• 대한화학회지
• /
• 제24권3호
• /
• pp.193-200
• /
• 1980

N-Acetyl-L-cysteine, $C_5H_9NO_3S,$의 결정 및 분자구조를 X-선 회절법으로 연구하였다. 이 화합물의 결정은 삼사비등축정계에 속하며 공간군은 $P_1$이다. 단위세포상수는 a = 7.04(3), b = 5.14(2), c = 8.25(3)${\AA}$, ${\alpha}$ = 106(2), ${\beta}$ = 51(1), ${\gamma}$ = 124(2)$^{\circ}$이고, 단위세포는 분자 한개만을 포함하고 있다. Weissenberg 사진촬영으로 얻은 회절반점의 총수는 629개이며 direct method를 적용하여 구조해명을 한 후 full matrix least-squares method로 정밀화하였으며 최종 R값은 0.12이다. C-카르복실기 및 N-아세틸기의 원자들은 각각 평면을 이루고 있다. 카르복실기의 산소원자 O(1)은 이웃분자의 아세틸기의 산소원자 O(3)와 $O-H{\cdot}{\cdot}{\cdot}O$ 수소결합을 하며 그 길이는 2.59${\AA}$이다.

• 한국결정성장학회지
• /
• 제22권2호
• /
• pp.99-104
• /
• 2012

BCP(biphasic calcium phosphate) 분말을 제조하기 위하여 $Ca(NO_3)_2{\cdot}4H_2O$, $(NH_4)_2HPO_4$를 출발 물질로 공침법(co-precipitation process)을 이용하여 합성하였다. 합성된 분말의 열처리 전 후의 HAp(Hydroxyapatite)/${\beta}$-TCP(${\beta}$-Tricalcium phosphate) 결정상 비율 및 분광학적 특성을 XRD 및 FT-IR를 이용하여 분석하였다. BCP 분말의 생체활성 거동을 평가하기 위하여 Hanks' Balanced Salt Solution(HBSS)에 침적시켜 시간에 따라 형상, 이온농도의 변화 및 결정상을 분석한 결과 낮은 결정화도의 HAp가 생성됨을 확인하였다. BCP분말의 세포독성 평가에서도 대조군에 비하여 세포성장률이 우수함을 관찰하였다.

• 한국결정성장학회지
• /
• 제3권2호
• /
• pp.176-184
• /
• 1993

$Li_2O-Al_2O_3-SiO_2$계 유리조성에서, 특히 주결정상으로 $\beta$-spodumene을 석출시킬 수 있는 조성영역에서 $P_2O_5, TiO_2, ZrO_2$ 등을 첨가하여 용융한 후 소결법을 이용하여 이론밀도에 가까운 결정화 유리를 만들기 위한 최적 열처리 조건, 유리 분말의 입도 변화에 따란 영향과 그 때의 물성을 시차열분석, X-선 회절분석, 비중 측정, 열팽창 측정, 전자현미경 관찰 등을 통하여 연구하였다. $P_2O_5$를 첨가하여 소결법으로 결정화할 때 소결을 증진시키는 효과가 있었으며 9wt% 첨가한 경우가 가장 치밀한 것으로 나타났다. 최적의 열처리 조건은 $740^{\circ}C$에서 소결하여 치밀화를 시키고$ 950^{\circ}C$에서 결정화를 시켰을 때로서 상대밀도는 90% 이상이었으며 열팽창계수는 $-1{\times}10^{-7}/^{\circ}C$ 정도로서 부팽창인 것으로 나타났다.

• 한국결정성장학회지
• /
• 제20권5호
• /
• pp.243-248
• /
• 2010

Si-BCP(si-substituted biphasic calcium phosphate)를 제조하기 위하여 $Ca(NO_3)_2{\cdot}4H_2O$, $(NH_4)_2HPO_4$, $Si(OC_2H_5)_4$을 출발 물질로 공침법(co-precipitation process)을 이용하여 합성하였다. 합성된 분말의 HAp/${\beta}$-TCP 결정상 비율 및 Si-P 치환 거동은 X-선 회절 상 분석을 이용하여 측정하였고, silicon ion 첨가 시 나타나는 BCP의 화학적 결합거동을 측정하기 위하여 FT-IR를 사용하여 분석하였다. 또한 Si-BCP 분말의 in-vitro 생분해거동 및 생체활성도를 측정하기 위하여 제조된 분말을 SBF(simulated body fluid) solution에 침적시킨 뒤 분말의 형상과 구성 성분은 SEM과 EDS를 통하여 확인하였다.

• Transactions on Electrical and Electronic Materials
• /
• 제2권1호
• /
• pp.27-31
• /
• 2001

$\beta$-$In_2S_3$ and $\beta$-$In_2S_3$:$Co^{2+}$ thin films were grown using the spray pyrolysis method. The thin films crystallized into tetragonal structures. The indirect energy band gap of the thin films was found to be 2.32 eV for $\beta$-$In_2S_3$ and 1.81 eV for $\beta$-$In_2S_3$:$Co^{2+}$(Co:1.0 mol%) at 198K. The direct energy band gap was found to be 2.67 eV for $\beta$-$In_2S_3$ and 2.17 eV for $\beta$-$In_2S_3$:$Co^{2+}$(Co:1.0 mol%). Impurity optical absorption peaks were observed for the ${\beta}$-$In_2S_3$:$Co^{2+}$ thin films. These impurity absorption peaks are assigned, based on the crystal field theory, to the electron transitions between the energy levels of the $Co^{2+}$ ion sited in $T_{d}$ symmetry.

• 열처리공학회지
• /
• 제17권6호
• /
• pp.346-355
• /
• 2004

The flame quenching process has been employed to modify the surfaces of commercial marine propeller material, aluminum bronze alloy (Cu-8.8Al-5Ni-5Fe), and the microstructure, hardness and wear properties of the flame-quenched layers have been studied. The thermal history was accurately monitored during the process with respect to both the designed maximum surface temperature and holding time. The XRD and EDX analyses have shown that at temperatures above $T_{\beta}$, the microstructure consisting of ${\alpha}+{\kappa}$ phases changed into the ${\alpha}+{\beta}^{\prime}$ martensite due to an eutectoid reaction of ${\alpha}+{\kappa}{\rightarrow}{\beta}$ and a martensitic transformation of ${\beta}{\rightarrow}{\beta}^{\prime}$. The ${\beta}^{\prime}$ martensite phase formed showed a face-centered cubic (FCC) crystal structure with the typical twinned structure. The hardness of the flame-quenched layer having the ${\alpha}+{\beta}^{\prime}$ structure was similar to that of the ${\alpha}+{\kappa}$ structure and depended sensitively on the size and distribution of hard ${\kappa}$ and ${\beta}^{\prime}$ phases with depth from the surface. As a result of the sliding wear test, the wear resistance of the flame-quenched layer was markedly enhanced with the formation of the ${\beta}^{\prime}$ martensite.

• 폴리머
• /
• 제35권2호
• /
• pp.130-135
• /
• 2011

전자 기기의 빠른 발전에 따른 무선 기기들의 사용은 급격히 늘어나고 있다. 그래서 이런 제품에 자가 발전이 가능한 재료를 적용시키는 사례가 점차 늘고 있다. 여기에 사용되는 재료로서 poly(vinylidene fluoride) (PVDF)가 있는데 PVDF는 piezoelectricity를 낼 수 있는 특별한 결정구조인 ${\beta}$-phase를 가지고 있다. 이 논문에서는 piezoelectricity에 결정적인 영향인 ${\beta}$-phase 함량을 증가시키기 위해 다층 PVDF 필름을 제조하였다. 이 PVDF 필름은 용매인 DMAc에 10%로 용해시킨 깃으로 spin rate는 850 rpm, spin time은 60초이며 건조온도는 $60^{\circ}C$이다. 비교적으로 다층 필름은 단열 층보다 더 높은 ${\beta}$-phase함량을 나타내었다 이 ${\beta}$-phase함량은 4-layer 필름이 되기까지 점차 증가되었으며 최대 함량은 7.72이다.

• 한국세라믹학회지
• /
• 제22권3호
• /
• pp.53-59
• /
• 1985

Nucleation and crystallization of $\beta$-eucryptite in a glass of molecular percentage composition Li2O.Al2O3.2SiO2 are studied. The glasses are made by quenching of the melts from 143$0^{\circ}C$ to room temperature. Heat-treatment for nucleation and crystal growth are caried out at various temperature in the range between 50$0^{\circ}C$ and 80$0^{\circ}C$ with different duration of time. The amounts of crystallization are estimated by the method of x-ray powder diffraction. As the results a time-temperature-transformation relation for crystallization is derived. The maximum rate of crystallization is observed at about 75$0^{\circ}C$ from the T-T-T-curve while the crystallization temperature is detected at 67$0^{\circ}C$ by DTA measurement. The crystallization temperature moved to 62$0^{\circ}C$ by adding 5 weight percents of TiO2 and it moved to 78$0^{\circ}C$ by adding 2 weight percents of V2O5. The crystallization temperature moved to 62$0^{\circ}C$ by adding 5 weight percent of TiO2 it moved to 78$0^{\circ}C$ by adding 2 weight percents of V2O5 The activation energy for crystallization from the pure glass is calculated as 68 Kcal/mol and it varied to 53 Kcal/mol and 110Kcal/mol when 5 weight percents of TiO2 and weight percents of V2O5 are added respectively.

• 대한치과기공학회지
• /
• 제21권1호
• /
• pp.5-14
• /
• 1999

Glass ceramics for dental crown prosthesis were prepared by crystallization of CaO-MgO-SiO2-$P_2O_5-TiO_2$ glasses. Their crystallization behaviors have been investigated as a function of heattreatment temperature, holding time and chemical composition in relation to mechinical properties. Crystallization peak temperatures were determined by differential thermal analysis(DTA). Crystalline phases and mircostructures of heat-treated sample were determined by the means of powder X-ray diffraction(XRD) and scanning electron microscopy(SEM). The final crystalline phase assemblages and the microstructures of the samples were found to be dependent on glass compositions, heattreatment temperature, and holding time. 1st crystallization peak temperature(TP), affected strongly by apatite, was found to be increased or decreased. From the experiment, the following results were obtained : 1. The crystallization peak temperature($T_P$) formed by apatite increased until adding up to 9wt% $TiO_2$ to base glass composition, then decreased above that. 2. Apatite($Ca_{10}P_6O_{25}$), whitlockite(${\beta}-3CaO-P_2O_5$), $\beta$-wollastonite($CaSiO_3$), magnesium tianate($MaTiO_3$) and diopside(CaO-MgO-$2SiO_2$) crystal phase were precipitated in MgO-CaO-$SiO_2-TiO_2-P_2O_5$ glass system containing 9wt% and 11wt% of $TiO_2$ 3. Vickers hardness of samples increased with increasing heat-treatment temperature and Vickers hardness of S415T9 samples heat-treated at 1075 was approxi-mately 813Kg $mm^{-2}$ as maximum value. 4. Vickers hardness of samples increased due to precipitation of apatite, whitlockite, $\beta$-wollastonite, magnesium titanate, and diopside crystal phases within glass matrix.

• 대한전기학회논문지:전기물성ㆍ응용부문C
• /
• 제53권7호
• /
• pp.352-357
• /
• 2004

The composites were fabricated, respectively, using 61vol.% SiC - 39vol.% TiB$_2$ and using 61vo1.% SiC - 39vo1.% WC powders with the liquid forming additives of 12wt% $Al_2$O$_3$＋Y$_2$O$_3$ by pressureless annealing at 180$0^{\circ}C$ for 4 hours. Reactions between SiC and transition metal TiB$_2$, WC were not observed in this microstructure. The result of phase analysis of composites by XRD revealed SiC(6H), TiB$_2$ and YAG(Al$_{5}$Y$_3$O$_{12}$) crystal phase on the SiC-TiB$_2$, and SiC(2H), WC and YAG(Al$_{5}$Y$_3$O$_{12}$) crystal phase on the SiC-WC composites. $\beta$\$\longrightarrow$$\alpha$-SiC phase transformation was ocurred on the SiC-TiB$_2$, but $\alpha$\$\longrightarrow$$\beta$-SiC reverse transformation was not occurred on the SiC-WC composites. The relative density, the vicker's hardness, the flexural strength and the fracture toughness showed respectively value of 96.2%, 13.34GPa, 310.19Mpa and 5.53Mpaㆍml/2 in SiC-WC composites. The electrical resistivity of the SiC-TiB$_2$ and the SiC-WC composites is all positive temperature coefficient resistance(PTCR) in the temperature ranges from $25^{\circ}C$ to 50$0^{\circ}C$. 2.64${\times}$10-2/$^{\circ}C$ of PTCR of SiC-WC was higher than 1.645${\times}$10-3/$^{\circ}C$ of SiC-TiB$_2$ composites.posites.