• Title/Summary/Keyword: Magnetic levitation force

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Linear Induction Motor for Magnetic Levitation Vehicle (자기부상열차용 선형 유도전동기)

  • Kim Jeong-Cheol;Park Yeong-Ho;Kim Dae-Kwang;Choi Jong-Mook
    • Proceedings of the KSR Conference
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    • 2005.05a
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    • pp.220-224
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    • 2005
  • EMU(Electric Multiple Unit) operated in local area is mostly consist of moving system on the rail and the traction motor drives the gear and wheel with the mechanical propulsion force. Most of countries are interested in Magnetic Levitation Vehicle for the transportation system on next generation and they have been studying about it continuously. Thus this paper is studied the Linear Induction Motor as the propulsion equipment of Magnetic Levitation Vehicle

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Limitation of a levitation system using a superconducting bulk (초전도 벌크를 이용한 자기부상 시스템의 한계)

  • 한승용;한송엽
    • Proceedings of the Korea Institute of Applied Superconductivity and Cryogenics Conference
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    • 2001.02a
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    • pp.61-64
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    • 2001
  • Levitation force of a new magnetic levitation system using a super-conducting bulk magnet(SBM) and a permanent magnet(PM) was numerically calculated. The non-linear J-E relation of a SBM was modeled using a critical state model and iteration method, and demagnetization of a PM was considered using a demagnetization curve of a real PM. The maximum limitation of levitation force was found according to increasing the trapped field in a SBM. Finite element method was used for numerical calculation.

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Study on the Optimal Design for HTS Magnetic Levitation Magnet (고온초전도 자기부상자석의 최적설계에 관한 연구)

  • Yoon, Kyung-Yong;Bae, Duck-Kweon;Cho, Heung-Je
    • Progress in Superconductivity and Cryogenics
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    • v.10 no.1
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    • pp.37-41
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    • 2008
  • Superconducting Electrodynamic suspension(EDS) system is generated by the interaction between the magnetic field made by the induced the eddy current in the ground conductor and the moving magnetic field made by onboard superconducting magnet. The levitation force of EDS system, which is proportional to the strength of the moving magnetic field, becomes saturated according to the increase of the velocity. Especially, the levitation force is influenced by the structure of HTS magnet and ground magnet. This paper deals with the optimal design condition for the HTS levitation magnet. The 3-D numerical analysis with FEM was used to find the distribution of the magnetic field, the optimal coil structure, and the calculation of the levitation force.

Orientation and thickness dependence of magnetic levitation force and trapped magnetic field of single grain YBa2Cu3O7-y bulk superconductors

  • Jung, Y.;Go, S.J.;Joo, H.T.;Lee, Y.J.;Park, S.D.;Jun, B.H.;Kim, C.J.
    • Progress in Superconductivity and Cryogenics
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    • v.19 no.1
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    • pp.30-35
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    • 2017
  • The effects of the crystallographic orientation and sample thickness on the magnetic levitation forces (F) and trapped magnetic field (B) of single grain YBCO bulk superconductors were examined. Single grain YBCO samples with a (001), (110) or (100) surface were used as the test samples. The samples used for the force-distance (F-d) measurement were cooled at 77 K without a magnetic field (zero field cooling, ZFC), whereas the samples used for the B measurement were cooled under the external magnetic field of a Nd-B-Fe permanent magnet (field cooling, FC). It was found that F and B of the (001) surface were higher than those of the (110) or (100) surface, which is attributed to the higher critical current density ($J_c$) of the (001) surface. For the (001) samples with t=5-18 mm, the maximum magnetic levitation forces ($F_{max}s$) of the ZFC samples were larger than 40 N. About 80% of the applied magnetic field was trapped in the FC samples. However, the F and B decreased rapidly as t decreased below 5 mm. There exists a critical sample thickness (t=5 mm for the experimental condition of this study) for maintaining the large levitation/trapping properties, which is dependent on the material properties and magnitude of the external magnetic fields.

Characteritic Analysis of Hybrid Levitation and Propulsion System for Super-Speed Maglev (초고속 자기부상열차를 위한 하이브리드형 부상 추진 시스템의 특성 해석)

  • Cho, Han-Wook;Lee, Jong-Min;Han, Hyung-Suk
    • Proceedings of the KIEE Conference
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    • 2009.07a
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    • pp.623_624
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    • 2009
  • This paper deals with the characteristic analysis of electro-magnet (EM)-permanent magnet (PM) hybrid levitation and propulsion device for magnetically levitated (maglev) vehicles. Several machine characteristics such as levitation force with/without control current and thrust are described. In order to verify the analysis results and feasibility of high-speed operation of the maglev vehicle, real-scale static test set is implemented and tested.

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A Levitation Controller Design for a Magnetic Levitation System (자기부상 시스템의 부상제어기 설계)

  • 김종문;강도현;박민국;최영규
    • The Transactions of the Korean Institute of Electrical Engineers D
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    • v.52 no.6
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    • pp.342-350
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    • 2003
  • In this paper, a levitation controller for a magnetic levitation(MagLev) system is designed and implemented. The target to be controlled is PEM(permanent and electromagnet) type with 4-corners levitation which is open-loop unstable, highly non-linear and time-varying system. The digital control system consists of a VME-based CPU board, AD board, PU board, 4-Quadrant chopper, and gap sensor, accelerometer as feedback sensors. In order to estimate the velocity of the magnet, we used 2nd-order state observer with acceleration and gap signal as input and output, respectively. Using the estimated states, a state feedback control law for the plant is designed and the feedback gains are selected by using the pole-placement method. The designed controller is experimentally validated by step-type gap reference change and force disturbance test.

Study on the Characteristics of a Small Scale HTSC Levitation Magnet (소형 초전도 부상자석의 특성 연구)

  • Cho, Hung-Je;Bae, Duck-Kweon;Lee, Jong-Min;Ko, Tae-Kuk
    • Progress in Superconductivity and Cryogenics
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    • v.9 no.1
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    • pp.76-81
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    • 2007
  • This paper deals with the characteristics of a small scale $high-T_c$ superconducting(HTSC) levitation system. The levitation tester. which models after electrodynamic suspension(EDS) maglev, consists of one HTSC magnet, a reaction plate, and force measuring components. Instead of moving magnet, AC current was applied to the fixed HTSC magnet. The magnet also has persistent current switch(PCS). The inductance of the magnet was 18.5 mH and total joint resistance of the magnet was $5.74{\times}10^{-7}\Omega$. AC current was applied into the HTSC magnet with various frequencies and the levitation force was calculated and measured. According to the increase of the vehicle speed, the levitation force was saturated.

Decoupling of Thrust Force and Levitation Force of Transverse Flux Linear Induction Motor by the Active Compensation of Magnetic force across the Air-Gap (공극력의 능동적 보상을 통한 횡자속 선형 유도 구동기의 추력과 부상력의 비연성화)

  • 정광석;백윤수
    • Journal of the Korean Society for Precision Engineering
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    • v.21 no.11
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    • pp.91-98
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    • 2004
  • TFLIM(Transverse Flux Linear Induction Motor), making its closed magnetic path with the direction of the traveling field orthogonal, had been developed to decrease an edge effect of the general induction motor. To control the levitation force and the thrust force on the secondary part of TFLIM independently, the various methodologies have been presented. When we try to achieve the independent control using only the multi-phase inputs assigned in the stator coils as an approach, in which condition we can minimize the coupling effect between two forces\ulcorner In this paper, we show the qualitative influence of a slip frequency, an ac magnitude, a dc offset superposed in the ac power, and a major parameter of TFLIM on the couple through the computer simulation. And to realize the independent motions between levitation and thrust motion without any auxiliary means fur isolation of the secondary part of TFLIM, the decouple compensator is suggested, including the experimental results.

Lorentz Force Type Self-Bearing Motor with 2-Pole Flux Distribution for Levitation and 4-Pole for Rotation (부상용 2극과 회전용 4극 자속 분포를 갖는 로렌쯔형 자기 부상 모터)

  • ;Yohji Okada
    • Proceedings of the Korean Society for Noise and Vibration Engineering Conference
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    • 2001.11a
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    • pp.482-487
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    • 2001
  • This paper introduces a Lorentz force type four-pole self-bearing motor, where the new pole arrangement of a stator is intended to function both as a synchronous PM motor and as a magnetic bearing. The Lorentz force type has some good points such as linearity of control force, freedom from flux saturation, and high efficiency unlike conventional self-bearing motors. Mathematical expressions of torque and radial force are derived to show that they can be separately controlled regardless of rotational speed and time. To verify the proposed theory, a prototype is made, where a ring-shape outer is actively controlled in two radial directions while the other motions are passively stable supposing the radial stability. Through some experiments, it is shown that the proposed scheme can provide high capability and feasibility for a small high-speed self-bearing motor.

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Magnetic levitation force and trapped magnetic field of top-seeded melt-processed YBCO superconductors with multiseeding (다중 종자결정성장법으로 제조한 YBCO 초전도체의 자기 부상력과 포획자력)

  • Kim, Chan-Joong;Jee, Young-A;Kim, Ho-Jin;Joo, Jin-Ho;Han, Young-Hee;Kim, Sang-Jun;Hong, Gye-Won
    • 한국초전도학회:학술대회논문집
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    • v.9
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    • pp.358-362
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    • 1999
  • Magnetic levitation forces and trapped magnetic fields of top-seeded melt growth-processed YBCO superconductors with multiseeding were studied. The number of seeds was varied from one to six. The surface magnetic field of the prepared YBCO samples was dependent on the number of the seeds. The trapped magnetic field of the top surface decreased with increasing the number of the seed. Particularly, it drastically decreased at the YBCO grain boundary, probably due to the weak rink nature of the boundary. The magnetic levitation force also decreased with increasing the number of the seeds, similar to the variation of the surface magnetic field.

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