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검색결과 4,024건 처리시간 0.028초

The B2-B19-B19' Transformation in Ti-(45-x)Ni-5Cu-xMn (at%) (x = 0.5-2.0) Alloys

  • Jeon, Yeong-Min;Kim, Min-Gyun;Kim, Min-Su;Lee, Yong-Hee;Im, Yeon-Min;Nam, Tae-Hyun
    • Transactions on Electrical and Electronic Materials
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    • 제12권1호
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    • pp.24-27
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    • 2011
  • Effect of substitution of Mn for Ni on transformation behavior, shape memory characteristics and superelasticity of Ti45Ni-5Cu alloy has been investigated by means of electrical resistivity measurements, X-ray diffraction, thermal cycling tests under constant load and tensile tests. The one-stage B2-B19' transformation occurred when Mn content was 0.5 at%, above which the two-stage B2-B19-B19' transformation occurred. A temperature range where the B19 martensite exists was expanded with increasing Mn content because decreasing rate of Ms (60 K / % Mn) was larger than that of Ms' (40 K / % Mn). Ti-(45-x)Ni-5Cu-xMn alloys were deformed in plastic manner with a fracture strain of 60 % ~ 32 % depending on Mn content. Clear superelasticity was found in fully annealed Ti-(45-x)Ni-5Cu-xMn alloys with Mn content more than 1.0 at%, which was ascribe to a solid solution hardening by substitution of Mn for Ni.

HDDR Characteristics and Magnetic Properties of Nd15(Fe1-xCox)77B8(x=0-0.6) Alloys

  • Kwon, H.W.
    • Journal of Magnetics
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    • 제7권4호
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    • pp.127-131
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    • 2002
  • HDDR characteristics and magnetic properties of $Nd_{15}{(Fe_{1-x}Co_{x})}_{77}B_{8}$(x=0-0.6) alloys were investigated. The effect of applying magnetic field during the recombination step on the anisotropic nature of the HDDR-treated material was also examined. The $Nd_{15}{(Fe_{1-x}Co_{x})}_{77}B_{8}$ phase in the Nd-Fe-B alloys with high Co-substitution alloy had remarkably enhanced phase stability. The $Nd_{15}{(Fe_{1-x}Co_{x})}_{77}B_{8}$(x=0-0.6) alloys with high Co-substitution could be HDDR-treated successfully by only using high pressure hydrogen. However, these alloys had no appreciable coercivity. The poor coercivity of the HDDR-treated $Nd_{15}{(Fe_{1-x}Co_{x})}_{77}B_{8}$(x=0-0.6) alloys with high Co-substitution was attributed to the $Nd{(Fe,Co)}_2$ phase in the alloys. The magnetic filed applied during the recombination step had little effect on the anisotropic nature of the HDDR-treated powder.

원자의 온도 매개변수의 정확한 표현 (The Explicit Expression of the Atomic Thermal Parameters)

  • William P. Jensen;Suh, Il-Hwan
    • 한국결정학회지
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    • 제9권2호
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    • pp.149-152
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    • 1998
  • The accurate expression of the anisotropic thermal parameters is either exp (-2$π^{2}$ < $h^{2}$ $\frac{$u_x^2$}{$a^{2}$}$ + $k^{2}$ $\frac{$u_y^2$}{$b^{2}$}$ + $l^{2}$ $\frac{$u_z^2$}{$c^{2}$}$ + 2hk $\frac{$u_{x}}{a}$ $\frac{$u_{y}}{b}$ 2hl $\frac{$u_{x}}{a}$ $\frac{$u_{z}}{c}$ 2kl $\frac{$u_{y}}{b}$ $\frac{$u_{z}}{c}$ > ) with the small displacements Ux, Uy, uz, in absolute measure or exp (-2$π^{2}$ < $h^{2}$ $u_x^2$ + $k^{2}$ $u_y^{2}$ + $l^{2}$ $u_z^{2}$ + 2hk$u_{x}$ $u_{y}$ + 2hl$u_{x}$$u_{z}$ + 2kl$u_{y}$ $u_{z}$ > ) with the small displacements Ux, Uy, Uz in fractional measure.

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자장중 열처리에 의한 $Nd_{2}Fe_{14}B/Fe_{3}B$ 초미세립 복합자성상의 자기특성 향상 (The Effect of Magnetic Field Treatment on Enhanced Exchange Coupling of $Nd_{2}Fe_{14}B/Fe_{3}B$ Magnet)

  • 박언병;양충진
    • 한국자기학회지
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    • 제6권2호
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    • pp.80-85
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    • 1996
  • $Nd_{2}Fe_{14}B/Fe_{3}B$ 복합자성상을 근간으로 한 급냉제조된 합금을 외부 자장중에서 열처리를 함으로써 자기특성이 월등하게 좋아짐을 확인하였다. $Nd_{4}Fe_{73.5}Co_{3}(Hf_{1-x}-Ga_{x})B_{18.5}$ 조성 합금을 1~5 kOe 자장중에서 열처리함으로써 연자성의 기지상$(Fe_{3}B)$ 및 강자성상$(Nd_{2}Fe_{14}B)$의 결정입도가 20% 감소하였고, 그 결과 잔류자속밀도 $(B_{r})$ 및 최대자기에너지적, ${(B.H)}_{max}$가 30% 이상 증가하였다. 이러한 증가는 입도의 감소 뿐만 아니라 미세입도의 고른 분포에도 기인한 것으로 판단되었다. 보자력의 극대점은 잔류자속밀도와는 달리 특정결정입도에서 발생하며, 이러한 기구를 교환상호작용변수 와 연관하여 설명한다. $Nd_{4}Fe_{73.5}Co_{3}Hf_{0.5}Ga_{0.5}B_{18.5}$ 합금을 자장중 열처리한 결과 ${(B.H)}_{max}=15.8$ MGOe의 고에너지적을 얻을 수 있음을 확인하였다.

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ON THE STRONG LAWS OF LARGE NUMBERS OF NEGATIVELY ASSOCIATED RANDOM VARIABLES

  • Baek, J.I.;Choi, J.Y.;Ryu, D.H.
    • Journal of applied mathematics & informatics
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    • 제15권1_2호
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    • pp.457-466
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    • 2004
  • Let{$X_{ni}$\mid$\;1\;{\leq}\;i\;{\leq}\;k_n,\;n\;{\geq}\;1$} be an array of rowwise negatively associated random variables such that $P$\mid$X_{ni}$\mid$\;>\;x)\;=\;O(1)P($\mid$X$\mid$\;>\;x)$ for all $x\;{\geq}\;0,\;and\; \{k_n\}\;and\;\{r_n\}$ be two sequences such that $r_n\;{\geq}\;b_1n^r,\;k_n\;{\leq}\;b_2n^k$ for some $b_1,\;b_2,\;r,\;k\;>\;0$. Then it is shown that $\frac{1}{r_n}\;max_1$\mid${\Sigma_{i=1}}^j\;X_{ni}$\mid$\;{\rightarrow}\;0$ completely convergence and the strong convergence for weighted sums of N A arrays is also considered.

Al 첨가가 $MgB_2$ 단결정의 비등방성에 미치는 영향에 대한 연구 (Effect of Al Doping on the Anisotropy of $MgB_2$ Single Crystals)

  • 강병원;이현숙;박민석;이성익
    • Progress in Superconductivity
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    • 제9권2호
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    • pp.183-187
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    • 2008
  • We have studied superconducting properties of $Mg_{1-x}Al_xB_2$ single crystals from reversible magnetization measurements. It was found that the upper critical fields $H_{c2}$ were decreased for both H // c and H // ab as Al is substituted for Mg. As a result, the large anisotropy of $H_{c2}$ observed in pure $MgB_2$, which is considered as one of the characteristics of two-gap superconductor, was decreased with Al doping. On the other hand, the irreversibility fields $H_{irr}$ were increased for x = 0.1 and were significantly decreased for x = 0.2. In contrary to the anisotropy of $H_{c2}$, the anisotropy of $H_{irr}$ was increased as Al concentration increases.

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Thermal Stability, Mechanical Properties and Magnetic Properties of Fe-based Amorphous Ribbons with the Addition of Mo and Nb

  • Han, Bo-Kyeong;Jo, Hye-In;Lee, Jin Kyu;Kim, Ki Buem;Yim, Haein
    • Journal of Magnetics
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    • 제18권4호
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    • pp.395-399
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    • 2013
  • The metallic glass ribbons of $[(Fe_xCo_{1-x})_{0.75}B_{0.2}Si_{0.05}]_{96}Mo_4$ (x = 0, 0.3, 0.6, 0.9 at.%) and $[(Fe_xCo_{1-x})_{0.75}B_{0.2}Si_{0.05}]_{96}Nb_4$ (x = 0, 0.3, 0.6, 0.9 at.%) were obtained by melt spinning with 25-30 ${\mu}m$ thickness. The thermal stability, mechanical properties and magnetic properties of Fe-Co-B-Si based systems were investigated. The values of thermal stability were measured using differential scanning calorimetry (DSC), including glass transition temperature ($T_g$), crystallization temperature ($T_x$) and supercooled liquid region (${\Delta}T_x=T_x-T_g$). These amorphous ribbons were identified as fully amorphous, using X-ray diffraction (XRD). The mechanical properties of Febased samples were measured by nano-indentation. Magnetic properties of the amorphous ribbons were measured by a vibrating sample magnetometer (VSM). The amorphous ribbons of $[(Fe_xCo_{1-x})_{0.75}B_{0.2}Si_{0.05}]_{96}Mo_4$ (x = 0, 0.3, 0.6, 0.9 at.%) and $[(Fe_xCo_{1-x})_{0.75}B_{0.2}Si_{0.05}]_{96}Nb_4$ (x = 0, 0.3, 0.6, 0.9 at.%) exhibited soft magnetic properties with low coercive force ($H_c$) and high saturation magnetization (Ms).

$Nd_{x}Fe_{77}B_{23-x}(4 급속응고 합금의 자기특성 (Magnetic Properties of $Nd_{x}Fe_{77}B_{23-x}(4 Melt-Spun Alloys)

  • 박우식;김윤배;김희태;조용수;김창석;박만장
    • 한국자기학회지
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    • 제5권1호
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    • pp.34-37
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    • 1995
  • 단롤법 급속응고장치를 이용하여 비정질 $Nd_{x}Fe_{77}B_{23-x}(x=4,\;6,\;8,\;11,\;13)$ 합금을 제작하고 $650^{\circ}C$ 이상에서 결정화 시키어 자기적 특성을 조사하였다. 열처리 후의 결정상을 조사한 결 과 x=8 조성에서 준안정상 $Nd_{2}Fe_{23}B_{3}$가 단일상에 가깝게 생성되며 연자기특성을 나타냄 을 알았다. 자기특성 조사결과 $8{\leq}x{\leq}13$ 조성범위에서 Nd 함유량이 증가할수록 보자력은 증가하나 잔류자속밀도는 감소함을 알았다. 그러나, $4{\leq}x{\leq}6$ 합금의 경우 Nd 함유량이 감소할수록 보자 력과 잔류자속밀도가 함께 증가하였다. x=4 합금의 경우 연자성:경자성=70:30의 혼합조직이 얻어지며 $96kJ/m^{3}(12MGOe)$의 높은 에너지적을 나타냈다.

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