• 제목/요약/키워드: thermal gradient furnace

검색결과 13건 처리시간 0.026초

아-크로 천장 사용후의 규석벽돌의 광물 및 화학적 변화 (Mineral and Chemical Changes in Silica Brick After Service in Arc-furnace Roofs)

  • 오기동;박홍채
    • 한국세라믹학회지
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    • 제18권4호
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    • pp.247-256
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    • 1981
  • Silica bricks had been in arc-furnace roofs of various sizes and steelmaking practices. The resulting materials were examined with reference to mineral and chemical changes. Silica bricks develope definite zones while in service. These zones represent a concentration gradient through the brick that results from the thermal gradient across the brick and from the furnace atmosphere. There are major brick losses by spalling as well as by melting of the hot-face surface in an iron-oxide rich liquid.

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GTD111M 초내열합금에서 응고속도 및 온도구배가 일방향응고 조직 에 미치는 영향 (The Effect of Solidification Rates and Thermal Gradients on Directionally Solidified Microstructure in the Ni-base Superalloy GTD111M)

  • 예대희;김현철;이재현;유영수;조창용
    • 한국재료학회지
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    • 제12권12호
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    • pp.897-903
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    • 2002
  • Morphological evolution and growth mechanism at the solid/liquid interface during solidification were investigated in the Ni-base superalloy GTD111M by directional soldification and quenching(DSQ) technique. The experiments were conducted by changing solidification rate(V) and thermal gradient(G) which are major solidification process variables. High thermal gradient condition could be obtained by increasing the furnace temperature and closely attaching the heating and cooling zones in the Bridgeman type furnace. The dendritic/equiaxed transition was found in the G/V value lower than $0.05$\times$10{^3}^{\circ}C$s/$\textrm{mm}^2$, and the planar interface of the MC-${\gamma}$ eutectic was found under $17 $\times$ 10{^3}^{\circ}C$ s/$\textrm{mm}^2$. It was confirmed that the dendrite spacing depended on the cooling rate(GV), and the primary spacing was affected by the thermal gradient more than solidification rate. The dendrite lengths were decreased as increasing the thermal graditne, and the dendrite tip temperature was close to the liquidus temperature at $50 \mu\textrm{m}$/s.

경사기능성 세라믹/ 금속 복합재료의 열충격특성에 관한 연구 (A Study on Thermal Shock Characteristics of Functionally Gradient Ceramic/Metal Composites)

  • 송준희;임재규
    • 대한기계학회논문집A
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    • 제20권7호
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    • pp.2134-2140
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    • 1996
  • This study was carried out to anlayze the heat-resistant characteristics of functionally gradient material(FGM) composed with ceramic and metal. The thermal fracture behavior of plasma-sprayed FGM and conventional coating material(NFGM) was exaimined by acoustic emession technique under heating and cooling. Furnace cooling and rapid cooling tests were used to examine the effect of temperature change under various conditions, respectively. At the high temperature above $800^{\circ}C$, it was shown that FGM gives higher thermal resistance compared to NFGM by AE signal and fracture surface analysis.

일방향 초내열합금에서 응고속도 및 온도구배 따른 수지상간격 및 탄화물 형상 변화 (Dendrite Arm Spacing and Carbide Morphology with Thermal Gradient and Solidification Rate in Directionally Solidified Ni-Base Superalloy)

  • 손승덕;김연희;최규석;이재현;서성문;조창용
    • 한국주조공학회지
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    • 제27권2호
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    • pp.77-82
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    • 2007
  • The effects of thermal gradient and solidification rate on the dendrite arm spacing and carbide morphology were investigated in directionally solidified Ni-base superalloy, CM 247LC. Thermal gradient was controlled by changing the position of the cold chamber and the furnace set temperature. The interface morphology changed from the planar to dendritic as increasing solidification rate. It was found that the dendrite spacing decreased as increasing the thermal gradient as well as the solidification rate. Also, as increasing solidification rate, carbide morphology changed from blocky shape to script and spotty shapes.

Development of the RE indirect-heating LPE furnace and the effect of impurity in YIG film on the MSSW properties

  • Fujino, M.;Fujii, T.;Sakabe, Y.
    • 한국결정성장학회지
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    • 제12권6호
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    • pp.288-291
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    • 2002
  • We developed a new RF indirect-heating LPE furnace. The thermal gradient of our newly developed furnace is less than that of direct heating, and is as gentle as that of the resistance-heating LPE furnace. With this new furnace, the heating and/or cooling is faster than that of the resistance-heating furnace. Impurity-doped YIG film was grown from a $PbO-B_{2}O_{3}$, based flux on a (111) GGG substrate. To study the effect of the impurities on the MSSW threshold power and the saturation response time, we used two microstrip lines to excite and propagate the MSSW at 1.9 GHz. The MSSW threshold power and saturation response time was found to be related to the $\Delta$H.

6.4cm 크기의 일방향 성장된Y$Ba_2$$Cu_3$$O_x$ 제조 (Fabrication of 6.4 cm single grain $YBa_2$$Cu_3$$O_x$)

  • 박병삼;한상철;한영희;정년호;윤희중;김경진;성태현;오제명
    • Progress in Superconductivity
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    • 제5권2호
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    • pp.114-117
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    • 2004
  • We fabricated large single grain YBa$_2$Cu$_3$O$_{x}$ (Y-123) superconductors. The single grain Y-123 was grown by top seeded melt growth (TSMG) method. In a conventional box furnace with uniform temperature distribution, it was very difficult to grow large single grain Y-123 superconductors due to the size limitation in growth. To overcome the size limitation, we applied a radial thermal gradient (lower temperature at sample center and higher temperature on the sample edge) to the TSMG process. In this case, large single grain Y-123 could be easily grown. This is attributed that the liquid of the sample edge was maintained at the high temperature compared to the growth front. Using this method, we successfully fabricated a large single grain Y-123 of 6.4 cm X6.4 cm

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일방향응고시킨 Al-Co 합금의 특성에 관한 연구 (Characteristics of the Unidirectionally Solidified Al-Co Alloy)

  • 박수정;전현용;이현규
    • 한국주조공학회지
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    • 제25권1호
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    • pp.30-35
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    • 2005
  • The structures and mechanical property of the unidirectionally solidified Al-Co eutectic alloy were investigated. Al-Co eutectic alloy was unidirectionally solidified with growth rates(R) between I cm/hr and 10 cm/hr in the induction furnace maintaining the thermal gradient (G) at solid-liquid interface, $32^{\circ}C$/cm. The eutectic microstructure was varied with the growth condition(G/R ratio). When the G/R ratio was larger than $8.5{\times}10^{3}^{\circ}C/cm^{2}/sec$, a lamellar structure was formed, But the G/R ratio was smaller than $8.5{\times}10^{3}^{\circ}C/cm^{2}/sec$, a colony structure was formed. It was found that the interlamellar spacing(${\lambda}$) was dependent on the growth rate(R) with the relationship, ${\lambda}^{2}{\cdot}R=constant$. The microhardness of this eutectic alloy increased with increase in the growth rate.

Cu-35%Sn 합금의 일방향 열처리에서 출현하는 미세조직 (Microstructural Evolution in the Unidirectional Heat Treatment of Cu-35%Sn Alloys)

  • 최광진;지태구;박장식
    • 열처리공학회지
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    • 제16권6호
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    • pp.320-328
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    • 2003
  • A specimen of Cu-35%Sn alloy has been subjected to the unidirectional heat treatment in an attempt to examine the evolution of microstructures under varying thermal conditions. The specimen was cast in the form of a cylinder 10 mm in diameter and 200 mm in length, which was then installed in the temperature gradient field established inside a vertical tube furnace. The furnace temperature was adjusted to make the upper part at $750^{\circ}C$ and bottom end part at $300^{\circ}C$ of the specimen. The experiment was terminated by dropping it into water after the 30 minutes holding at given temperature. By the rapid cooling, the high temperature phases, ${\gamma}$ and ${\zeta}$, were retained at ambient temperature with some of ${\gamma}$ phase transformed to ${\varepsilon}$ phase, especially at the grain boundaries of ${\gamma}$ phase. The presence of ${\varepsilon}$ phase was found to determine the nature of phase transformations of the ${\zeta}$ phase undergoes upon cooling. In the close area of the ${\varepsilon}$ phase, ${\varepsilon}$ phase grew separately out of ${\zeta}$, and adds to the preexisting ${\varepsilon}$ whereas in areas away from ${\varepsilon}$, both ${\delta}$ and ${\varepsilon}$ grew simultaneously out of ${\zeta}$, and formed a lamella eutectoid structure. The transformation to ${\delta}$ was found to occur only in slow cooling. The hardness on each phase showed that the retained phases, ${\gamma}$ and ${\zeta}$, could be plastically deformed without brittle fracture while the phases, ${\varepsilon}$ and ${\delta}$, were too brittle to be deformed.

실리콘 용융 공정에서 방향성 응고에 관한 특성 분석 (Analysis with Directional Solidification in Silicon Melting Process)

  • 조현섭
    • 한국산학기술학회논문지
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    • 제15권3호
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    • pp.1707-1710
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    • 2014
  • 본 논문은 실리콘 원료의 용융과 방향성 응고에 의해 결정성이 양호한 방향성 응고에 대한 연구이다. 방사화 분석 결과 총 10가지 금속 불순물이 검출 되었지만, 농도 분포는 같은 위치에서 위와 아래의 차이는 크게 나지 않고, 어떤 특정한 위치에서 한쪽으로 집중되거나 어떤 경향성 없이 전체의 샘플의 모든 부분에서 농도가 거의 일정하게 분포를 나타냈다. 열 해석 시뮬레이션에 의한 결과, 용융은 유지 시간이 80분일 때 실리콘이 전체적으로 고르게 용융 온도에 도달하였고 냉각은 상부 냉각 온도가 $1,400^{\circ}C$와 60분 냉각 시 가장 좋은 결과 값을 나타내었다. 제작된 웨이퍼가 기존의 상용 웨이퍼보다 결정립계에서의 에칭이 훨씬 적게 이루어졌다.

천연베릴을 이용한 온도구배 환류법에 의한 합성 Emerald 단결정 육성 (Single Crystal Growth of Synthetic Emerald by Reflux Method of Temperature Gradient used Natural Beryl)

  • 최의석;김무경;이종민;안영필;서청교;안찬준
    • 한국결정성장학회:학술대회논문집
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    • 한국결정성장학회 1996년도 The 9th KACG Technical Annual Meeting and the 3rd Korea-Japan EMGS (Electronic Materials Growth Symposium)
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    • pp.519-521
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    • 1996
  • Emerald (3BeO.Al2O3.6SiO2 : Cr3+) single crystals were crystals were grown by reflux method of temperature gradient in the flux solution of Li2O-MoO3-V2O5 system. The composition of flux materials were 3 mole ratio of MoO3-V2O5/Li2O, subtituted 0.2 mole% of K2O, Na2O, Nb2O5 etc to Li2O content, solved 10-15% of beryl to flux quantity and doped 1% of Cr2O3 to emerald amount. Those of mixing were melted at 110$0^{\circ}C$ in Pt containers of the 3 zone furnace of melt-growth-return to circulate continniously, specially it has been grown large emerald single crystal when thermal fluctuation was treated for 2hrs of once time a day at 1050-95$0^{\circ}C$ in growth zone, substitutional solid solution effect of Cr+3 ion for Al+3 to the growth of emerald single crystal was good. Emerald single crystals were c(0001) hexagonal crystal face of preferencial growth direction and m(1010) post side. When it had been durated for 5 months emerald single crystals of the firet size of 0.6mm thickness of seed crystal were grown 32$\times$65mm(c x m) of maximum size and 6.2mm thickness.

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