• Title/Summary/Keyword: magnetic field distribution

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Analysis on the magnetic field of PMLSM according to skew (Skew에 따른 PMLSM의 자계특성 해석)

  • Jang, Seok-Myeong;Seo, Jung-Chul;You, Dae-Joon;Choi, Jang-Yung;Cho, Han-Wook
    • Proceedings of the KIEE Conference
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    • 2005.04a
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    • pp.102-104
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    • 2005
  • This paper deal with the prediction of magnetic field distribution for permanent magnet linear synchronous motor (PMLSM) with infinite operation range. The magnetic field distribution is predicted using a two-dimensional (2-D) analytical solution derived in terms of magnetic vector potential. The slotting and skew is considered using the relative permeance function. The results are validated extensively by finite element (FE) analyses.

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A Study of the Characteristics on the Vacuum Interrupter with Axial Magnetic Field Type using 3 Dimension Finite Element Analysis (3차원 유한요소해석을 이용한 종자게형 진공 인터럽터의 특성고찰)

  • 하덕용;강형부
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.15 no.5
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    • pp.460-467
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    • 2002
  • This paper deals with the distribution characteristics of the current density and axial magnetic flux density on the vacuum interrupter with axial magnetic field type using 3 dimension finite element analysis. An axial magnetic field parallel to the current flow in the arc column can improve the current breaking capacity of vacuum interrupter by affecting the arc mode. The axial magnetic flux density on the contact electrode surface is analyzed by inputting external current as a function of the transient time for sine half wave. And it also is analyzed within the gap distance of the contact electrode. The peak value of current but is decreased with the descending current on the contact electrode surface and within the gap distance of the contact electrode. The residual magnetic field is generated on the contact electrode surface and within the gap distance in the instant of zero current, which is due to the influence of eddy currents. The phase shift due to eddy currents, defined as time difference between the maximum value of current and axial magnetic field, is about 1ms in the center point of gap distance.

The Development of Axial Magnetic Field Type Vacuum Interrupter (종자계형 진공인터럽터의 개발)

  • 박홍태;안희일;김성일;이경행
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2001.07a
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    • pp.231-233
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    • 2001
  • Axial magnetic field(AMF) type electrodes can be increase the interrupting capability of vacuum interrupters. Depending on the design, the principle of the local axial magnetic field arrangement are different. In this paper, a new AMF contact design based on a unipolar field arrangement and its characteristics are introduced. The influence of the unipolar AMF on the arc behavior is described by high-speed video camera. In addition, three-dimensional AMF simulations have been peformed by means of a finite element analysis(FEM) program to analyze the influence of magnetic field distribution on the AMF performance. The high interrupting capability of the unipolar AMF type electrode has been confirmed by three-phase test.

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Power Frequency Magnetic Field Reduction Method for Residents in the Vicinity of Overhead Transmission Lines Using Passive Loop

  • Lee, Byeong-Yoon;Myung, Sung-Ho;Cho, Yeun-Gyu;Lee, Dong-Il;Lim, Yun-Seog;Lee, Sang-Yun
    • Journal of Electrical Engineering and Technology
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    • v.6 no.6
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    • pp.829-835
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    • 2011
  • A power frequency magnetic field reduction method using passive loop is presented. This method can be used to reduce magnetic fields generated within the restricted area near transmission lines by alternating current overhead transmission lines. A reduction algorithm is described and related equations for magnetic field reduction are explained. The proposed power frequency magnetic field reduction method is applied to a scaled-down transmission line model. The lateral distribution of reduction ratio between magnetic fields before and after passive loop installation is calculated to evaluate magnetic field reduction effects. Calculated results show that the passive loop can be used to cost-effectively reduce power frequency magnetic fields in the vicinity of transmission lines generated by overhead transmission lines, compared with other reduction methods, such as active loop, increase in transmission line height, and power transmission using underground cables.

Influences on Distribution of Solute Atoms in Cu-8Fe Alloy Solidification Process Under Rotating Magnetic Field

  • Zou, Jin;Zhai, Qi-Jie;Liu, Fang-Yu;Liu, Ke-Ming;Lu, De-Ping
    • Metals and materials international
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    • v.24 no.6
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    • pp.1275-1284
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    • 2018
  • A rotating magnetic field (RMF) was applied in the solidification process of Cu-8Fe alloy. Focus on the mechanism of RMF on the solid solution Fe(Cu) atoms in Cu-8Fe alloy, the influences of RMF on solidification structure, solute distribution, and material properties were discussed. Results show that the solidification behavior of Cu-Fe alloy have influenced through the change of temperature and solute fields in the presence of an applied RMF. The Fe dendrites were refined and transformed to rosettes or spherical grains under forced convection. The solute distribution in Cu-rich phase and Fe-rich phase were changed because of the variation of the supercooling degree and the solidification rate. Further, the variation in solute distribution was impacted the strengthening mechanism and conductive mechanism of the material.

Effect of Low Magnetic Field on Dose Distribution in the SABR Plans for Liver Cancer

  • Son, Jaeman;Chun, Minsoo;An, Hyun Joon;Kang, Seong-Hee;Chie, Eui Kyu;Yoon, Jeongmin;Choi, Chang Heon;Park, Jong Min;Kim, Jung-in
    • Progress in Medical Physics
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    • v.29 no.2
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    • pp.47-52
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    • 2018
  • To investigate the effect of low magnetic field on dose distribution in SABR plans for liver cancer, we calculated and evaluated the dose distribution to each organ with and without magnetic fields. Ten patients received a 50 Gy dose in five fractions using the $ViewRay^{(R)}$ treatment planning system. For planning target volume (PTV), the results were analyzed in the point minimum ($D_{min}$), maximum ($D_{max}$), mean dose ($D_{mean}$) and volume receiving at least 90% ($V_{90%}$), 95% ($V_{95%}$), and 100% ($V_{100%}$) of the prescription dose, respectively. For organs at risk (OARs), the duodenum and stomach were analyzed with $D_{0.5cc}$ and $D_{2cc}$, and the remained liver except for PTV was analyzed with $D_{mean}$, $D_{max}$, and $D_{min}$. Both inner and outer shells were analyzed with the point $D_{min}$, $D_{max}$, and $D_{mean}$, respectively. For PTV, the maximum change in volume due to the presence or absence of the low magnetic field showed a percentage difference of up to $0.67{\pm}0.60%$. In OAR analysis, there is no significant difference for the magnetic field. In both shell structure analyses, although there are no major changes in dose distribution, the largest value of deviation for $D_{max}$ in the outer shell is $2.12{\pm}2.67Gy$. The effect of low magnetic field on dose distribution by a Co-60 beam was not significantly observed within the body, but the dose deposition was only appreciable outside the body.

Magnetic Interaction in FeCo Alloy Nanotube Array

  • Zhou, D.;Wang, T.;Zhu, M.G.;Guo, Z.H.;Li, W.;Li, F.S.
    • Journal of Magnetics
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    • v.16 no.4
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    • pp.413-416
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    • 2011
  • An array of FeCo nanotubes has been successfully fabricated in the pores of porous anodic aluminum oxide (AAO) templates by wetting templates method. The morphology and structure of the nanotube array were characterized by scanning electron microscopy, transmission electron microscopy and x-ray diffraction. The average diameter of the nanotubes was about 200 nm, and the length was more than 10 ${\mu}m$. Vibrating sample magnetometer and superconducting quantum interference device were used to investigate the magnetic properties of the nanotube array. Interaction between the nanotubes has been found to be demagnetizing as expected and the switching field distribution is broad.

Efficient Magnetic Field System for High Speed Electric Machines (초고속 전기기기용 고성능 자기회로 시스템)

  • Jang, S.M.;Seo, J.H.;Jeong, S.S.;Lee, S.H.;Choi, S.K.
    • Proceedings of the KIEE Conference
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    • 1997.11a
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    • pp.19-21
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    • 1997
  • This paper treated a new method that generates the dipole magnetic field for high speed machines by using Halbach array, which was suggested by Klaus Halbach. The Halbach array can produce the various field distribution without magnetic materials. Therefore, the iron losses can be reduced. This paper presented the magnetic characteristics on both linear and cylindrical Halbach array. And the Halbach array for dipole field was manufactured with Nd-Fe-B magnets having 1.17(T), the measured flux density was compared the theoretical values acquired by three dimensional FEM analysis. Finally, the magnetic characteristics of Halbach array were compared with those of other conventional dipole field systems.

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A Study on the Development of Vacuum Interrupter with Axial Magnetic Field type (종자계방식 진공인터럽터 개발에 관한 연구)

  • Kim, Sung-Il;Park, Hong-Tae;Ahn, Hee-Il;Seo, Jung-Min
    • Proceedings of the KIEE Conference
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    • 2000.07b
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    • pp.943-945
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    • 2000
  • In this paper described that study on the distribution and characteristics of axial magnetic field by mathematical analysis and experiment for axial magnetic field type vacuum interrupter that important part on vacuum circuit breaker. And, it was shown that inspected results of arc shape at breaking the current by typical axial magnetic field type model and new axial magnetic field type model.

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Magnetic Properties of YBCO Superconducting Bulk

  • Lee, Sang-Heon
    • Transactions on Electrical and Electronic Materials
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    • v.6 no.2
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    • pp.67-69
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    • 2005
  • Magnetic properties of a field cooled YBaCuO superconductor beneath the toroidal permanent magnet was examined by means of improved magneto-balancing method at 77 K. Magnetic flux measurements of a toroidal magnet revealed a concave shaped field distribution with a single minimum and a null field along the axis of the torus at the point where the field reversed. The observed values of both the suspension position and the force exerted upon the superconductor specimen were in good agreement with those calculated from the magnetization curve of the specimen and the intensity of the magnetic field of the used permanent magnet.