• 대한화학회지
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• 제39권8호
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• pp.589-597
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• 1995

물과 에탄올 혼합 용매에서 전도도법으로 염의 한계 당량 전도도를 구한 후, TATB법으로 이온의 당량전도도를 구하고 Nightingale법으로 이온의 보정 유효반지름을 얻고, 이온에 용매화된 용매의 부피를 계산하여 몇가지 용매화수를 제안하고 이들중에서 해당 이온에 가장 타당한 용매화수$(h_{H_2O}/+h_o)$를 구하고, 해당 이온에 대한 등용매화점을 얻었다. 물과 에탄올 혼합 용매에서의 해당 이온에 대한 등용매화점이 물과 메탄올 혼합 용매에서의 해당 이온에 대한 등용매화점보다 높은 곳에서 나타남을 알 수 있었다. 이는 용매의 $E_T$의 경향과 잘 일치했으며, 이 경향으로 결과 해석이 가능했다. 그리고 해당 이온에 가장 타당한 용매화수로부터 물과 에탄올 혼합 용매의 조성이 바뀜에 따라 해당 이온에 선택적으로 용매화하는 용매를 알았다.

• 한국세라믹학회지
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• 제38권7호
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• pp.678-682
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• 2001

복합 페롭스카이트(P $b_{1-x}$C $a_{x}$)(C $a_{1}$3/N $b_{2}$3/) $O_3$(0.6$\leq$x$\leq$0.8) 세라믹스의 마이크로파 유전특성과 결합원자가사이의 관계에 대하여 고찰하였다. 유전상수(K)는 Ca 치환량이 증가함에 따라 A-자리의 이온반경 세제곱에 비례하여 감소하며, Qf 값은 증가하였다. Ca 치환량이 증가함에 따라 관찰된 이온분극률($\alpha$$_{obs}$)과 이론적인 이온분극률($\alpha$$_{theo}$) 사이의 편차는 3.47%에서 6.37%로 증가하였다. 이는 A-자리 결합원자가의 감소에 따른 결합강도의 감소로 해석하였다. 소결시편의 공진주파수의 온도계수(TCF)는 AB $O_3$페롭스카이트 화합물의 A-자리 결합원자가에 의존하였다.

• 센서학회지
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• 제29권2호
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• pp.105-111
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• 2020

Interest and demand for hydrogen sensors are increasing in the field of H₂ leakage detection during storage/transport/use and detection of H₂ dissolved in transformer oil for safety issues as well as in the field of breath analysis for non-invasively diagnosing a number of disease states for a healthy life. In this study, various ZnO-based sensors were synthesized by controlling the reduction in crystallite size, decoration of Pt nanoparticles, doping of electron donating atoms, and doping of various atoms with different ionic radii. The sensing response of the various prepared ZnO-based nanoparticles and quantum dots (QDs) for 10 ppm H₂ was investigated. Among the samples, the smallest-sized (3.5 nm) In³⁺-doped ZnO QDs showed the best sensing response, which is superior to those in previously reported hydrogen sensors based on semiconducting metal oxides. The higher sensing response of In-doped ZnO QDs is attributed to the synergic effects of the increased number of oxygen vacancies, higher optical band gap, and larger specific surface area.

• 한국재료학회지
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• 제17권12호
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• pp.637-641
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• 2007

The total energy and strength of Mg alloy doped with Al, Ca and Zn, were calculated using the density functional theory. The calculations was performed by two programs; the discrete variational $X{\alpha}\;(DV-X{\alpha})$ method, which is a sort of molecular orbital full potential method; Vienna Ab-initio Simulation Package (VASP), which is a sort of pseudo potential method. The fundamental mixed orbital structure in each energy level near the Fermi level was investigated with simple model using $DV-X{\alpha}$. The optimized crystal structures calculated by VASP were compared to the measured structure. The density of state and the energy levels of dopant elements was discussed in association with properties. When the lattice parameter obtained from this study was compared, it was slightly different from the theoretical value but it was similar to Mk, and we obtained the reliability of data. A parameter Mk obtained by the $DV-X{\alpha}$ method was proportional to electronegativity and inversely proportional to ionic radii. We can predict the mechanical properties because $\Delta{\overline{Mk}}$is proportional to hardness.

• 한국세라믹학회지
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• 제47권6호
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• pp.540-545
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• 2010

In this study, we have investigated new plasma resistant materials with less usage of rare-earth oxides than $Y_2O_3$ which is currently used in the semiconductor industry. We observed the stability ranges of $(Gd{\cdot}Y)_3Al_5O_{12}$ and $(La{\cdot}Y)Al_{11}O_{18}$ ternary systems, and measured their etch rates under typical fluorine plasma. $(Gd{\cdot}Y)_3Al_5O_{12}$ system showed an extensive solid solution up to 80 mol% gadolinium, but $(La{\cdot}Y)Al_{11}O_{18}$ showed a negligible substitution between rare-earth ions, which can be explained by the differences between the ionic radii. The etch rates depended on the total amount of rare-earth oxides but not on the substitution of the rare-earth ions. When the specimen was examined using XPS after the exposure to fluorine plasma, the strong surface fluorination was observed with a shift of the binding energy to higher energy.

• 한국세라믹학회지
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• 제45권11호
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• pp.694-700
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• 2008

Proton conducting oxides based on the $BaCe_{0.9}M_{0.1}O_{3-{\delta}}$ (M = La, AL) were tested for the alternative electrolyte materials of fuel cell. The power density for single cell of Air |Pt| $BaCe_{0.9}M_{0.1}O_{3-{\delta}}$ |Pt| $H_2(3%H_2O)$ system was maximum $0.04W/cm^2$ at $1000^{\circ}C$. In this system, proton transport number was proved to depend on the lattice parameters and the distortion of $CeO_6$ octahedral as a function of the ionic radii of acceptor ions. This proton conducting oxide system requires developing the new electrode materials for application.

• Bulletin of the Korean Chemical Society
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• 제6권6호
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• pp.344-347
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• 1985

Perovskite type oxides of $SrTiO_3,SrZrO_3,and\;SrTi_{1-x}Zr_xO_3$ have been systematically synthesized at $1250^{\circ}C$and $1550^{\circ}C$ with specimens containing additions of up to x=0.9 of zirconium by solid state reactions and characterized by X-ray diffraction. X-ray diffraction studies showed that the compound $SrTi_{1-x}Zr_xO_3$ has cubic structure. The lattice paramters of $SrTi_{1-x}Zr_xO_3$ solid solutions obey the Vegard's law and fairly large increase in volume can acompany the formation of this solution with increasing Zr content(X). Assuming the lattice constants of perovskite type compounds $A(B_{1-x}B'_x)O_3$where $B_{1-x}B'_x$ is $Ti_{1-x}Zr_x$, to be a linear function of the ionic radii of B and B' ions, the disordered ion pair of $Ti^{4+}$and $Zr^{4+}$ was verified from the lattice constants of a series compounds varying x=0,0.05, 0.25, 0.5, 0.75, 0.9, and 1.0 with known isovalent pairs.

• Bulletin of the Korean Chemical Society
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• 제22권1호
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• pp.30-36
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• 2001

The crystal structures of fully dehydrated $Pd^{2+}$ - and $TI^{+}$ -exchanged zeolite X, $Pd_{18}TI_{56}Si_{100}Al_{92}O_{384}(Pd_{18}TI_{50-}X$, a = $24.935(4)\AA$ and $Pd_{21}TI_{50}Si_{100}Al_{92}O_{384}(Pd_{21}TI_{50-}X$ a = $24.914(4)\AA)$, have been determined by single-crystal X-ray diffraction methods in the cubic space group Fd3 at $21(1)^{\circ}C.$ The crystals were prepared using an exchange solution that had a $Pd(NH_3)_4Cl_2\;:TINO_3$ mole ratio of 50 : 1 and 200 : 1, respectively, with a total concentration of 0.05M for 4 days. After dehydration at $360^{\circ}C$ and 2 ${\times}$$10^{-6}$ Torr in flowing oxygen for 2 days, the crystals were evacuated at $21(1)^{\circ}C$ for 2 hours. They were refined to the final error indices $R_1$ = 0.045 and $R_2$ = 0.038 with 344 reflections for $Pd_{18}Tl_{56-}X$, and $R_1$ = 0.043 and $R_2$ = 0.045 with 280 reflections for $Pd_{21}Tl_{50-}X$; I > $3\sigma(I).$ In the structure of dehydrated $Pd_{18}Tl_{56-}X$, eighteen $Pd^{2+}$ ions and fourteen $TI^{+}$ ions are located at site I'. About twenty-seven $TI^{+}$ ions occupy site II recessed $1.74\AA$ into a supercage from the plane of three oxygens. The remaining fifteen $TI^{+}$ ions are distributed over two non-equivalent III' sites, with occupancies of 11 and 4, respectively. In the structure of $Pd_{21}Tl_{50-}X$, twenty $Pd^{2+}$ and ten $TI^{+}$ ions occupy site I', and one $Pd^{2+}$ ion is at site I. About twenty-three $TI^{+}$ ions occupy site II, and the remaining seventeen $TI^{+}$ ions are distributed over two different III' sites. $Pd^{2+}$ ions show a limit of exchange (ca. 39% and 46%), though their concentration of exchange was much higher than that of $TI^{+}$ ions. $Pd^{2+}$ ions tend to occupy site I', where they fit the double six-ring plane as nearly ideal trigonal planar. $TI^{+}$ ions fill the remaining I' sites, then occupy site II and two different III' sites. The two crystal structures show that approximately two and one-half I' sites per sodalite cage may be occupied by $Pd^{2+}$ ions. The remaining I' sites are occupied by $TI^{+}$ ions with Tl-O bond distance that is shorter than the sum of their ionic radii. The electrostatic repulsion between two large $TI^{+}$ ions and between $TI^{+}$ and $Pd^{2+}$ ions in the same $\beta-cage$ pushes each other to the charged six-ring planes. It causes the Tl-O bond to have some covalent character. However, $TI^{+}$ ions at site II form ionic bonds with three oxygens because the super-cage has the available space to obtain the reliable ionic bonds.

• 한국세라믹학회지
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• 제39권11호
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• pp.1055-1062
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• 2002

정방정 지르코니아의 상안정성 및 저온열화기구를 고찰하기 위해 Y2O3 안정화 지르코니아에 3가 양이온 산화물을 첨가한 후 그 소결체의 기계적 물성, 라만 스펙트럼 및 격자상수 변화 등을 관찰하였다. 2Y-TZP에 $Zr^{4+}$ 보다 이온크기가 큰 3가 양이온($Sc^{3+},\;Yb^{3+},\;Y^{3+},\;Sm^{3+},\;Nd^{3+},\;La^{3+}$)들을 2 mol%까지 첨가하여 $1500{\circ}C$에서 1시간 소결후, X-ray 상분석 결과 $La^{3+}$의 경우에는 0.5 mol% 이상 첨가시 pyrochlore 상$(La_2Zr_2O_7)$의 형성으로 정방정상의 상안정성이 저하되었다. 첨가량이 증가할수록 $Zr6{4+}$과 이온크기가 거의 비슷한 $Sc^{3+}$를 첨가한 경우에는 정방정상만 관찰되었으나 $Yb^{3+},\;Y^{3+},\;Sm^{3+},\;Nd^{3+}$를 첨가한 경우에는 입방정상이 형성되었다. 양이온 크기가 커질수록 c/a비는 증가하였으나 $220{\circ}C$에서 500시간까지 열처리후 상분석 결과 단사정량은 감소하였다.

• 대한화학회지
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• 제23권4호
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• pp.237-242
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• 1979

물아닌 용매이고 비양성자성 용매인 탄산에틸렌에서 NaI, KI, $NH_4I,\;(CH_3)_4NI,\;(C_2H_5)_4NI,\;(C_2H_5)_3NHI,\;(C_2H_5)_2NH_2I,\;(C_2H_5)NH_3I$, NaPic, (Pic피크르산이온) 및 KPic의 전기전도도를 40$^{\circ}C에서 측정하고, Fuoss-Onsager-Skinner식에 의하여 한계당량전도도와 한계이온당량전도도를 구한 결과, $Na^+의 순위로서 용매화현상의 역순위과 일치하며 $(C_2H_5)_4N^+<(C_2H_5)_3NH^+<(CH_3)_4N^+<(C_2H_5)_2NH_2^+<(C_2H_5)NH_3^+ $ 로서 질량이동의 순위와 일치했다. Fuosso-Krauss 식으로 염들의 해리상수를 구한 결과 탐산에틸렌은 이들 염에 대하여 좋은 이온화 용매임을 알았다. 한편 이온들의 Stokes 반지름으로 부터 유효 반지름을 구한 결과 요오드화이온은 분명히 용매화 되었고 테트라알킬암모늄이온과 그의 치환체이온들은 거의 용매화 되어있지 않은것 같다.