• Title/Summary/Keyword: Flux2D

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Subcooled Burnout Heat Flux on a Heated Surface with Impinging Water Jet (충돌수분류(衝突水噴流)에 의한 서브쿨 Burnout열류속(熱流束)에 관한 연구)

  • Ohm, K.C.;Lee, J.S.;Park, S.Y.
    • Korean Journal of Air-Conditioning and Refrigeration Engineering
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    • v.8 no.4
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    • pp.527-536
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    • 1996
  • Convective nucleate boiling and burnout heat flux have been studied on a flat, downward facing, constant heat flux surface cooled by an impinging water jet. The tests are progressed from low, nonboiling power to high, burnout heat flux power. The jet velocity and the subcooling do not affect the nucleate boiling curve of $q{\sim}{\Delta}T_{sat}$ diagram, but the supplementary water height affects the curve. For the case of dimensionless height of supplementary water S/D=1, the boiling curve shift to the heigher heat flux than that of S/D=0 or S/D=2. Burnout heat flux is enhanced with increasing jet velocity and subcooling. Also. by using the supplementary water(S/D=1 or S/D=2), burnout heat flux is larger than that of the simple water jet(S/D=0). A generalized correlation for the burnout heat flux data in the present boiling system with an impinging water jet is successfully evolved.

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Characteristic Analysis of a Permanent Magnet Transverse Flux Linear Motor with Spiral Core

  • Lee, Ji-Young;Kim, Ji-Won;Woo, Byung-Chul;Kang, Do-Hyun
    • Journal of Magnetics
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    • v.18 no.2
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    • pp.111-116
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    • 2013
  • This paper presents a characteristic analysis method of a permanent magnet type transverse flux linear motor (TFLM) with spiral cores. The spiral cores are used as the mover cores in order to make 3-dimensional (3-D) magnetic flux paths at the TFLM which have 3-D magnetic flux flows. The 3-D Equivalent Magnetic Circuit Network Method is used to analyse the magnetic characteristics of the machine, and an imaginary part, 'flux barrier,' is introduced to consider the spiral core characteristic. Magnetic parameters such as flux, inductance, and thrust are calculated from the analysis results. The computed thrust forces are compared to measured values to confirm the accuracy of the analysis.

Characteristics of Carbon Circulation for Ascidian Farm in Jindong Bay in Summer and Winter (진동만 미더덕 양식장의 하계 및 동계 탄소 순환 특성)

  • Park, Jihye;Cho, Yoonsik;Lee, Won-Chan;Hong, Sokjin;Kim, Hyung-Chul;Kim, Jeong-Bae;Park, Junghyun
    • Journal of Wetlands Research
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    • v.14 no.2
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    • pp.211-221
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    • 2012
  • The ascidian Styela clava has been one of the favorite seafood in Korea. Suspended culture of Styela clava was initiated in 2001 and the annual production reached 15,084 M/T, but declined to 2,655 M/T in 2011. In order to solve this problem, it is necessary to estimate the material balance according to the farm-environment. Vertical particulate fluxes and release fluxes were estimated at 2 stations, an ascidian farm (AF) and a non-cultivated area (control) in Jindong Bay. An in-situ benthic chamber(BelcI) was used in summer and winter season. The sedimentation fluxes of organic carbon were 72 mmol C $m^{-2}\;d^{-1}$, 93 mmol C $m^{-2}\;d^{-1}$, 34 mmol C $m^{-2}\;d^{-1}$ in Jul. AF, Feb. AF, Feb. control. The organic carbon oxidation rates were 13 mmol C $m^{-2}\;d^{-1}$, 81 mmol C $m^{-2}\;d^{-1}$, 31 mmol C $m^{-2}\;d^{-1}$, in each. The release fluxes of nutrients followed the general pattern, well. Consequently, the ratio of the organic carbon burial fluxes were 20:4:1, in each. By the estimation of the carbon circulation, it could be a scientific basis to analyze the reason of production decline for cultivated organism.

Performance Analysis of Linear Brake by Using Efficient 2-D Model (유효한 2차원 모델을 이용한 리니어 브레이크 성능 해석)

  • Han, Pil-Wan;Chun, Yon-Do;Lee, Ju;Lee, Kwan-Seop
    • Proceedings of the KSR Conference
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    • 1998.11a
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    • pp.601-607
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    • 1998
  • This paper presents the efficient 2-D linear brake analysis model which can compensate the lateral leakage flux by changingng the airgap length and magneto-motive force(MMF). The linkage flux of the 2-D analysis is larger than that of 3-D analysis. This is caused by the assumption in 2-D analysis that geometric and physical values are constant along the perpendicular direction(z) to the analysis region. The equivalent MMF have been calculated from the linkage flux difference between the 2-D and 3-D analyses which are performed at zero velocity. The performances of the linear brake have been analyzed effectively by using the compensated 2-D models without using 3-D FEM.

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Analysis of Flux Distribution in 2 Phase 8 Pole HB type LPM by 3D FEM (3차원 유한요소법에 의한 2상 8극 HB형 LPM의 가동자의 자속분포 해석)

  • Lee, Dong-Ju;Lee, Eun-Woong;Kim, Sung-Hun;Kim, Sung-Jong
    • Proceedings of the KIEE Conference
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    • 1999.07a
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    • pp.34-36
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    • 1999
  • 2 phase 8 pole HB type LPM(linear pulse motor) has the suitable structure for it's microstep drive. Hence, if this LPM will be drived by this method, the limited(mechanically) step resolution can be increased further and vibration and noise can be decreased considerably. But, It is difficult that this LPM was analyzed in detail because of it's complex magnetic circuits to be composed the LF(longitudinal flux) and TF(transverse flux.) path. If LPM was analyzed by the approximate 2D model, we could not be obtained satisfactory result. Therefore, It is necessary to be analyzed the 3D model in detail for the more satisfactory results. In this paper, we obtain 3D flux distribution of the mover using by 3D FEM(finite element method)

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Characteristic Analysis of a Magnet for Magnetically Levitated Vehicle using FLUX3D (FLUX3D를 이용한 자기부상용 전자석의 특성 해석)

  • Lee, Jae-Kun;Shin, Pan-Seok
    • Proceedings of the KIEE Conference
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    • 1996.07a
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    • pp.127-129
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    • 1996
  • A 3-dimensional analysis is desired for a magnet of magnetically levitated vehicle because the geometrical shape of the magnet is complicated and nonsymmetric. A FEM package of FLUX3D is used to analyze the characteristic of the magnet. Various quantities could be observed like levitation force, flux density distribution along the air gap, edge and fringing effect, leakage flux pattern, etc. The simulation results from FLUX3D are compared with those of 2-D analysis and test results. There are a little difference between results due to the boundary conditions and magnetized B-H curve of the core.

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Experimental study of the heat pipe phenomenon in porous media heated from above (상부가열인 다공물질내의 열파이프 현상에 관한 실험적 연구)

  • 이진호;김홍제;함윤영;남궁규완
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.12 no.4
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    • pp.825-832
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    • 1988
  • An experiment was performed to study the heat pipe phenomenon of porous media heated above at one-dimensional steady state for the range of heat flux, 300 W/ $m^{2}$ ~ 2000w/ $m^{2}$. Glass beads, sand, and copper particles were used as porous media and distilled water was used as a working fluid. Result of experiment shows that the length of the two-phase zone increases with the decreasing particle size for the same heat flux. At relatively lower heat flux the length of the two-phase zone increases with the increasing heat flux, which contradicts the result of earlier work. However, its length remains nearly constant when the heat flux increases above a certain value. The length of the two-phase zone is proportional to the product of the heat flux by the hydrostatic capillary height under the limited value on heat flux, that is, $l_{t}$ = A(q. $l_{cap}$)+B, q.leg.1/A(C+B/ $l_{cap}$) where A is 1.7*10$^{-4}$ $m^{2}$/w, B is 1.9*10$^{-2}$ m, and C is 0.43 for copper particles and 0.31 for glass beads and sand.d.d.d.

Interlaminar Flux Density Distribution at Joints of Overlapping Stacked Electrical Steel and Amorphous Ribbons

  • Erdem, Sezer;Derebasi, Naim
    • Journal of Magnetics
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    • v.15 no.4
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    • pp.190-193
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    • 2010
  • The design of joints in a transformer core significantly affects the transformer's efficiency. Air gaps cause variations in the flux distribution at the joints of the laminations, which depend on the geometry. Two similar samples consisting of electrical steel strips and amorphous ribbons were made. The spatial flux distributions were determined using an array of search coils for each sample. 2D models of these samples were created and examined by finite element analysis. The magnetic flux distribution for each lamination in the samples was computed. The results show that the flux density in amorphous ribbons above and below the air gap starts to approach saturation at lower flux density levels than for electrical steel. The flux density measured using the search coil under the air gap is increased in amorphous ribbons and decreased in the electrical steel with increasing frequency.

Dependence of the peak fluxes of solar energetic particles on CME parameters and magnetic connectivity

  • Park, Jinhye;Moon, Yong-Jae;Lee, Harim;Kahler, S.W.
    • The Bulletin of The Korean Astronomical Society
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    • v.42 no.2
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    • pp.82.3-83
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    • 2017
  • We investigate the relationships between the peak fluxes of 18 solar energetic particle (SEP) events and associated coronal mass ejection (CME) 3D parameters (speed, angular width, and separation angle) obtained from SOHO, STEREO-A and/or B for the period from 2010 August to 2013 June. We apply the STEREO CME Analysis Tool (StereoCAT) to the SEP-associated CMEs to obtain 3D speeds and 3D angular widths. The separation angles are determined as the longitudinal angle between flaring regions and magnetic footpoints of the spacecraft, which are calculated by the assumption of Parker spiral field. The main results are as follows. 1) We find that the dependence of the SEP peak fluxes on CME 3D speed from multi-spacecraft is similar to that on 2D CME speed. 2) There is a positive correlation between SEP peak flux and 3D angular width from multi-spacecraft, which is much more evident than the relationship between SEP peak flux and 2D angular width. 3) There is a noticeable anti-correlation (r=-0.62) between SEP peak flux and separation angle. 4) The multiple regression method between SEP peak fluxes and CME parameters shows that the longitudinal separation angle is the most important parameter, and the CME 3D speed is secondary on SEP peak flux.

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