• 제목/요약/키워드: Calcined powder

검색결과 251건 처리시간 0.028초

$Ca-PO_4-H_2O$계로부터 수산화아파타이트의 침전조건 결정 (Determination of Hydroxyapatite Precipitation Condition from the $Ca-PO_4-H_2O$ System)

  • 오영제
    • 분석과학
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    • 제13권2호
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    • pp.208-214
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    • 2000
  • 수산화물, 탄산염 및 수산화아파타이트(HAp)의 형성과 해리는 용액의 pH에 따라 달라지며 $Ca-PO_4-H_2O$계로부터 균질하고 미세한 HAp, $Ca_{10-x}(HPO_4)_x(PO_4)_{6-x}(OH)_{2-x}(x=0)$, 세라믹 분말을 제조하는데 매우 중요한 인자가 된다. 각 복합이온의 용해도는 pH와 직선적인 관계에 있으므로 용해도 도형은 수산화물, 탄산염 및 수산화아파타이트(HAp)의 평형상수와 용해도적으로부터 계산된 대수 몰농도로 그릴 수 있다. $Ca-PO_4-H_2O$계로부터 $25^{\circ}C$에서 단일상의 $Ca_{10-x}(HPO_4)_x(PO_4)_{6-x}(OH)_{2-x}(x=0)$ 분말을 제조하기 위한 최적의 pH조건은 이론적인 고찰 결과 $10.5{\pm}0.5$로 결정되었다. 실온에서 제조하여 $80^{\circ}C$에서 건조시킨 HAp분말은 75nm의 입자크기를 갖는 미세한 응집분말 이었으며, $1,000^{\circ}C$에서 하소시킨 HAp분말은 450nm 크기의 거의 균질한 형태의 분말을 얻었다. HAp분말들이 응집되어 있었지만 소결후 미세구조는 양호하여 우수한 기계적 특성을 보유하였다.

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폐 전지로부터 재활용 과정을 통한 란타넘, 네오디뮴 회수에 관한 연구 (A Study on the Recovery of Lantanum and Neodymium from Waste Battery Through the Recycling Process)

  • 채병만;이석환;김득현;서은주;김현일;이승환;이상우
    • 청정기술
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    • 제26권2호
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    • pp.116-121
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    • 2020
  • 본 연구에서는 유가금속 회수를 한 전기차 폐배터리 부산물의 재활용에 관하여 연구하였다. 폐배터리 부산물에는 희토류들이 남아있으나, 부산물의 형태로는 소재로서의 가치가 없기에 정제과정을 거쳐 희토류 산화물로 회수하였다. 희토류침전분말 형태의 부산물을 30% 수산화나트륨을 이용하여 가공이 편한 수산화물로 변환한 뒤, 옥살산의 용해도 차이를 이용하여 남아 있는 불순물을 정제한 뒤, D2EHPA (Di-(2-ethylhexyl) phosphoric acid)를 사용하여 이트륨을 분리하였다. 과망가니즈산 칼륨을 이용하여 세륨을 분리 후, PC88A (2-ethylhexylphosphonic acid mono-2-ethylhexyl ester)를 사용하여 란타넘과 네오디뮴을 분리하였다. 그 후 800 ℃의 온도에서 소성하여 란타넘, 네오디뮴 산화물로 재생하는 방법을 확인하였다.

La-Co치환량에 따른 스트론튬 페라이트의 미세구조 (Morphology of La-Co substituted SrM ferrite)

  • 장세동
    • 자원리싸이클링
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    • 제13권6호
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    • pp.31-36
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    • 2004
  • La-Co원소 치환량에 따른 스트론튬 페라이트의 미세구조효과와 자기특성변화를 연구하였다. La-Co치환된 스트론튬 페라이트는 La원소 치환량 x는 Fe와 Sr의 몰비 n과 Co원소 치환량 y와 x=2ny의 관계식에서, 하소분말의 보자력(Hcj) 값은 Fe와 Sr의 몰비 n=6.0에서 치환량 x=0.3일때 270 kA/m 및 x=0.2일때 240 kA/m 의 값을 나타내었다. La-Co원소가 치환된 스트론튬 페라이트 소결자석의 미세구조는 판상형으로 성장하고, 몰비가 높을수록 결정의 크기는 감소하였다. 이는 하소후 형성된 초기 결정상태에 의하여 결정된 것으로 판단된다. La-Co치환 스트론튬 페라이트의 소결자석의 자기특성은 몰비 n=0.6에서 치환량 x=0.3의 조건으로 제조한 경우, 잔류자속밀도(Br) 415 mT와 보자력(Hcj) 355 kA/m의 특성이 얻어졌으며, 몰비 n=6.0에서 치환량 x=0.2의 조건으로 제조한 경우 잔류자속밀도(Br) 410 mT와 보자력(Hcj)은 370 kA/m의 특성이 얻어졌다. 또한 자기특성곡선의 각성형은 치환량 x=0.2일때 더욱 향상되었다.

La-Co 치환량에 따른 스트론튬 페라이트의 미세구조 (Morphology of La-Co substituted SrM ferrite)

  • 장세동
    • 한국자원리싸이클링학회:학술대회논문집
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    • 한국자원리싸이클링학회 2004년도 13회 산화철워크샵
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    • pp.27-34
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    • 2004
  • 스트론튬 페라이트에 La-Co원소 치환량에 따른 미세구조효과와 자기특성변화를 연구하였다 La-Co치환된 스트론튬 페라이트는 La원소 치환량(x)은 Fe와 Sr의 몰비(n)과 Co원소치환량(y)와 x=2ny의 관계식을 갖으며, 하소분말의 보자력(HcJ) 값은 Fe와 Sr의 몰비 n=6.0에서 치환량 x=0.3일때 270kA/m 및 x=0.2일때 240kA/m의 값을 나타내었다 La-Co원소가 치환된 스트론튬 페라이트 소결자석의 미세구조는 판상형으로 성장하고, 몰비가 높을수록 결정의 크기는 감소하였다 이는 하소 후 형성된 초기 결정상태에 의하여 결정된 것으로 판단된다 La-Co치환 스트론들 페라이트의 소결자석의 자기특성은 몰비 n=6.0에서 치환량 x=0.3의 조건으로 제조한 경우 잔류자속밀도(Br) 415 mT와 보자력(HcJ) 355 kA/m의 특성이 얻어졌으며, 몰비 n=6.0에서 치환량 x=0.2의 조건으로 제조한 경우 잔류자속밀도(Br) 410 mT와 보자력(HcJ)은 370 kA/m의 특성이 얻어졌다. 또한 자기특성곡선의 각 형성은 치환량 x=0.2일때 더욱 향상되었다.

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침전법으로 제조된 Mg(OH)2의 잔류 Na염이 MgO 입자 형성에 미치는 영향 (Effect of Na Salt on the Formation of MgO Obtained from Mg(OH)2 by Precipitation Method)

  • 이동현;유승범;김대성;임형미;이승호
    • 한국재료학회지
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    • 제22권1호
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    • pp.54-60
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    • 2012
  • The particle size of MgO was examined as a function of the Na content in $Mg(OH)_2$ powders and the calcination temperature. $Mg(OH)_2$ suspension was obtained by dropwise precipitation of $Mg(NO_3)_2{\cdot}6H_2O$ and NaOH solutions. The suspension was diluted by varying the dilution volume ratio of distilled water to $Mg(OH)_2$ suspension to change the Na salt concentration in the suspension. $Mg(OH)_2$ slurry was filtered and dried at $60^{\circ}C$ under vacuum, and then its $Mg(OH)_2$ powder was calcined to produce MgO with different amount of Na content at $500\sim900^{\circ}C$ under air. Investigation of the physical and chemical properties of the various MgO powders with dilution ratio and calcination temperature variation was done by X-ray diffraction, transmission electron microscopy, BET specific surface area and thermal gravimetric analysis. It was observed that MgO particle size could depend on the condition of calcination temperature and dilution ratio of the $Mg(OH)_2$ suspension. The particle size of the MgO depends on the Na content remaining in the $Mg(OH)_2$ powder, which powder was prepared by changing the dilution ratio of the $Mg(OH)_2$ suspension. This change increased as the calcination temperature increased and decreased as the dilution ratio increased. The growth of MgO particle size according to the increase of temperature was more effective when there was a relatively high content of Na. The increase of Na content lowered the temperature at which decomposition of $Mg(OH)_2$ to MgO took place, thereby promoting the crystal growth of MgO.

Improved Magnetic Anisotropy of YMn1-$xCrxO_3 $ Compounds

  • Yoo, Y.J.;Park, J.S.;Kang, J.H.;Kim, J.;Lee, B.W.;Kim, K.W.;Lee, Y.P.
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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    • pp.218-218
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    • 2012
  • Recently, hexagonal manganites have attracted much attention because of the coexistence of ferroelectricity and antiferromagnetic (AFM) order. The crystal structure of hexagonal manganites consists of $MnO_5$ polyhedra in which $Mn^{3+}$ ion is surrounded by three oxygen atoms in plane and two apical oxygen ions. The Mn ions within Mn-O plane form a triangular lattice and couple the spins through the AFM superexchange interaction. Due to incomplete AFM coupling between neighboring Mn ions in the triangular lattice, the system forms a geometrically-frustrated magnetic state. Among hexagonal manganites, $YMnO_3$, in particular, is the best known experimentally since the f states are empty. In addition, for applications, $YMnO_3$ thin films have been known as promising candidates for non-volatile ferroelectric random access memories. However, $YMnO_3$ has low magnetic order temperature (~70 K) and A-type AFM structure, which hinders its applications. We have synthesized $YMn1_{-x}Cr_xO_3$ (x = 0, 0.05 and 0.1) samples by the conventional solid-state reaction. The powders of stoichiometric proportions were mixed, and calcined at $900^{\circ}C$ for $YMn1_{-x}Cr_xO_3$ for 24 h. The obtained powders were ground, and pressed into 5-mm-thick disks of 1/2-inch diameter. The disks were directly put into the oven, and heated up to $1,300^{\circ}C$ and sintered in air for 24 h. The phase of samples was checked at room temperature by powder x-ray diffraction using a Rigaku Miniflex diffractometer with Cu $K{\alpha}$ radiation. All the magnetization measurements were carried out with a superconducting quantum-interference-device magnetometer. Our experiments point out that the Cr-doped samples show the characteristics of a spin-glass state at low temperatures.

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고체산화물 연료전지의 공기극으로서 La1-xSrxMnO3 계의 합성 및 특성 (Synthesis and Properties of La1-xSrxMnO3 System as Air Electrode for Solid Oxide Fuel Cell)

  • 이유기;이영기
    • 한국재료학회지
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    • 제22권9호
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    • pp.470-475
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    • 2012
  • $La_{1-x}Sr_xMnO_3$(LSM,$0{\leq}x{\leq}0.5$) powders as the air electrode for solid oxide fuel cell were synthesized by a glycine-nitrate combustion process. The powders were then examined by X-ray diffraction(XRD) and scanning electron microscopy (SEM). The as-formed powders were composed of very fine ash particles linked together in chains. X-ray maps of the LSM powders milled for 1.5 h showed that the metallic elements are homogeneously distributed inside each grain and in the different grains. The powder XRD patterns of the LSM with x < 0.3 showed a rhombohedral phase; the phase changes to the cubic phase at higher compositions($x{\geq}0.3$) calcined in air at $1200^{\circ}C$ for 4 h. Also, the SEM micrographs showed that the average grain size decreases as Sr content increases. Composite air electrodes made of 50/50 vol% of the resulting LSM powders and yttria stabilized zirconia(YSZ) powders were prepared by colloidal deposition technique. The electrodes were studied by ac impedance spectroscopy in order to improve the performance of a solid oxide fuel cell(SOFC). Reproducible impedance spectra were confirmed using the improved cell, which consisted of LSM-YSZ/YSZ. The composite electrode of LSM and YSZ was found to yield a lower cathodic resistivity than that of the non-composite one. Also, the addition of YSZ to the $La_{1-x}Sr_xMnO_3$ ($0.1{\leq}x{\leq}0.2$) electrode led to a pronounced, large decrease in the cathodic resistivity of the LSM-YSZ composite electrodes.

Travelin Solvent Floating Zone법에 의한 LaAlO$_3$ 단결정의 성장 및 특성 (Growth and Characterization of LaAlO$_3$ Single Crystals by the Traveling Solvent Floating Zone Method)

  • 정일형;임창성;오근호
    • 한국세라믹학회지
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    • 제35권3호
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    • pp.280-286
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    • 1998
  • LaAlO3 Single crystals used as a substrate for thin film depositions of a high temperature oxide su-perconductor YB2Cu3O7 and applied to microwave frequencies were grown by the Traveling Solvent Flati-ing Zone (TSFZ) method and characterized. For the growth of LaAlO3 single crystals polycrystalline fe-edrods were prepared from powder mixture of La2O3 and Al2O3 with a mole ratio of 1:1 calcined at 110$0^{\circ}C$ for 3h and sintered at 140$0^{\circ}C$ for 4h The growth LaAlO3 crystals was 4-5mm in diameter 30mm in length and dark brown. The growth rate was 2-3mm/h and the rotation speeds were 10rpm for an upper ro-tation and 40 rpm for a lower rotation The growing crystals and the feedrods were counter-rotated. The orientation of the grown single crystals of LaAlO3 was identified to be [111] direction. Dielectric constants were measured to be 30-33 between 100 kHz and 1 MHz in the 30$0^{\circ}C$ to 45$0^{\circ}C$ temperature range and 102 in a range of 100 kHz at the phase transformation temperature of 522$^{\circ}C$ Dielectric losses were calculated to be 1.8$\times$10-4 at the room temperature and 5.7$\times$10-3 at the phase transformation temperature. Lattice con-stants of the grown crystlals were determined to be aR=5.3806 $\AA$ and $\alpha$=60.043$^{\circ}$ by the least square method.

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NiO가 도핑된 BaZr0.85Y0.15O3-δ의 소결거동 및 전도도에 관한 연구 (A Study on Sintering Behavior and Conductivity for NiO-doped BaZr0.85Y0.15O3-δ)

  • 박영수;김진호;김혜경;황광택
    • 한국수소및신에너지학회논문집
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    • 제23권6호
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    • pp.670-677
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    • 2012
  • Perovskite-type oxides such as doped barium zirconate ($BaZrO_3$) show high proton conductivity and chemical stability when they are exposed to hydrogen and water vapour containing atmospheres, thus it can be applicable to the hydrogen separation and the fuel cell electrolyte membranes. However the high temperature ($1700-1800^{\circ}C$) and long sintering times (24h) are generally required to prepare the fully densified $BaZrO_3$ pellets. These sintering conditions lead to the limitation of the grain size growth and the degradation of conductivity due to the acceleration of BaO evaporation at $1200^{\circ}C$. Here we demonstrate NiO-doped $BaZr_{0.85}Y_{0.15}O_{3-{\delta}}$ with lower calcination and sintering temperature, less experimental procedure and lower process cost than the conventional mixing method. The stoichiometry of $BaZr_{0.85}Y_{0.15}O_{3-{\delta}}$ was optimized by the control of excess amount of Ba (5mol%) to minimized BaO evaporation. We found that the crystal size of NiO-doped $BaZr_{0.85}Y_{0.15}O_{3-{\delta}}$ was increased with increase of calcination temperature from XRD analysis. NiO-doped $BaZr_{0.85}Y_{0.15}O_{3-{\delta}}$ powder was calcined at $1000^{\circ}C$ for 12h when its showed the highest conductivity of $3.3{\times}10^{-2}s/cm$.

부분 안정화 지르코니아의 파괴거동 (Fracture Behaviour of PSZ Composite)

  • 김환;임은극;고정하;황규홍
    • 한국세라믹학회지
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    • 제21권3호
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    • pp.239-244
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    • 1984
  • The effect of tetragonal $ZrO_2$ phase on the mechanical behavior in 7 mole% calcia partially stabilized zirconia has been studied. The $ZrO_2$ powder containg 7 mole% CaO prepared by Hot Petroleum Drying Method calcined at 80$0^{\circ}C$ for 1 hour was nearly 100% tetragonal but as the calcining temperature increased certain amount of monoclinic phase appeared. The sintered specimen at 1$700^{\circ}C$ for 5 hours was aged at 130$0^{\circ}C$ for 0, 24, 48, 72 hours. X-ray diffraction data showed that in the aged specimen monoclinic tetragonal and cubic phase coexisted. The Kc value of aged specimen for 48 hr was about 4.5MN/m3/2 much greater than unaged sample. But aged for 72 hr the KiC value was decreased. The increasing of toughness in PSZ is based on the Stress-Induced Phase Transformation that is metastable tetra-gonal $ZrO_2$ changes t stable monoclinic phase within the stress field of crack and the mechanical fracture energy absorption is occured But in this case due to certain amount of tetragonal phase transformed to monoclinic phase during cooling the microcrack effect by transformation also considered. Trerefore both Stress-Induced Phase Transformation and inclusion induced microcracking effect contrbute to the increase of fracture toughness of 7 mole% CaO-$ZrO_2$ containing monoclinic and tetragnola phase simulataneously.

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