• Korean Journal of Materials Research
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• v.7 no.2
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• pp.140-144
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• 1997

The effects of the particle size of precursor powder on the microstructure and Jc of Ag-sheathed Ri-2223 tapes were investigated. The calcined powder with overall composition of $Bi_{1-89}Pb_{0-41}Sr_{2-01}Ca_{2-23}Cu_{3-03}O_{y}$ was milled for various times using planetary ball mill. The transport property of the tapes were found to depend strongly on the particle size of the precursor powder Enhanced reactivity of the milled powder facilitated the formation of 2223 phase and resulted in an increase of Jc. Excessive milling, however, led to the amorphisation of the powder and degraded the electrical property of the tapes.

• Journal of the Mineralogical Society of Korea
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• v.20 no.4
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• pp.255-260
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• 2007

The loess on the Chinese loess plateau is not only the accumulation of Asian dust but also the source materials of Hwangsa. The eolian carbonates of the loess were dissolved and reprecipitated to form secondary pedogenic carbonates by the post-depositional weathering during the interglacial time. Mineralogical analysis shows that the secondary calcites are composed mostly of a nanosized fibrous calcite with rather constant width ($30{\sim}50nm$) and highly variable length. The nano calcite is the major authigenic mineral, which occurs as the fine-grained matrix of the loess and paleosol. The nano calcite was recently reported in the Hwangsa, where it was originated from the source regions of Chinese loess plateau.

• Korean Chemical Engineering Research
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• v.55 no.2
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• pp.163-169
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• 2017

In order to investigate the electrochemical properties and the particle size effect of $LiNi_{1-x-y}Co_xAl_yO_2$ (x=0.15, y=0.045 or 0.05, NCA) for lithium ion batteries (LIBs), two commercial NCA cathode materials (NCA#1, NCA#2) were used as cathode materials for LIB. The average particle size of the NCA#1 which consisted of uniform spherical particles was found to be approximately $5m{\mu}$. NCA#2 consisted of particles with bimodal size distribution of approximately $5m{\mu}$ and $11m{\mu}$. From the results of charge-discharge performance test, a high initial discharge capacity of 197.0 mAh/g was obtained with NCA#2, which is a higher value than that with NCA#1. The cycle retentions of NCA#1 and NCA#2 up to 30 cycles were 92% and 94%, respectively.

• Korean Journal of Materials Research
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• v.1 no.1
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• pp.54-61
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• 1991

YBCO films deposited on MgO(100) and Si(100) by rf-magnetron sputtering using stoichiometric single target were annealed under oxygen atmosphere at $880^{\circ}C$ for 1 hr. The microstructure and superconducting properties of YBCO thin films depended on the composition of pre-annealed thin films. Basal planesuperconducting particles grown on MgO(100) substrate had small and rod-like shade due to preferred orientation, while superconducting film grown on the basal plane-superconducting particles showed round-shape particles. If pre-annealed thin film had nonstoichiometric composition, liquid phase was formed during the heat treatment, which made it easy for particles to grow in the preferred orientation and thus to form textured structure. But the thin films with the textured structure did not show good superconducting properties, especially $T_c$, since the liquid phase transformed into second phase in the grain boundary during the cooling. The effect of the second phase on $T_{c, \;zero}$ was greater than that on $T_{c, \;on}$.

• Korean Journal of Materials Research
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• v.1 no.1
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• pp.37-45
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• 1991

In order to control the microstructures, the sintering behavior and abnormal grain growth with Ba/Ti ratio variation of $BaTiO_3$were investigated. The $BaTiO_3$powders used in this study were prepared by conventional calcination of $BaCO_3$ and $TiO_2$. The onset temperatures of the sintering were lowered and the densification was enhanced with increasing amounts of $TiO_2$ excess. These results are because of decrease of calcined particle sizes. A eutectic melt above temperature of $1320^{\circ}C$ did not assist the densification. Grain growth was strongly inhibited with increasing amounts of $TiO_2$ excess. The inhibition of grain growth caused abnormal grain growth due to inhomogeneous distribution of Ti-rich second phase.

• Journal of the Korean Geotechnical Society
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• v.19 no.2
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• pp.171-178
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• 2003

Wing and secondary cracks are unique types of cracks observed in rock masses subjected to uniaxial and biaxial compressive loading conditions. In this study, morphological features of wing and secondary cracks developed in gypsum specimens are investigated in the macro and micro scales. Along the path of wing crack, microtensile cracks are observed. Microtensile cracks coalesce with pores and show branch phenomenon. From the onset of the wing crack, multiple initiations of microtensile cracks are observed. Microtensile cracks show tortuous propagation paths and relatively constant aperture of the cracks during the propagation. It is shown that microtensile cracks propagate by splitting failure. At the micro scale, microfsults are observed in the path of the secondary cracks. Along the path of the secondary cracks, separation of grains and conglomerate grains, oblique microfaults, and irregular aperture of microfault are observed. These features show that the secondary cracks are produced in shear mode. The measured sizes of fracture process zone across the propagation direction near the tip of wing and secondary cracks range from 10$\mu{m}$ to 20$\mu{m}$ far wing cracks and from 100$\mu{m}$ to 200$\mu{m}$ for secondary cracks, respectively.

• Journal of the Korean Vacuum Society
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• v.10 no.4
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• pp.396-402
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• 2001

MgO thin films with 1000 $\AA$ thickness were deposited on Cu substrates by using an electron gun evaporator at room temperature. A 1000 $\AA$ thick Al layer was deposited on the MgO for removing the charging effect of the MgO thin film during the measurements of the sputtering yields. A Ga ion liquid metal was used as the focused ion beam(FIB) source. The ion beam was focused by using double einzel lenses, and a deflector was employed to scan the ion beams into the MgO layer. Both currents of the secondary particle and the probe ion beam were measured, and they dramatically changed with varying the applied acceleration voltage of the source. The sputtering yield of the MgO layer was determined using the values of the analyzed probe current, the secondary particle current, and the net current. When the acceleration voltage of the FIB system was 15 kV, the sputtering yield of the MgO thin film was 0.30. The sputtering yield of the MgO thin film linearly increases with the acceleration voltage. These results indicate that the FIB system is promising for the measurements of the sputtering yield of the MgO thin film.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2007.11a
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• pp.510-510
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• 2007

Titanate nanotube(TNT)는 높은 비표면적과 우수한 물리화학적 특성을 가지고 있어 광촉매, 수소 저장재료, 태양전지용 전극재료 등에 적용되고 있다. 또한, 티타네이트 나노튜브는 전자 이동이 원활한 구조적 특징을 가지고 있어 리듐 이차전지용 호스트 재료로서 많은 연구가 진행 중이다. 이에 본 연구에서는 저온균일침전법으로 제조한 루틸상 $TiO_2$ 분말에 Lithium chloride를 1~10wt%를 동시에 첨가한 후 10M의 sodium hydroxide 수용액 내에서 수열합성하여 리튬이 도핑된 티타네이트 나노튜브를 제조하였다. 제조된 분말의 입자형상 및 크기는 전자주사 현미경을 이용하여 관찰하였으며, X-선 회절분석을 이용하여 리튬 첨가에 따른 결정상 변화를 관찰하였다. 또한 리튬이 도핑된 티타네이트 나노튜브의 전기화학적 특성 평가를 위해 양극 활물질 : 도전제 : 바인더를 75 : 20 : 5의 비율로 혼합한 후 coin cell을 제조하였고, potentiostat를 이용하여 용량 측정 및 cycle 특성을 실시하였다. 수열 합성법에 의해 형성된 입자는 직경 10nm, 길이 수 ${\mu}m$로 관찰되었으며, X-선 회절 시험 결과 LiO와 같은 이차상은 발견되지 않았다. 측정된 coin cell의 용량은 240mAh/g을 나타내었으나, 싸이클 특성이 빠르게 저하됨을 확인할 수 있었다.

• Computational Structural Engineering
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• v.11 no.4
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• pp.267-274
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• 1998

본 연구에서는 기지개와 미시구멍으로 구성된 복합재료에 입자보강 복합재료의 등가 재료상수 예측기법인 평균장 근사이론과 등가원리를 적용하여 위상 최적화에 필요한 등가 재료상수와 설계변수와의 상관관계식을 유도하였다. 또한, 유도된 관계식에 중간값을 갖는 설계변수의 수를 줄이기 위하여 벌칙인자를 도입하였다. 그리고 본 연구의 타당성을 검증하기 위하여 벌칙인자가 도입된 위상 최적화문제를 순차이차계획법인 PLBA 알고리즘을 이용하여 해석하였다.

• Proceedings of the Korea Society for Energy Engineering kosee Conference
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• 1994.05a
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• pp.28-38
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• 1994

분류층 가스화기 설계를 위한 일차연구로서 가스화기 이차공기 주입방법에 따른 비반응 난류장에 대한 수치해석을 검사체적에 기초한 유한차분방법을 이용하여 수행하였다. 압력과 속도의 연계문제는 SIMPLEC 알고리즘을, 레이놀즈 전단력은 k-$\varepsilon$ 난류모델을 사용하였다. 입자궤적 계산은 공기역학적 항력만을 고려하였으며 비선형적인 공기저항력에 의한 난류변동상관모델은 고려치 않았다. 이차공기 주입방법(parallel injection과 nonparallel 3$0^{\circ}C$ injection)에 따른 수치해석을 수행하여 Ar tracer의 질량분율에 대한 실험자료와 비교하여 만족할 만한 결과를 얻었으며 이차공기의 주입각 및 기타 제반변수에 따른 유동장 변화를 분석하였다.