• Title/Summary/Keyword: Magnetic levitation

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Development of Rotary Actuator Including Function of Axial Bearing (축방향 베어링 통합 회전 구동기의 개발)

  • 허진혁;정광석;백윤수
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 2003.06a
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    • pp.1083-1086
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    • 2003
  • Recently, the study on bearingless motors which integrate both motor and magnetic bearing function in one stator is very active, as many machines have high rotational speed, high precision, smaller size and lighter weight. In this paper, we propose a novel rotary actuator including function of axial bearing using Lorentz force as a preceding research for development of a bearingless motor. As using Lorentz force, this type has some merits such as the linearity of control force, freedom from flux saturation and high efficiency unlike conventional rotary actuators using a reluctance force. This type is cotrolled independently in levitation and rotational directions respectively. It shows by mathematical expression of levitation force and torque in the proposed rotary actuator. And also, the levitation force is generated by magnetic interaction between the magnetic materials and the rotational torque is generated by Lorentz force. Finally. for verification of this proposed system, a prototype is made and some experiments will be performed in the near future.

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Analysis on Superconducting Electrodynamic Suspension for Very High Speed Maglev (초고속 자기부상열차를 위한 초전도 반발식 자기부상 특성 해석)

  • Bae, Duck-Kweon;Lee, Jong-Min;Cho, Han-Wook;Han, Hyung-Suk
    • Proceedings of the KIEE Conference
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    • 2009.04b
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    • pp.198-200
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    • 2009
  • This paper presents the numerical simulation results on the moving type electrodynamic suspension (EDS) simulator. Superconducting 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 conductor. 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.

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Levitation Control Simulation of a Maglev Vehicle Considering Guideway Flexibility (가이드웨이 유연성이 고려된 자기부상열차 부상제어 시뮬레이션)

  • Han, Jong-Boo;Lim, Jaewon;Kim, Chang-Hyun;Han, Hyung-Suk;Kim, Sung-Soo
    • Journal of the Korean Society for Railway
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    • v.18 no.1
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    • pp.15-24
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    • 2015
  • In magnetic levitation vehicles, the clearance between the magnet and track should be maintained within an allowable range through a feedback control loop. The flexibility of the guideway would introduce additional modes in the overall suspension system, resulting in dynamic interaction between the guideway vibration and the electromagnetic suspension control system. This dynamic interaction can be a serious problem, particularly at very low speeds or standstill, and may cause airgap instability. To optimize the overall system dynamics, an integrated dynamic model including mechanical and electrical parts and a flexible guideway as well as a control loop was developed. With the proposed model, airgap simulations at standstill were performed while varying the control gains, specifically with the aim of understanding the effects of gains of the PID controller on the airgap variation. The findings may be used to achieve a stable levitation controller design.

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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Development of Magnetic Bearing Controller with High Magnetic Levitation Accuracy (높은 자기부상 정밀도를 갖는 자기베어링 제어기 개발)

  • Lee, Seokwon;Huh, Heon
    • The Journal of the Institute of Internet, Broadcasting and Communication
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    • v.19 no.1
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    • pp.225-229
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    • 2019
  • Magnetic bearings are widely used in vacuum and clean environments or in high-precision applications, because they have no mechanical friction and have stable dynamic characteristics. Despite the aforementioned advantages of magnetic bearings, their applications are generally limited due to the controller complexity. In this paper, we proposed a reduced-complexity digital controller for magnetic bearings. In addition, we analyzed and solved the problems, such as quantization errors in the analog-to-digital conversion and integral windup in a feedback controller, which are known as the main causes of performance degradation. Experiments showed that the proposed digital controller achieves a target magnetic levitation accuracy.

Magnetic Properties of $GdBa_2Cu_3O_{7-y}$ Bulk Superconductors Fabricated by a Top-seeded Melt Growth Process (종자 결정 성장법으로 제조된 $GdBa_2Cu_3O_{7-y}$ 벌크 초전도체의 자기적 특성)

  • Kim, K.M.;Park, S.D.;Jun, B.H.;Ko, T.K.;Kim, C.J.
    • Progress in Superconductivity
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    • v.14 no.1
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    • pp.39-44
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    • 2012
  • The fabrications condition and superconducting properties of top-seeded melt growth (TSMG) processed $GdBa_2Cu_3O_{7-y}$ (Gd123) bulk superconductors were studied. Processing parameters (a maximum temperature ($T_{max}$), a temperature for crystal growth ($T_G$) and a cooling rate ($R_G$) through a peritectic temperature ($T_P$) for the fabrication of single grain Gd123 superconductors were optimized. The magnetic levitation forces, trapped magnetic fields, superconducting transition temperature ($T_c$) and critical current density ($J_c$) of the Gd123 bulks superconductors were estimated. Single grain Gd123 bulk superconductors were successfully fabricated at the optimized processing condition. The $T_c$ of a TSMG processed Gd123 sample was 92.5 K and the $J_c$ at 77 K and 0 T was approximately $50kA/cm^2$. The trapped magnetic field contour and magnetic levitation forces were dependent on the top surface morphology of TSMG processed Gd123 samples. The single grain Gd123 samples, field-cooled at 77 K using a Nd-B-Fe permanent magnet with 5.27 kG and 30 mm dia., showed the trapped magnetic field contour of a single grain with a maximum of 4 kG at the sample center. The maximum magnetic levitation forces of the single grain Gd123 sample, field-cooled or zero field-cooled, were 40 N and 107 N, respectively.

Experiments of a Novel Magnetic Levitation Stage for Wide Area Movements

  • Jeon, Jeong-Woo;Caraiani, Mitica;Oh, Hyeon-Seok;Kim, Sung-Shin
    • Journal of Electrical Engineering and Technology
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    • v.7 no.4
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    • pp.558-563
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    • 2012
  • In this paper, a novel planar type magnetic levitation system without other assistant devices is proposed and it can move with 6 degree of freedom (X, Y, Z, ${\theta}_X$, ${\theta}_Y$, ${\theta}_Z$) in wafer size as well as in nano scale positioning.The mover is composed with 2-D Halbach permanent magnet array and the stator is composed with $10{\times}10$ coil arrays.It was composed in laboratory and tested with short stroke (4 [mm]) and long stroke (160 [mm])movements. The errors of short movement test is [X, Y, Z, ${\theta}_X$, ${\theta}_Y$, ${\theta}_Z$]${\leq}$ [${\pm}200nm$, ${\pm}200nm$, ${\pm}250nm$, ${\pm}3urad$, ${\pm}2urad$, ${\pm}1urad$]The errors of long stroke movement test is [X, Y, Z, ${\theta}_X$, ${\theta}_Y$, ${\theta}_Z$]${\leq}$ [${\pm}200nm$, ${\pm}200nm$, ${\pm}250nm$, ${\pm}1.5urad$, ${\pm}2urad$, ${\pm}0.5urad$].