• Title/Summary/Keyword: Tube Furnace

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PZT thin capacitor characteristics of the using Pt-Ir($Pt_{80}Ir_{20}$)-alloy (Pt-Ir($Pt_{80}Ir_{20}$)-alloy를 이용한 PZT 박막 캐패시터 특성)

  • Jang, Yong-Un;Chang, Jin-Min;Lee, Hyung-Seok;Lee, Sang-Hyun;Moon, Byung-Moo
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.05c
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    • pp.47-52
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    • 2002
  • A processing method is developed for preparing sol-gel derived $Pb(Zr_{1-x}Ti_x)O_3$ (x=0.5) thin films on Pt-Ir($Pt_{80}Ir_{20}$)-alloy substrates. The as-deposited layer was dried on a plate in air at $70^{\circ}C$. And then it was baked at $1500^{\circ}C$, annealed at $450^{\circ}C$ and finally annealed for crystallization at various temperatures ranging from $580^{\circ}C$ to $700^{\circ}C$ for 1hour in a tube furnace. The thickness of the annealed film with three layers was $0.3{\mu}m$. Crystalline properties and surface morphology were examined using X-ray diffractometer (XRD). Electrical properties of the films such as dielectric constant, C-V, leakage current density were measured under different annealing temperature. The PZT thin film which was crystallized at $600^{\circ}C$ for 60minutes showed the best structural and electrical dielectric constant is 577. C-V measurement show that $700^{\circ}C$ sample has window memory volt of 2.5V and good capacitance for bias volts. Leakage current density of every sample show $10^{-8}A/cm^2$ r below and breakdown voltage(Vb) is that 25volts.

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Pressureless Sintering and Spark-Plasma Sintering of Fe-TiC Composite Powders (Fe-TiC 복합재료 분말의 상압소결과 방전플라즈마소결)

  • Lee, B.H.;Bae, S.W.;Bae, S.W.;Khoa, H.X.;Kim, Ji Soon
    • Journal of Powder Materials
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    • v.22 no.4
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    • pp.283-288
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    • 2015
  • Two sintering methods of a pressureless sintering and a spark-plasma sintering are tested to densify the Fe-TiC composite powders which are fabricated by high-energy ball-milling. A powder mixture of Fe and TiC is prepared in a planetary ball mill at a rotation speed of 500 rpm for 1h. Pressureless sintering is performed at 1100, 1200 and $1300^{\circ}C$ for 1-3 hours in a tube furnace under flowing argon gas atmosphere. Spark-plasma sintering is carried out under the following condition: sintering temperature of $1050^{\circ}C$, soaking time of 10 min, sintering pressure of 50 MPa, heating rate of $50^{\circ}C$, and in a vacuum of 0.1 Pa. The curves of shrinkage and its derivative (shrinkage rate) are obtained from the data stored automatically during sintering process. The densification behaviors are investigated from the observation of fracture surface and cross-section of the sintered compacts. The pressureless-sintered powder compacts show incomplete densification with a relative denstiy of 86.1% after sintering at $1300^{\circ}C$ for 3h. Spark-plasma sintering at $1050^{\circ}C$ for 10 min exhibits nearly complete densification of 98.6% relative density under the sintering pressure of 50 MPa.

Low-temperture Synthesis of CdTe/Te Core-shell Hetero-nanostructures by Vapor-solid Process

  • Song, Gwan-U;Kim, Tae-Hun;Bae, Ji-Hwan;Lee, Jae-Uk;Park, Min-Ho;Yang, Cheol-Ung
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.02a
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    • pp.580-580
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    • 2012
  • Heterostructures has unique and important properties, which may be helpful for finding many potential applications in the field of electronic, thermoelectric, and optoelectronic devices. We synthesized CdTe/Te core-shell heterostructures by vapor-solid process at low temperatures using a quartz tube furnace. Two step vapor-solid processes were employed. First, various tellurium structures such as nanowires, nanorods, nanoneedles, microtubes and microrods were synthesized under various deposition conditions. These tellurium nanostructures were then used as substrates in the second step to synthesize the CdTe/Te core-shell heterostructures. Using this method, various sizes, shapes and types of CdTe/Te core-shell structures were fabricated under a range of conditions. These structures were analysed by scanning electron microscopy, high resolution transmission electron microscopy, and energy dispersive x-ray spectroscopy. The vapor phase process at low temperatures appears to be an efficient method for producing a variety of Cd/Te hetero-nanostructures. In addition, the hetero-nanostructures can be tailored to the needs of specific applications by deliberately controlling the synthetic parameters.

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A Study on the Effect of Automotive Engine Performance by Using Carbon Nano Colloid Cooling Water (탄소나노콜로이드 냉각수를 사용하여 자동차 엔진성능의 향상에 관한 연구)

  • Yi, Chung-Seob;Lee, Byung-Ho
    • Transactions of the Korean Society of Automotive Engineers
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    • v.19 no.5
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    • pp.134-142
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    • 2011
  • Although combustion is essential in most energy generation processes, it is one of the major causes of air pollution. Exhaust pipes with circular fin were designed to study the effect of cooling the recirculated exhaust gases (EGR) of Diesel engines on the chemical composition of the exhaust gases and the reduction in the percentages of pollutant emissions. The gases examined in this study were oxides of nitrogen (NOx), carbon dioxide ($CO_2$) and carbon monoxide (CO). In addition, $O_2$ concentration in the exhaust was measured. The designs adopted in this study were about exhaust pipes with solid and hollow fins around them direct surface force measurement in water using a nano size colloidal probe technique. The direct force measurement between colloidal surfaces has been an essential topic in both theories and applications of surface chemistry. As particle size is decreased from micron size down to true Carbon nano Colloid size (<10 nm), surface forces are increasingly important. Nano particles at close proximity or high solids loading are expected to show a different behavior than what can be estimated from continuum and mean field theories. The current tools for directly measuring interaction forces such as a surface force apparatus or atomic force microscopy (AFM) are limited to particles much larger than nano size. This paper use Water and CNC fluid at normal cooling system of EGR. Experimental result showed all good agreement at Re=$2.54{\times}10^4$ by free convection and Re=$3.36{\times}10^4$ by forced air furnace.

Study on Leaching Behavior for Recovery of Ga Metal from LED Scraps (LED 공정스크랩으로부터 Ga 회수를 위한 침출 거동 연구)

  • Park, Kyung-Soo;Swain, Basudev;Kang, Lee Seung;Lee, Chan Gi;Uhm, Sunghyun;Hong, Hyun Seon;Shim, Jong-Gil;Park, Jeung-Jin
    • Applied Chemistry for Engineering
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    • v.25 no.4
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    • pp.414-417
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    • 2014
  • LED scraps consisting of highly crystalline GaN and their leaching behavior are comprehensively investigated for hydro-metallurgical recovery of rare metals. Highly stable GaN renders the leaching of the LED scraps extremely difficult in ordinary acidic and basic media. More favorable state can be obtained by way of high temperature solid-gas reaction of GaN-$Na_2CO_3$ powder mixture, ball-milled thoroughly at room temperature and subsequently oxidized under ambient air environment at $1000-1200^{\circ}C$ in a horizontal tube furnace, where GaN was effectively oxidized into gallium oxides. Stoichiometry analysis reveals that GaN is completely transformed into gallium oxides with Ga contents of ~73 wt%. Accordingly, the oxidized powder can be suitably leached to ~96% efficiency in a boiling 4 M HCl solution, experimentally confirming the feasibility of Ga recycling system development.

Morphology and Segregation of Sulfide Inclusions in Cast Steels (I) (A Fabrication of Fe-FeS Alloys and the Observation of Their Sulfide Morphology) (주강의 유화물 형태와 편석에 대한 연구 (I) (Fe-FeS 합금의 제조와 유화물 형태 관찰))

  • Park, Heung-Il;Kim, Ji-Tae;Kim, Sung-Gyoo
    • Journal of Korea Foundry Society
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    • v.29 no.5
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    • pp.220-224
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    • 2009
  • In order to investigate the microstructural morphology of the sulfide expected from the Fe-FeS phase diagram, a vacuum-sealed quartz tube where pure iron (99.9%) and sulfur (99.99%) powders were charged was heated upto $1000^{\circ}C$ in the electric resistance furnace, held for 96 hours and quenched in cold water and then, rod specimen was produced. Compositional difference of the sulfur between upper and lower parts of the rod was 7.5wt.% and segregation of the sulfur was gradually increased from the lower part to the upper one of the rod. The rod specimen was divided into three parts by the microstructural morphology of the sulfide. The upper part of the rod specimen revealed single phase FeS intermetallic. In the middle part of the specimen, hyper-eutectic microstructure where primary FeS was precipitated first and then, eutectic of $\alpha$-Fe and FeS was formed in the inter-dendritic region of the FeS. Especially, hypo-eutectic microstructure was appeared in the lower part of the specimen. After primary dendrite of $\alpha$-Fe solidified, FeS dendrite which included small amount of $\alpha$-Fe and FeS eutectic in the inter-dendritic region was formed.

Growth of RIG Single Crystals by Flux Technique (융제법에 의한 RIG 단결정 육성)

  • 김성현;이석희;정수진
    • Journal of the Korean Ceramic Society
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    • v.26 no.4
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    • pp.459-470
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    • 1989
  • Single crystals of rare-earth iron garnets were grown from solutions of molten lead oxide, lead fluoride, baric oxide, iron oxide, and the oxides of yttrium, samarium orgadolinium. The crystals were grown by slow cooling technique. A convenient composition was 41.8mol% PbO, 20.59mol% PbF2, 8.23mol% B2O3, 20.00mol% Fe2O3 and 10.00mol% R2O3 where R is Y, Sm or Gd. For this experiment, platinum crucibles of size 20, 30cc and a vertical siliconit tube furnace were used. The precipitation temperature of YIG was observed in the range of 115$0^{\circ}C$-112$0^{\circ}C$ and the optimum growth conditions in this experiment were determined. The nucleation rate was controlled by the holding time after the fast colling, the growth rate by the slow cooling conditiions. The form of the grown YIG crystals showed a combination of {110} and {211}, and the size of the crystals grown in this experiment was up to about 9mm under the conditions of holding time 16hour, cooling rate 2$^{\circ}C$/hr. and temperature range 115$0^{\circ}C$-90$0^{\circ}C$. The precipitatin temperature of SmIG was observed in the range of 105$0^{\circ}C$-98$0^{\circ}C$ and the size of the crystals grown in this experiment was up to about 5mm under the conditiions of holding time 16hours, cooling rate 2$^{\circ}C$/hr. and temperature range 100$0^{\circ}C$-80$0^{\circ}C$.

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Characteristic Evaluation of the Fe-Al Alloy Preform Fabrication by Reactive Sintering Process for the Al Matrix Composites. (반응소결법으로 제조한 Al기 복합재용 Fe-Al합금 예비성형체의 특성평가)

  • Choi, Dap-Chon;Park, Sung-Hyuk;Joo, Hyung-Gon
    • Journal of Korea Foundry Society
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    • v.19 no.6
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    • pp.493-500
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    • 1999
  • Squeeze casting was used for fabricating a light metal base composite having high strength and wearresistance. Reactive sintering was used to prepare the preform of Squeeze casting. To utilize Fe-Al intermetallic compounds and SiC particle as a reinforcement, there needs to prepare Fe-Al mixed powder at 50, 60, 70at.%Al, and add SiC powder to the above mixture at 4, 7, 16, 24wt.%. The prepared mixture with SiC was reactive sintered in a tube furnace at $660^{\circ}C$ to get a porous hybrid preform of intermetallic compound and SiC. The preform prepared above was placed in a metal mold, preheated at $660^{\circ}C$ AC4C matrix was injected into the mold with the temperature of the melt at $610^{\circ}C$ After these processes, 66MPa was applied to the mold for 5 minute to finish the whole procedure. The maximum reaction temperature was increased with the increased Al amount, but decreased with the increased SiC amount. The density of the preform was decreased with SiC amount increase in the compacts due to swelling of the preform. An optical microscope was applied to observe the micro structure and the dispersion of the reinforcements. To analyze phases, We utilized XRD, EDS. Hardness test were chosen to get the information of mechanical properties. There were no significant changes in micro structure between the composite and preform. However, it was shown that uniform dispersion of the reinforcers and complete infiltration of the melt into the preform were achieved through the procedure of the squeeze casting. It was observed that the hardness of the composite is decreased with increased SiC amount, resulting from the volumetric expansion of the preform.

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The Status of Domestic Hydrogen Production, Consumption, and Distribution (국내 수소 생산, 소비 및 유통 현황)

  • Gim, Bong-Jin;Kim, Jong-Wook;Choi, Sang-Jin
    • Transactions of the Korean hydrogen and new energy society
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    • v.16 no.4
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    • pp.391-399
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    • 2005
  • This paper deals with the survey of domestic hydrogen production, consumption, and distribution. The amount of domestic hydrogen production and consumption has not been identified, and we survey the amount of domestic hydrogen production and consumption by industries. The hydrogen production industries are classified into the oil industry, the petrochemical industry, the chemical industry, and the other industry. In 2004, the amount of domestic hydrogen production was 972,601 ton, which corresponded to 1.9% of the global hydrogen production. The oil industry produced 635,683 ton(65.4%), the petrochemical industry produced 241,970 ton(24.9%), the chemical industry produced 66,250 ton(6.8%), the other industry produced 28,698 ton(2.9%). The hydrogen consumptions of corresponding industries were close to the hydrogen productions of industries except that of the other industry. Most hydrogen was used as non-energy for raw materials and hydrogen additions to the process. Only 122,743 ton(12.6%) of domestic hydrogen was used as energy for heating boilers. In 2004, 47,948 ton of domestic hydrogen was distributed. The market shares of pipeline, tube trailers and cylinders were 84.4% and 15.6%, respectively. The purity of 31,848 ton(66.4%) of the distributed hydrogen was 99.99%, and 16,100 ton(33.6%) was greater than or equal to 99.999%. Besides domestic hydrogen, we also identify the byproduct gases which contain hydrogen. The iron industry produces COG( coke oven gas), BFG(blast furnace gas), and LDG(Lintz Donawitz converter gas) that contain hydrogen. In 2004, byproduct gases of the iron industry contained 355,000 ton of hydrogen.

Co/Ti 다층 박막 구조 시스템에서의 계면반응

  • 이상훈;박세준;고대홍
    • Proceedings of the Korean Vacuum Society Conference
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    • 1999.07a
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    • pp.143-143
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    • 1999
  • Co/Ti 다층 박막을 제조하기 위해 직류원 마그네트론 스퍼터링 시스템을 이용하여 (100)실리콘 단결정 기판위에 Co와 Ti층을 각각 2/2, 5/5, 10/10 nm 정도의 두께로 조절하여 세가지 조성의 Co/Ti 다층 박막을 제조하였다. 이러한 Co/Ti 다층 박막의 후속 열처리는 Ar 가스분위기 하에서 Tube furnace를 이용하여 20$0^{\circ}C$와 30$0^{\circ}C$, 40$0^{\circ}C$의 온도에서 진행하였다. 증착초기에서부터 후속 열처리 공정을 진행하는 동안, Co/Ti 다층 박막에서의 계면반응을 미세 구조 변화 및 전기, 자기적 특성변화와 연관지어 관찰하였다. Co/Ti 다층 박막의 결정 구조와 미세 구조 변화를 관찰하기 위해 각각 X-선 회절기와 투과 전자 현미경을 사용하였고, 다층 박막의 전기적, 자기적 특성 변화를 관찰하기 위해 각각 4점 탐침기, 진동 시료형 자속계를 이용하였다. Co/Ti 다층 박막을 20$0^{\circ}C$의 저온에서 열처리를 한 경우에는 증착 초기의 계면반응에 의해 형성된 비정질 층이 성장하였고, 30$0^{\circ}C$와 40$0^{\circ}C$의 고온에서 열처리를 하는 경우에는 비정질 측의 성장보다는 새로운 화합물 CoTi 결정상이 형성되면서 비정질상은 오히려 감소하였다. 즉, Co/Ti 다층 박막의 계면 반응은 결정질 Co와 Ti을 계면 반응물로 소모시키면서 비정질 층을 성장시키는 비정질화 반응이 활발히 일어났다. 특히, 소모된 계면 반응물로 소모시키면서 비정질 층을 성장시키는 비정질화 반응일 활발히 일어났다. 특히, 계면 반응물로 소모시키면서 비정질 층을 성장시키는 비정질화 반응일 활발히 일어났다. 특히, 소모된 계면 반응물 Co와 Ti 중에서 Ti의 소모속도가 더 빠르게 관찰되었다. 이로부터 Ti 이 증착초기에서 저온 열처리 과정동안 Co/Ti 다층 박막의 계면에서 일어나는 비정질화 반응의 주 확산자로 작용했다는 것을 알 수 있다. 한편, 30$0^{\circ}C$와 40$0^{\circ}C$의 고온에서 열처리한 Co/Ti 다층 박막의 계면 반응은, 비정질 반응에 의한 비정질층의 형성보다는 새로운 화합물 결정질 CoTi상을 형성시키는 결정화 반응이 우세했다. Co/Ti 다층 박막의 전기적 저항은, 열처리에 의한 비정질 층의 생성 및 성장으로 인해 증가하였고 새로운 저저항 CoTi 결정상의 형성으로 인해 감소하는 것을 알 수 있었다. 또한 Co/Ti 다층 박막의 포화 자화값은, 열처리에 의한 계면에서의 비정질화 반응과 CoTi 결정화 반응으로 인해 강자성체인 Co 결정상이 감소됨에 따라 감소하는 경향을 나타냈다.

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