wherein the first transformer or the second transformer, or both, are operated at high frequencies.
50. The device of claim 11, wherein the primary winding and the secondary winding of at least one of the first and second transformers are arranged axially side-by-side.
51. The device of claim 11, wherein the primary winding and the secondary winding of at least one of the first and second transformers are radially stacked on top of one another.
52. The device of claim 11, wherein the primary winding and the secondary winding of at least one of the first and second transformers are arranged at, on, or in a common magnetic flux-conducting body.
53. The device of claim 11, wherein the primary winding and the secondary winding of the first transformer are arranged at, on, or in a first magnetic flux-conducting body, and the primary winding and the secondary winding of the second transformer are arranged at, on, or in a second magnetic flux-conducting body.
54. The device of claim 1, wherein the superconductor comprises a superconducting winding.
55. The device of claim 11, wherein the superconductor comprises a superconducting winding.
56. An electric motor, comprising:
at least one superconducting winding;
a device for supplying electric energy to the at least one superconducting winding, said superconducting winding being cooled in a cooled region to at least one predetermined temperature for achieving superconductivity;
at least one electric energy source, a transformer for transferring electric energy between the at least one energy source and the superconducting winding, said transformer having a primary winding electrically connected with the energy source and a secondary winding electrically connected with the superconducting winding, wherein at least the secondary winding of the transformer is arranged within the cooled region.
57. The electric motor of claim 56, further comprising a rotor, wherein the at least one superconducting winding is disposed on the rotor.
58. An electric motor, comprising
at least one superconducting winding;
a device for supplying electric energy to the at least one superconducting winding, said superconducting winding being cooled in a cooled region to at least one predetermined temperature for achieving superconductivity;
at least one electric energy source; and
a first transformer and a second transformer, each transformer having a primary winding and a secondary winding for transferring electric energy between the at least one energy source and the superconducting winding, wherein the primary winding of the first transformer is electrically connected with the energy source and the secondary winding of the second transformer is electrically connected with the superconducting winding, and wherein at least the primary winding of the first transformer is arranged outside the cooled region.
59. The electric motor of claim 58, further comprising a rotor, wherein the at least one superconducting winding is disposed on the rotor.
US10/846,361 2001-11-15 2004-05-14 Device for supplying electric power to a superconductor Abandoned US20040256922A1 (en)

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Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20090273251A1 (en) * 2005-09-30 2009-11-05 Ralf Cordes Synchronous Machine
US20110025438A1 (en) * 2009-01-30 2011-02-03 Aisin Seiki Kabushiki Kaisha Superconducting apparatus
US20130197821A1 (en) * 2010-12-10 2013-08-01 Mitsubishi Electric Corporation Rotating electrical machine
WO2016024214A1 (en) * 2014-08-11 2016-02-18 Victoria Link Limited Superconducting current pump
US9998047B2 (en) 2015-01-16 2018-06-12 Hamilton Sundstrand Corporation Synchronous machine with rechargeable power storage devices
US10886820B2 (en) 2015-10-09 2021-01-05 Oswald Elektromotoren Gmbh Electrical machine
US20230188011A1 (en) * 2021-12-14 2023-06-15 Schaeffler Technologies AG & Co. KG Telemetry system for electric motor rotor

Families Citing this family (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005204492A (en) * 2003-12-19 2005-07-28 Sumitomo Electric Ind Ltd Superconducting motor device
DE102004048961A1 (en) * 2004-10-07 2006-04-27 Siemens Ag Electric machine with high temperature superconducting rotor winding for exciters has excitation device placed inside partially axial hollow shaft of rotor whereby excitation device is provided at B-side shaft extension
DE102005047541A1 (en) * 2005-09-30 2007-05-03 Siemens Ag Method for supplying and removing energy to and from an ohmic-inductive load and rectifier used in the process
WO2007036430A1 (en) * 2005-09-30 2007-04-05 Siemens Aktiengesellschaft Method and device for the inductive transfer of energy to super-conductive excitation coils of an electric machine
US8134345B2 (en) * 2005-11-29 2012-03-13 General Electric Company Cryogenic exciter
CN100571007C (en) * 2006-05-16 2009-12-16 中国科学院电工研究所 Superconducting energy storage bidirectional multi-level soft switch DC/DC and voltage side phase-shift controlling method thereof
JP5201551B2 (en) * 2008-08-06 2013-06-05 株式会社Ihi Superconducting coil and magnetic field generator
TWI379328B (en) * 2008-12-02 2012-12-11 Delta Electronics Inc Magnetic element
US8320088B2 (en) * 2010-12-20 2012-11-27 Varian Semiconductor Equipment Associates, Inc. Power transfer mechanism for use in transmission and distribution level electrical power systems
EP2551999A1 (en) * 2011-07-27 2013-01-30 Siemens Aktiengesellschaft Electric machine with excitation without slip ring
KR101446866B1 (en) * 2013-04-16 2014-10-06 정윤도 Contactless Power Transfer Apparatus Using High Temperature Superconducting Magnet
US11387741B2 (en) * 2017-03-28 2022-07-12 Allison Naito Superconducting magnet engine

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4598241A (en) * 1982-07-12 1986-07-01 Mykola Sereda Rectifier commutation in electrical machines
US5442956A (en) * 1992-06-03 1995-08-22 Trw Inc. Torque sensor for a power assist steering system
US5482919A (en) * 1993-09-15 1996-01-09 American Superconductor Corporation Superconducting rotor
US5532532A (en) * 1993-09-17 1996-07-02 Martin Marietta Energy Systems, Inc. Hermetically sealed superconducting magnet motor
US5572178A (en) * 1992-11-25 1996-11-05 Simmonds Precision Products, Inc. Rotary transformer
US5965959A (en) * 1996-07-02 1999-10-12 American Superconductor Corporation Superconducting magnets and power supplies for superconducting devices
US6362588B1 (en) * 2000-02-09 2002-03-26 Reliance Electric Technologies, Llc Excitation system for rotating synchronous machines
US6420842B1 (en) * 2000-01-11 2002-07-16 American Superconductor Corporation Exciter and electronic regulator for rotating machinery

Family Cites Families (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2448028A (en) * 1943-12-24 1948-08-31 Raytheon Mfg Co Electrical system
US3273046A (en) * 1961-05-08 1966-09-13 Gen Electric Inverter circuits with independent commutation circuits
DE1238098B (en) * 1964-06-19 1967-04-06 Siemens Ag Method for exciting a superconducting magnet coil
DE1488730B2 (en) * 1965-11-17 1971-03-25 Siemens AG, 1000 Berlin u 8000 München SYNCHRONOUS GENERATOR IN PARTICULAR TURBOGEN GENERATOR WITH SUPRA CONDUCTIVE EXCITER DEVELOPMENT
US3934332A (en) * 1974-11-26 1976-01-27 Westinghouse Electric Corporation Method of making electrical coils having improved strength and oil permeability
DE3027340C2 (en) * 1980-07-18 1983-10-27 Valentin Nikolaevič Leningrad Šachtarin Contactless superconducting synchronous machine
JPS63310366A (en) 1987-06-10 1988-12-19 Hitachi Ltd Synchronous machine
DE4019241A1 (en) * 1990-06-15 1991-12-19 Telefunken Electronic Gmbh Energy and signal transmission system - for transmitting measurement signals from vehicle tyres
EP0860936A3 (en) * 1997-02-20 1999-05-19 Charles Bowker Transfer of electrical energy
WO2001058005A2 (en) * 2000-01-11 2001-08-09 American Superconductor Corporation Exciter assembly telemetry

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4598241A (en) * 1982-07-12 1986-07-01 Mykola Sereda Rectifier commutation in electrical machines
US5442956A (en) * 1992-06-03 1995-08-22 Trw Inc. Torque sensor for a power assist steering system
US5572178A (en) * 1992-11-25 1996-11-05 Simmonds Precision Products, Inc. Rotary transformer
US5482919A (en) * 1993-09-15 1996-01-09 American Superconductor Corporation Superconducting rotor
US5532532A (en) * 1993-09-17 1996-07-02 Martin Marietta Energy Systems, Inc. Hermetically sealed superconducting magnet motor
US5965959A (en) * 1996-07-02 1999-10-12 American Superconductor Corporation Superconducting magnets and power supplies for superconducting devices
US6420842B1 (en) * 2000-01-11 2002-07-16 American Superconductor Corporation Exciter and electronic regulator for rotating machinery
US6362588B1 (en) * 2000-02-09 2002-03-26 Reliance Electric Technologies, Llc Excitation system for rotating synchronous machines

Cited By (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7816828B2 (en) 2005-09-30 2010-10-19 Siemens Aktiengesellschaft Synchronous machine
CN101278464B (en) * 2005-09-30 2012-10-10 西门子公司 Synchronous machine
US20090273251A1 (en) * 2005-09-30 2009-11-05 Ralf Cordes Synchronous Machine
US20110025438A1 (en) * 2009-01-30 2011-02-03 Aisin Seiki Kabushiki Kaisha Superconducting apparatus
US8362860B2 (en) * 2009-01-30 2013-01-29 Aisin Seiki Kabushiki Kaisha Superconducting apparatus
US9696178B2 (en) * 2010-12-10 2017-07-04 Mitsubishi Electric Corporation Rotating electrical machine
US20130197821A1 (en) * 2010-12-10 2013-08-01 Mitsubishi Electric Corporation Rotating electrical machine
WO2016024214A1 (en) * 2014-08-11 2016-02-18 Victoria Link Limited Superconducting current pump
KR20170070003A (en) * 2014-08-11 2017-06-21 빅토리아 링크 엘티디 Superconducting current pump
CN107077944A (en) * 2014-08-11 2017-08-18 维多利亚联结有限公司 Supercurrent pump
KR102312084B1 (en) 2014-08-11 2021-10-13 빅토리아 링크 엘티디 Superconducting current pump
US9998047B2 (en) 2015-01-16 2018-06-12 Hamilton Sundstrand Corporation Synchronous machine with rechargeable power storage devices
EP3046235B1 (en) * 2015-01-16 2019-06-05 Hamilton Sundstrand Corporation Synchronous machine with rechargeable power storage devices
US10886820B2 (en) 2015-10-09 2021-01-05 Oswald Elektromotoren Gmbh Electrical machine
US20230188011A1 (en) * 2021-12-14 2023-06-15 Schaeffler Technologies AG & Co. KG Telemetry system for electric motor rotor

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US20070070559A1 (en) 2007-03-29
KR100991301B1 (en) 2010-11-01
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EP1454404A1 (en) 2004-09-08
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US7355307B2 (en) 2008-04-08
KR20040053312A (en) 2004-06-23

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