• Title/Summary/Keyword: 자속 밀도

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Flux saturation detector for Reactor (리액터 포화 검출시스템)

  • BAE, Joung-Hwan;Baik, Bo-Hyun;Won, Chung-Yuen
    • Proceedings of the KIPE Conference
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    • 2015.07a
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    • pp.141-142
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    • 2015
  • 전기전자 기술발달에 따라 여러 가지 형태의 전기전자 부품이 많이 사용되고 있다. 이러한 전기전자 부품은 트랜지스터, Op Amp 등의 능동소자와 저항, 캐패시터, 리액터 등의 수동소자로 구분할 수 있다. 능동소자의 경우에는 사용용도에 따라 대부분 제조사에서 명확한 사양을 제공하지만, 수동소자의 경우는 명확한 사양을 제공하지 못하는 부품들도 있다. 정격범위를 명확히 제시하지 못하는 소자에 대표적으로 리액터가 있으며, 경우에 따라 정격에 미달하는 수준의 제품도 유통되고 있는 실정이다. 본 논문은 리액터 설계사양에 해당하는 철심의 자속밀도에 대한 실제 제품의 자속밀도포화 여부를 확인할 수 있는 기기의 동작설명과 그 실험결과를 제시한다.

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Design of 700kHz 1.8kW GaN-based Isolated DC-DC Converter for xEV using Planar Matrix Transformer (평면 변압기를 이용한 xEV용 GaN 기반 1.8kW 700kHz 절연형 DC-DC컨버터 설계)

  • Adhistira, Adhistira;Kim, Sang-jin;Choi, Se-wan;Yang, Dae-ki;Hong, Seok-yong
    • Proceedings of the KIPE Conference
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    • 2018.11a
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    • pp.193-194
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    • 2018
  • 본 논문은 $6kW/L(98W/in^3)$의 전력밀도를 갖는 xEV LDC를 위한 절연형 DC-DC컨버터의 설계 방법을 제안한다. 부피를 가장 많이 차지하는 수동소자의 부피를 줄이기 위해 GaN소자를 적용하여 스위칭 주파수를 700kHz를 적용하였다. 또한 자속 상쇄 개념이 적용된 매트릭스 평면 변압기를 적용하여 변압기의 부피를 크게 줄일 수 있었다. 본 논문에서는 후보 토폴로지들의 비교를 통해 고 전력 밀도에 가장 적합한 토폴로지를 선정하였으며, 자속상쇄 개념 기반의 매트릭스 평면 변압기를 설계방법을 제안하였다.

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Development of stimulator for peripheral disturbance therapy using A variable Micro-electromagnetic (미약 전자기장을 이용한 말초장애 치료시스템 개발)

  • Kim, Soo-Byung;Lee, Seung-Wook;Shim, Ta-Kyu;Lee, Na-Ra;Lee, Yong-Heum
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.14 no.5
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    • pp.1209-1216
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    • 2010
  • It has increased that peripheral disturbance(blood flow, nerve, Raynaud's phenomenon) and finger rheumatoid arthritis which is caused by the diabetic complications. To improve these pain issues, we proposed new method for the Finger Disease Therapy(FDT). In this paper, we manufactured solenoid cylindrical coil which was only for the FDT using a variable micro-electromagnetic. Also, we designed the Finger Disease Therapy System(FDTS) which could select three stimulation modes(N_pulse, S_pulse, N/S_pulse) and frequency(0.25hz, 0.5hz, 1hz). We used a Teslameter to measure magnetic flux inner solenoid, and measured magnetic flux as distance(0 ~ 3cm) inner solenoid with stimulation modes and frequency. In the results, magnetic flux was the highest in center of solenoid(0cm) for all stimulation modes. Also, the highest magnetic flux was measured as N_pulse(294.3mT), S_pulse(293.8mT) in 1Hz and N/S_pulse (275.4mT) in 0.25Hz, respectively. Therefore, we developed the FDTS using various pattern and intensity for finger diseases therapy, and checked therapy clinic application possibility of the FDTS as measuring magnetic flux inner solenoid.

Diagnosis Method and Characteristic Analysis of Shorted Turns on Generator Rotor using Flux Sensorless (자속센서리스 회전자 층간단락 진단기법 및 특성해석)

  • Kim Sun-Ja;Jeon Ywun-Seok;Lee Seung-Hak;Jeong Byung-Hwan;Lee Myung-Un;Choe Gyu-Ha
    • The Transactions of the Korean Institute of Power Electronics
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    • v.10 no.3
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    • pp.257-263
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    • 2005
  • Short-circuit rotor windings on a generator causes unstable oscillation of unbalance of flux, asymmetrical heat. In order to prevent serious accidents of short-circuit rotor windings, it is important to study the shorted-turn diagnosis method for rotor windings of the generator. To improve the defects of the diagnosis with sensors, the new sensorless method for rotor shorted-turn diagnosis is proposed, which is to measure the electrical values of the voltage and current at the generator and then to detect if the shorted-turned phenomena would occurred. For the feasibility of the suggested method the theoretical results are shown in the aspects of the air-gap flux density, the flux leakage, the generated output voltage and the shorted field current through the digital simulation. Also the possibility of decision for the suggested sensorless method could be shown in this paper.

Soft Magnetic Properties of FeTaNC Nanocrystalline Thin Films (FeTaNC 초미세결정박막의 반응가스 분압에 따른 자기특성 변화)

  • 고태혁;신동훈;김형준;남승의;안동훈
    • Journal of the Korean Magnetics Society
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    • v.6 no.3
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    • pp.151-157
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    • 1996
  • Magnetic properties and microstructures of FeTaNC thin films, which were deposited by magnetron reactive sputtering rrethod, were investigated as a function of $CH_{4}$ and $N_{2}$ gas partial pressures. Magnetic properties of FeTaNC films depended on total reactive gas pressure as well as $CH_{4}/N_{2}$ pressure ratios. For reactive gas partial pressures of 5~10 %, optimum magnetic properties were observed in the FeTaNC films with proper $CH_{4}/N_{2}$ ratio. On the other hand, at 15% of gas partial pressure, FeTaN and FeTaC films showed superior properties to FeTaNC films. Above 15%, the magnetic properties of films rapidly degraded due to an excess incorporation of C and/or N atoms. Excellent soft magnetic properties of 17 kG of Bs, 0.3 Oe of He, and 4000 of $\mu'$(at 5 MHz) were obtained in the FeTaNC films. High permeabilities of FeTaNC films could be explained by the Fe lattice distortion caused by N atoms, hence reduction of magnetic anisotopy. While precipitated TaN and TaC particles effectively supress the growth of $\alpha-Fe$ grains leading to a good soft magentic properties, FeN and FeC phases such as $Fe_3N$, $Fe_4N$, FexC have detrimental effects.

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Magnetic properties of Sr-ferrite by La-Co substitution (La-Co 치환량에 따른 스트론튬 페라이트의 자기특성)

  • 장세동
    • Resources Recycling
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    • v.11 no.5
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    • pp.16-20
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    • 2002
  • This experiment was carried out to examine the effects of La-Co substitution on Sr-ferrite. The magnetic properties of calcined and sintered materials varied with the substitutional amount of La and Co elements in Sr-ferrite. Anisotropy field and coercivity for Sr ferrite were increased with raising La-Co substitution amounts. The microstructure observation for Sr ferrite substituted by La-Co revealed that La-Co inhabited grain growth during calcination and promoted lateral grain growth during sintering. The relationship between $B_{r}$ and $_{i}$ /$H_{c}$ for La-Co substituted Sr-ferrite was found to be $B_{r}$$≒0.097_{i}$ /$H_{c}$/+4500. In case of $SrFe_{12}$ $O_{19}$, $B_{r} was 4090 G and $_{ i}$$H_{c}$ was 3560 Oe, but $B_{r}$ was 4080 G and and $_{i}$ $H_{c}$ was 4800 Oe for $Sr_{0.7}$ $La_{0.3}$ $Fe_{11.7}$ /$Co_{0.3}$ $O_{19}$.

Magnetoresistive Effect in Ferromagnetic Thin Films( I ) (강자성체 박막(Fe-Ni, Co-Ni)의 자기-저항 효과에 관한 연구( I ))

  • Chang, C.G.;Yoo, J.Y.;Song, J.Y.;Yun, M.Y.;Park, J.H.;Son, D.R.
    • Journal of Sensor Science and Technology
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    • v.1 no.1
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    • pp.23-34
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    • 1992
  • In order to fabricate magnetoresistive sensor, Fe-Ni and Co-Ni alleys were evaporated on the slide glass and the silicon wafers. Saturation magnetic induction($B_{s}$), coercive field strength($H_{c}$) and magnetoresistance were measured for fabricated samples. The evaporated Fe-Ni thin films show that the saturation magnetic induction was 0.65 T, and coercive field strength was 0.379 A/cm, and this value was changed to 0.370 A/cm(//), 0.390 A/cm(${\bot}$), respectively after magnetic annealing. For the measurement of coercive field strength, magnetizing frequency of 1 kHz was used. For the fabricated sensor element, the change of magnetoresistance (${\Delta}R/R$) was excessively unstable due to oxidation in the process of fabrication. The evaporated Co-Ni alloy thin films show that saturation magnetic induction was 0.66 T, and coercive field strengthes were 5.895 A/cm(//), 5.898 A/cm(${\bot}$), respectively, after magnetic annelaing. The change of magnetoresistance(${\Delta}R/R$) was $3.6{\sim}3.7%$ of which value was excessively stable to room temperature. Fe-Ni thin film could have many problems due to large affinity in the process of fabrication of magnetoresistance sensor, but Co-Ni thin film could be a suitable material for fabrication of magnetoresistance sensor, because of its small affinity and definite magnetoresistance effects.

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Major B-H Loop Measurement of Toroidal Shape Magnetic Powder Core (토로이드형 분말코어의 Major B-H Loop 측정)

  • Son, Derac
    • Journal of the Korean Magnetics Society
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    • v.24 no.3
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    • pp.76-80
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    • 2014
  • Toroidal cores made of metallic powder requires large magnetic field strength up to few decade kA/m to obtain major hysteresis loop. To overcome thermal heat generation problem from large exciting current during measurement, we have employed a real time hysteresis loop tracer which can digitize and calculate B-H signals in personal computer as real time. For example, when we magnetize specimen at 10 Hz frequency, we could display hysteresis loops 10 times per second. Using the real time hysteresis loop tracer, we could measure major hysteresis loop of toroidal shape metallic powder core at maximum flux density or maximum magnetic field strength to be measured within 5 second not to significant increasement of specimen temperature due to the heat dissipation from coil windings. For the constructed hysteresis loop tracer, we could measure hysteresis loop at magnetic field strength higher than 50 kA/m for the toroidal shape specimen.

Field Analysis in the Ferrite Core at 100 kHz Band Magnetic Field (100 kHz 대역의 자계 환경내(內)에서의 페라이트 코어의 계(界) 해석)

  • Koo, Bon-Chul;Yoo, Jae-Sung;Kim, Mi-Ja;Gimm, Yoon-Myoung
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.18 no.8
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    • pp.977-983
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    • 2007
  • Recently, the number of systems which utilize wireless power transmission to a receiving module in a short distance is increasing. For efficient use of receiving space, coils are wound around the ferrite core to produce electromotive force(emf) in suppling power by wireless transmission. This paper analyzed the magnetic flux density distribution in the ferrite core in magnetic field environment which is uniformly oriented along to a single axis at 125kHz. For numerical analysis, Ansoft Maxwell which is applying the FEM(Finite Element Method) method was used. We studied the variations of the gathered magnetic fluxes to the changes of the relative permeabilities of the ferrite cores. Also we calculated the magnetic flux variation by shaving the ferrite core off for the groove of coil winding. Results showed that using a small ferrite core in magnetic field at 100kHz band can increase the amount of magnetic flux $3{\sim}4 times$ than without the core. The magnetic flux decreased 23% by shaving the core 0.5 mm on the periphery of 4.75 mm radius core with the relative permeability 800.

Calculation of Critical Current for High Temperature Superconducting Coil (HTS-코일의 임계전류 계산)

  • Li, Zhu-Yong;Ma, Yong-Hu;Ryu, Kyung-Woo;Park, Kwon-Bae;Oh, Il-Sung
    • Proceedings of the KIEE Conference
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    • 2008.07a
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    • pp.766-767
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    • 2008
  • 임계온도가 높아 시스템응용에서 매우 안정한 장점을 지닌 고온초전도(HTS)도체를 이용한 HTS-SMES(Superconducting Magnetic Energy Storage)장치에 대하여 많은 연구가 진행되고 있다[1]-[2]. 이런 HTS-SMES 장치의 고가성, 복잡성 등 원인에 기인하여 운전에 앞서 장치의 임계전류, 자속유동손실 및 충.방전시 불가피하게 발생되는 교류손실 등과 같은 기본적인 특성들이 선행하여 연구되어야 한다. 따라서 본 연구에서는 600 kJ급 HTS-SMES코일에 대한 자장분석을 기반으로 코일의 임계전류밀도 분포를 계산하였고 최소 임계전류밀도에 근거하여 코일의 임계전류를 결정하였다. 그 주요 결과를 요약하면 코일에서 자장과 임계전류밀도 분포는 코일의 형상에 무관하게 같은 분포 경향을 보여주며 최소 임계전류밀도는 코일의 top과 bottom의 중심에 위치하며, model코일에서 임계전류의 계산값과 측정값이 비교적 잘 일치하였기 때문에 600 kJ급 HTS-SMES코일도 잘 일치할 것으로 사료된다. 또한 SMES코일을 20 K에서 운전한다고 가정하면 코일 임계전류의 ${\sim}60%$, 4.2 K에서는 ${\sim}40%$에서 각각 운전하게 될 것으로 예측된다.

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