• 제목/요약/키워드: B. Graphite

검색결과 191건 처리시간 0.021초

Effects of Coating Materials on Fluidity and Temperature Loss of Molten Metals from Runner Systems in Full Moulds.

  • Cho, Nam-Don;Kim, Yong-Hyun;Choi, Jung-Kwon
    • 한국주조공학회지
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    • 제10권1호
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    • pp.31-42
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    • 1990
  • The full mould casting process in one of the newly developed techniques which has many advantages. Unbonded sand mould has been prepared for the major mould and $CO^2$ gas mould has been used occasionally for comparison. Patterns were built up with expanded polystyrene and coated with three different materials. Silica, graphite and zircon were used for the coating layer. The effects on fluidity and temperature loss of molten metals were investigated. The molten metals were Al-5% Si alloy, Cu-30% Zn alloy and gray iron of approximately 4.0% of carbon equivalent. Experimental variables were runner section area, superheat, sprue height, coating materials, coating thickness and apparent density of EPS pattern. The effects of coating materials on fluidity and temperature loss of the molten metals during transient pouring are summarized as follows : As runner section area, superheat and sprue height increased, fluidity increased. Temperature loss decreased as runner section area and sprue height increased. However, reversed effects were observed in the case of superheat increment. The coating materials decreased the fluidity of each alloy in the order of silica, graphite and zircon. Zircon brought to the highest temperature loss among the coating materials used. The fluidity increased in the order gray iron, Cu-30% Zn and Al-5% Si alloy while temperature loss in the reverse order. Especially in case of reduced pressure process, the fluidity was increased apparently. Al-5% Si alloy showed the lowest temperature loss among the alloys. The increment of the apparent density of EPS pattern resulted in the fluidity decrease and temperature loss increase. The relation between fluidity and temperature loss of each alloy can be expressed by the following equation within the coating thickness limit of 0.5-1.5㎜. F^*={\frac{a}{T^*-b}}-c$ where, $F^*$ : fluidity in the Full mould, $T^*$ : temperature loss in the mould. a : parameter for full mould. b, c : constants.

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Pyrolyzed Fuel Oil/Coal-tar 혼합원료의 열중합 반응에 따른 Pitch 제조 특성 (Characteristics of Pitch Production of Pyrolyzed Fuel Oil/Coal-tar Blending Feedstock by Thermal Polymerization Reaction)

  • 이은별;김형기
    • 공업화학
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    • 제31권3호
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    • pp.328-333
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    • 2020
  • 본 연구에서는 PFO와 Coal-tar의 구조와 열 중합 거동 분석을 통해 PFO와 Coal-tar으로 구성된 혼합 원료의 피치 합성 간 제조 특성을 확인하였다. 원소분석과 FT-IR 분석을 통해, PFO와 Coal-tar 각각 0.355, 0.818로 방향족화도 수치를 확인하였다. 또한, PFO와 Coal-tar의 열중량 분석을 통해 질량 감소곡선의 차이를 확인하였으며, 이러한 현상은 방향족 화도와 관능기 함량에 따른 구조적 안정성에 기인한 것으로 판단된다. 피치 제조 특성은 PFO를 원료로 사용한 피치가 혼합원료로부터 제조된 피치보다 평균적으로 낮은 수율과 높은 연화점을 보임을 확인하였다. 특히 유사한 연화점을 가지는 P360 (138.5 ℃)과 B420 (141.4 ℃)을 비교하였을 때, 두 피치의 탄화수율은 각각 29.89, 49.03 wt%로 Coal-tar가 혼합된 경우 약 20 wt% 향상됨을 확인하였다. 이러한 결과는 다량의 알킬기를 포함하여 높은 피치 중합 반응성을 가지는 PFO와 높은 열적 안정성을 가지는 Coal-tar의 혼합에 기인한 것으로 판단된다.

$CaC_6$ 결정에 대한 정상상태에서의 $^{13}C$ 핵자기공명 측정 ($^{13}C$ Nuclear Magnetic Resonance Study of Graphite Intercalated Superconductor $CaC_6$ Crystals in the Normal State)

  • 김성훈;강기혁;민병진;;이무희;김준성
    • Progress in Superconductivity
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    • 제12권1호
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    • pp.51-56
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    • 2010
  • $^{13}C$ NMR (nuclear magnetic resonance) measurements have been performed to investigate the local electronic structure of a superconducting graphite intercalation compound $CaC_6$ ($T_c$ = 11.4 K). A large number of single crystals were stacked and sealed in a quartz tube for naturally abundant $^{13}C$ NMR. The spectrum, Knight shift, linewidth, and spin-lattice relaxation time $T_1$ were measured in the normal state as a function of temperature down to 80 K at 8.0 T perpendicular to the c-axis. The $^{13}C$ NMR spectrum shows a single narrow peak with a very small Knight shift. The Knight shift and the linewidth of the $^{13}C$ NMR are temperature-independent around, respectively, +0.012% and 1.2 kHz. The spin-lattice relaxation rate, $1/T_1$, is proportional to temperature confirming a Korringa behavior as for non-magnetic metals. The Korringa product is measured to be $T_1T\;=\;210\;s{\cdot}K$. From this value, the Korringa ratio is deduced to be $\xi$ = 0.73, close to unity, which suggests that the independent-electron description works well for $CaC_6$, without complications arising from correlation and many-body effects.

Synergistic Effect of Molybdate and Monoethanolamine on Corrosion Inhibition of Ductile Cast Iron in Tap Water

  • Kim, K.T.;Chang, H.Y.;Lim, B.T.;Park, H.B.;Kim, Y.S.
    • Corrosion Science and Technology
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    • 제16권1호
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    • pp.31-37
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    • 2017
  • A synergistic effect was observed in the combination of nitrite and ethanolamines. Ethanolamine is one of the representative organic corrosion inhibitors and can be categorized as adsorption type. However, nitrosamines can form when amines mix with sodium nitrite. Since nitrosamine is a carcinogen, the co-addition of nitrite and ethanolamine will be not practical, and thus, a non-toxic combination of inhibitors shall be needed. In order to maximize the effect of monoethanolamine, we focused on the addition of molybdate. Molybdate has been used to alternate the addition of chromate, but it showed insufficient oxidizing power relative to corrosion inhibitors. This work evaluated the synergistic effect of the co-addition of molybdate and monoethanolamine, and its corrosion mechanism was elucidated. A high concentration of molybdate or monoethanolamine was needed to inhibit the corrosion of ductile cast iron in tap water, but in the case of the co-addition of molybdate and monoethanolamine, a synergistic effect was observed. This synergistic effect could be attributed to the molybdate that partly oxidizes the metallic surface and the monoethanolamine that is simultaneously adsorbed on the graphite surface. This adsorbed layer then acts as the barrier layer that mitigates galvanic corrosion between the graphite and the matrix.

C_{28}H_{41}N_4O_4Br\;{\cdot}\;2H_2O$의 결정구조 ([ $C_{28}H_{41}N_4O_4Br\;{\cdot}\;2H_2O$ ])

  • 김문집;이정아;조경진;최기영
    • 한국결정학회지
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    • 제15권2호
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    • pp.93-98
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    • 2004
  • X-선 회절법을 이용하여 C_{28}H_{41}N_4O_4Br\;{\cdo}t\;2H_2O$의 분자 및 결정구조를 해석하였다. 이 결정의 결정계는 Triclinic이고 공간군은 Pl이며, 단위포 상수 a=9.000(1) $\AA$, b=9.312(3) $\AA$, c=9.344(2) $\AA$, $\alpha=89.37(20)^{\circ},\;\beta=68.81(3)^{\circ},\;\gamma=84.70(4)^{\circ},\;V=726.7(8){\AA},\;T=298K,\;Z=1,\;D_c=1.402Mgm^{-3}$이다. 회절반점들의 세기는 Enraf-Nonius CAD4 Diffractometer로 얻었으며 사용한 X-선은 graphite로 단색화한 $MoK{\alpha}$$(\lambda=0.71073\;{\AA}$을 사용하였다. 분자구조는 Direct method로 풀었으며, $F_o>4{\sigma}(F_0)$인 2521개의 독립 회절 데이터에 대하여 최소 자승법으로 370개의 변수를 정밀화하여 최종 신뢰도 값 $R=5.95\%$를 얻었다.

$C_{16}H_{19}O_2N_3CuCl_2\;{\cdot}\;H_2O$의 결정 구조 ([ $C_{16}H_{19}O_2N_3CuCl_2\;{\cdot}\;H_2O$ ])

  • 김문집;김영수;최기영
    • 한국결정학회지
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    • 제15권2호
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    • pp.99-103
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    • 2004
  • X-선 회절법을 이용하여 $C_{16}H_{19}O_2N_3CuCl_2\;{\cdot}\;H_2O$의 분자 및 결정구조를 해석하였다. 이 결정의 결정계는 Triclinic이고 공간군은 Pl이며, 단위포 상수는 $a=7.6202(9)\;{\AA},\;b=8.5943(7){\AA},\;c= 8.6272(6){\AA},\;\alpha=67.518(6)^{\circ},\; \beta= 68.043(8)^{\circ},\;\gamma=74.370(8)^{\circ},\;V=478.89(8)\;{\AA}^3,\;T=295K,\; Z=1,\;D_c=1.504Mgm^{-3}$이다. 회절반점들의 세기는 Enraf-Nonius CAD-4 Diffractometer로 얻었으며 graphite로. 단색화한 $MoK{\alpha}$,$(\alpha=0.7107\;\AA)$을 사용하였다. 분자구조는 Direct method로 풀었으며, $F_0>4\sigma(F_0)$인 1659개의 독립회절데이터에 대하여 최소 자승법으로 234개의 변수를 정밀화하여 최종 신뢰도 값 $R=2.47\%$를 얻었다.

Cholesteryl Isopropyl Carbonate의 결정구조에 관한 예비연구 (Preliminary Study on the Crystal Structure of Cholesteryl Isopropyl Carbonate)

  • 박영자
    • 한국결정학회지
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    • 제7권2호
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    • pp.126-132
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    • 1996
  • Cholesteryl Isopropyl Carbonate(C31O3H52)의 결정구조를 X-선 회절법으로 연구하였다. 결정의 공간군은 P212121이고, 단위세포 길이는 a=6.266(4), b=10.836(5), c=47.364(20)Å, Z=4, Dc=0.98 g/cm3 이고, Dm=1.01 g/cm3이다. 회절강도들은 Nonius CAD-4 diffractometer로 얻었으며, graphite-monochromatized MoKα radiation를 사용하여 2θ로 40°까지 얻었다. 분자구조는 직접법으로 풀었으며, 정밀화는 Fourier 법과 최소자승법으로 수행하였다. 현재 R값은 0.22로 아직 풀어야 할 연구과제로 남아있다. 이 화합물의 cholesterol 부분의 구조는 다른 화합물과 비교적 잘 일치하고 있다. 결정에서 분자들이 길게 c-axis에 평행하게 놓여있고, monolayer을 이루며 쌓여있는데 cholesterol 부분은 촘촘하게 모여있는 반면 isopropyl carbonate chain들은 느슨하게 모여있어 이 결정의 liquid crystalline state성질을 나타냄을 구조로서 설명하여 준다.

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Diamond-Like Carbon Films Deposited by Pulsed Magnetron Sputtering System with Rotating Cathode

  • Chun, Hui-Gon;You, Yong-Zoo;Nikolay S. Sochugov;Sergey V. Rabotkin
    • 한국표면공학회지
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    • 제36권4호
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    • pp.296-300
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    • 2003
  • Extended cylindrical magnetron sputtering system with rotating 600-mm long and 90-mm diameter graphite cathode and pulsed power supply voltage generator were developed and fabricated. Time-dependent Langmuir probe characteristics as well as carbon films thickness were measured. It was shown that ratio of ions flux to carbon atoms flux for pulsed magnetron discharge mode was equal to $\Phi_{i}$ $\Phi$sub C/ = 0.2. It did not depend on the discharge current in the range of $I_{d}$ / = 10∼60 A since both the plasma density and the film deposition rate were found approximately proportional to the discharge current. In spite of this fact carbon film structure was found to be strongly dependent on the discharge current. Grain size increased from 100 nm at $I_{d}$ = 10∼20 A to 500 nm at $I_{d}$ = 40∼60 A. To deposit fine-grained hard nanocrystalline or amorphous carbon coating current regime with $I_{d}$ = 20 A was chosen. Pulsed negative bias voltage ($\tau$= 40 ${\mu}\textrm{s}$, $U_{b}$ = 0∼10 ㎸) synchronized with magnetron discharge pulses was applied to a substrate and voltage of $U_{b}$ = 3.4 ㎸ was shown to be optimum for a hard carbon film deposition. Lower voltages were not sufficient for amorphization of a growing graphite film, while higher voltages led to excessive ion bombardment and effects of recrystalization and graphitization.

근거리장에 놓인 저전도율 차폐막의 차폐 효과 분석 (Analysis of Shielding Effectiveness of Low Conductivity Shield Layers within Near-field Region)

  • 이원선;이원희;허정
    • 한국인터넷방송통신학회논문지
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    • 제19권2호
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    • pp.59-65
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    • 2019
  • 노이즈 소스의 근거리장에 저전도율 차폐막이 놓여있을 때 차폐막 두께에 따른 EMI 차폐효과를 분석하였다. 노이즈 소스로는 광대역 특성을 갖는 나선형 안테나를 이용하였으며, 저전도율 차폐 재료로는 그래파이트를 선정하였다. 나선형 안테나 두 개를 만들어 두 안테나 사이의 투과계수를 분석하였고, 송수신 안테나 사이의 거리는 5 cm와 10 cm인 두 경우에 대해 수행하였다. 차폐막의 두께는 1 um에서 200 um까지 변화시켰다. 주파수는 100 MHz에서 6 GHz까지 변화시켜 최대 70 dB의 SE(Shielding Effectiveness)를 얻었다. 본 시뮬레이션에서는 차폐막 재료인 그래파이트의 특성상 전기적 차폐(electronic shielding)를 이용하였다. 이 결과를 바탕으로 향후 자기 차폐를 구현하여 차폐 성능을 향상시킬 수 있는 방법을 연구할 예정이다.

고온고압법에 의한 Type II, Type I aB 갈색 다이아몬드의 색향상 (Color Enhancement of the Type II and Type I aB Brown Diamonds into Colorless by HPHT Process)

  • 송정호;송오성
    • 한국세라믹학회지
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    • 제49권3호
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    • pp.221-225
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    • 2012
  • It is possible to enhance the color of the natural diamond with a high pressure high temperature(HPHT) process. We employed a pyrophyllite tube cell and cubic press apparatus for HPHT treatment on the brown colored Type II (5.6 GPa/ $1700^{\circ}C$/ 52 min), and Type I aB(5.6 GPa/ $1650^{\circ}C$/ 30 min) diamond samples. We investigated the microstructure, Types, fluorescence, properties of the diamonds with an optical microscopy, FT-IR, photoluminescence(PL) spectroscopy, Diamond-View, and micro-Raman spectroscopy. Two tinted brown diamonds changed into colorless just after the HPHT process. Optical microscopy showed that no crack and significant inclusion evolution occurred during the HPHT process except the small graphite spot appeared in Type I aB sample. FTIR spectrum confirmed that no Type, amber center, and platelet defect change with the HPHT treatment. Diamond-View could not distinguish the HPHT treated diamonds from the naturals. PL spectroscopy showed that N3 and H3 color centers remained even after HPHT process. Consequently, we successfully changed the color of diamonds into colorless by 5.6 GPa HPHT process.