• 한국수소및신에너지학회논문집
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• 제13권3호
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• pp.181-189
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• 2002

A series of multicomponent $Zr_{0.8}Ti_{0.2}Mn_{0.4}V_{0.6}Ni_{1-x}Fe_{x}$ (x=0.00, 0.08, 0.15, 0.22, and 0.30) alloys are prepared and their oystal structure and P-C-T curves are examined. The electrochemical properties of these allqys such as activation conditions, discharge capacity, cycling performance are also investigated. $Zr_{0.8}Ti_{0.2}Mn_{0.4}V_{0.6}Ni_{1-x}Fe_{x}$ (x=0.00, 0.08, 0.15, 0.22 and 0.30) have the C14 Laves phase hexagonal structure. The electrode was activated by the hot-charging treatment. The best activation conditions were the current density 120 mA/g and the hot-charging time 12h at $80^{\circ}C$ in the case of the alloy with x=0.00. The discharge capacity increased rapidly until the fourth cycle and then decreased. The discharge capacity increased again from the 13th cycle, arriving at 234 mAh/g at the 50th cycle. The discharge capacily just after activation decreases with the increase in the amount of the substituted Fe but the cycling performance is improved. The discharge capacity after activation of the alloy with x=0.00 is 157 mAh/g at the current density 120 mA/g. $Zr_{0.8}Ti_{0.2}Mn_{0.4}V_{0.6}Ni_{0.85}Fe_{0.15}$ is a good composition with a medium quantity of discharge capacities and a good cycling performance. The ICP analysis of the electrolyte for these electrodes after 50 charge-discharge cycles shows that the concentrations of V and Zr are relatively high. Another series of multicomponent $Zr_{0.8}Ti_{0.2}Mn_{0.4}V_{0.6}Ni_{0.85}M_{0.15}$ (M = Fe, Co, Cu, Mo and Al) alloys are prepared. They also have the C14 Laves phase hexagonal structure. The alloys with M = Co and Fe have relatively larger hydrogen storage capacities. The discharge capacities just after activation are relatively large in the case of the alloys with M = Al and Cu. They are 212 and 170 mAh/g, respectivety, at the current density 120mA/g. The $Zr_{0.8}Ti_{0.2}Mn_{0.4}V_{0.6}Ni_{0.85}Co_{0.15}$ alloy is the best one with a relatively large discharge capacity and a good cycling performance.

• 한국세라믹학회지
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• 제48권4호
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• pp.307-311
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• 2011

Solid solutions of the (1-x)$BiFeO_3-xSrTiO_3$ ceramic system (x = 0~0.4) are explored here in attempts to obtain multiferroic properties in these systems. The polarization-electric field hysteresis, magnetization-magnetic field curves, and dielectric properties are also characterized. This solid-solution system shows a crystal structural transition from a noncentrosymmetric (R3c) structure to a centrosymmetric (Pm-3m) structure at 0.3 < x < 0.4. The solid solution ceramic shows unsaturated M-H behavior and low remanent magnetization over the composition region of 0.1 ${\leq}$ x ${\leq}$ 0.3. The $0.7BiFeO_3-0.3SrTiO_3$ system shows the largest value of $M_s$ at 0.17 emu/g and the smallest value of $H_c$ at 1.06 kOe. The P-E hysteresis curves were not saturated under an electric field as high as E = 70 kV/cm. This system is considered to have multiferroic characteristics in the composition range of 0.1 ${\leq}$ x ${\leq}$ 0.3.

• 한국재료학회지
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• 제25권6호
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• pp.288-292
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• 2015

New lead-free piezoelectric ceramics $0.96[\{Bi_{0.5}(Na_{0.84}K_{0.16})_{0.5}\}_{1-x}La_x(Ti_{1-y}Nb_y)O_3]-0.04SrTiO_3$ (BNKT-ST-LN, where $x=y=0.00{\leq}(x=y){\leq}0.015)$ were synthesized using the conventional solid-state reaction method. Their crystal structure, microstructure, and electrical properties were investigated as a function of the La and Nb (LN) content. The X-ray diffraction patterns revealed the formation of a single-phase perovskite structure for all the LN-modified BNKT-ST ceramics in this study. The temperature dependence of the dielectric curves showed that the maximum dielectric constant temperature ($T_m$) shifted towards lower temperatures and the curves became more diffuse with an increasing LN content. At the optimum composition (LN 0.005), a maximum value of remnant polarization ($33C/cm^2$) with a relatively low coercive field (22 kV/cm) and high piezoelectric constant (215 pC/N) was observed. These results indicate that the LN co-modified BNKT-ST ceramic system is a promising candidate for lead-free piezoelectric materials.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2009년도 제38회 동계학술대회 초록집
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• pp.4-5
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• 2010

The surface phonon is defined as a coherent vibrational excitation of surface atoms propagating along the surface. It is characterized by a phonon dispersion curves, which were extensively studied in 1990's using helium atom scattering and high-resolution electron-energy-loss spectroscopy (HREELS)[1].The understanding is mainly based on the theoretical framework of a classical bond model or cluster calculations. The recent sample preparation and first principles calculations open the naval way to deep insight for surface phonon problems. The surface phonon dispersion on the hydrogen-terminated Si(111)-($1{\times}1$) surface [H:Si(111)] is the typical system and already reported experimentally [2] and theoretically [3], although the understandingis incomplete. The sample contaminated by the oxygen atoms on the surface and the calculations were also classical. In this study, firstly, we have prepared an ultra-clean H:Si(111) surface [4] and measured the surface phonon dispersion curvesusing HREELS. Secondly, we have performed first-principles density functional calculations with the projector augmented wave functionals, as implemented in VASP, using generalized gradient approximations. We used aslab of six silicon layers and both top and bottom surfaces were terminated with hydrogen atoms. Finally, we have compared with the surface phonon dispersion of deuterium-terminatedSi(111)-($1{\times}1$) surface[5] and led to our conclusions. The Si-H stretching and the bending modes are observed at 258.5 and 78.2 meV, respectively. These energies are the same as the previously reported values [2], but the energy-loss peaks at the lower energy regions are dramatically shifted. Through this combination study, we have formulated the procedure of preparing ultra-clean H:Si(111)/D:Si(111), which was confirmed by HREELS vibrational analysis. The Si surface will be utilized for further nano-physics research as well as for the materials for nano-fubrication.

• 공업화학
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• 제9권5호
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• pp.661-666
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• 1998

고시리카제올라이트 (HSZ), 거대망상수지입자(MR) 및 입상활성탄(GAC)에 의한 수용액중의 12가지 아민유도체의 평형흡착 실험 데이터와 Freundlich, Langmuir, Toth, Redlich-Peterson 식의 인자들을 각각 구하였다. 아민류의 흡착특징에 있어서는 고시리카제올라이트는 unfavourable, 입상활성탄은 favourable로 비선형이나, 거대망상수지흡착제는 선형관계의 특성을 나타내며, 변수가 2개인 Freundlich 식과 3개인 Redlich-Peterson 흡착등온식에 잘 일치하였다. HSZ, MR, GAC에 의한 아민류의 흡착능은 방향족>1급아민>2급아민 순이었으며, Freundlich상수 k와 n의 곱인 (k n)값은 HSZ와 MR 및 GAC에서 아민류의 끓는 점 $T_B$, 몰부피 $V_m$, 그리고 해리상수 $pK_a$에 비례하여 증가하였다.

• 한국환경과학회지
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• 제28권10호
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• pp.873-885
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• 2019

In this study, a load duration curve was applied to the Jangseongcheon, one of the tributaries of the Yeongsan River, to assess whether the target water quality was achieved. In addition, pollution of the water body was investigated to develop and suggest the optimal management time with respect to polluted flow sections and monthly conditions. The average flow rates of sections JS1 and JS2 were $0.25m^3/s$ and $1.08m^3/s$, respectively. The BOD and T-P for water-quality standards at JS1 were rated at II, whereas the COD and TOC were rated at III, thus indicating a fair level of water quality. By contrast, the BOD at JS2 was rated at III, the T-P at IV, and the TOC at V, indicating poor water quality in this section. The load duration curve was plotted using the actual flow data measured in eight-day intervals for eight years from 2011 to 2018 at locations JS1 and JS2 in the Jangsungcheon Basin. In an assessment using the load duration curve on whether the target water quality was met at location JS1, all of the water quality parameters (BOD, COD, TOC, T-N, T-P, and SS) satisfied the target water quality. By contrast, at location JS2, parameters COD, TOC, T-N, and T-P exceeded target values by more than 50%, indicating the target water quality was not met. The discharge loads of locations JS1 and JS2 were analyzed to identify the reasons the target water quality was exceeded. Results revealed that the land system contributed considerably. Furthermore, the discharge load of JS2 accounted for more than 80% of the load on the entire basin, excluding that of JS1. Therefore, the best method for restraining the inflow of pollutants into the stream near location JS2 must be applied to manage the water quality of the Jangsungcheon.

• 한국세라믹학회지
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• 제33권11호
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• pp.1292-1300
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• 1996

PLZT(x/70/30)의 x=7.5, 8.0, 8.5, 10.5 조성에 대하여 전계인가와 동시에 X-선 회절측정을 전계 20kV/cm에 이르기까지 수행하였다. 모든 PLZT는 입방상에 속하였다. x=7.5, 8.0, 8.5에서 PLZT는 4~8kV/cm의 낮은 전계에 이르기까지 반강유전적인 특성을 보였으며 보다 높은 전계에서는 강유전적인 특성을 나타내었다. 온도에 따른 유전상수의 측정에 따르면 x=7.5, 8.0, 8.5 조성에서 PLZT는 완화형 강유전체와 유사하였으며 50-7$0^{\circ}C$에서 확산적인 반강유전-상유전 상전이가 나타났다. 자발분극-전계(P-E) 이력곡선은 이들이 반강유전적인 특성을 가지고 있음을 보여주었다. 매우 넓은 큐리점의 분포는 이들 PLZT의 결정구조에서 La 치환에 의한 양이온 및 빈자리의 무질서도가 상당함을 시사한다. PLZT (10.5/70/30)의 전계에 따른 변형은 매우 미미하였으며 이력현상이 없는 상유전적인 특성을 보였다. 전계인가에 따른 변형률은 La 치환량이 증가함에 따라 감소하였다. PLZT(7.5/70/30)에서 110회절선의 강도는 전계인가에 민감하게 변화하여, [110] 방향에 평행한 자발분극을 가지는 분역이 전계인가로 유도된 PLZT의 강유전상에서 발달된 것처럼 여겨진다.

• 한국재료학회지
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• 제12권12호
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• pp.962-966
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• 2002

The $SrBi_2$$Nb_2$$O_{9}$ (SBN) thin films were deposited with $SrNb_2$$O_{6}$ / (SNO) and $Bi_2$$O_3$ targets by co-sputtering method. For the growth of SBN thin films, we adopted the various power ratios of two targets; the power ratios of the SNO target to $Bi_2$$O_3$ target were 100 W : 20 W, 100 W : 25 W, and 100 W : 30 W during sputtering the SBN films. We found that the electrical properties of SBN films were greatly dependent on Bi content in films. The $Bi_2$Pt and $Bi_2$$O_3$ phase as second phases occurred at the films with excess Bi content greater than 2.4, resulting in poor ferroelectric properties. The best growth condition of the SBN films was obtained at the power ratio of 100 W : 25 W for the two targets. At this condition, the crystallinity and electrical properties of the films were improved at even low annealing temperature as $700^{\circ}C$ for 1h in oxygen ambient and the Sr, Bi and Nb component in the SBN films were about 0.9, 2.4, and 1.8 respectively. From the P-E and I-V curves for the specimen, the remnant polarization value ($2P_{r}$) of the SBN films was obtained about 6 $\mu$C/c $m^2$ at 250 kV/cm and the leakage current density of this thin film was $2.45$\times$10^{-7}$ $A/cm^2$ at an applied voltage of 3 V.V.

• 대한화학회지
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• 제41권2호
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• pp.98-104
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• 1997

한국에서 전통적으로 사용되고 있는 생약제제 중 베르베린, 계피산 및 글리시리진의 정량을 위한 간단하고, 정확하고, 재현성 있는 모세관 전기이동법을 개발하였다. 이 성분들의 분리는 25$^{\circ}C$, 20 mM 인산완충액(pH 7.5)에서 실리카 캐필러리($57 cm{\times}75 {\mu}m$ i.d.)를 사용하여 수행하였다. 350 V/cm의 전기장으로 베르베린, 계피산 및 글리시리진의 동시 정량을 13분내에 할 수 있었다. 검정곡선은 베르베린에 대해서는 1~100 ${\mu}g/mL$, 계피산은 0.3~100 ${\mu}g/mL$, 글리시리진은 2.5~100 ${\mu}g/mL$의 농도 범위 안에서 좋은 직선성을 보여 주었다. 이 성분들에 대한 상대 표준편차(n=5)의 범위는 0.96∼2.35%이었다. 베르베린, 계피산 및 글리시리진에 대한 검출한계(S/N=3)는 각각 0.5, 0.1 및 2.0 ${\mu}g/mL$이었다. 이론단수는 181,000(베르베린), 88,000(계피산) 및 169,000(글리시리진)이었다. HPLC에서는 3,100~4,800이었다.

• 분석과학
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• 제20권4호
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• pp.347-354
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• 2007

본 연구에서는 축산 식품으로 소고기, 돼지고기, 닭고기를 선택하고, 수산 식품으로는 광어와 뱀장어를 선택하여 축 수산 식품 중에 잔류하는 노보비오신의 신속하고 간단한 고속액체크로마토그래피(HPLC) 분석법을 확립하였다. 각 대상 조직시료 일정량에 메탄올을 가하여 균질화한 후, 헥산 용매를 가하여 분석에 방해가 되는 지용성 불순물을 추출 제거하였다. 남은 액을 질소 기류 하에서 완전 건고하고, 여기에 이동상을 가하여 재분산한 후, $0.45{\mu}m$ syringe filter로 여과하고, 이 중 $20{\mu}L$를 HPLC에 주입하였다. HPLC 칼럼으로 phenyl hexyl 칼럼($4.6{\times}150mm$, $5{\mu}m$)을 사용하였고, 이동상으로는 아세토니트릴과 10 mM 인산수소나트륨(monobasic sodium phosphate, pH 2.5)의 혼액(50/50, v/v)을 사용하였으며, 유속은 1.0 mL/min, UV 검출 파장은 254 nm이었다. 각 대상 조직시료에 $0.5{\sim}5{\mu}g/g$의 농도 범위로 표준품을 가하고 검량선을 작성한 결과, 상관계수($r^2$)는 모든 조직 시료에서 CODEX 기준에 적합한 직선성($r^2$ > 0.95)을 보였으며, 정량한계는 $0.5{\mu}g/g$이었다. 각 조직별 평균 회수율은 소 등심 시료가 99.8%, 돼지 삼겹살 시료가 102.4%, 닭 가슴살 시료가 91.0%, 광어 살코기 시료가 104.0%, 뱀장어 살코기 시료가 93.0 %이었다. CODEX 기준을 참조하여 분석법에 대한 검증을 실시한 결과, 양호한 직선성, 정밀성, 정확성 및 회수율을 얻었다.