• 제목/요약/키워드: magnetic particle

검색결과 602건 처리시간 0.027초

이동통신주파수 대역에서 순철 분말-고무 복합체 Sheet의 전파흡수특성 (Microwave Absorbing Properties of Iron Particles-Rubber Composites in Mobile Telecommunication Frequency Band)

  • 김선태;김상근;김성수;윤여춘;이경섭;최광보
    • 한국자기학회지
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    • 제14권4호
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    • pp.131-137
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    • 2004
  • 이동통신주파수 대역에서 박형의 전파흡수체를 제작하기 위해 순철 분말을 흡수 충진재로 사용한 고무 복합체의 고주파 특성(복소투자율, 복소유전율) 및 전파흡수특성에 대해 조사하였다. 주요 실험변수는 순철 분말의 초기입도와 형상(구형, 압분체) 변화였다. Attrition milling에 의해 두께가 표피두께보다 작은 순철 압분체를 제작함으로써 임피던스정합 조건에 근접하는 고투자율과 고유전율을 동시에 얻을 수 있었다. 이는 milling에 의해 구형에서 평판상으로 모양이 바뀜에 따라 와전류 손실이 감소하고(복소투자율의 증가), 압분체 간의 정전용량이 증가한 것(복소유전율의 증가)에 기인한다. 초기입도가 10$\mu\textrm{m}$인 순철 압분체를 흡수 충진재로 사용함으로써 이동통신주파수 대역(0.8-2.0㎓)에서 반사손실이 -5㏈(70% 전력흡수율), 두께가 0.7mm 수준인 박형의 전파흡수체를 제안할 수 있었다.

Photoionization of $TiO_2$ Particles Incorporated into Silica Gels Studied by EPR Spectroscopy

  • Ahn, Sang-Won;Kang, Kee-Hoon;Hong, Dea-Il
    • 한국자기공명학회논문지
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    • 제4권1호
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    • pp.50-63
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    • 2000
  • Titanium dioxide particles with three different average sizes, prepared by three different methods, were incorporated into silica gel pores by impregnation. The titanium dioxide incorporated into the silica gel pores was photoionized by 240-400 nm irradiation at 77 K by a one-photon process to from trapped hole centers on OH group and trapped electron centers on titanium which were detected by electron paramagnetic resonance at 77 K. During the impregnation the smallest size range of TiO2 particles can be incorporated into silica gels with 2.5-1.5 nm pores. However, the largest size range of TiO2 particles can only be incorporated into silica gels with 6-15 nm pores and not into silica gels with 2.5-4 nm pores. The photoyield and stability of photoinduced hole and electron centers depends on the silica pore sizes of silica gels and surface area as well as on the TiO2 loading. In large pore silica gels and large particle size of TiO2, photoinduced charge separation reaches to a plateau at shorter irradiation times and the trapped hole and electron centers are more stable to decay.

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직류 열 플라즈마를 이용한 다이아몬드 합성에 관한 연구 (PREPARATION OF DIAMOND FILM BY DC THERMAL PLASMA)

  • 김원규;황기웅
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1990년도 추계학술대회 논문집 학회본부
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    • pp.101-105
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    • 1990
  • A DC thermal plasma system has been designed and constructed to obtain diamond films from a mixture of CH4 and H2. The effects of the deposition conditions such as substrate temperature ($850^{\circ}C-1050^{\circ}C$), gas mixing ratio (0.5-1.5% CH4 in H2), chamber pressure (50 - 200 Torr), axial magnetic field (0 - 900 Gauss) on the diamond film properties such as morphology, purity of the film and deposition rate, etc. have been examined with the aids of Scanning Electron Microscopy, X-Ray Diffraction and Raman Spectroscopy. Under optimum conditions, high quality diamond films can be obtained with high deposition rate (>$1{\mu}m/min$). Both of the growth rate and' particle size increased with the substrate temperature but the morphology changed from the faceted to unshaped when the temperature deviates its proper range. Furthermore, higher growth rates of $1.5{\mu}m/min$ can be obtained by applying an axial magnetic field to plasma torch. The observed values of interplanar spacings of diamond were in a good agreement with the values reported in ASTM data and all deposits have the diamond peak of $1332.5\;cm^{-1}$ in the Raman Spectra.

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나노크기 Ni-Fe 합금입자 분산${Al_2}{O_3}$ 나노복합재료의 합성 및 특성 (Synthesis and Properties of Nano-sized Ni-Fe Alloy Particle Dispersed ${Al_2}{O_3}$Nanocomposite)

  • 남궁석;오승탁;이재성;정영근;김형섭
    • 한국재료학회지
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    • 제11권11호
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    • pp.986-990
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    • 2001
  • An optimum route to fabricate the $A1_2O_3/Fe-Ni$ alloy nanocomposites with sound microstructure and enhanced mechanical properties as well as magnetism was investigated. To prepare homogeneous nanocomposite powders of Fe-Ni alloy and $Al_2O_3$, the solution-chemistry routes using $Al_2O_3 \; Ni(NO_3)_2{\cdot}6H_2O$ and $Fe(NO_3)_3{\cdot}9H_2O$ powders were applied. Microstructural observation of the powder mixture revealed that the Fe-Ni alloy particles of about 20 nm in size were homogeneously surrounded $A1_2O_3$, forming nanocomposite powder. The hot-pressed composite showed improved fracture toughness and magnetic response. These results suggest that the synergy materials with an improved mechanical properties and excellent functionality can be fabricated by controlled powder preparation and consolidation processing.

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Lung Perfusion Imaging and $Tc^{99m}-Macroaggregated$ Human Serum Albumin

  • Haider, Kh.H.;Ilyas, M.;Hyder, Q.;Kim, Chong-Kook
    • Journal of Pharmaceutical Investigation
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    • 제31권2호
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    • pp.73-80
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    • 2001
  • Lung perfusion scanning, invariably combined with ventilation studies provides a reliable and non-invasive mean to diagnose lung related pathologies despite the availability of modern techniques such as angiography, magnetic resonance imaging, magnetic resonance angiography, and helical (spiral) computed tomography. The technique involves the generation of images by radiations emitted from radioisotopes introduced in to the lungs. Various radiopharmaceuticals have been proposed and designed to incorporate $Tc^{99m}$ in to macroparticulate form for lung perfusion imaging. However, most of these have associated difficulties such as reproducibility of the product with regards to particle size distribution and poor elimination from the lung capillary bed. $Tc^{99m}$ macroaggregated albumin $(Tc^{99m}-MAA)$ is used extensively for clinical lung perfusion imaging and is considered as the radiopharmaceutical of choice. It is non-toxic, safe, and being biodegradable, is easily eliminated from the lung capillary bed by proteolytic enzyme metabolism and by mechanical forces due to lung movement.

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부양가스응축법에 의해 제조된 철산화물 나노 분말의 자기적 특성연구 (A Study on Magnetic Iron Oxide Nano Particles Synthesized by the Levitational Gas Condensation (LGC) Method)

  • 엄영랑;김흥회;이창규
    • 한국분말재료학회지
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    • 제11권1호
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    • pp.50-54
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    • 2004
  • Nanoparticles of iron oxides have been prepared by the levitational gas condensation (LGC) method, and their structural and magnetic properties were studied by XRD, TEM and Mossbauer spectroscopy. Fe clusters were evaporated from a surface of the levitated liquid Fe droplet and then condensed into nanoparticles of iron oxide with particle size of 14 to 30 nm in a chamber filled with mixtures of Ar and $O_2$ gases. It was found that the phase transition from both $\gamma$-$Fe_2O_3$ and $\alpha$-Fe to $Fe_3O_4$, which was evaluated from the results of Mossbauer spectra, strongly depended on the $O_2$ flow rate. As a result, $\gamma$-$Fe_2O_3$ was synthesized under the $O_2$ flow rate of 0.1$\leq$$Vo_2$(Vmin)$\leq$0.15, whereas $Fe_3O_4$ was synthesized under the $O_2$, flow rate of 0.15$\leq$$Vo_2$(Vmin)$\leq$0.2.

Polar rain flux variations in northern hemisphere observed by STSAT_1 with IMF geometry

  • Hong, Jin-Hy;Lee, J.J.;Min, K.W.;Kim, K.H.
    • 한국우주과학회:학술대회논문집(한국우주과학회보)
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    • 한국우주과학회 2008년도 한국우주과학회보 제17권2호
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    • pp.25.2-25.2
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    • 2008
  • Polar rain is a spatially uniform precipitation of electrons with energies around 100eV that penetrate into the polar cap region where geomagnetic field lines are connected to the Interplanetary Magnetic Fields (IMF). Since their occurrences depend on the IMF sector polarity, they are believed to originate from the field aligned component of the solar wind. However, statistically direct correlation between polar rain and solar wind has not been shown. In this presentation, we examined specifically the IMF strength influence on the polar rain flux variation by classifying of IMF sector polarities. For this study, we employed the polar rain flux data measured by STSAT-1 and compared them with the solar wind parameters obtained from the WIND and ACE satellites. We found the direct mutuality between polar rain flux and IMF strength with correlation coefficient above 0.5. This proportional tendency appears stronger when the northern hemisphere is in the away sector of the IMF, which could be associated with a favorable geometry for magnetic reconnection. Simple particle trajectory simulation clearly shows why polar rain intensity depends on the IMF sector polarity. These results are consistent with the direct entry model of Fairfield et al.(1985), while low correlation coefficient with solar wind density, the similarity between slops of both energy spectra shows that transport process occur without acceleration.

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초미립 MnxZn1-xFe2O4(x = 0.69~0.74)분말의 제조 및 자기적 성질 (Synthesis of Ultra Eine MnxZn1-xFe2O4(x = 0.69~0.74) Powder and Its Magnetic Properties)

  • 곽재은;이완재
    • 한국분말재료학회지
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    • 제9권6호
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    • pp.449-454
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    • 2002
  • $MnxZn_{1-x}Fe_2O_4$ (x=0.69~0.74) powders synthesized by the thermal decomposition of organic acid salts. The obtained powders were uniform in composition and ultra-fine particle with about 400 nm. The amount of spinel phase of these powders was about 50% in X-ray diffraction patterns. The calcination of powder was carried out at $900^{\circ}C$ for 2 hours in air. After the powders were calcined. the mean size of powder was about 500 nm and the amount of spinel phase was increased over about 65%. The maximum amount of spinel phase was about 75% in the specimen of X=0.72. The magnetic properties of calcined $Mn_{0.72}Zn_{0.28}Fe_2O_4$ powders were the best among the different among the different compositions.

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.
    • 천문학회보
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    • 제42권2호
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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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CME propagation and proton acceleration in solar corona

  • Kim, Roksoon;Kwon, Ryunyoung;Lee, Jaeok;Lario, David
    • 천문학회보
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    • 제43권1호
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    • pp.53.3-54
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    • 2018
  • Solar Proton Events (SPEs) are the energetic phenomena related particle acceleration occurred in solar corona. Conventionally, they have been classified into two groups as the impulsive and gradual cases caused by reconnection in the flaring site and by shock generated by CME, respectively. In the previous studies, we classified these into four groups by analyzing the proton acceleration patterns in multi-energy channel observation. This showed that acceleration due to the magnetic reconnection may occur in the corona region relatively higher than the flaring site. In this study, we analyzes 54 SPEs observed in the energy band over 25 MeV from 2009 to 2013, where STEREO observations as well as SOHO can be utilized. From the multi-positional observation, we determine the exact time at which the Sun-Earth magnetic field line meets the CME shock structure by considering 3-dimensional structure of CME. Also, we determine the path length by considering the solar wind velocity for each event, so that the SPE onset time near the sun is obtained more accurately. Based on this study, we can get a more understanding of the correlation between CME progression and proton acceleration in the solar coronal region.

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