• 제목/요약/키워드: Pure Ni

검색결과 283건 처리시간 0.024초

수소저장용 금속수소화물$(Mm\;(La_{0.6-0.8})\;Ni_{4.0}Co_{0.6}Mn_{0.2}Al_{0.2})$의 전열촉진 (Heat transfer enhancement of metal hydride $(Mm\;(La_{0.6-0.8})\;Ni_{4.0}Co_{0.6}Mn_{0.2}Al_{0.2})$ for hydrogen storage)

  • 배상철
    • 한국신재생에너지학회:학술대회논문집
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    • 한국신재생에너지학회 2006년도 춘계학술대회
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    • pp.33-36
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    • 2006
  • The effective thermal conductivities of $Mm\;(La_{0.6-0.8})\;Ni_{4.0}Co_{0.6}Mn_{0.2}Al_{0.2}$ (TL-492) with hydrogen and helium have been examined. Experiment results show that pressure has great influence on effective thermal conductivity in Low pressure range (below 0.5 MPa). And that influence decreases rapidly with increase of gas pressure. The reason is at low pressure, the mean free path of gas becomes greater than effective thickness of gas film which is important to the heat transfer mechanism in this research. And, carbon fibers have been used to try to enhance the poor thermal conductivity of TL-492. Three types of carbon fibers and three mass fractions have been examined and compared. Naturally, the highest effective thermal conductivity has been reached with carbon fiber which has highest thermal conductivity, and highest mass fraction. This method has acquired 4.33 times higher thermal conductivity than pure metal hydrides with quite low quantity of additives, only 0.99wt% of carbon fiber. This is a good result comparing to other method which can reach higher effect ive thermal conductivity but needs much higher mass fraction of additives too.

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Temperature dependence of the effective anisotropy in Ni nanowire arrays

  • Meneses, Fernando;Urreta, Silvia E.;Escrig, Juan;Bercoff, Paula G.
    • Current Applied Physics
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    • 제18권11호
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    • pp.1240-1247
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    • 2018
  • Magnetic hysteresis in Ni nanowire arrays grown by electrodeposition inside the pores of anodic alumina templates is studied as a function of temperature in the range between 5 K and 300 K. Nanowires with different diameters, aspect ratios, inter-wire distance in the array and surface condition (smooth and rough) are synthesized. These microstructure parameters are linked to the different free magnetic energy contributions determining coercivity and the controlling magnetization reversal mechanisms. Coercivity increases with temperature in arrays of nanowires with rough surfaces and small diameters -33 nm and 65 nm- when measured without removing the alumina template and/or the Al substrate. For thicker wires -200 nm in diameter and relatively smooth surfaces- measured without the Al substrate, coercivity decreases as temperature rises. These temperature dependences of magnetic hysteresis are described in terms of an effective magnetic anisotropy $K_a$, resulting from the interplay of magnetocrystalline, magnetoelastic and shape anisotropies, together with the magnetostatic interaction energy density between nanowires in the array. The experimentally determined coercive fields are compared with results of micromagnetic calculations, performed considering the magnetization reversal mode acting in each studied array and microstructure parameters. A method is proposed to roughly estimate the value of $K_a$ experimentally, from the hysteresis loops measured at different temperatures. These measured values are in agreement with theoretical calculations. The observed temperature dependence of coercivity does not arise from an intrinsic property of pure Ni but from the nanowires surface roughness and the way the array is measured, with or without the alumina template and/or the aluminum support.

Addition of $B_2O_3$ precursors and their effect on texture and surface roughness of $La_2Zr_2O_7$ buffer layers

  • Kim, Young-Kuk;Yoo, Jai-Moo;Chung, Kook-Chae;Shin, Pyung-Woo
    • 한국초전도ㆍ저온공학회논문지
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    • 제10권2호
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    • pp.20-23
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    • 2008
  • [ $La_2Zr_2O_7$] (LZO) buffer layers were deposited on biaxially textured Ni-W substrates by chemical solution deposition method (CSD). In this study, the effect of $B_2O_3$ addition on texture and surface roughness of LZO films was investigated. The alkoxide-based precursor solution was employed to synthesize the precursor solution of LZO and the solution was coated on biaxially textured Ni-W substrates and subsequently annealed at $900^{\circ}C$ for crystallization. The pure LZO film without $B_2O_3$ addition showed a (222) reflection in the X-ray diffraction (XRD) profile. The intensity of (222) reflection was enhanced and more rough surface was obtained after further repetition of coating. Contrary to this, the LZO film prepared by $B_2O_3$ added precursor solution shows well-developed (400) reflection peak in the XRD profile and excellent biaxial texture (${\Delta}{\theta}=4.3^{\circ}$, ${\Delta}{\phi}=6.8^{\circ}$). The surface roughness of LZO films were also improved by addition of $B_2O_3$ even after multicoating ($R_{rms}{\sim}3.1nm$). It was shown that the LZO film with smooth surface and biaxial texture was grown on the biaxially textured Ni-W substrates with addition of $B_2O_3$ in the precursor solution.

Research of Diffusion Bonding of Tungsten/Copper and Their Properties under High Heat Flux

  • Li, Jun;Yang, Jianfeng
    • 한국재료학회:학술대회논문집
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    • 한국재료학회 2011년도 춘계학술발표대회
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    • pp.14-14
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    • 2011
  • W (tungsten)-alloys will be the most promising plasma facing armor materials in highly loaded plasma interactive components of the next step fusion reactors due to its high melting point, high sputtering resistance and low deuterium/tritium retention. The bonding technology of tungsten to Cu alloy was one of the key issues. In this paper, W/CuCrZr diffusion bonding has been performed successfully by inserting pure metal interlay. The joint microstructure, interfacial elements migration and phase composition were analyzed by SEM, EDS, XRD, and the joint shear strength and micro-hardness were investigated. The mock-ups were fabricated successfully with diffusion bonding and the cladding technology respectively, and the high heat flux test and thermal fatigue test were carried out under actively cooling condition. When Ni foil was used for the bonding of tungsten to CuCrZr, two reaction layers, Ni4W and Ni(W) layer, appeared between the tungsten and Ni interlayer with the optimized condition. Even though Ni4W is hard and brittle, and the strength of the joint was oppositely increased (217 MPa) due primarily to extremely small thicknesses (2~3 ${\mu}m$). When Ti foil was selected as the interlayer, the Ti foil diffused quickly with Cu and was transformed into liquid phase at $1,000^{\circ}C$. Almost all of the liquid was extruded out of the interface zone under bonding pressure, and an extremely thin residual layer (1~2 ${\mu}m$) of the liquid phase was retained between the tungsten and CuCrZr, which shear strength exceeded 160 MPa. When Ni/Ti/Ni multiple interlayers were used for bonding of tungsten to CuCrZr, a large number of intermetallic compound ($Ni_4W/NiTi_2/NiTi/Ni_3T$) were formed for the interdiffusion among W, Ni and Ti. Therefore, the shear strength of the joint was low and just about 85 MPa. The residual stresses in the clad samples with flat, arc, rectangle and trapezoid interface were estimated by Finite Element Analysis. The simulation results show that the flat clad sample was subjected maximum residual stress at the edge of the interface, which could be cracked at the edge and propagated along the interface. As for the rectangle and trapezoid interface, the residual stresses of the interface were lower than that of the flat interface, and the interface of the arc clad sample have lowest residual stress and all of the residual stress with arc interface were divided into different grooved zones, so the probabilities of cracking and propagation were lower than other interfaces. The residual stresses of the mock-ups under high heat flux of 10 $MW/m^2$ were estimated by Finite Element Analysis. The tungsten of the flat interfaces was subjected to tensile stresses (positive $S_x$), and the CuCrZr was subjected to compressive stresses (negative $S_x$). If the interface have a little microcrack, the tungsten of joint was more liable to propagate than the CuCrZr due to the brittle of the tungsten. However, when the flat interface was substituted by arc interfaces, the periodical residual stresses in the joining region were either released or formed a stress field prohibiting the growth or nucleation of the interfacial cracks. Thermal fatigue tests were performed on the mock-ups of flat and arc interface under the heat flux of 10 $MW/m^2$ with the cooling water velocity of 10 m/s. After thermal cycle experiments, a large number of microcracks appeared at the tungsten substrate due to large radial tensile stress on the flat mock-up. The defects would largely affect the heat transfer capability and the structure reliability of the mock-up. As for the arc mock-up, even though some microcracks were found at the interface of the regions, all microcracks with arc interface were divided into different arc-grooved zones, so the propagation of microcracks is difficult.

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Crystallographic and Magnetic Properties of Co, Zn, Ni-Zn Substituted Nano-size Manganese Ferrites Synthesized by Sol-gel Method

  • Noh, Kwang Mo;Lee, Young Bae;Kwon, Woo Hyun;Kang, Jeoung Yun;Choi, Won-Ok;Chae, Kwang Pyo
    • Journal of Magnetics
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    • 제21권3호
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    • pp.308-314
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    • 2016
  • Cobalt-, zinc-, and nickel-zinc-substituted nano-size manganese ferrite powders, $MnFe_2O_4$, $Mn_{0.8}Co_{0.2}Fe_2O_4$, $Mn_{0.8}Zn_{0.2}Fe_2O_4$ and $Mn_{0.8}Ni_{0.1}Zn_{0.1}Fe_2O_4$, were fabricated using a sol-gel method, and their crystallographic and magnetic properties were subsequently studied. The $MnFe_2O_4$ ferrite powder annealed at temperatures above 523 K exhibited a spinel structure, and the particle size increased as the annealing temperature increased. All ferrites annealed at 773 K showed a single spinel structure, and the lattice constants and particle size decreased with the substitution of Co, Zn, and Ni-Zn. The $M{\ddot{o}}ssbauer$ spectrum of the $MnFe_2O_4$ ferrite powder annealed at 523 K only showed a doublet due to its superparamagnetic phase, and the $M{\ddot{o}}ssbauer$ spectra of the $MnFe_2O_4$, $Mn_{0.8}Co_{0.2}Fe_2O_4$, and $Mn_{0.8}Zn_{0.2}Fe_2O_4$ ferrite powders annealed at 773 K could be fitted as the superposition of two Zeeman sextets due to the tetrahedral and octahedral sites of the $Fe^{3+}$ ions. However, the $M{\ddot{o}}ssbauer$ spectrum of the $Mn_{0.8}Ni_{0.1}Zn_{0.1}Fe_2O_4$ ferrite powder annealed at 773 K consisted of two Zeeman sextets and one quadrupole doublet due to its ferrimagnetic and paramagnetic behavior. The area ratio of the $M{\ddot{o}}ssbauer$ spectra could be used to determine the cation distribution equation, and we also explained the variation in the $M{\ddot{o}}ssbauer$ parameters by using this cation distribution equation, the superexchange interaction and the particle size. Relative to pure $MnFe_2O_4$, the saturation magnetizations and coercivities were larger in $Mn_{0.8}Co_{0.2}Fe_2O_4$ and smaller in $Mn_{0.8}Zn_{0.2}Fe_2O_4$, and $Mn_{0.8}Ni_{0.1}Zn_{0.1}Fe_2O_4$. These variations could be explained using the site distribution equations, particle sizes and magnetic moments of the substituted ions.

3중박막 NiFe/IrMn/CoFe에서 Mn 함유량에 의존하는 교환결합세기 (Exchange coupling field of NiFe/IrMn/CoFe trilayer depending on Mn composition)

  • 김보경;이진용;함상희;김순섭;이상석;황도근;김선욱;이장로
    • 한국자기학회:학술대회 개요집
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    • 한국자기학회 2003년도 하계학술연구발표회 및 한.일 공동심포지엄
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    • pp.130-131
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    • 2003
  • Mn 합금형태의 반강자성체 물질인 IrMn은 열처리 전과 후에 교환결합세기를 400 Oe 이상 쉽게 얻을 수 있다. IrMn 스핀밸브나 터널링 접합 소자는 높은 교환 결합세기와 우수한 열적안정성으로 인하여 자기센서로서 실용화하기에 이르렀다. Mn이 계면의 이웃층으로 확산이 왕성하므로 자성층의 종류에 따라 교환결합세기의 변화에 심각한 영향을 주게 된다. 더욱이 열처리시에 일어나는 Mn 확산 및 이동을 통해 이웃층의 계면 손상과 자기 수송 특성을 완화 내지 손상시키는 중요한 요인으로 밝혀져 있다. 열처리 전과 후에 따른 자기적 특성의 변화가 비교적 큰 IrMn에서 Mn 성분에 따른 fcc 결정성 및 교환결합세기의 변화를 상세히 관찰함으로서 Mn 확산에 의한 반자성층의 Mn 결핍 또는 상변화를 극-초박막 Mn층 삽입으로 보상효과를 이용하여 교환결합세기 강화 및 열적안정성을 향상시킨 실험결과를 소개한다.

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ZrO2와 NiO가 첨가된 Ba(Zn1/3Ta2/3)O3에서 표면 미세조직이 고주파 유전특성에 미치는 영향 (Effects of Surface Microstructure on Microwave Dielectric Properties of ZrO2-NiO added Ba(Zn1/3Ta2/3)O3 Ceramics)

  • 강성우;김태희;문주호;김성열;박준영;최선희;김주선
    • 한국세라믹학회지
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    • 제45권11호
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    • pp.701-706
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    • 2008
  • High frequency dielectric ceramics have potential for applications in mobile and satellite communications systems at frequencies higher than 10GHz. The Ba$(Zn_{1/3}Ta_{2/3})O_3$ ceramics are known to have a high quality factor, a small temperature coefficient of the resonance frequency and a high dielectric constant. On the other hands, sintering at high temperature for extended time is required to obtain the ordered structure for high quality factor. In this study, the microwave dielectric properties of $ZrO_2$ and NiO-added Ba$(Zn_{1/3}Ta_{2/3})O_3$ ceramics prepared by solid-state reaction have been investigated. Adding $ZrO_2$ and NiO could effectively promote the densification even the case of decreasing the sintering time. At the surface of samples, secondary phase of Ba-Ta compounds was formed possibly due to the evaporation of ZnO, however, the interior of the samples remained as pure Ba$(Zn_{1/3}Ta_{2/3})O_3$. The samples sintered at $1600^{\circ}C$ for 2h exhibited 1:2 ordering of Zn and Ta cations. Excellent microwave dielectric properties of $Q{\cdot}f$(>96,000 GHz) and ${\varepsilon}_r$=30 has been obtained.

Ni80Fe20/[Ir22/Mn78-Mn]/Co75Fe25 다층박막에서 Mn 함유량에 의존하는 교환결합력과 열적안정성 (Exchange Coupling Field and Thermal Stability of Ni80Fe20/[Ir22/Mn78-Mn]/Co75Fe25 Multilayer Depending on Mn Content)

  • 김보경;이진용;김순섭;황도근;이상석;황재연;김미양;이장로
    • 한국자기학회지
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    • 제13권5호
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    • pp.187-192
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    • 2003
  • IrMn에 Mn을 첨가시킨 N $i_{80}$F $e_{20}$/[I $r_{22}$M $n_{78}$-Mn] $Co_{75}$F $e_{25}$ 다층박막을 상온에서 이온빔 증착(ion beam deposition: IBD)법으로 제작하여 그 자기적 및 열적 특성을 연구하였다. Mn이 첨가된 NiFe/[IrMn-Mn]/CoFe다층박막은 Mn이 첨가되지 않은 순수 합금 IrMn 박막 위의 CoFe 고정층 보다 큰 교환결합력( $H_{ex}$)과 방해온도(blocking temperature: $T_{b}$)을 가지고 있었다. Mn이 첨가되지 않는 I $r_{22}$M $n_{78}$ 와 CoFe 사이의 $H_{ex}$는 상온에서 거의 없었으나, 25$0^{\circ}C$ 열처리 후 100 Oe로 나타났다. IrMn 내에서 76.8-78.1 vol% Mn일 때, $H_{ex}$$T_{b}$는 크게 향상되었고, Mn이 0.6 vol%씩 증가함에 따라 크게 줄어들었다. NiFe/[IrMn-Mn]/CoFe 다층박막 구조에서 [(111)CoFe, NiFe]/(111)IrM $n_3$인 x-선 회절 피크비 평균값은 75.5, 77.5, 79.3 vol% Mn일 때 각각 1.4, 0.8, 0.6였다. 특히, 열처리 전 77.5과 78.7 vol% Mn일 때, $H_{ex}$는 각각 259와 150 Oe였다. 77.5 vol% Mn인 경우, $H_{ex}$가 열처리 온도 35$0^{\circ}C$까지 475 Oe였으며, 450 $^{\circ}C$에서는 200 Oe로 크게 감소하였다. 따라서 합금형 반강자성체 IrMn에서 높은 $H_{ex}$$T_{b}$을 얻을 수 있는 최적의 Mn 함유량의 존재를 확인하였다.다.다. 확인하였다.다.하였다.다.

월정사 팔각구층석탑내 발견 유물의 자연과학적 분석 연구 (A scientific analytical study on the sarira reliquary recovered from the octagonal ninestoried pagoda of Woljeongsa Temple)

  • 홍종욱;한민수;이오희
    • 보존과학연구
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    • 통권25호
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    • pp.5-29
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    • 2004
  • This research carried out ancient technique and composition of the relics recovered from the octagonal nine-storied pagoda of Woljeongsa temple using the scientific methods and obtained the following results. Firstly, The silver sarira inner case is consists of Ag, its materials comes out near 98wt%and comparing with the relics of Hwangnamdaechong, the contents of Ag and Ni are almost same with it. Secondly, The bronze sarira outer case, its contents of Cu is almost same with pure copper of which average is 99.7wt%. So, it should be named the copper sarira outer caserather than the bronze sarira outer case that has been called. Thirdly, The bronze mirror, though the contents of tin and lead are less than other contents which have been studied, they tend to have white color so they need to be made a close study. Especially, Because cultural property of nondestructive surface analytic method is not analyzed by the analysis of cross section and the moisten analysis, it may be occurred analytical errors by other factors.

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Synthesis and Characterization of One-Dimensional GaN Nanostructures Prepared via Halide Vapor-Phase Epitaxy

  • Byeun, Yun-Ki;Choi, Do-Mun;Han, Kyong-Sop;Choi, Sung-Churl
    • 한국세라믹학회지
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    • 제44권3호
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    • pp.142-146
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    • 2007
  • High-quality one-dimensional GaN nanorods and nanowires were synthesized on Ni-coated c-plan sapphire substrate using halide vapor-phase epitaxy (HVPE). Their structure and optical properties were investigated by X-ray diffraction, scanning and transmission electron microscopy, and photoluminescence techniques. Full substrate coverage of densely packed, uniform, straight and aligned one-dimensional GaN nanowires with a diameter of 80nm were grown at $700{\sim}900^{\circ}C$. The X-ray diffraction patterns, transmission electron microscopic image, and selective area electron diffraction patterns indicate that the one-dimensional GaN nanostructures are a pure single crystalline and preferentially oriented in the [001] direction. We observed high optical quality of GaN nanowires by photoluminescence analysis.