• Title/Summary/Keyword: NmF2

Search Result 991, Processing Time 0.032 seconds

Preparation of Porous Polyacrylonitrile Nanofibers Membrane for the MF Application (MF 적용을 위한 다공성 PAN 나노섬유막의 제조)

  • Ahn, Hyeonryun;Jang, Wongi;Tak, Taemoon;Byun, Hongsik
    • Membrane Journal
    • /
    • v.23 no.2
    • /
    • pp.112-118
    • /
    • 2013
  • Polyancrylonitrile nanofiber membrane (PAM) was prepared by using the electrospinning method with a solution of polyacrylonitrile (PAN) in DMF. The pore-diameter of PAMs and the number of PAM's layer were controlled for the microfiltration (MF) application. In addition, in order to improve the water-flux, AN-PEGMA copolymers have been synthesized via free radical polymerization with poly (ethylene glycol) methyl ether methacrylate and azobisisobutylronitrile (AIBN), and then PAN/AN-PEGMA nanofiber membranes (PAM/APM) were prepared by electrospinning with a mixture of PAN (9 wt%) and AN-PEGMA (3 wt%) in DMF (88 wt%). The prepared membranes were investigated with FT-IR and E.D.S. It was confirmed through scanning electron microscope (SEM), porometer, and porosity analysis that the porous membrane with a uniform diameter (400~600 nm) and a uniform pore characteristics (0.5~0.4 ${\mu}m$) was prepared. For the MF application, water-flux measurements were investigated and then the result was shown that the water permeability value of PAM/APMs introduced AN-PEGMA copolymers was relatively higher than that of the PVdF commercial membrane. From these results, PAN nanofiber membranes prepared by electrospinning could be utilized as a MF membrane.

유연소재 천 기반의 슈퍼캐패시터 저장체의 전기화학적 성능 향상

  • Yun, Tae-Gwang;O, Min-Seop;Hu, Liangbing;Hyeon, Seung-Min;Han, Seung-Min
    • Proceedings of the Korean Vacuum Society Conference
    • /
    • 2013.02a
    • /
    • pp.697-698
    • /
    • 2013
  • 최근에 유연한 성질을 갖는 전자기기들의 수요가 증가하면서, 그에 따라서 유연 전자기기를 뒷받침 해줄 수 있는 에너지 저장체의 유연한 성질도 중요성이 점점 부각되고 있으며 많은 연구가 진행되고 있다. 유연한 에너지 저장체의 많은 연구들이 유연한 금속 박막이나 특수 공정처리가 필요한 고분자를 이용하고 있으나, 대부분의 유연 에너지 소자들은 에너지 저장체의 성능에 비해 고온과 산 약품과 같은 환경이 필요하며, 비용과 시간이 많이 소모되고 있다. 그에 반해 섬유는 앞에서와 같이 특수 공정 처리가 따로 필요하지 않으며 상온에서도 손 쉽게 이용 가능하며, 신축성이 뛰어난 장점이 있기 때문에 효율적, 비용적으로 유연한 에너지 저장체에 유리한 소재이다. 몸에 해로운 산과 같은 약품처리의 필요도 없으며, 용매를 흡수하는 능력이 뛰어나기 때문에 용매를 이용한 도포 방법을 사용하면 다양한 물질을 폭넓게 적용 가능하다. 그리고 적용 분야에 맞춰서 섬유의 종류를 조절하면 다양한 성질을 갖는 천 기반의 에너지 저장체가 형성되며, 면 섬유가 수소 결합과 높은 반데르 발스 결합에 의해 탄소나노튜브와 결합하여 높은 에너지 밀도를 갖는 에너지 저장체를 형성하는 것을 분석한 논문들도 보고되고 있다. 면 섬유의 특수한 성질을 이용하여 에너지 저장체를 제작하고 이를 확인하기 위해서 일반 합성 섬유인 polyester와 면 섬유를 비교 제작하였으며, 용매의 형태로 손쉽게 도포 가능한 물질은 탄소 계열의 활물질들이며, 탄소 나노 튜브나 그래핀 등이 분산된 용액을 이용해 천에 도포 가능하다. 탄소 계열의 활물질들은 대표적인 슈퍼캐패시터 물질이며, 천에 도포를 함으로써 천 기반의 슈퍼캐패시터를 제작하였다. 일반 합성 섬유 polyester와 CNT를 결합한 형태의 전극은 최대 에너지 축전 용량(Maximum specific capacitance)이 53.6 F/g으로 나타났으며, 면 섬유와 CNT를 결합한 형태의 전극은 최대 에너지 축전 용량이 122.1 F/g으로 나타났다. 따라서 면 섬유에서 높은 에너지 저장 능력을 보이는 것을 실험적으로 확인하였으며, 에너지 저장 능력이 뛰어난 면 섬유를 다음 전극 디자인에서도 일률적으로 적용하였다. 슈도캐패시터의 대표적 물질인 금속 산화물인 망간 산화물(MnO2)을 3전극 도금 시스템을 이용하여 에너지 축전 용량과 에너지 밀도를 올리는 전극을 제작하였다. 특히 망간 산화물의 형태는 표면적을 극대화하기 위해서 평균 지름은 200~300 nm 정도 되는 나노 입자의 형태로 제작하였다. 그 결과, 확연하게 에너지 축전 용량이 향상되었으며, 최대 에너지 축전 용량은 282.0 F/g, 에너지전력 밀도는 14.2 Wh/kg으로 나타나서 금속 산화물의 형태가 주는 효과를 확인할 수 있었다. 하지만 나노 입자의 형태로 제작된 금속 산화물은 문제점이 발생하였다. 금속 산화물의 전기 전도성이 매우 낮기 때문에, 전기 전도성에 비례해서 전력 밀도의 값이 표현되는데, 전기 전도성이 급격히 감소하기 때문에 전력 밀도도 급격한 감소가 나타난다. 다음과 같이 전기 전도성 물질을 첨가하는 방법은 추가의 공정이 필요한 단점이 있지만 오직 기계적인 인장응력만을 가해서 에너지 밀도와 전력 밀도를 증가시키는 전극을 제작하였다. 인장응력을 섬유 기반의 전극에 가했을 시에 가닥들간의 접촉 증가와 CNT가 정렬되면서 특정 변형률(strain) 이전에서는 전기 전도성이 최대 50% 이상 증가하는 것을 확인할 수 있었으며, 선행 연구에서 보고되었다. 이를 이용해서 전기 전도성과 직결되는 전력 밀도의 양도 증가시키고 에너지 밀도의 증가 여부까지 확인한 결과 인장을 가하기 전 면 섬유의 전력 밀도와 에너지 밀도는 6.4 kW/kg and 6.1 Wh/kg으로 나타났으나 30% 변형 인장 후에는11.4 kW/kg과 7.1 Wh/kg으로 나타났다. 그리고 망간 산화물을 첨가한 전극 역시 4.9 kW/kg과 14.2 Wh/kg으로 나타났었으나 인장 이후 전력 밀도는 14.2 kW/kg, 에너지 밀도는 17.6 Wh/kg으로 확연하게 증가한 것을 확인하였다.

  • PDF

Radiation Hardness Characteristics of Fiber Bragg Gratings on the High Temperature Annealing Condition (고온 어닐링 조건에 따른 FBG 센서의 내방사선 특성)

  • Kim, Jong-Yeol;Lee, Nam-Ho;Jung, Hyun-Kyu
    • Journal of the Korea Institute of Information and Communication Engineering
    • /
    • v.20 no.10
    • /
    • pp.1980-1986
    • /
    • 2016
  • In this study, we studied the gamma-radiation effect of fiber Bragg gratings (FBGs) on the high temperature annealing condition after grating inscription using a KrF UV laser (248 nm). The FBGs were fabricated in a different annealing temperature using the same commercial Ge-doped silica core fiber (SMF-28e) and exposed to gamma-radiation up to a dose of 31 kGy at the dose rate of 115 Gy/min. The high temperature annealing procedure for grating stabilization was applied to change the radiation sensitivity of the FBGs. According to the experimental data and analysis results, the gratings that were stabilized at different temperatures at 100, 150 and $200^{\circ}C$ have clearly shown that exposure to higher temperatures increases their radiation sensitivity. The radiation-induced Bragg wavelength shift (BWS) was shown a difference of up to about a factor of two depending on the annealing temperature conditions of the gratings.

Er(III)-chelated Prototype Complexes Based on Benzoate and Pentafluorobenzoate Ligands : Synthesis and Key Parameters for Near IR Emission Enhancement

  • Roh, Soo-Gyun;Oh, Jae-Buem;Nah, Min-Kook;Baek, Nam-Seob;Lee, Young-Il;Kim, Hwan-Kyu
    • Bulletin of the Korean Chemical Society
    • /
    • v.25 no.10
    • /
    • pp.1503-1507
    • /
    • 2004
  • New synthetic methodology of the saturated and unsaturated Er(III)-chelated prototype complexes based on benzoate and pentafluorobenzoate ligands was developed through ligand-exchange reaction. The saturated 8-coordinated Er(III) complexes exhibit stronger near-IR emission than those of the unsaturated 6-coordinated Er(III) complexes, obtained from the direct photoexcitation of Er ions with 488 nm. Three $H_2O$ molecules coordinated in the unsaturated 6-coordinated complexes seriously quenched the near IR emission by the harmonic vibration relaxation decay of O-H bonds. Also, the stronger emission of the Er(III) complexes was obtained by the indirect photoexcitation of ligands than by the direct photoexcitation of the Er(III) ions, due to the energy transfer between the excited ligand and the erbium ion. Furthermore, the saturated Er(III)-chelated complex with C-F bonds shows much stronger near IR emission than that of the saturated Er(III)-chelated complex with C-H bonds. It is attributed to the influence of C-F bonds on near IR emission.

Effect of the Crystalline Phase of Al2O3 Nanoparticle on the Luminescence Properties of YAGG:Ce3+ Phosphor under Vacuum UV Excitation (진공자외선 여기에 의한 YAGG:Ce3+ 형광체의 광발광 특성에 미치는 Al2O3 나노입자 원료의 결정상의 영향)

  • Wu, Mi-Hye;Choi, Sung-Ho;Jung, Ha-Kyun
    • Korean Journal of Materials Research
    • /
    • v.22 no.4
    • /
    • pp.195-201
    • /
    • 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.

EFFECTS OF UV-B RADIATION ON GROWTH AND DEVELOPMENT OF RICE CULTIVARS (ORYZA SATIVA L.).

  • T.Kumagai;Kang, H.S.;J.Hidema;T.Sato
    • Proceedings of the Botanical Society of Korea Conference
    • /
    • 1994.09a
    • /
    • pp.29-39
    • /
    • 1994
  • Serious issues about the changes in the environmental conditions on earth associated with human activities have arisen, and the interest in these problems has increased. It is urgent to determine how the expansion of terrestrial UV-B radiation due to the stratospheric ozone depletion influences living matters. In this connection, we have been investigating the effects of UV-B radiation on the growth of rice cultivars (Oryza sativa L.). We report here some physiological and genetic aspects of resistance to inhibitory effects of UV-B radiation on growth of rice cultivars as described below. Elevated UV radiation containing large amount of UV-B and a small amount of UV-C inhibited the development of plant height, the photosynthetic rate and the chlorophyll content in rice plants in a phytotron. Similar results were obtained in experiments, in which elevated UV-V radiation. Similar results were obtained in experiments, in which elevated UV-B radiation (transmission down to 290 nm) was applied instead of UV-B radiation containing a small amount of UV-C. The inhibitory effects of UV radiation was alleviated by the elevated CO2 atmospheric environment or by the exposure to the high irradiance visible radiation. The latter suggested the possibility that the resistance to the effects of UV radiation was either due to a lower sensitivity to UV radiation or to a greater ability to recover from the injury caused by UV radiation through the exposure to visible radiation. The examination of cultivar differences in the resistance to UV radiation-caused injuries among 198 rice cultivars belonging to 5 Asian rice ecotypes (aus, aman, boro, bulu and tjeleh) from the Bengal region and Indonesia and to Japanese lowland and upland rice groups showed the following: Various cultivars having different sensitivities to the effects of UV radiation were involved in the same ecotype and the same group, and that the Japanese lowland rice group and the boro ecotype were more resistant. Among Japanese lowland rice cultivars, Sasanishiki (one of the leading varieties in Japan) exhibited more resistance to UV rakiation, while Norin 1 showed less resistance, although these two cultivars are closely related. It was thus indicated that the resistance to the inhibitory effects of UV radiation of rice cultivars is not simply due to the difference in the geographical situation where rice cultuvars are cultivated. Form the genetic analysis of resistance to the inhibitory effects of UV radiation on growth of rice using F2 plants generated by reciprocally crossing Sasanishiki and Norin 1 and F3 lines generated by self-fertilizing F2 plants, it was evident that the resistance to the inhibitory of elebated UV radiation in these rice plants was controlled by recessive polygenes.

  • PDF

Electron microscopic studies on Flavobacterium branchiophila in experimentally induced gill disease of rainbow trout (세균성(細菌性) 아가미병(病)에 실험적(實驗的)으로 감염(感染)된 무지개송어에 있어서 Flavobacterium branchiophila에 대한 전자현미경학적(電子顯微鏡學的) 연구(硏究))

  • Heo, Gang-joon
    • Korean Journal of Veterinary Research
    • /
    • v.32 no.3
    • /
    • pp.381-387
    • /
    • 1992
  • Gill epithelia of normal rainbow trout fingerlings and abnormal ones suffering bacterial gill disease by experimental infection were examined by transmitting electron microscopy (TEM) and scanning electron microscopy (SEM). TEM observations revealed that Flavobacterium branchiophila consisted of slender rods measuring 0.5 by 5 to $8{\mu}m$, and they had which were long, thin, flexible filaments measuring approximately 4 nm by $1{\mu}m$, and packed together to organize into bundles. Morphological alterations of the diseased epithelia started at hypertrophy of the lamellar epithelium. F branchiophila attached to the gill surface of infected fish through pili with a regular distance, and did not invade into gill tissue. In SEM observations, normal surface ultrastructure of epithelial cell in the outermost layer were characterized by a typical labyrinth-like structure branching and anastomosing microridges on the cell surface. Hyperplastic lesions in experimentally infected gill were most serious at near the tips. Each filament exhibited a club-like, and fusion between the filaments was sometimes observed at their tips. On the surface of gill filaments, thread-like bacterial cells attached and were entangled. The bacterial cells almost covered the surface. After immersion in 5 % NaCl, the cell of F branchiophila, however, appeared to be indeterminate shape.

  • PDF

The Evidence for Pepsin-Catalyzed Transpeptidation (펩신촉매에 의한 Transpeptide의 생성)

  • 조용권
    • Journal of Life Science
    • /
    • v.8 no.4
    • /
    • pp.410-415
    • /
    • 1998
  • Procine pepsin hydrolysis of hexapeptide L-S-pNF-Nle-A-OMe in the presence of dipeptide L-L generates a new peak on HPLC analysis of reaction mixtures that is not seen when enzyme is incubated with either peptide alone. The peaks can be detected spectroscopically at either 214 or 254 nm, the latter consistent with a new peptide containing the p-nitro-F residue. The data suggest acyl transpeptidation between E(L-S-pNF) and L-L to form L-S-pNF-L-L. Consistent with this inference are (1) the ability of L-L-NH$_{2}$ and inability of Boc-L-L to undergo a similar transpeptidation reaction, and (2) the data from electrospray mass spectrum. This synthesis requires that Nle-A-L-OMe be released before L-S-pNF, an order opposite to that proposed on the basis of product inhibition kinetics. Consistent with this inference are reciprocal solvent isotope effects ; normal isotope effects of 1.736$\pm$0.121 on the formation of Nle-A-L-OMe and 2.281$\pm$0.184 in the formation of L-S-pNF, coupled to an inverse isotope effects of 0.576$\pm$0.045 on the formation of L-S-pNF-L-L. Because transpeptidation precedes faster in D$_{2}$O, the isotopically-sensitive step must occur after release of Nle-A-L-OMe. Isotopically-enhanced transpeptidation is consistent with the Uni-Bi iso memchanism postulated on the basis of an isotope effects on Vmax but not on Vmax/Km$^{1)}$ and confirmed by isotope effects on the onset of inhibition by pepstatin$^{2)}$.

  • PDF

Influence of AZO Thin Films Grown on Transparent Plastic Substrate with Various Working Pressure and $O_2$ Gas Flow Rate (공정 압력과 산소 가스비가 투명 플라스틱 기판에 성장시킨 AZO 박막에 미치는 영향)

  • Lee, Jun-Pyo;Kang, Seong-Jun;Joung, Yang-Hee;Yoon, Yung-Sup
    • Journal of the Institute of Electronics Engineers of Korea SD
    • /
    • v.47 no.2
    • /
    • pp.15-20
    • /
    • 2010
  • In this study, AZO (Al: 3 wt%) thin films have been prepared on PES Plastic substrates at various working pressure (5~20 mTorr), $O_2$ gas flow rate(0~3%) and the fixed substrate temperature of 200 f by using the RF magnetron sputtering and their optical and electrical properties have been studied. The XRD measurement shows that AZO thin films exhibit c-axis preferred orientation. From the results of AFM measurements, it is known that the lowest surface roughness (3.49 nm) is obtained for the AZO thin film fabricated at 5 mTorr of working pressure and 3% of $O_2$ gas flow rate. The optical transmittance of AZO thin films is measured as 80% in the visible region. We observe that the energy band gap of AZO thin films increases with decreasing the working pressure and the $O_2$ gas flow rate. This phenomenon is due to the Burstein-Moss effect. Hall measurement shows that the maximum carrier concentration ($2.63\;{\times}\;10^{20}\;cm^{-3}$) and the minimum resistivity ($4.35\;{\times}\;10^{-3}\;{\Omega}cm$) are obtained for the AZO thin film fabricated at 5mTorr of working pressure and 0% of $O_2$ gas flow rate.

Extraction of Freeze Dried Young Antler Residue by Proteases and HCl (단백질 가수분해 효소 및 염산에 의한 녹용 각질의 추출)

  • 안용근
    • The Korean Journal of Food And Nutrition
    • /
    • v.16 no.4
    • /
    • pp.388-396
    • /
    • 2003
  • The freeze dried young antler residue was extracted by proteases and hydrochloric acid(HCl). The young antler was extracted by water at 50$^{\circ}C$ and the residue was reacted by proteases for 5 hours at 50$^{\circ}C$. The extraction rate of its residue was 32.8%(absorbance 3.61 at 280nm) of bacteria protease, 23.8%(absorbance 0.69) of papain, and 31.2% (absorbance 2.96) of pepsin. The young antler was extracted by boiling water and the residue was reacted by proteases for 5 hours at 50$^{\circ}C$. The extraction rate of its residue was 45.0%(absorbance 3.61) of bacteria protease, 30.4%(absorbance 0.33) of papain, and 51.2% (absorbance 2.77) of pepsin. The result of HPLC analysis reveals that in 50$^{\circ}C$ water extract and boiling water extract, all high molecular peak was reduced under MW 1,000 by proteases. The result from the extract of young antler residue reacted by HCl for 5 hours at 50$^{\circ}C$ shows that its extraction rate was 45% (absorbance 0.78) in concentration of 0.1N HCl, 61% (absorbance 1.82) in 0.2N, 81% (absorbance 2.29) in 0.4N, and 82.0% (absorbance 3.28) in 2.0N. The result of HPLC analysis also reveals that in the extract by 0.8N HCl, the peak of about MW 70,000 accounted for 78% in total. Protein content of the extract by 0.8N HCl was 8.2%, and content of amino acid was 81.6%, ash was 1.3%, and mineral contents were 0.1 % of Ca, 2.3% of P, 0.8 % of Mg, 3.4% of Na, 0.002% of F by dry base.