• 제목/요약/키워드: peak-shifting

검색결과 67건 처리시간 0.023초

장군광산과 동남광산에서 산출되는 부서라이트의 광물학적 특성 (Mineralogical Characterization of Buserite from the Janggun and Dongnam Mines, Korea)

  • 최헌수;김수진;김정진
    • 한국광물학회지
    • /
    • 제18권4호통권46호
    • /
    • pp.259-266
    • /
    • 2005
  • 장군광산과 동남광산에서 산출되는 부서라이트에 대한 광물학적 특성을 연구하기 위하여 X-선 회절분석, 전자현미분석, 열분석 실험을 실시하였다. 장군 광산과 동남 광산에서의 부서라이트는 망간탄산염광상의 표성 산화 작용에 의해 형성된 산화망간 광석 내에 란시아이트와 함께 산출된다. 전자현미분석결과 장군광산 부서라이트의 화학 조성은 ($Ca_{0.78}Mg_{0.64}Mn^{2+}_{0.45})Mn^{4+}_{8.03}O_{18}\cdot13.2H_{2}O$이며 동남광산에서 산출되는 부서라이트는 ($Zn_{0.81}Ca_{0.77}Mg_{0.26}Mn^{4+}_{8.00}O_{18}\cdot10.9H_{2}O$이다. 장군광산의 부서라이트의 저면 격자 간격은 $40^{\circ}C$에서 $9.86\;{\AA}$이며, $90^{\circ}C$에서는 $7.60\;{\AA}$로 온도가 상승함에 따라 점진적으로 감소한다. 그러나 동남광산에서 $40^{\circ}C$부터 $90^{\circ}C$까지의 온도가 변화함에 따라 점진적인 회절선의 이동은 나타나지 않고 $9.67\;{\AA}$의 회절선의 강도는 감소하고 $7.53\;{\AA}$의 회절강도는 증가하는 경향을 보여준다.

O-Ethyl S-methyl ethylphosphonothioate의 대사(代謝) 주생성물(主生成物인) O-ethyl ethylphosphonic acid의 $^{31}P-NMR$ chemical shift 에 대한 pH 및 용매 효과 (($^{31}P-NMR$ chemical shift variation of O-ethyl ethylphosphonic acid with change of pH's and solvents in metabolic and chemical oxidation of O-ethyl S-methyl ethyphosphonothioate)

  • 허장현;한대성
    • 한국환경농학회지
    • /
    • 제12권2호
    • /
    • pp.169-175
    • /
    • 1993
  • 유기인계 화합물중 독성이 매우 강한 O-ethyl S-methyl ethylphosphonothioate (1)의 화학적, 대사적 산화생성물들에 대한 $^{31}P-NMR$ 분석에서 주된 산화 생성물인 O-ethyl ethylphosphonic acid (2)의 chemical shift가 MCPBA 반응에서 40.15ppm, MMPP 반응에서 30.98ppm, microsomal oxidation system에서 29.31ppm, 그리고 집파리 생체실험에서 29.10ppm으로 반응조건에 따라 서로 상당히 상이하게 관찰되었다. 이 산화 생성물의 $^{31}P-NMR$ spectrum 상에서의 chemical shift에 대한 용매효과는 deutero-chloroform을 사용했을때 30.70ppm, 극성 용매인 deuterium oxide를 사용했을때 40.15ppm으로 관찰되었으며, pH에 대한 효과는 pH 3, 5.6, 14에서는 30ppm을 전후하여, pH 1의 강산성 조건하에서는 47.91ppm에서 나타났다. 이는 유기산 형태의 생성물 (2)가 ionized form이 형성될수있는 조건하에서는 산소원자의 비공유전자쌍들에 의하여 인원자가 차폐되어 chemical shift가 upfield쪽으로 이동을하고, 반면 비극성과 강산성 조건하에서는 Protonated form으로 존재하여 인(燐)원자에 대한 차폐효과가 줄어들기 때문에 downfield쪽으로 이동하는 것으로 관찰되었다.

  • PDF

진동·충격음 흡수성 목질계 복합재료의 개발 -폭 넓은 감쇠곡선을 나타내는 고분자의 합성- (Development of Vibration and Impact Noise Damping Wood-Based Composites -Synthesis of the Polymer Showing a Broad Damping Peak)

  • 이현종
    • Journal of the Korean Wood Science and Technology
    • /
    • 제27권2호
    • /
    • pp.15-22
    • /
    • 1999
  • 진동 충격음 흡수성능을 지니는 샌드위치구조 목질 복합재료 제조용 폴리머는 넓은 온도범위(또는 주파수 범위)에서 높은 손실계수를 지니면서, 동시에 $5{\times}10^7\sim-10^9\;dyne/cm^2$의 탄성율을 지녀야 한다. 본실험에서는 이러한 점탄성 거동율 나타내는 고분자재료의 제조를 목적으로 에폭시 수지/아크릴 수지 상호침투망목고분자(IPNs)를 동시망목형성법으로 합성하였다. 고분자의 동적 점탄성은 Rheovibron을 사용하여 110Hz에서 측정하였으며, 복합체의 손실계수 및 동탄성 계수는 Rheovibron을 개조한 양단지지 강제 휨 진동법으로 주파수 110Hz에서 측정하였다. 동력학적 측정 결과, 손실탄성율의 최대값 온도 및 손실계수의 최대값 온도가 이동하고, 유리전이 영역이 확대되어, 이 IPNs계는 부분 상용계임을 알 수 있었다. 특히, 70/30 및 50/50 조성의 Epikote871/P(n-BMA) IPNs는 넓은 온도 범위에서 비교적 높은 손실계수 및 적당한 탄성율을 나타냈다. 또한 이를 적층한 목질 복합체는 넓은 온도 범위에서 비교적 높은 진동흡수 계수를 나타냈다.

  • PDF

위탁급식전문업체 사업체 급식소의 음식 맛 및 메뉴 관련 세부 개선 속성의 규명을 위한 탐색적 사례연구 (Exploratory Case Study for Identifying Detail Attributes on the Food Taste & the Menu in Office Foodservice of Contract Foodservice Management Company)

  • 박옥진;박문경;양일선;이민준
    • 대한영양사협회학술지
    • /
    • 제10권4호
    • /
    • pp.467-475
    • /
    • 2004
  • The purposes of this exploratory study were to a) verify the first image remember percentage about foodservice and the desire to eat, b) identify detail attributes on the 'food taste' and 'menu variety', the most important problem of the foodservice, c) decide the ranking for improvement of the identified detail attributes, and d) applicate from customer feedback to foodservice operation in the B&I(business & industry) foodservice. For the more reliable result, customer opinion was collected by qualitative research methodology, such as open-ended questionnaire and in-depth interview. The result was followed as : the firstly, the operation circumstance was total 6,700 meal number a day through in-depth interview and 3 types of meal was served. The secondly, the average usage a week was the 7.4 times(B foodservice(B1F)) and the 1.8 times(A foodservice(3F)), respectively. Using reasons of foodservice were 'broad extent', 'menu type', 'shifting convenience' and etc on B foodservice(B1F) and 'menu type', 'clean space' and etc on A foodservice(3F), but the disadvantages of both foodservice were 'complication on peak time', 'the decline of food taste', and 'the absence of menu variety'. 'The decline of food taste' and 'the absence of menu variety' were pointed out the problem asked immediate improvement. The thirdly, it was examined that the first remember about foodservice were 'menu type' and 'foodservice environment' on A foodservice(3F) and 'foodservice environment(atmosphere)' on B foodservice(B1F). The last result, the detail attributes about food taste were ranked respectively 'a salt taste', 'balance of 5 taste at a meal', 'taste of food characteristic' and the unsatisfaction attributes about menu variety were ranked respectively 'serving frequently a same menu', 'the absence of various taste', 'using frequently a same cooking preparation'.

  • PDF

High-k ZrO2 Enhanced Localized Surface Plasmon Resonance for Application to Thin Film Silicon Solar Cells

  • Li, Hua-Min;Zang, Gang;Yang, Cheng;Lim, Yeong-Dae;Shen, Tian-Zi;Yoo, Won-Jong;Park, Young-Jun;Lim, Jong-Min
    • 한국진공학회:학술대회논문집
    • /
    • 한국진공학회 2009년도 제38회 동계학술대회 초록집
    • /
    • pp.276-276
    • /
    • 2010
  • Localized surface plasmon resonance (LSPR) has been explored recently as a promising approach to increase energy conversion efficiency in photovoltaic devices, particularly for thin film hydrogenated amorphous silicon (a-Si:H) solar cells. The LSPR is frequently excited via an electromagnetic (EM) radiation in proximate metallic nanostructures and its primary con sequences are selective photon extinction and local EM enhancement which gives rise to improved photogeneration of electron-hole (e-h) pairs, and consequently increases photocurrent. In this work, high-dielectric-constant (k) $ZrO_2$ (refractive index n=2.22, dielectric constant $\varepsilon=4.93$ at the wavelength of 550 nm) is proposed as spacing layer to enhance the LSPR for application to the thin film silicon solar cells. Compared to excitation of the LSPR using $SiO_2$ (n=1.46, $\varepsilon=2.13$ at the wavelength of 546.1 nm) spacing layer with Au nanoparticles of the radius of 45nm, that using $ZrO_2$ dielectric shows the advantages of(i) ~2.5 times greater polarizability, (ii) ~3.5 times larger scattering cross-section and ~1.5 times larger absorption cross-section, (iii) 4.5% higher transmission coefficient of the same thickness and (iv) 7.8% greater transmitted electric filed intensity at the same depth. All those results are calculated by Mie theory and Fresnel equations, and simulated by finite-difference time-domain (FDTD) calculations with proper boundary conditions. Red-shifting of the LSPR wavelength using high-k $ZrO_2$ dielectric is also observed according to location of the peak and this is consistent with the other's report. Finally, our experimental results show that variation of short-circuit current density ($J_{sc}$) of the LSPR enhanced a-Si:H solar cell by using the $ZrO_2$ spacing layer is 45.4% higher than that using the $SiO_2$ spacing layer, supporting our calculation and theory.

  • PDF

두 가지 축구 골킥 동작의 운동역학적 비교 분석 (Biomechanical Comparative Analysis of Two Goal-kick Motion in Soccer)

  • 진영완;신제민
    • 한국운동역학회지
    • /
    • 제15권1호
    • /
    • pp.29-44
    • /
    • 2005
  • The purpose of this study is to reveal the effects of two different kicks, the drop kick and the punt kick, into the kicking motion, through the kinetic comparative analysis of the kicking motion, which is conducted when one kicks a soccer goal. To grasp kinetic changing factors, which is performed by individual's each body segment, I connected kicking motions, which were analyzed by a two dimension co-ordination, into the personal computer to concrete the digits of it and smoothed by 10Hz. Using the smoothed data, I found a needed kinematical data by inputting an analytical program into the computer. The result of comparative analysis of two kicking motions can be summarized as below. 1. There was not a big difference between the time of the loading phase and the time of the swing phase, which can affect the exact impact and the angle of balls aviation direction. 2. The two kicks were not affected the timing and the velocity of the kicking leg's segment. 3. In the goal kick motion, the maximum velocity timing of the kicking leg's lower segment showed the following orders: the thigh(-0.06sec), the lower leg(-0.05sec), the foot(-0.018sec) in the drop kick, and the thigh(-0.06sec), the lower leg(-0.05sec), the foot(-0.015sec) in the punt kick. It showed that whipping motion increases the velocity of the foot at the time of impact. 4. At the time of impact, there was not a significant difference in the supporting leg's knee and ankle. When one does the punt kick, the subject spreads out his hip joint more at the time of impact. 5. When the impact performed, kicking leg's every segment was similar. Because the height of the ball is higher in the punt kick than in the drop kick, the subject has to stretch the knees more when he kicks a ball, so there is a significant affect on the angle and the distance of the ball's flying. 6. When one performs the drop kick, the stride is 0.02m shorter than the punt kick, and the ratio of height of the drop kick is 0.05 smaller than the punt kick. This difference greatly affects the center of the ball, the supporting leg's location, and the location of the center of gravity with the center of the ball at the time of impact. 7. Right before the moment of the impact, the center of gravity was located from the center of the ball, the height of the drop kick was 0.67m ratio of height was 0.37, and the height of the punt kick was 0.65m ratio of height was 0.36. The drop kick was located more to the back 0.21m ratio of height was 0.12, the punt kick was located more to the back 0.28m ratio of height was 0.16. 8. There was not a significant difference in the absolute angle of incidence and the maximum distance, but the absolute velocity of incidence showed a significant difference. This difference is caused from that whether players have the time to perform of not; the drop kick is used when the players have time to perform, and punt kick is used when the players launch a shifting attack. 9. The surface reaction force of the supporting leg had some relation with the approaching angle. Vertical reaction force (Fz) showed some differences in the two movements(p<0.05). The maximum force of the right and left surface reaction force (Fx) didn't have much differences (p<0.05), but it showed the tendency that the maximum force occurs before the peak force of the front and back surface (Fy) occurs.

Contrast Media in Abdominal Computed Tomography: Optimization of Delivery Methods

  • Joon Koo Han;Byung Ihn Choi;Ah Young Kim;Soo Jung Kim
    • Korean Journal of Radiology
    • /
    • 제2권1호
    • /
    • pp.28-36
    • /
    • 2001
  • Objective: To provide a systematic overview of the effects of various parameters on contrast enhancement within the same population, an animal experiment as well as a computer-aided simulation study was performed. Materials and Methods: In an animal experiment, single-level dynamic CT through the liver was performed at 5-second intervals just after the injection of contrast medium for 3 minutes. Combinations of three different amounts (1, 2, 3 mL/kg), concentrations (150, 200, 300 mgI/mL), and injection rates (0.5, 1, 2 mL/sec) were used. The CT number of the aorta (A), portal vein (P) and liver (L) was measured in each image, and time-attenuation curves for A, P and L were thus obtained. The degree of maximum enhancement (Imax) and time to reach peak enhancement (Tmax) of A, P and L were determined, and times to equilibrium (Teq) were analyzed. In the computed-aided simulation model, a program based on the amount, flow, and diffusion coefficient of body fluid in various compartments of the human body was designed. The input variables were the concentrations, volumes and injection rates of the contrast media used. The program generated the time-attenuation curves of A, P and L, as well as liver-to-hepatocellular carcinoma (HCC) contrast curves. On each curve, we calculated and plotted the optimal temporal window (time period above the lower threshold, which in this experiment was 10 Hounsfield units), the total area under the curve above the lower threshold, and the area within the optimal range. Results: A. Animal Experiment: At a given concentration and injection rate, an increased volume of contrast medium led to increases in Imax A, P and L. In addition, Tmax A, P, L and Teq were prolonged in parallel with increases in injection time The time-attenuation curve shifted upward and to the right. For a given volume and injection rate, an increased concentration of contrast medium increased the degree of aortic, portal and hepatic enhancement, though Tmax A, P and L remained the same. The time-attenuation curve shifted upward. For a given volume and concentration of contrast medium, changes in the injection rate had a prominent effect on aortic enhancement, and that of the portal vein and hepatic parenchyma also showed some increase, though the effect was less prominent. A increased in the rate of contrast injection led to shifting of the time enhancement curve to the left and upward. B. Computer Simulation: At a faster injection rate, there was minimal change in the degree of hepatic attenuation, though the duration of the optimal temporal window decreased. The area between 10 and 30 HU was greatest when contrast media was delivered at a rate of 2 3 mL/sec. Although the total area under the curve increased in proportion to the injection rate, most of this increase was above the upper threshould and thus the temporal window was narrow and the optimal area decreased. Conclusion: Increases in volume, concentration and injection rate all resulted in improved arterial enhancement. If cost was disregarded, increasing the injection volume was the most reliable way of obtaining good quality enhancement. The optimal way of delivering a given amount of contrast medium can be calculated using a computer-based mathematical model.

  • PDF