• Title/Summary/Keyword: Bulk melting

검색결과 110건 처리시간 0.029초

Calculating the Threshold Energy of the Pulsed Laser Sintering of Silver and Copper Nanoparticles

  • Lee, Changmin;Hahn, Jae W.
    • Journal of the Optical Society of Korea
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    • 제20권5호
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    • pp.601-606
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    • 2016
  • In this study, in order to analyze the low-temperature sintering process of silver and copper nanoparticles, we calculate their melting temperatures and surface melting temperatures with respect to particle size. For this calculation, we introduce the concept of mean-squared displacement of the atom proposed by Shi (1994). Using a parameter defined by the vibrational component of melting entropy, we readily obtained the surface and bulk melting temperatures of copper and silver nanoparticles. We also calculated the absorption cross-section of nanoparticles for variation in the wavelength of light. By using the calculated absorption cross-section of the nanoparticles at the melting temperature, we obtained the laser threshold energy for the sintering process with respect to particle size and wavelength of laser. We found that the absorption cross-section of silver nanoparticles has a resonant peak at a wavelength of close to 350 nm, yielding the lowest threshold energy. We calculated the intensity distribution around the nanoparticles using the finite-difference time-domain method and confirmed the resonant excitation of silver nanoparticles near the wavelength of the resonant peak.

Zr-V-Mn-Ni계 라브스상 합금의 미세 구조와 전기 화학적 특성 (The Microstructure and the Electrochemical Characteristics of Zr based Zr-V-Mn-Ni Laves Phase Alloy)

  • 정치규;한동수;정원섭;김인곤;김원백
    • 한국수소및신에너지학회논문집
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    • 제8권3호
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    • pp.121-129
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    • 1997
  • 아크 용해법으로 제작한 $ZrV_{0.1}Mn_{0.7}Ni_{1.2}$ 합금(bulk 합금) 잉고트는 $ZrV_{0.2}Mn_{0.98}Ni_{1.04}$의 조성식을 가지는 fcc 구조의 C15형 Laves상이 주류를 이루는 matrix와 $ZrV_{0.01}Mn_{0.13}Ni_{1.2}$의 조성으로 $Z_9Ni_{11}$의 금속간 화합물 구조를 가지는 2nd phase가 균일하게 분포된 2개의 상으로 구성되어 있었다. $ZrV_{0.1}Mn_{0.7}Ni_{1.2}$ 합금의 방전 특성에 이 두 가지 상들이 미치는 영향을 알아보기 위해서 matrix와 2'nd phase합금을 분리 제작하였고, 이들 전극에 대한 전기 화학적인 충방천 특성들을 조사하였다. 그 결과 방전용량은 2nd phase가 가장 낮은 $160mAh/g$, 그 다음으로 matrix가 200mAh/g으로 bulk의 250mAh/g보다 낮았다. Matrix조성의 합금은 bulk합금과 거의 유사한 활성화, 고율 방전율, 자기방전 특성을 가졌고, 또한 활성화 후에 충방전에 따른 용량감소의 경향이 현저히 관찰되었다. 그러나 2nd phase 조성의 합금은 이들과는 확연한 차이를 보였다. 즉 활성화되기 어렵지만 활성화된 후에 용량감소의 경향은 거의 없었고 또한 자기방전 특성도 우수하였다.

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용융법에 의한 YBa2Cu3O7-y 초전도체 제작 (Preparation of YBa2Cu3O7-y Superconductor Using Melt Method)

  • 이상헌
    • 한국전기전자재료학회논문지
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    • 제35권6호
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    • pp.622-625
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    • 2022
  • YBa2Cu3O7-y bulk as a high temperature oxide superconducting conductor has the high critical temperature of 92 K. YBa2Cu3O7-y bulk superconductors have been fabricated by a seeded melting growth. Magnetic properties were studied by using superconductor of melted YBa2Cu3O7-y oxides. It was demonstrated that Y2BaCuO5 particles acts as a pinning center which plays an important role on the magnetic properties. The thickness of the upper and lower pellets of the YBa2Cu3O7-y bulk was formed at 40 mm with 55 g of the composition, and the YBa2Cu3O7-y superconductor was manufactured through a heat treatment process. Manufacturing the superconducting bulk, it is possible to improve the pore density of the superconducting bulk by providing a path through which oxygen could be emitted.

열처리 조건에 따른 Bi-2212 초전도 튜브의 특성 (Characteristics of Bi-2212 Superconductor Tube Depending on Heat-treatment Conditions)

  • 박용민;장건익
    • 한국전기전자재료학회논문지
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    • 제14권7호
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    • pp.606-610
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    • 2001
  • Bi-2212 HTS tube was fabricated by centrifugal forming and partial melting processes. Bi-2212 bulk tube has been optimized to achieve smooth surface and uniform thickness. The slurry was prepared in the mixing ratio of 10:1 between Bi-2212 powder and binder and initially charged into the rotating mold under the speed of 300~450 rpm. Heat-treatment was performed at the temperature ranges of 860~89$0^{\circ}C$ in air for partial melting. the HTS tube fabricated by centrifugal forming process at 89$0^{\circ}C$ under the rotating speed of 450 rpm was highly densified and the plate-like grains with more than 20${\mu}{\textrm}{m}$ were well oriented along the rotating axis. The measured Tc and J$_{c}$ at 10K on specimen heat treated at 89$0^{\circ}C$ was around 85 K and 1,200 A/$\textrm{cm}^2$ respectively.y.

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NdBCO 벌크 HTS 초전도 특성 (Superconducting Properties of NdBCO Bulk HTS)

  • 소대화;이영매;번점국
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2002년도 추계학술대회 논문집 Vol.15
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    • pp.91-94
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    • 2002
  • The conditions of zone-melting method such as a sample travel speed in a furnace, content of Nd422, control of melting temperature, and heat-treatment with/without Ar gas for $NdBa_{2}Cu_{3}O_{7-\delta}$ superconductor was optimized, As a results, a $NdBa_{2}Cu_{3}O_{7-\delta}$ sample with a surface area of $25mm^{2}$ showed a good superconducting properties when its travel speed was 6 mm/h, The improvement of superconductivity added with 10~20 wt% of Nd422 phase increasing pinning effect was also shown. The critical current density, $J_{c}$ was remarkable affected by the condition of heat-treatment temperature of $NdBa_{2}Cu_{3}O_{7-\delta}$superconductor with/without Ar ambient gas.

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Fabrication of a large grain YBCO bulk superconductor by homo-seeding melt growth method

  • Lee, Hee-Gyoun
    • 한국초전도ㆍ저온공학회논문지
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    • 제24권3호
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    • pp.35-40
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    • 2022
  • To fabricate large grain YBCO bulk superconductors by melt process, Sm123 single crystal with a high melting point are mostly used as seeds. However, it also uses Y123 film deposited on MgO single crystal substrate. This study investigated the growth behavior of the Y123 grain during a melt process when single grain YBCO bulk was used as a seed. Single grain Y123 bulk was grown when the seed size was small. When the seed size was relatively large, multiple grains were grown but the grains were still large. Y123 seed crystal was completely decomposed during high temperature anneal at 1040℃ and new Y123 crystals were nucleated during a slow cooling stage below a peritectic temperature. Thereafter, newly formed Y123 crystals from the seed area are thought to grow into the Y1.8 powder compact. The crystallographic orientations of newly nucleated Y123 grains are independent of the crystallographic orientation of Y123 seed. It is thought that the crystallographic orientation of newly nucleated Y123 crystal can be controlled by using Y211-free Y123 single crystal as a seed of homo-seeding melt growth.

Bloating Mechanism for Artificial Light Weight Aggregate of Surface Modification with Coal ash

  • Lee, Ki Gang
    • 한국세라믹학회지
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    • 제52권2호
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    • pp.159-164
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    • 2015
  • We manufacture artificial lightweight aggregates (ALWAs) using bottom-ash as the primary raw material. We coat the ALWA surfaces with low-melting point materials in order to enable them to bloat, which is essential to reduce the bulk density of the aggregate. Then, we sinter the prepared aggregates at 1000, 1100, and $1200^{\circ}C$ using either the direct or two-step firing schedules. Finally, we evaluate the properties of the fired samples through analyzing their bulk density, water absorption, and microstructure. The surface-modified samples result in a reduction of their bulk density by $0.3{\sim}0.4g/cm^3$ regardless of the firing method used. Based on these results, we conclude that this approach could provide a viable method for the mass-production of ALWAs from industrial waste such as bottom-ash.

용융법에 의한 수용성 유리의 제조 및 특성(II) : 용해 특성, 살균 효과 및 세포 독성 (Preparation and Characterization of Water-Soluble Glass Through Melting Process(II) : Dissolution Characteristics, Bactericidal Effects and Cytotoxicity)

  • 오승한;조종호;최세영;오영제
    • 한국세라믹학회지
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    • 제34권1호
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    • pp.13-22
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    • 1997
  • 은 이온과 구리 이온을 동시에 함유하는 살균용 인산염계 수용성 유리를 용융법으로 제조하였다. 분말상의 유리 시편을 상온의 증류수에 넣어 조성과 시간에 따른 용해 특성을, bulk상 시편에 대해서는 용해 전.후의 표면변화를 각각 관찰하였고, 살균 효과 및 세포독성을 평가하였다. 은 이온:구리 이온=1:1인 조성에서 최대 용해량을 나타내었으며 용해거동은 초기부터 total dissolution이 지배적이었다. 시간의 경과에 따라 용해는 진행이 되지만, 표면에 생성되는 새로운 층은 관찰되지 않았다. Pseudomonas sp, e. coli, staphylococcus aureus, 및 salmonella균에 대한 살균 효과는 용해량의 증가에 따라 증가하여 우수한 살균효과를 나타내었다. L929 세포에 대한 독성 실험 결과, 은 이온의 농도가 10ppm이상에서만 독성을 나타내었다.

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대기 플라즈마 용사공정을 이용한 Cu계 벌크 비정질 금속 코팅의 미세조직 분석과 나노 압입시험을 이용한 상 분석 (Microstructure Evolution of Cu-based BMG Coating during APS Process and Phase Analysis by Nano-indentation Test)

  • 김정환;강기철;윤상훈;나현택;이창희
    • Journal of Welding and Joining
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    • 제27권6호
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    • pp.43-48
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    • 2009
  • In this study, Cu-based bulk metallic glass (BMG) coatings were deposited by atmospheric plasma spraying (APS) process with different process conditions (with- and without hydrogen gas). As adding the hydrogen gas, thermal energy in the plasma flame increased and induced difference in the melting state of the Cu-based BMG particles. The microstructure and mechanical properties of the coatings were analyzed using a scanning electron microscope (SEM) with an energy dispersive spectroscopy (EDS) and nano-indentation tester in the light of phase analysis. It was elucidated by the nano-indentation tests that un-melted region was a mainly amorphous phase which showed discrete plasticity observed as the flow serrations on the load.displacement (P - h) curves, and the curves of solidified region showed lower flow serrations as amorphous phase mingled with crystalline phase. Oxides produced during the spraying process had the highest hardness value among the phases and were well mixed with other phases resulted from the increase in melting degree.

용융온도와 유지시간이 용융법으로 제작한 고온초전도체의 임계특성에 미치는 영향 (The Effects of Melting Temperature and Holding Time on Critical Characteristics of HTSC Fabricated by Melting Method)

  • 임성훈;한태희;박경국;임성우;조동언;한병성
    • 한국전기전자재료학회논문지
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    • 제11권2호
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    • pp.154-161
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    • 1998
  • The effects of melting temperature and holding time on the critical current density($J_c$) of $YBa_2Cu_3O_x$ based superconducting bulk fabricated by MPMG process were investigated. The amount of the formed $Y_2BaCuO_5$ phases increased with the melting temperature. However, the value of critical current density was highest at 1120 $^{\circ}C$. With this proper melting temperature, the effect of holding time on the critical characteristics was also investigated. In the case of Ag addition, the volume of the formed $Y_2BaCuO_5$ phase when the amount of Ag addition was 10 wt% and 20 wt% was observed to be highest at 20 minute and 40 minute respectively. But in the specimen without Ag, volume of $Y_2BaCuO_5$ phase increased as the holding time increased. The proper melting temperature and the holding time obtained were 1120 $^{\circ}C$ and 20 minute. The long holding time was not effective for the $J_c$ improvement as well as the formation of $Y_2BaCuO_5$.

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