• 한국자기학회:학술대회 개요집
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• 한국자기학회 2014년도 자성 및 자성재료 국제학술대회
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• pp.110-111
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• 2014

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2012년도 임시총회 및 하계학술연구발표회
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• pp.99-100
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• 2012

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2011년도 임시총회 및 하계학술연구발표회
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• pp.175-175
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• 2011

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2013년도 임시총회 및 하계학술연구발표회
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• pp.78-78
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• 2013

• 한국자기학회지
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• 제3권1호
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• pp.34-40
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• 1993

급속냉각기술로 제조된 $Nd_{10.5}Fe_{79}Co_{2}Zr_{1.5}B_{7}$ 합금분말을 사용하여 사출성형용 자성 펠렛을 제조하였다. 입도분포가 다른 두 종류의 분말($38~75\;\mu\textrm{m}$ 및 $75~50\;\mu\textrm{m}$)을 사용하여 열가소성(Nylon 6) 펠렛을 제조한 후 자성분말의 임계분율(critical volume fraction) 을 결정하고 수지자석의 성형밀도에 따른 자기특성을 고찰하였다. Nylon 6 수지를 사용한 Nd-Fe-Co-Zr-B계 펠렛은 분말입도가 $38~75\;\mu\textrm{m}$인 경우 임계 부피분율은 70%로 나타났고, 그때의 성형밀도는 이론밀도 의 90%를 상회 했으나 $75~150\;\mu\textrm{m}$ 분말의 경우는 같은 분율에서 이론밀도의 87% 수준에 머물렀다. 최적의 자기특성은 분말에 윤활제로서 silicone oil만을 0.5wt.% 첨가한 경우이며 이때의 자기특성으로, $(BH)_{max}=5.2\;MGOe,\;B_{r}=5.1\;kG$ 그리고 $_{i}H_{c}=8.8\;kOe$의 높은 수준을 보였다. Nylon 6수지자석의 성형밀도를 예측할 수 있는 경험식으로서, ${\rho}(g/cm^{3})=1.1+K.V_{s}$을 얻었으며 K(5.3~5.6)는 자성분말 입도에 따른 기울기 상수이고 $V_{s}$는 분말의 부피분율이다.

• 열처리공학회지
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• 제7권1호
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• pp.61-71
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• 1994

This study is to investigate the stress distributions, crystal orientations and magnetic properties during die-upsetting according to working temperature of Nd-Fe-B-Cu alloys. The stress distributions in the specimens during compressing process were calculated by a finite element method program(SPID). The calculated stresses were effective stress (${\sigma}_{eff}$), compression stress(${\sigma}_z$), radial direction stress(${\sigma}_r$) rotational direction stress(${\sigma}_e$) and shear stress(${\tau}_{rz}$). The stress distributions of ${\sigma}_z$, obtained by a computer simulation showed that the stress components causing the magnetic alignment during die-upsetting of the cast magnets were very high at the center-part of a specimen, and decreased toward the periphery-part of a specimen. In view of the above results the magnetic properties should be better at the center-part of a specimen than any other parts. But the measured magnetic properties were better at the mid-part. These results should be due to the fact that the specimens were casted. Normally the magnetic properties are affected by the casting process as well as by the stress levels. ${\sigma}_r$, ${\sigma}_e$ are thought to affect the liquid phase flowing and domain patterns, respectively. The influence of ${\tau}_{rz}$ was trivial, ${\sigma}_{eff}$ distributed similar throughout the specimen. The Nd-rich phase appeared at the peripheral of the specimen where the stress level of ${\sigma}_r$, ${\sigma}_z$, was low or the stress level of ${\sigma}_e$ was high. The Nd-rich phase was squeezed out during die-upsetting. This phase had an effect on the crystal orientation and grain growth. The stress distributions of alloy were irregular at the parts of the specimen where the die contacted with specimen.