• 한국재료학회지
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• 제34권6호
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• pp.303-308
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• 2024

The semiconductor and display industries require the development of plasma resistant materials for use in high density plasma etching process equipment. Yttria (Y₂O₃) is a ceramic material mainly used to ensure good plasma resistance properties, which requires a dense microstructure. In commercial production, a sintering process is applied to reduce the sintering temperature of Y₂O₃. In this study, the effect of the addition of glass frit to the sintered specimen was examined when manufacturing yttria sintered specimens for semiconductor process equipment parts. The Y₂O₃ specimen was shaped into a Ø50 mm size and then sintered at 1,600 ℃ for 1~8 h. The characteristics, X-ray diffraction pattern, densities, contraction rate of the specimen, and swelling of the surface of the Y₂O₃ specimens were investigated as a function of the sintering time and glass frit addition. The Y₂O₃ specimen exhibited a density of over 4.9 g/cm³ as the sintering time increased, and the swelling phenomenon characteristics were improved by glass frit, by controlling particle size.

• 한국결정성장학회지
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• 제21권4호
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• pp.181-186
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• 2011

$WO_3$ 첨가가 $TiO_2$계 SCR 촉매의 고온안정성에 미치는 영향을 구조적, 형상학적 분석을 통해 규명하였다. 순수한 $TiO_2$시편과 10 wt%의 $WO_3$를 첨가한 $WO_3-TiO_2$ 시편을 제조하여 $800^{\circ}C$에서 5시간 동안 열적 스트레스를 인가하였다. FT-IR을 이용하여 촉매의 산점 변화를 확언한 결과 $WO_3-TiO_2$ 시편의 경우가 순수한 $TiO_2$ 시편에 비해 열적 열화로 인한 산점의 감소가 상대적으로 적었다. 반면 $WO_3-TiO_2$ 와 $TiO_2$의 anatase에 서 rutile로의 상전이 정도는 각각 28.4%와 22.9%로 오히려 $WO_3-TiO_2$ 시편에서 rutile 상이 더 많이 증가한 것을 확인하였다. 형상학적 분석 결과 $WO_3-TiO_2$ 시편은 고온에서 $TiO_2$에 고용되어 있던 amorphous 상태의 $WO_3$가 $TiO_2$ 입자 표면에 석출되며 결정화가 일어나게 되고 이로 인해 촉매의 입자성장을 억제함을 확인하였다. 따라서 SCR용 $TiO_2$ 촉매에 첨가된 $WO_3$는 anatase에서 rutile로의 상전이를 촉진시켜 고온에서의 촉매 활성을 저하시킬 수 있지만, 입성장 억제에 대한 영향이 커 결과적으로 고온안정성을 향상시킴을 확인하였다.

• 한국응용과학기술학회지
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• 제20권1호
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• pp.33-43
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• 2003

$LiMn_2O_4$ catalyst for $CO_2$ decomposition was synthesized by oxidation method for 30 min at 600$^{\circ}C$ in an electric furnace under air condition using manganese(II) nitrate $(Mn(NO_3)_2{\cdot}6H_2O)$, Lithium nitrate ($LiNO_3$) and Urea $(CO(NH_2)_2)$. The synthesized catalyst was reduced by $H_2$ at various temperatures for 3 hr. The reduction degree of the reduced catalysts were measured using the TGA. And then $CO_2$ decomposition rate was measured using the reduced catalysts. Phase-transitions of the catalysts were observed after $CO_2$ decomposition reaction at an optimal decomposition temperature. As the result of X-ray powder diffraction analysis, the synthesized catalyst was confirmed that the catalyst has the spinel structure, and also confirmed that when it was reduced by $H_2$, the phase of $LiMn_2O_4$ catalyst was transformed into $Li_2MnO_3$ and $Li_{1-2{\delta}}Mn_{2-{\delta}}O_{4-3{\delta}-{\delta}'}$ of tetragonal spinel phase. After $CO_2$ decomposition reaction, it was confirmed that the peak of $LiMn_2O_4$ of spinel phase. The optimal reduction temperature of the catalyst with $H_2$ was confirmed to be 450$^{\circ}C$(maximum weight-increasing ratio 9.47%) in the case of $LiMn_2O_4$ through the TGA analysis. Decomposition rate(%) using the $LiMn_2O_4$ catalyst showed the 67%. The crystal structure of the synthesized $LiMn_2O_4$ observed with a scanning electron microscope(SEM) shows cubic form. After reduction, $LiMn_2O_4$ catalyst became condensed each other to form interface. It was confirmed that after $CO_2$ decomposition, crystal structure of $LiMn_2O_4$ catalyst showed that its particle grew up more than that of reduction. Phase-transition by reduction and $CO_2$ decomposition ; $Li_2MnO_3$ and $Li_{1-2{\delta}}Mn_{2-{\delta}}O_{4-3{\delta}-{\delta}'}$ of tetragonal spinel phase at the first time of $CO_2$ decomposition appear like the same as the above contents. Phase-transition at $2{\sim}5$ time ; $Li_2MnO_3$ and $Li_{1-2{\delta}}Mn_{2-{\delta}}O_{4-3{\delta}-{\delta}'}$ of tetragonal spinel phase by reduction and $LiMn_2O_4$ of spinel phase after $CO_2$ decomposition appear like the same as the first time case. The result of the TGA analysis by catalyst reduction ; The first time, weight of reduced catalyst increased by 9.47%, for 2${\sim}$5 times, weight of reduced catalyst increased by average 2.3% But, in any time, there is little difference in the decomposition ratio of $CO_2$. That is to say, at the first time, it showed 67% in $CO_2$ decomposition rate and after 5 times reaction of $CO_2$ decomposition, it showed 67% nearly the same as the first time.

• Korean Chemical Engineering Research
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• 제54권1호
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• pp.120-126
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• 2016

본 연구에서는 아크릴과 소량의 스티렌 모노머에 나노클레이인 순수한 몬모릴로나이트(Pristine monmorillonite: PM) 또는 개질된 몬모릴로나이트(30B 또는 25A)를 첨가한 후 비수계 분산(NAD) 중합에 의해 환경친화성 아크릴/나노클레이 NAD수지 복합재료를 제조하고 나노클레이가 이 NAD 수지의 중합물성 및 복합재료의 물리적 물성에 주는 영향에 대해 연구하였다. 중합 후의 NAD 수지의 입자 균일성 측면에서 나노클레이는 초기에 안정제와 함께 투입하는 것이 유리하였고 중합된 NAD수지의 고형분, 산가, 점도 결과에서는 유기화제로 개질된 25A를 첨가할 경우가 다른 나노클레이를 첨가할 경우보다 좋은 물성을 주는 것으로 나타났다. 25A첨가 NAD수지는 GPC 측정시 분자량의 증가와 다분산지수의 감소로도 좋은 물성이 확인되었다. 나노클레이 25A가 수지내에 잘 분산된 것은 XRD결과에서 나노클레이의 층간거리 증가로 확인 되었고 열적 물성 측정 결과와 동적 기계적 물성 측정에서도 나노클레이 25A를 포함한 NAD 수지의 유리전이온도가 가장 높게 나타났으며 저장 탄성율 또한 25A경우가 가장 우수한 것으로 관찰되었다. 따라서 비수계 분산중합에 의해 아크릴/나노클레이 NAD수지를 제조할 경우에는 나노클레이로 25A를 첨가하는 것이 가장 좋은 물성을 얻을 수 있음을 확인할 수 있었다.

• 한국재료학회지
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• 제22권4호
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• pp.195-201
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• 2012

$Ce^{3+}$-doped yttrium aluminum gallium garnet (YAGG:$Ce^{3+}$), which is a green-emitting phosphor, was synthesized by solid state reaction using ${\alpha}$-phase or ${\gamma}$-phase of nano-sized $Al_2O_3$ as the Al source. The processing conditions and the chemical composition of phosphor for the maximum emission intensity were optimized on the basis of emission intensity under vacuum UV excitation. The optimum heating temperature for phosphor preparation was $1550^{\circ}C$. Photoluminescence properties of the synthesized phosphor were investigated in detail. From the excitation and emission spectra, it was confirmed that the YAGG:$Ce^{3+}$ phosphors effectively absorb the vacuum UV of 120-200 nm and emit green light positioned around 530 nm. The crystalline phase of the alumina nanoparticles affected the particle size and the luminescence property of the synthesized phosphors. Nano-sized ${\gamma}-Al_2O_3$ was more effective for the achievement of higher emission intensity than was nano-sized ${\alpha}-Al_2O_3$. This discrepancy is considered to be because the diffusion of $Al^{3+}$ into $Y_2O_3$ lattice is dependent on the crystalline phase of $Al_2O_3$, which affects the phase transformation of YAGG:$Ce^{3+}$ phosphors. The optimum chemical composition, having the maximum emission intensity, was $(Y_{2.98}Ce_{0.02})(Al_{2.8}Ga_{1.8})O_{11.4}$ prepared with ${\gamma}-Al_2O_3$. On the other hand, the decay time of the YAGG:$Ce^{3+}$ phosphors, irrespective of the crystalline phase of the nano-sized alumina source, was below 1 ms due to the allowed $5d{\rightarrow}4f$ transition of the $Ce^{3+}$ activator.

• 한국광물학회지
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• 제32권4호
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• pp.259-271
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• 2019

채색 문화재 및 전통회화의 적색, 황색 안료로 사용되는 진사, 웅황, 그리고 자황의 광물학적 특성을 분석하고 촉진내후성 평가를 통한 안정성을 평가하였다. 진사는 시료명을 JB, JS로 하였고, 웅황과 자황은 각각 UH, JH로 하였다. 광물학적 특성 평가 결과 JB, JS는 cinnabar (HgS)로 주구성 광물이 확인되었고, 품위에 따른 화학성분에 차이를 보이지 않았다. UH와 JH는 각각 realgar (AsS), orpiment (As₂S₃)로 주구성 광물이 확인되었다. 편광현미경 관찰 결과 쪼개짐, 색상 등 편광학적 특성을 통해 모두 천연적으로 생성된 무기안료임을 알 수 있었다. 특히 진사의 경우 성분분석으로는 천연적으로 생성된 안료인지 인공안료인지 판별이 쉽지 않은데 편광현미경을 통해 천연안료가 가지는 입자특성 및 쪼개짐을 확인하였으며, 열적 반응 특성을 확인하였다. 열분석 결과 JH가 UH에 비해 유리전이 온도가 높고 안정한 것을 확인하였다. 촉진내후성 평가 결과 진사, 웅황 그리고 자황은 모두 광열화에 의한 색변화가 크게 나타나며, 진사는 최종적으로 흑색(blackening)되고 웅황과 자황은 밝은 노란색으로 변한다. Meta-cinnabar로 예상되는 JB가 cinnabar인 JS에 비해 흑화현상이 더 빨리 촉진되었으며, UH (realgar)는 광조사에 의해 arsenolite (As₂O₃)로 변하는 것을 확인하였다.

• 대한화학회지
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• 제59권5호
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• pp.454-465
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• 2015

본 연구의 목적은 액체 혼합물의 끓음에 대한 예비 화학교사의 인식을 알아보는 것이다. 이를 위해 사범대학에 재학 중인 예비 화학교사 65명을 대상으로 에탄올 수용액의 끓는점과 가열 곡선 유형, 용액이 끓을 때의 기포 속 입자 모형 등에 대한 설문조사를 실시하고, 이 중 9명을 면담하였다. 그 결과, 50% 몰분율의 에탄올 수용액의 끓는점에 대한 예비교사의 인식은 ‘78-100 ℃ 구간에서 끓기 시작한다’는 과학적인 응답이 52.3%이었고, ‘에탄올 끓는점인 78 ℃에서 끓기 시작한다’고 생각하는 응답이 35.4%이었다. 전자의 경우, 물과 에탄올의 부분 증기압력의 합이 순수한 에탄올의 증기압력보다 작고, 물의 증기압력보다 커진다는 과학적인 설명에 비해 ‘끓을 때 에탄올 분자가 물 분자와의 인력이나 진로 방해 등을 통해 순수한 끓는점보다 높아진다’고 생각하는 설명이 많았다. 후자의 경우, 에탄올이 먼저 끓는데, 끓는점은 물질의 고유성질이므로 혼합물이 되어도 변하지 않는다고 생각하였다. 액체 혼합물의 가열 시 온도변화에 대해서는 끓기 시작하면서 온도가 증가하다가 일정한 온도가 된다고 생각하는 응답자가 69.2%이었으나 이들은 에탄올이 끓으면서 기화되어, 액체상에 물의 비율이 높아지기 때문에 점점 끓는점이 증가하게 된다는 설명을 하거나, 에탄올은 상태 변화하지만 액체로 남아있는 물이 열에너지를 흡수하기 때문에 혼합액체의 온도가 증가한다는 설명을 제시하였다. 상당수의 예비교사는 두 개의 일정한 온도 구간이 나타난다는 응답을 하였는데 이들은 액체 혼합물의 각 성분이 자신의 고유한 끓는점에서 상태변화를 한다고 생각하고 있었다. 또한, 액체 혼합물의 증발과 끓음 상황에서 기체상에서의 입자 모형을 분석한 결과, 증발 상황에서는 대부분의 예비교사가 기체상에 물과 에탄올이 동시에 존재하는 모형을 그렸으나, 끓음 상황에서는 기체상에 에탄올만 존재하는 모형을 그리는 비율이 증가하였다. 결과를 바탕으로 예비교사들이 혼합액체의 끓음에 대해 가지고 있는 대체적 개념과 이들의 인식 개선을 위한 시사점을 논의하였다.

• 한국감성과학회:학술대회논문집
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• 한국감성과학회 2000년도 추계학술대회 논문집
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• pp.105-112
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• 2000

The conventional model did not take momentum conservation into consideration when the electron absorbs and emits the photons. II-ray provides momentum conservations on any directions of the entering photons, and also the electrons have radial momentum conservations and fully elastic bouncing between two atoms, in the new atom model. Conventional atom model must be criticized on the following four points. (1) Natural motions between positive and negative entities are not circular motions but linear going and returning ones, fur examples sexual motion, tidal motion, day and night etc. Because the radius of hydrogen atom's electron orbit is the order of 10$^{-11}$ m and the radia of the nucleons in the nucleus are the order of 10$^{-l4}$m and then the converging $\pi$-gamma rays to the nucleus have so great circular momentum, the electron can not have a circular motion. We can say without doubt that any elementary mass particle can have only linear motion, because of the $\pi$-rays' hindrances, near the nucleus. (2) Potential energy generation was neglected when electron changes its orbit from outer one to inner one. The h v is the kinetic energy of the photo-electron. The total energy difference between orbits comprises kinetic and potential energies. (3) The structure of the space must be taken into consideration because the properties of the electron do not change during the transition from outer orbit to inner one even though it produces photon. (4) Total energy conservation law applies to the energy flow between mind and matter because we daily experiences a interconnection between mind and body. Any magnet absorbs n-rays to S pole and sends out the $\pi$-rays from N pole. Proton are constructed with the closed n-rays quantum-mechanically. The crystallizing n-bonding makes two $\pi$-far infrared rays of one wave length between two protons if two $\pi$-rays are supplied to each proton. It is easily done for a $\pi$-ray to be absorbed to a proton if there is a parallel magnetic flow to the blood flow because a $\pi$-ray advances axially under a magnetic field and a proton looks like a sphere. A axially advancing disk-like $\pi$-ray can meet more easily the coming spheres than from the other directions. The blood crystals stimulate the autonomous nerves on the blood vessels during the flow by their mechanical sliding collisions. SM n-ray meridian therapy and SMACN $\pi$-ray meridian therapy show the stimulation of blood flow and also combinational experiment between SM $\pi$-ray meridian therapy and n-ray psycho-physics acupuncture shows more clearly that magnet is forcing to make $\pi$-rays absorbed to the nucleons.s.ons.

• 한국감성과학회:학술대회논문집
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• 한국감성과학회 2000년도 추계학술대회 논문집
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• pp.98-104
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• 2000

The conventional model did not take momentum conservation into consideration when the electron absorbs and emits the photons. II-ray provides momentum conservations on any directions of the entering photons, and also the electrons have radial momentum conservations and fully elastic bouncing between two atoms, in the new atom model. Conventional atom model must be criticized on the following four points. (1) Natural motions between positive and negative entities are not circular motions but linear going and returning ones, for examples sexual motion, tidal motion, day and night etc. Because the radius of hydrogen atom's electron orbit is the order of 10$^{-11}$ m and the radia of the nucleons in the nucleus are the order of 10$^{-14}$ m and then the converging $\pi$-gamma rays to the nucleus have so great circular momentum, the electron can not have a circular motion. We can say without doubt that any elementary mass particle can have only linear motion, because of the $\pi$-rays'hindrances, nearthenucleus. (2) Potential energy generation was neglected when electron changes its orbit from outer one to inner one. The h v is the kinetic energy of the photo-electron. The total energy difference between orbits comprises kinetic and potential energies. (3) The structure of the space must be taken into consideration because the properties of the electron do not change during the transition from outer orbit to inner one even though it produces photon. (4) Total energy conservation law applies to the energy flow between mind and matter because we daily experiences a interconnection between mind and body. Conventional Concept of Electric Field must be extended in the case of the direct and alternating current. Conventional concept is based on coulomb's force while the electric potential in the direct and alternating current is from Gibb's free energy. And also conventional concept has not any consciousness with human being but the latters has a conscious sensibility. The cell emf is from the kinetic energy of the open $\pi$-rays flow through the conducting wire. The electric potential in alternating current is from that the trans-orbital moving of the induced change of magnetic field in the wire produces flows of open $\pi$-rays, which push the rotating electrons on the orbital and then make the current flow. Human consciousness can induce a resonance with the sensibility of the open $\pi$-rays in the electric measuring equipment. Specially treated acupunctures with Nasucon is for sending an acupunctural effect from one place to another via space by someone's will power.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제40회 동계학술대회 초록집
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• pp.407-408
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• 2011

Natural boron consists of two stable isotopes 10B and 11B with natural abundance of 18.8 atom percent of 10B and 81.2 atom percent of 11B. The thermal neutron absorption cross-section for 10B and 11B are 3837 barn and 0.005 barn respectively. 10B enriched specific compounds are used for control rods and as a reactor coolant additives. In this work 2 methods for boron enrichment were analysed: 1) Gas irradiation in static conditions. Dissociation occurs due to multiphoton absorption by specific isotopes in appropriately tuned laser field. IR shifted laser pulses are usually used in combination with increasing the laser intensity also improves selectivity up to some degree. In order to prevent recombination of dissociated molecules BCl3 is mixed with H2S 2) SILARC method. Advantages of this method: a) Gas cooling is helpful to split and shrink boron isotopes absorption bands. In order to achieve better selectivity BCl3 gas has to be substantially rarefied (~0.01%-5%) in mixture with carrier gas. b) Laser intensity is lower than in the first method. Some preliminary calculations of dissociation and recombination with carrier gas molecules energetics for both methods will be demonstrated Boron separation in SILARC method can be represented as multistage process: 1) Mixture of BCl3 with carrier gas is putted in reservoir 2) Gas overcooling due to expansion through Laval nozzle 3) IR multiphoton absorption by gas irradiated by specifically tuned laser field with subsequent gradual gas condensation in outlet chamber It is planned to develop software which includes these stages. This software will rely on the following available software based on quantum molecular dynamics in external quantized field: 1) WavePacket: Each particle is treated semiclassicaly based on Wigner transform method 2) Turbomole: It is based on local density methods like density of functional methods (DFT) and its improvement- coupled clusters approach (CC) to take into account quantum correlation. These models will be used to extract information concerning kinetic coefficients, and their dependence on applied external field. Information on radiative corrections to equation of state induced by laser field which take into account possible phase transition (or crossover?) can be also revealed. This mixed phase equation of state with quantum corrections will be further used in hydrodynamical simulations. Moreover results of these hydrodynamical simulations can be compared with results of CFD calculations. The first reasonable question to ask before starting the CFD simulations is whether turbulent effects are significant or not, and how to model turbulence? The questions of laser beam parameters and outlet chamber geometry which are most optimal to make all gas volume irradiated is also discussed. Relationship between enrichment factor and stagnation pressure and temperature based on experimental data is also reported.