Satoshi Fukui’s research while affiliated with Niigata University and other places

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Publications (198)


Test of High Temperature Superconducting REBCO Coil Assembly for a Multi-Frequency ECR Ion Source
  • Article

August 2024

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41 Reads

IEEE Transactions on Applied Superconductivity

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Tetsuhiko Yorita

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[...]

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Takashi Kitamura

High temperature superconducting REBCO tape has the characteristic of maintaining high critical current density under strong external magnetic field, which makes it an ideal material for the construction of air-core electromagnets of accelerator and electron cyclotron resonance (ECR) ion source. In Research Center for Nuclear Physics, Osaka University, a non-insulated air-cored REBCO coil assembly has been constructed. This coil assebmly consists of three circular REBCO solenoid and six racetrack REBCO coil. This coil assembly will be used as an electromagnet of a multi-frequency ECR ion source, and is also developed as a key technology development of an air-core cyclotron. The magnetic field of this ion source are designed, and 77K performance tests of the assembly are carried out in order to examine the capability of REBCO coils of inducing magnetic field under external field. In this work, the test results and the magnetic field designed for the ECR ion source will be presented and discussed.


AC Loss Estimation Model for High-Temperature Superconducting Cables Derived From Experiments Simulating Electromagnetic Environments

August 2023

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12 Reads

IEEE Transactions on Applied Superconductivity

In a previous study, the AC loss characteristics of each layer of a high-temperature superconducting (HTS) AC cable were experimentally investigated [1]–[3]. Based on these data, we modeled the AC loss in a superconducting cable by considering the maxi-mum and minimum values of the loss. A comparison between this model and the experimental data showed good agreement. Hence, it is possible to estimate AC loss under electromagnetic conditions in a high-temperature superconducting cable. This model makes it possible to determine the losses of each layer in the superconducting cable and to design the minimum AC loss load of the superconducting cable. This model estimates the AC losses of a three-layer twisted HTS cable.


Development of 400 kW Class Aluminum Billet Heater Using HTS Magnet

August 2023

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46 Reads

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1 Citation

IEEE Transactions on Applied Superconductivity

In this paper, design, fabrication, and test results of the demonstration device for 400 kW-class aluminum billet heating using the HTS magnet were reported. Based on our user's request, the target of the demonstration device was to heat the aluminum billet of 155 mm in diameter and 500 mm in length from room temperature to 500 ℃ within 60 seconds. In the heating test using the demonstration device, it was demonstrated that the input heating power to the aluminum billet of 155 mm in diameter and 500 mm long was more than 400 kW. Based on the measured data of the heating tests, the heating efficiency was estimated to be 74.5%. It was shown that at least 30% reduction of energy consumption could be possible compared to conventional induction heating devices.


Noncontact Evaluation of HTS Cylinder for Compact Cryogen-free NMR

August 2023

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12 Reads

IEEE Transactions on Applied Superconductivity

Herein, a compact cryogen-free nuclear magnetic resonance (NMR) system is developed using a stacked high-temperature superconducting (HTS) bulk system. To compensate for magnetic field uniformity, an HTS cylinder is installed inside the measurement space. The cylinder is wound with REBCO tapes placed on the surface of a copper cylinder. The uniformity of its critical current density is important for NMR signal detection. Such an operation requires an examination of the quality of the critical-current-density distribution of the cylinder. A noncontact measurement method is required for such an examination. When a magnetic field is applied, the superconductor exhibits a demagnetization effect. Moreover, if any defect exists in any part of the superconducting tape, that particular part would contain no demagnetization, thus disturbing the relevant magnetic field distribution. In this study, this phenomenon is investigated using DC and AC magnetic fields. The magnets and sensor are placed inside the HTS cylinder, and magnetic fields are applied to the HTS cylinder surface. The results confirm that the proposed method is effective and applicable for evaluating the critical-current distribution.


Development of 400 kW-class DC Induction Heating Device Using HTS Magnet for Aluminum Extrusion Process高温超電導マグネットを用いたアルミ押出成形用400 kW級直流誘導加熱装置の開発: Continuous Repetitive Heating Test and Evaluation of Soundness of HTS Magnet―連続繰り返し加熱試験と高温超電導マグネットの健全性評価―

May 2023

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5 Reads

TEION KOGAKU (Journal of the Cryogenic Society of Japan)

We have been conducting research and development of the DC induction heating device of aluminum billet using HTS magnets. In this R&D, following the development of main components such as the HTS magnet system, the heating control system and the mechanism for grasping and rotating the aluminum billet, the demonstration device for 400 kW-class billet heater was developed and the heating power of over 400 kW was demonstrated. In this study, as the final step of the R&D, we conducted a continuous repetitive heating test and evaluation of the electromagnetic and mechanical influence due to the heating operation on the HTS coil. It was demonstrated that the continuous repetitive heating of 90 billets(more than two hours)with the rated power was possible. The temperature increase and the behavior of mechanical stress of the HTS coil during the continuous heating operation were evaluated. It was confirmed that the soundness of the HTS coil through the continuous repetitive heating was not compromised.


Influence of the Current Distribution in Superconducting Resonators for Wireless Power Transmission on the AC Loss Characteristics非接触給電用超電導共振器の電流分布が交流損失特性に及ぼす影響

January 2023

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10 Reads

TEION KOGAKU (Journal of the Cryogenic Society of Japan)

This paper investigates the AC loss characteristics in the resonator of the superconducting wireless power transmission system proposed by Prof. Sekiya. This superconducting resonator is characterized by the fact that the current distribution is not constant in the tape length, the REBCO tapes are double layered, and the operating frequency is 10 MHz. Since the influence of eddy current loss cannot be ignored due to the high operating frequency, we investigated the effect of the REBCO tape configuration using the finite element method.


Figure 1. REBCO solenoids and sextupole coils in HTS-ECR.
Figure 2. REBCO solenoid (left) and sextupole (right).
Figure 3. I-V characterstic of one of the sextupole in 77 K.
Figure 4. Magnetic field induction of one of the solenoid in 31 K.
Figure 5. Axial magnetic field configuration induced by REBCO solenoids.
Development of ECR ion source with high-temperature superconducting REBCO coils
  • Article
  • Full-text available

April 2022

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120 Reads

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2 Citations

Journal of Physics Conference Series

A new High-Temperature Superconducting ECR (HTS-ECR) ion source is under development in Research Center for Nuclear Physics (RCNP), Osaka University. This ion source will be used for production of high intensity proton, deuteron and He ion beams. The HTS-ECR magnets are composed of three solenoid coils and a set of sextupole coils made of REBCO tapes, a high-temperature superconductor. The HTS-ECR ion source is designed to operate at frequency of 2.45 GHz and 10 GHz. Performance test of the HTS coils had been carried out at 31 K and 77 K. This HTS coil technology will be applied to development of a meter-size HTS coil system of a high intensity compact AVF cyclotron. This paper introduces the basic design of the HTS-ECR ion source. The performance test results showed that REBCO solenoids remain superconducting state with a current up to 400 A. Simulation results of the magnetic field and electromagnetic field distributions in a plasma chamber fulfilled the requirements of electron cyclotron resonance conditions at 2.45 GHz and 10 GHz. Simulation result of mirror ratios and electromagnetic field amplitudes are also presented in this paper.

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Fabrication and Test of HTS Magnet for Induction Heating Device in Aluminum Extrusion Processing

December 2021

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23 Reads

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8 Citations

IEEE Transactions on Applied Superconductivity

This paper reported the fabrication and the test results of the high temperature superconducting (HTS) magnet developed for the aluminum billet heater for aluminum extrusion processing. In this magnet, the HTS coils were combined with iron cores, because the required magnetic field in the working region was about 1T. Two HTS coils wound directly on the convex shape iron cores were fabricated. The HTS coils were made by the no-insulation winding of REBCO tape with the YOROI-coil technique. Each of them was separately installed in an individual cryostat. Two HTS coils with iron cores were disposed oppositely to each other and were magnetically connected by a C-shape yoke placed in room temperature. The HTS coil was cooled down to about 15 K by the GM cryocooler in the initial cooling. The magnetic field of 1.06 T at the center of the heating region was stably generated with the rated current of 200 A. It was also demonstrated that the HTS magnet could be charged up to 300 A without quench. According to the observation of the electromagnetic force direction from the outside of the cryostat, it was confirmed the validity of the force balance design of the magnet.


Trapped magnetic field characteristics of MgB2 bulk with different additive contents and MgB2 bulk with different types of additives by pulse magnetization

December 2020

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40 Reads

When the MgB2 bulk body is magnetized by the pulse magnetizing method, the MgB2 bulk can take the role of a pseudo permanent magnet. However, it was confirmed that the temperature at which MgB2 is expected to be used is close to the critical temperature (TC) of MgB2 and the specific heat is small, so that the heat generated by the pulse magnetizing method causes flux jump and the trapped magnetic field performance deteriorates. In this study, pulse magnetizing was performed on different samples to verify and consider changes in the trapped magnetic field performance. As the sample, the sample obtained by changing the amount of titanium added was synthesized by uniaxial hot pressing and the sample synthesized by spark plasma sintering (SPS). Figure (a) shows a comparison of the trapped magnetic fields of the samples synthesized by the uniaxial hot press. From Fig. (A), it was shown that the capture magnetic field performance may be improved or deteriorated by the composition ratio of the material, the addition of impurities, and the method of synthesizing the bulk material.


Figure 4 Time evolution profiles of flux motion at the center of sample surface (a) (b)
Occurrence of Flux Jumps in MgB 2 Bulk Magnets during Pulse-Field Magnetization

June 2020

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91 Reads

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1 Citation

Journal of Physics Conference Series

The magnetic flux capturing of MgB 2 bulk magnets made by spark plasma sintering process has been precisely investigated to clarify the mechanism of flux motions during the pulse-field magnetization processes. The field trapping ratio B T / B P was evaluated as a key parameter of field trapping ability which strongly relates to the heat generation due to the rapid flux motion in the samples. The time dependence of magnetic flux density revealed the actual flux motion which penetrated the samples. The trapped fields B T and field trapping ratios B T / B P of various samples were classified into three regions of ‘no flux flow’, ‘fast flux flow’ and ‘flux jump’ according to the generation of heat and its propagation. A flux jump was observed late at 280 ms from the beginning of PFM process, while the field penetration B P showed its peak at 10 ms. Considering the heat propagation speed, the long-delayed flux jump should be attributed to the macroscopic barriers against the heat propagation to the surface centre of bulk magnet.


Citations (70)


... The heater was assembled and manufactured in 2019, and extensive experiments were conducted [15][16][17][18], which laid the foundation for the commercial point of HTS DC induction heating. In 2022, Tetsuya Ito et al. developed a C-core and two-coil DC induction heated superconducting magnet with a target heating center field of over 1 T. The superconducting magnet is based on the conventional "C" core topology, with an increased number of superconducting coils, and a larger leakage due to the failure to shorten the closed path of the magnetic lines of force [19,20]. ...

Reference:

Design and Operating Characteristics Analysis of HTS Magnets for Dipole-Type DC Induction Heating
Development of 400 kW Class Aluminum Billet Heater Using HTS Magnet
  • Citing Article
  • August 2023

IEEE Transactions on Applied Superconductivity

... The heater was assembled and manufactured in 2019, and extensive experiments were conducted [15][16][17][18], which laid the foundation for the commercial point of HTS DC induction heating. In 2022, Tetsuya Ito et al. developed a C-core and two-coil DC induction heated superconducting magnet with a target heating center field of over 1 T. The superconducting magnet is based on the conventional "C" core topology, with an increased number of superconducting coils, and a larger leakage due to the failure to shorten the closed path of the magnetic lines of force [19,20]. ...

Fabrication and Test of HTS Magnet for Induction Heating Device in Aluminum Extrusion Processing
  • Citing Article
  • December 2021

IEEE Transactions on Applied Superconductivity

... The precursors were sintered by SPS with applying pressure of 75 MPa and heat-treated at 950 °C for 1 min. More details about our sample can be found in our earlier reports [21]. The lower density sample of 1.45 g/cm 3 was considered for this study because of the ease of machining during preparation. ...

Occurrence of Flux Jumps in MgB 2 Bulk Magnets during Pulse-Field Magnetization

Journal of Physics Conference Series

... Modern high-temperature superconductors (HTSs) exhibit large potential for new technologies. Superconducting trapped-field (TF) magnets could significantly reduce the size and enhance the performance of numerous magnetic devices such as (but not restricted to) motors and wind power generators [1][2][3][4][5][6][7][8], flywheels and maglev trains [1,[9][10][11], and the magnetic resonance imaging [1,[12][13][14][15]. To obtain such a magnet, one needs a method that would, ideally, provide maximum TF of high uniformity with minimum cash and energy cost. ...

Formation of uniform magnetic flux distribution for NMR magnets using HTS bulk magnets activated by pulsed-field magnetization

... Recently, variable flux memory machines (VFMMs) 1-10 have received increasing research interest due to their adjustable air-gap flux density, as well as the potential to be promising alternatives for permanent magnet synchronous machines (PMSMs). [11][12][13][14] With the employment of low coercive force (LCF) PMs, the magnetization states (MSs) of VFMMs can be effectively manipulated by transient current pulses with negligible copper loss, realizing wide speed range and high efficiency. ...

Magnetizing Technique for Permanent Magnets in IPM Motor Rotors Using HTS Bulk Magnet
  • Citing Article
  • April 2020

IEEE Transactions on Applied Superconductivity

... The superconducting part of a high-temperature superconducting cable is usually formed by placing the superconducting wire on a support column, forming a cylindrical structure. Therefore, the structure of superconducting wires can affect the magnetic field distribution of superconducting cables, thereby affecting their AC loss level [6][7] . The new type of high-temperature superconducting square wire is developed using narrow wire and stacking treatment to form YBCO wire. ...

Experimental Investigation of AC Loss Characteristics under HTS Cable Electromagnetic Conditions
  • Citing Article
  • January 2020

IEEE Transactions on Applied Superconductivity

... The distance between face-to-face poles was set to 30 mm. As reported in [13], the best uniformity of 463 ppm was obtained at 1.25 T over a wide area of less than 1,500 ppm at the center portion of the pole, which is thinly painted by colors in the figure. The area whose uniformity was less than 1,500 ppm was estimated to be 23 mm 2 . ...

Generation of Uniform Magnetic Field between Face-to-Face HTS Bulk Magnets

Journal of Physics Conference Series

... Our previous studies reported the time evolutional profiles showing the field trapping and flux jumping behaviors during the PFM processes with respect to the MgB2 samples with variable thickness [18], [19], and fabrication methods [20]. In this study, we have investigated the flux motion profiles and the resultant trapped field performances which employed different fabrication methods. ...

Study on Magnetic Flux Dissipation and Field-Trapping Performance of HTS Bulk-Shaped Magnesium Diboride in Pulse-Field Magnetizing Processes

... Numerous studies of bulk superconductors and stacks of HTS-tapes [1,15,18,24,[26][27][28][29][30][31][32][33][34][35][36][37] are dedicated to the socalled flux jumps (or 'giant field leaps' as first introduced in [27]). These jumps occur at certain critical (or activation) fields and result in a rapid invasion of the magnetic flux into the superconducting samples. ...

Study on Magnetic Flux Dissipation and Field-Trapping Performance of HTS Bulk-Shaped Magnesium Diboride in Pulse-Field Magnetizing Processes
  • Citing Article
  • April 2019

IEEE Transactions on Applied Superconductivity

... In [19] the AC loss of a 66kV HTS cable was studied and reduced by the variation in the topology of the HTS cable. This change is based on the increase of the radius of the former. ...

AC Loss in each layer of three-layer twisted HTS cable
  • Citing Article
  • February 2019

IEEE Transactions on Applied Superconductivity