• 한국전기전자재료학회논문지
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• 제20권6호
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• pp.561-565
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• 2007

Because of a good wear resistance and a stable contact resistance, Ag-CdO is widely used as electrical contact material. But, the Cd-oxide mainly exists as a coarse particle and adversely affected to environment. As a reason, $Ag-SnO_2$ alloy has been developed. The Sn-oxide maintains stable and fine particle even at high temperature. In order to investigate the effect of Misch metal (Mm) additional that affects the formation of the oxide and the formation of fine matrix Ag, we studied the microstructures and properties of Ag-Sn-In(-Mm) material fabricated by rapid solidification process. The experimental procedure were melting using high frequency induction, melt spinning, and internal oxidation. The Mm addition makes Ag matrix more fine than no Mm addition. The reason is that the addition of Misch metal decreased a latent heat of fusion of alloy, as a result the rapid solidification effect of alloy is increased. The maximum hardness shows at 0.3 wt%Mm. after that the hardness is decreased until 0.4 wt% Mm, but still larger than no Mm addition alloy. At 0.5 wt% Mm alloy, the precipitation of Misch metal causes a decrease of hardness than no Mm addition alloy.

• Transactions on Electrical and Electronic Materials
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• 제12권1호
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• pp.20-23
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• 2011

Amorphous Ti-(50-x)Ni-xCu (at%) (x = 20, 25, 27, 30) alloy ribbons were prepared by melt spinning. Subsequently, the crystallization behavior of the alloy ribbons was investigated by X-ray diffraction and differential scanning calorimetry. ${\Delta}T$ (the temperature gap between $T_g$ and $T_x$) increased from 33 K to 47 K and the wavenumber ($Q_p$) decreased from 29.44 $nm^{-1}$ to 29.29 $nm^{-1}$ with increasing Cu content from 20 at% to 30 at%. The activation energy for crystallization decreased from 188.5 kJ/mol to 170.6 kJ/mol with increasing Cu content from 20 at% to 25 at%; afterwards, the activation energy remained near constant. Crystallization occurred in two-stage: amorphous-B2-$TiCu_2$ in Ti-Ni-Cu alloys with Cu content less than 25 at%, while it occurred in three-stage; amorphous-B2-TiCu-$TiCu_2$ in Ti-Ni-Cu alloys with Cu content more than 27 at%.

• 한국주조공학회지
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• 제20권1호
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• pp.29-37
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• 2000

The purpose of this study is to investigate the effect of misch metal addition on the microstructure and mechanical property of rapidly solidified AZ91 alloy by melt spinning process. As the contents of misch metal(rare earth element:Ce,La, Nd, Pr)was increased, the microstructure of RS ribbons and extrudates became finer than those of AZ91, and RE related phases($Al_{11}RE_3$, $Al_2RE$) were formed. At room temperature, the rapidly solidified AZ91+1 wt%Mm alloy showed the highest tensile strength, 430 MPa due to precipitation strengthening of${\beta}(Mg_{17}Al_{12})$ phase and Al11RE3 phase. At the elevated temperature, the mechanical property of AZ01+3 wt%Mm alloy was higher than those of other Mg alloys. The reasons were that $Al_{11}La_3$ phase was thermally stable and suppressed the grain growth. In contrast with $Al_{11}La_3$ phase, ${\beta}$ phase was thermally unstable and could not suppress the grain growth at the elevated temperature. Therefore, Al11RE3 phase contributed to improve the thermal stability of RS AZ91 Alloy.

• Journal of Magnetics
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• 제7권4호
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• pp.160-164
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• 2002

A new discovery of the super-giant magneto-impedance (SGMI) effect was found out in a LC-resonator consisted of a glass-coated amorphous $CO_{83.2}B_{3.3}Si_{5.9}Mn_{7.6}$ microwire. The measurement was carried out at high frequency range from 100 MHz up to 1 GHz of an ac-current flowing along the wire and at varying axial dcmagnetic field in its range of $\pm$120 Oe. The wires, about 16${\mu}m$ in diameter, were fabricated by a glass-coated melt spinning technique. The shape of the impedance curves plotted vs. a dc-field is changing dramatically with the frequency. The phase angle was also strongly dependent on this field. The external dc-magnetic field changes the circumferential permeability as well as the penetration depth, both in turn change the impedance of the sample. The drastic increments of SGMI at high frequency can be understood in terms of the LC-resonance phenomena. The sudden change of the phase angle, as large as $180^{\circ}$ evidenced the occurrence of the resonance at a given intensity of the external dc-field. The maximum ratio of SGMI reached in the experiment by precise tuning frequency equals 450,000％ at the frequency of around 551.9075 MHz.

• 한국자기학회지
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• 제5권5호
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• pp.496-499
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• 1995

Amorphous $Co_{80+x}TM_{12}B_{8-x}$ (TM = Ti, Zr, Hf, Nb and x = 0, 2, 4 at%) alloys were prepared by single roll melt spinning technique. Saturation magnetization of the amorphous ribbons was measured by SQUID and vibrating sample magnetometer from 5 to 800 K under applied fields up to 10 kOe. Typical thermo-magnetization curves were observed and the average values of the spectroscopic splitting g factor were estimated from the ferromagnetic resonance curve. For all the amorphous alloys studied here the saturation magnetization in the temperature range 5 K up to about $0.3T_{c}$ can be described by the Bloch relation: $M_{s}(T)\;=\;M_{s}(0)(1-BT^{3/2}-CT^{5/2})$. From the values of $M_{s}(0)$, B and spectroscopic splitting g factor the spin wave stiffness constants were calculated.

• 열처리공학회지
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• 제14권3호
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• pp.160-166
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• 2001

The change of ribbon geometry, microstructure and shape recovery with Mn contents, wheel speed and various annealing temperature have been studied in Fe-X%Mn-5Cr-5Co-4Si (X%=15, 20, 24) shape memory alloy (SMA) ribbons rapidly solidfied by single roll chill-block melt-spinning process. The thickness and width of melt-spun ribbons are reduced, results in refining and uniformalizing grains with increasing wheel speed. In the ribbons melt-spun at a wheel speed of 15m/sec, both ${\varepsilon}$ and ${\alpha}^{\prime}$martensites are formed in ribbon 1 (15.5wt%Mn), while only ${\varepsilon}$ martensite is revealed in ribbon 2 (20.2wt%Mn) and ribbon 3 (23.5wt%Mn). The volume fraction of ${\varepsilon}$ martensite is decreased with increasing Mn contents, and those of ${\varepsilon}$ as well ${\alpha}^{\prime}$martensites are increased due to thermal stress relief and grain growth with increasing annealing temperature. Ms temperatures of the ribbons 1, 2 and 3 are fallen with increasing Mn contents. $M_s$ temperatures of the ribbons 1, 2 and 3 annealed at $300^{\circ}C$ for 3 min are risen abruptly, but are nearly constant even at higher annealing temperature, i.e., 400, 500 and $600^{\circ}C$ for 3 min. Shape recovery of the ribbons 1, 2 and 3 increased 30%, 52% and 69% with Mn contents, respectively. Shape recovery of ribbon 1 (15.5wt%Mn) formed ${\varepsilon}$ and ${\alpha}^{\prime}$martensites decreased because of the presence of ${\alpha}^{\prime}$martensite but those of ribbon 2 (20.2wt%Mn) and ribbon 3 (23.5wt%Mn) formed ${\varepsilon}$ martensite increased with increasing annealing temperature.

• Korean Chemical Engineering Research
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• 제43권6호
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• pp.745-750
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• 2005

등방성 피치계 탄소섬유 및 활성탄소섬유를 얻기 위한 프리커서 피치를 제조하기 위하여 NCB(naphtha cracking bottoms) oil을 열처리온도, 처리시간, 질소유량을 변화시키면서 개질하였다. 개질된 피치의 수율, 연화점, 원소분석, 분자량분포를 측정하고 용융방사하여 최적의 개질조건을 얻었다. 질소유량 1.25 vvm, 열처리온도 $380^{\circ}C$, 처리시간 3 h 일 때 약 $240^{\circ}C$의 연화점을 갖는 방사성이 우수한 프리커서 피치를 제조할 수 있었다. 이때의 수율은 약 21 wt％, C/H 몰비는 1.07에서 1.34로, 방향족화도는 0.85에서 0.88으로 증가하였고, 벤젠 및 퀴놀린 불용분은 각각 30.0 wt％, 1.5 wt％ 이었다, 방사 온도는 프리커서 피치의 연화점보다 약 $50^{\circ}C$ 높았으며 분자량은 250~1,250 범위에 분포되어 있지만 80％ 이상은 250~700의 좁은 범위에 몰려있었다.

• 한국재료학회지
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• 제4권8호
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• pp.847-854
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• 1994

Mg-Zn-Ce계 합금에서 비정질 단상 및 hcp-Mg입자분산형 비정질합금이 20-40%, Zn, 0-10%Ce과 5-20%Zn, 0-5%Ce 의 조성범위에서 각각 생성되었다. 초미세 hcp-Mg입자분산형 $Mg_{85}Zn_{12}Ce_{3}$비정질합금은 급속응고 또는 급속응고리본의 열처리에 의해 Mg입자의 입경을 4-20nm의 범위로 조절할 수 있었으며, 이 범위에서는 밀착굽힘이 가능할 만큼 충분한 인성을 가지고 있었다. 이 합금의 최대인장강도($\sigma_{B}$)와 파단 연신율($\varepsilon_{f}$)은 hcp-Mg입자의 체적분율에 따라서 670-930MPa, 5.2-2.0%의 범위였으며, 최대 비강도($\sigma_{B}$밀도 =$\sigma_{s}$)는 $3.6 \times 10^5N \cdot m/kg$에 달하였다. 이와 같이 Mg입자분산형 비정질 합금의($\sigma_{B}$), ($\sigma_{s}$)그리고 $\varepsilon_{f}$의 최대치가 Mg-Zn-Ce계 비정질합금(690MPa, $2.5 \times 10^5N \cdot m/kg$, 2.5%)보다 월등하게 높다는 것은 주목할 만 하다. 복합상 조직이 형성됨으로서 기계적 강도가 증가하는 것은 동일 조성의 비정질상보다 강한 hcp과포화 고용체의 분산강화에 기인하는 것이라고 고찰되었다.

• 전기화학회지
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• 제18권2호
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• pp.68-74
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• 2015

본 실험에서는 리튬이차전지의 고용량 음극활물질로 주목받는 Si 합금의 부피팽창을 억제하기 위한 방법의 하나인 비활성-matrix상을 이용하고, 상태도를 이용하여 동일한 용량을 발현하는 Si계 이원계 합금 (Cr-Si, Ni-Si) 조성에서의 미세구조 및 전기화학적 특성을 비교/분석하였다. 급속응고공정(Rapid Solidification Process, Melt-spinning법)를 이용하여 동일조건하에서 리본 모양의 합금을 제작하였고, 제작된 리본합금은 동일조건에서 분쇄하여 X-선회절 (X-Ray Diffraction) 분석을 실시하였다. XRD 분석 결과, 상태도에서 예측된 것과 같이, 두 합금 모두 Si 상 및 비활성-matrix상($CrSi_2$ 및 $NiSi_2$)이 관찰되었으며, 이외의 제3의 상은 관찰되지 않았다. 또한, 주사전자현미경(SEM, Scanning Electron Microscope) 및 투과전자현미경-에너지분산분광법(TEM-EDS, Transmission Electron Microscopy - Energy Dispersive X-ray Spectroscopy)으로 미세구조를 살펴본 결과 Cr-Si 합금의 미세구조가 Ni-Si 합금보다 fine한 것을 알 수 있었고 이것은 상태도로부터 예측 가능하였다. 두 합금 조성에서 미세구조에 따른 전기화학적 특성을 비교 평가하기 위해 코인형 하프셀과 풀셀로 충방전 실험을 진행하였고 이와 별도로, 전극의 두께변화 측정이 가능하게 설계된 시험셀을 이용하여 반응 중 Si의 수축팽창을 측정하였다. coarse한 미세구조를 가진 Ni-Si 합금보다 fine한 미세구조를 갖는 Cr-Si 합금의 전극팽창이 비교적 잘 억제됨을 확인하였고, 충방전에 따른 수명 내구성도 우수함을 확인하였다. 이런 결과들로부터 합금의 조성에 따른 미세구조, 체적변화 및 전기화학적 열화와의 연관성을 유추할 수 있었다.

• 한국자기학회지
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• 제2권1호
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• pp.1-7
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• 1992

melt-spinning 방법에 의해 제조된 비정질 $Fe_{90}Zr_{10}$ ribbon에 전해수소화 반응법에 의해 증수소를 주입하였다. 중수소가 주입된 $D_{x}Fe_{90}Ze_{10}$계의 자기적 성질에 대하여 연구 하였다. 이 결과와 이미 보고된 수소가 주입된 $H_{x}Fe_{91}Zr_{9}$계의 결과와 비교하여 자기적인 성질에 미치는 phonon의 효과에 대하여 연구하였다. 또한 $M\"{o}ssbauer$분광법을 이용하여 Curie온도 $T_{c}$를 조사한 결과 중수소가 주입되기 전 시료의 $T_{c}$보다 75K 상승하였는데, 이는 수소 주위의 local de-formation에 의한 것으로 보인다. 그리고 $M\"{o}ssbauer$분광법에서 얻은 $D_{47}Fe_{90}Zr_{10}$의 자발 자율화을 온도의 함수로 표시하여, 중수소를 주입하지 않은 $Fe_{90}Zr_{10}$의 자발 자화율과 비교한 결과 중수소 주입시 교환 상호작용의 요동이 줄어듬이 확인되었다.