• 한국분말재료학회지
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• 제26권4호
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• pp.299-304
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• 2019

Nb-Si-B alloys with Nb-rich compositions are fabricated by spark plasma sintering for high-temperature structural applications. Three compositions are selected: 75 at% Nb (Nb0.7), 82 at% Nb (Nb1.5), and 88 at% Nb (Nb3), the atomic ratio of Si to B being 2. The microstructures of the prepared alloys are composed of Nb and $T_2$ phases. The $T_2$ phase is an intermetallic compound with a stoichiometry of $Nb_5Si_{3-x}B_x$ ($0{\leq}x{\leq}2$). In some previous studies, Nb-Si-B alloys have been prepared by spark plasma sintering (SPS) using Nb and $T_2$ powders (SPS 1). In the present work, the same alloys are prepared by the SPS process (SPS 2) using Nb powders and hypereutectic alloy powders with composition 67at%Nb-22at%Si-11at%B (Nb67). The Nb67 alloy powders comprise $T_2$ and eutectic ($T_2+Nb$) phases. The microstructures and hardness of the samples prepared in the present work have been compared with those previously reported; the samples prepared in this study exhibit finer and more uniform microstructures and higher hardness.

• Journal of Magnetics
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• 제16권3호
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• pp.211-215
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• 2011

The dynamic magnetostriction characteristics of an Fe-based nanocrystalline FeCuNbSiB alloy are investigated as a function of the dc bias magnetic field. The experimental results show that the piezomagnetic coefficient of FeCuNbSiB is about 2.1 times higher than that of Terfenol-D at the low dc magnetic bias $H_{dc}$ = 46 Oe. Moreover, FeCuNbSiB has a large resonant dynamic strain coefficient at quite low Hdc due to a high mechanical quality factor, which is 3-5 times greater than that of Terfenol-D at the same low $H_{dc}$. Based on such magnetostriction characteristics, we fabricate a new type of transducer with FeCuNbSiB/PZT-8/FeCuNbSiB. Its maximum resonant magnetoelectric voltage coefficient achieves ~10 V/Oe. The ME output power reaches 331.8 ${\mu}W$ at an optimum load resistance of 7 $k{\Omega}$ under 0.4 Oe ac magnetic field, which is 50 times higher than that of the previous ultrasonic-horn-substrate composite transducer and it decreases the size by nearly 86%. The performance indicate that the FeCuNbSiB/PZT-8/FeCuNbSiB transducer is promising for application in highly efficient magnetoelectric energy conversion.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 1992년도 춘계연구발표회 논문개요집
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• pp.72-73
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• 1992

• 한국분말재료학회지
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• 제22권6호
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• pp.426-431
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• 2015

Microstructural examination of the Nb-Si-B alloys at Nb-rich compositions is performed. The Nb-rich corner of the Nb-Si-B system is favorable in that the constituent phases are Nb (ductile and tough phase with high melting temperature) and $T_2$ phase (very hard intermetallic compound with favorable oxidation resistance) which are good combination for high temperature structural materials. The samples containing compositions near Nb-rich corner of the Nb-Si-B ternary system are prepared by spark plasma sintering (SPS) process using $T_2$ and Nb powders. $T_2$ bulk phase is made in arc furnace by melting the Nb slug and the Si-B powder compact. The $T_2$ bulk phase was subsequently ball-milled to powders. SPS is performed at $1300^{\circ}C$ and $1400^{\circ}C$, depending on the composition, under 30 MPa for 600s, to produce disc-shaped specimen with 15 mm in diameter and 3 mm high. Hardness tests (Rockwell A-scale and micro Vickers) are carried out to estimate the mechanical property.

• Journal of Magnetics
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• 제16권4호
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• pp.431-434
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• 2011

The reduction of the Nb content in the $(Fe_{0.75}B_{0.20}Si_{0.05})_{96}Nb_4$ bulk metallic glass (BMG) has been studied. The glass-forming ability (GFA) is reduced by decreasing the Nb content, but it can be enhanced by replacing partially Fe by Co. Furthermore, the saturation magnetization of the $(Fe_{0.8}Co_{0.2})_{76}B_{18}Si_3Nb_3$ BMG is 1.35 T, being with 13% larger than that of the base alloy $(Fe_{0.75}B_{0.20}Si_{0.05})_{96}Nb_4$. $(Fe_{0.8}Co_{0.2})_{76}B_{18}Si_3Nb_3$ BMG exhibits slightly larger $B_{800}$ (the magnetic flux density at 800 A/m) and smaller core losses (20%-30%) compared with the commercial Fe-6.5 mass% Si steel.

• 한국재료학회지
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• 제8권3호
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• pp.189-194
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• 1998

SIMS를 사용하여 Co/metal 이중층 구조의 실리사이드화 열처리시 발생하는 기판내 도펀트의 재분포 거동에 대하여 조사하였다. Co실리사이드화 반응의 중간층으로는 Ti, Nb, 또는 Hf를 사용하였고, 여러 도펀트들 중 실리사이드 내에서의 확산속도가 특히 빠른 B에 대하여 조사하였다. Co/Ti과 co/Nb의 경우 열처리후 B피크의 높이는 1 order 정도 낮아지지만 표면으로부터의 주피크의 상대적인 위치는 열처리전과 동일하였다. B의 분포양상은 Ti 및 Nb의 그것과 일치하는데, 이것은 B와 Ti 및 Nb간의 친화력이 크기 때문이다. Co/Hf의 경우에도 B의 피크는 Hf과 거의 같았으나, Ti나 Nb에 비해서 약간 차이가 나는 것으로 보다 B-Hf간의 친화력은 다소 떨어지는 것으로 보인다. 전체적으로 열처리후 Co/metal 이중층 실리사이드에서의 B의 재분포는 Si계면에서 고갈되는 반면, Co-metal/Co 실리사이드 계면에서 pile-up되는 양상을 보였다.

• 한국자기학회지
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• 제3권2호
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• pp.130-134
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• 1993

초급냉법중 단롤법으로 제작한 $Fe_{73.5-X}Co_{X}Cu_{1}Nb_{3}Si_{13.5}B_{9}(x=2,\;4)$ 비정질 합금을 $400~650^{\circ}C$에서 열처리하여 자기적 특성을 조사하였다. $Fe_{71.5}Co_{2}Cu_{1}Nb_{3}Si_{13.5}B_{9}$ 비정질 합금의 최적 열처리 온도는 $550^{\circ}C$이며, 이온도에서 열처 리된 시료의 상대 투자율과 항자력은 1 kHz에서 각각 $1.1{\times}10^{4}$, 0.22 Oe이다. $Fe_{69.5}Co_{4}Cu_{1}Nb_{3}Si_{13.5)B_{9}$의 경우는 $600^{\circ}C$에서 열처리 했을때 상대 투자율과 항자력이 각각 $1.0{\times}10^{4}$, 0.19 Oe로 가장 우수한 연자성 특성을 보였다. X-선 실험결과, 이러한 연자성 특성의 향상은 $\alpha$-Fe(Si) 결정립의 형성에 의한 것임을 확인 할 수 있었으며, 강자성 공명 실험에 의하면 최적 열처리 조건은 공명 흡수선의 반치폭이 급격히 증가하기 직전의 온도임을 알 수 있었다.

• Corrosion Science and Technology
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• 제7권4호
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• pp.233-236
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• 2008

Halide-activated pack cementation was utilized to deposit B-doped silicide coating. The pack powders were consisted of $3Wt.c/oNH_4Cl$, 7Wt.c/oSi, $90Wt.c/oAl_2O_3+TiB_2$. B-doped silicide coating was consisted of two layers, an outer layer of $NbSi_2$ and an inner layer of $Nb_5Si_3$. Isothermal oxidation resistance of B-doped silicide coating was tested at $1250^{\circ}C$ in static air. B-doped silicide coating had excellent oxidation resistance, because continuous $SiO_2$ scale which serves as obstacle of oxygen diffusion was formed after oxidation.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 1992년도 추계연구발표회 논문개요집
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• pp.60-61
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• 1992

• 한국자기학회:학술대회 개요집
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• 한국자기학회 1993년도 춘계연구발표회 논문개요집
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• pp.62-63
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• 1993