• 제목/요약/키워드: Nd)_2(Zr\

검색결과 96건 처리시간 0.026초

$ZrO_2$ 첨가 $MnO_2/Mn_2O_3$/NaOH 계를 이용한 열화학적 물분해 수소제조 실험 연구 (Experimental Study on Thermochemical Water Splitting Hydrogen Production Using $MnO_2/Mn_2O_3$/NaOH System Added with $ZrO_2$)

  • 차광서;류재춘;이동희;김영호;박주식;김종원
    • 한국수소및신에너지학회논문집
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    • 제17권4호
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    • pp.353-361
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    • 2006
  • As one of the thermochemical water splitting hydrogen production cycles, which could be operated at the lower temperature below 1200 K, we investigated the feasibility of the cyclic operation of Ispra Mark 2 cycle with the addition of $ZrO_2$. The cycle is theoretically composed of three reaction steps; (1) 1st step($2MnO_2{\rightarrow}Mn_2O_3+0.5O_2$), (2) 2nd step($Mn_2O_3+4NaOH{\rightarrow}2Na_2O{\cdot}MnO_2+H_2+H_2O$) and (3) 3rd step($2Na_2O{\cdot}MnO_2H_2O{\rightarrow}4NaOH+2MnO_2$). From the TPR tests, the temperature ranges for $O_2$ production in 1st step and $H_2$ production in 2nd step were $550{\sim}750^{\circ}C$ and $650{\sim}750^{\circ}C$, respectively. In $MnO_2/Mn_2O_3/NaOH$ system, the formation of molten products due to the reaction between manganese oxides and NaOH were greatly decreased with the addition of $ZrO_2$. In addition, the results of a cyclic test were discussed with the viewpoint of $H_2$ production amounts and the feasibility of the process improvement.

Synthesis of Zr0.73Y0.27O1.87 Crystals by the Bridgman-Stockbager Method

  • Kim, Won-Sa;Yu, Young-Moon;Lee, Jin-Ho
    • 한국지구과학회지
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    • 제23권1호
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    • pp.52-58
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    • 2002
  • A colorless and transparent zirconium oxide ($Zr_{0.73}Y_{0.27}O_{1.87}$) crystal has been synthesized by the Bridgman-Stockbager method. The gem-quality material is produced by adding 20${\sim}$25 wt.% $Y_2O_3$ (stabilizer) and 0.04 wt.% $Nd_2O_3$ (decolorising agent) to the $ZrO_2$ powder. It shows a vitreous luster with a slight oily appearance. Under a polarizing microscope, it shows isotropic nature with no appreciable anisotropism. Mohs hardness value and specific gravity is measured to be 8${\sim}$$8{\frac{1}{2}}$ and 5.85, respectively. Under ultraviolet light it shows a faint white glow. The crystal structure of yttria-stabilized zirconia with 0.27 at.% Y has been re-investigated, using single crystal X-ray diffraction, and confirmed to be a cubic symmetry, space group $Fm{\overline{3}}m$ ($O^5_h$) with a=5.1552(5) ${{\AA}}$, V=136.99(5) ${{\AA}}^3$, Z=4. The stabilizer atoms randomly occupy the zirconium sites and there are displacements of oxygen atoms with amplitudes of ${\Delta}/a{\sim}$0.033 and 0.11 along <110> and <111> from the ideal positions of the fluorite structure, respectively.

다층 경사기능재료의 제조를 위한 Zr(Y,Ce)$O_2$ TZP/Mullite 현탁액의 가압여과 (Pressure Filtration of Zr(Y,Ce)$O_2$ TZP/Mullite Suspensions for the Preparations of Functionally Gradient Materials with Multi-layer)

  • 이상진;박상희;박홍채;전병세
    • 한국세라믹학회지
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    • 제37권7호
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    • pp.693-699
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    • 2000
  • Casting behavior of Zr(Y,Ce)O2 TZP/Mullite suspension during pressure filtration was investigated to prepare multi-layered Functionally Gradient Materials(FGM). The dispersion stabilities of each layer suspension were investigated by examination of zeta potential and viscosity. The each suspensions with 20 vol.% solid loading and 100 첸 of viscosity was prepared after fix of the dispersing agent (Sodium hexa-meta phosphate) and the binder (Hydroxyethyl cellulose), and then the cakes were formed at the 2.5 MPa~10.0MPa pressure range. The cake thickness of all suspensions was increased with the square root of time at the constant pressure, and the relations between filtration pressure(P)a nd dehydration rate (Q=dh/dt) showed that the flows of filtrates in the consolidated layers were laminar. The permeabilities were nearly constant during filtration, and kozeny constants(Kc) of the suspensions were 4.8~6.7. These valumes were seen as close to 5, which might be homogeneous particle packing during filtration. On the basis of those data, the multi layered compaction with 9 mm thickness and 52.5% green density was prepared by continuous pressure filtration.

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PLT buffer층의 삽입에 따른 강유전 PZT박막의 특성 향상 (Enhancement of the ferroelectric properties of $Pb(Zr,Ti)O_3$ thin films with $Pb(La,Ti)O_3$ buffers fabricated by pulsed laser deposition)

  • 임성훈;이은선;정현우;이상렬
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2004년도 하계학술대회 논문집 Vol.5 No.1
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    • pp.67-69
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    • 2004
  • The $Pb(Zr,Ti)O_3$ thin films were fabricated with $Pb(La,Ti)O_3$ buffers in-situ onto $Pt/Ti/SiO_2/Si$ substrates by pulsed laser deposition technique using a Nd:YAG laser with energy density of $2.5J/cm^2$, and deposited for 10 minutes at $550^{\circ}C$ of substrate temperature. And then, the films have been annealed at $550^{\circ}C$ in oxygen ambient pressure. The remanent polarization value is increased by using buffer layers but coercive field of films is slightly increased.

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보석용 무색 큐빅 저코니아의 최적 육성 조건 (Optimum Conditions for Growing Gem-quality Colorless Cubic Zirconia)

  • 김원사;유영문;신현숙
    • 한국광물학회지
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    • 제14권2호
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    • pp.99-110
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    • 2001
  • 보석용으로 적합한 무색 투명한 큐빅 저코니아를 스컬용융법으로 합성하였다. 사용한 합성 고온로는 고주파 전기로이고, 수냉식 도가니를 제작하여 실험하였다. 원료물질은 $ZrO_2$를 주원료 물질로 하였으며 25 wt.%의 $Y_2O_3$를 안정제로, 0.03~0.05 wt.%의 $Nd_2O_3$를 소색제로 첨가하였다. 육성된 단결정의 크기는 약 20$\times$63 mm이며, 화학성분은 $Zr_{0.73}$ $Y_{0.27}$ $O_{1.87}$ 이었다. 등방성을 띠며 굴절율이 2.15~2.18이고 비중은 5.85, 모스 경도는 8~8.5, 반사도는 13.47%이다. 큐빅 저코니아 결정은 등축정계의 면심격자(Z=4)를 하고 있으며 공간군 Fm3 m에 속한다. 단위포 상수는 a=5.157 $\AA$이며, $CaF_2$구조를 하고 있다. 합성공정의 최적 조건은 고주파 출력이 50 kW, 2.94 MHz이고 도가니의 직경과 높이는 각각 105 mm, 135mm일 때, 또 도가니의 하강 속도가 16 mm/hr일 때 최대인 42% 회수율을 나타내었다. 큐빅 저코니아의 굴절율(2.15~2.18)은 다이아몬드보다 작기 때문에 크라운과 퍼빌리언의 각도를 다이아몬드의 경우($40.5^{\circ}$)보다 작게 가공 처리하여야만 최대의 광채 및 화이어를 얻을 수 있다.

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과잉 Zr을 첨가한 MmNi4.5Mn0.5Zrx(x=0, 0.025, 0.05, 0.1) 합금의 수소용기 적용에 관한 연구 (Study on the Application for Hydrogen Storage Tank of MmNi4.5Mn0.5Zrx(x=0, 0.025, 0.05, 0.1) Alloys Containing Excess Zr)

  • 강길구;박승갑;강세선;권호영
    • 한국재료학회지
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    • 제12권8호
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    • pp.624-633
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    • 2002
  • In order to improve the hydrogen storage capacity and the activation properties of the hydrogen storage alloys, the rare-earth metal alloy series, MmN $i_{4.5}$M $n_{0.5}$Z $r_{x}$(x=0, 0.025, 0.05, 0.1), are prepared by adding excess Zr in MmN $i_{4.5}$M $n_{0.5}$ alloy. The various parts in hydrogen storage vessel consisted of copper pipes reached the setting temperature within 4~5 minutes after heat addition, which indicated that storage vessel had a good heat conductivity required in application. The performance test on storage vessel filled with rare-earth metal alloys of 1000 gr was also conducted after hydrogen charging for 10 min at $18^{\circ}C$ under 10 atm. It showed that the average capacity of discharged hydrogen volume was found to be for $MmNi_{4.5}$ $Mn_{0.5}$ and $MmNi_{4.5}$ $Mn_{x}$ 0.5/$Zr_{samples}$ indicated that the released amount of hydrogen for this $AB_{5}$ type alloys was more than 92 % of theoretic value, and also it was found that the optimum discharging temperature for obtaining an appropriate pressure of 3 atm was determined to be $V^{\circ}C$ for $MmNi_{4.5}$ $Mn_{0.5}$$Zr_{x}$(x=0, 0.025, 0.05, 0.1) hydrogen storage alloys. The released amount of these hydrogen storage samples was 125 $\ell$ , 122.4 $\ell$ and 108.15 $\ell$/kg for $MmNi_{4.5}$ $Mn_{0.5}$ $Zr_{0.025}$ $MmNi_{4.5}$M $n_{0.5}$Z $r_{0.05}$, and MmN $i_{4.5}$ Mn_0.5$Zr_{0}$, at $70^{\circ}C$ respectively. Amount of the 2nd phases increase with increase on Zr contents in $MmNi_{4.5}$$Mn_{0.5}$ $Zr_{ 0.1}$/ alloy. This phenomenon indicates that$ ZrNi_3$ in $MmNi_{4.5}$ $Mn_{0.5}$ $Zr_{x}$ / phase, which shows the maximum storage capacity and the strong resistance to intrinsic degradation, is considered as a proper alloy for hydrogen storage. As the Zr contents increase, the activation time and the plateau pressure decreases and sloping of the plateau pressure increases.creases.eases.s.

펄스형 Nd:YAG 레이저를 이용한 Al의 용접 특성연구 (A study on the pure Al weldability using a pulsed Nd : YAG laser)

  • 김덕현
    • Journal of Welding and Joining
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    • 제11권1호
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    • pp.52-61
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    • 1993
  • Laser welding of ASTM no. 1060 Al plate with a pulsed Nd: YAG laser of 200W average power was performed for end capping of KMRR nuclear fuel elements In this research, we performed basic welding experiments. Firstly, laser output parameters which affect laser welding parameters were studied by changing laser input parameters for effective welding of 1060 Al plates. We found that laser power density and pulse energy are important parameters for smooth bead shape. Secondly, welding parameters which affect weld width-to-depth ratio were studied by changing power density and pulse energy, shielding gas, and defocusing. We found that power density must be higher than 0.3 Mw/cm$^{2}$ pulse energy must be higer than 3 J. travel speed must not exceed 200mm/sec, laser focus must be existed beneath 2-3mm from plate surface and helium is proper shielding gas. Thirdly, we studied the weld defects of Al-1060 such as crack and porosity in lap-joint welding. We designed new welding geometry for crack free welding of Al-1060 plates, and obtained crack free weldment but with lack of fusion. However, with Ti, Zr grain refiner elements, we can weld Al plates without solidification hot crack. Finally, we studied the origin of porosity by changing shielding gas. And we found that porosity was resulted from entrapment of shielding gas by the collapsing keyhole.

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Zr을 함유한 di-(2-ethylhexyl)phosphoric acid에 의한 Am과 Eu의 상호분리(III) (Mutual Separation of Am and Eu by Solvent Extraction with di-(2-ethylhexyl)phosphoric acid Containing Zirconium(III))

  • 양한범;이일희;임재관;김종구;김정석;유재형
    • 공업화학
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    • 제8권6호
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    • pp.1006-1013
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    • 1997
  • 방사성 폐액에 존재하는 악티늄족과 란탄족의 대표원소로 Am과 Eu을 각각 선정하여 Zr을 함유한 di-(2-ethylhexyl) phosphoric acid 추출제를 사용하여 회분식으로 이들 원소의 상호분리에 대한 분리특성을 고찰하였다. 0.5M $HNO_3$에서 Zr을 함유한 1M DEHPA/n-dodecane(Zr 농도:$8.7g/{\ell}$)에 의한 Am 및 Eu의 추출율은 각각 92.3%와 99.1%이었으며, 추출제 1M DEHPA/n-dodecane에 함유된 Zr 농도에 비례하여 Am과 Eu의 추출율이 증가하는 상승효과를 보였다. 그리고 pH가 3.0으로 조정된 0.05M DTPA와 1M lactic acid의 혼합용액에 의한 제 1단계 역추출에서는 유기상으로 추출된 Am과 Eu의 38.1% 및 3%가 각각 역추출되었으며, 이때 Am 과 Eu의 분배계수로부터 구한 상호 분리 계수는 14.2였다. 또한 6M $HNO_3$용액에 의한 제2단계 역추출에서는 제1단계 역추출에서 역추출되지 않고 유기상에 남아 있는 Eu의 94.4%가 역추출되었다.

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(Ba1-2xNa2x)(Mg0.5-xZrxW0.5)O3 세라믹스의 마이크로파 유전특성 (Microwave Dielectric Properties of (Ba1-2xNa2x)(Mg0.5-xZrxW0.5)O3 Ceramics)

  • 윤상옥;홍창배;이윤중;김신
    • 한국전기전자재료학회논문지
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    • 제30권6호
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    • pp.356-360
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    • 2017
  • We investigated the phase evolution, microstructure, and microwave dielectric properties of Na- and Zr-doped $Ba(Mg_{0.5}W_{0.5})O_3$ [i.e., ($Ba_{1-2x}Na_{2x})(Mg_{0.5-x}Zr_xW_{0.5})O_3$] ceramics. $BaWO_4$ as a secondary phase was observed in all compositions, and it increased as the dopant concentration increased. All specimens revealed a dense microstructure. For the composition of x=0.01, polyhedral grains were observed. As the dopant concentration increased, the densification and the grain growth were promoted by a liquid phase. The quality factor($Q{\times}f_0$) decreased remarkably, whereas the dielectric constant (${\varepsilon}_r$) tended to decrease as the dopant concentration increased. The dielectric constant, quality factor, and temperature coefficient of the resonant frequency of the composition of x=0.01 sintered at $1,700^{\circ}C$ for 1 h were 18.6, 216,275 GHz, and $-22.0ppm/^{\circ}C$, respectively.

La와 Nd가 치환된 PZT 세라믹의 구조 및 전기적 성질 (Structure and Electric Properties of PZT Ceramics Substituted by La and Nd)

  • 정수철;박휴범;김정;김건;김시중
    • 한국세라믹학회지
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    • 제31권2호
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    • pp.155-160
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    • 1994
  • PZT ceramics substituted by La3+ and Nd3+ were fabricated according to the formula: [Pb1-x(La or Nd)x][Zr0.58Ti0.42]1-x/4$\square$x/4O3(x=0.00, 0.02, 0.05, 0.08, 0.15, 0.20). The crystal structure and microstructure were investigated by XRD and SEM. It was observed that the phase transitions among rhombohedral, tetragonal, and cubic symmetry occured as the substitutional quantity increased. Dielectric constant, dissipation factor and piezoelectric coefficient (d33), of each sample were measured. The dielectric properties were changed as the substitutional quanity of rare earth ion increased. These changes could be explained by crystal structure and compositional fluctuaction. Its d33 was higher at tetragonal region near to phase boundry between rhombohedral and tetragonal, which was explained by reorientation of domain wall.

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