• 제목/요약/키워드: M2 polarization

검색결과 643건 처리시간 0.026초

질소 이온이 주입된 STS 316L 스테인리스 강에서의 상변화와 집합조직이 내식성에 미치는 영향 (Influence of Phase Evolution and Texture on the Corrosion Resistance of Nitrogen Ion Implanted STS 316L Stainless Steel)

  • 전신희;공영민
    • 한국재료학회지
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    • 제25권6호
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    • pp.293-299
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    • 2015
  • In this study, nitrogen ions were implanted into STS 316L austenitic stainless steel by plasma immersion ion implantation (PIII) to improve the corrosion resistance. The implantation of nitrogen ions was performed with bias voltages of -5, -10, -15, and -20 kV. The implantation time was 240 min and the implantation temperature was kept at room temperature. With nitrogen implantation, the corrosion resistance of 316 L improved in comparison with that of the bare steel. The effects of nitrogen ion implantation on the electrochemical corrosion behavior of the specimen were investigated by the potentiodynamic polarization test, which was conducted in a 0.5 M $H_2SO_4$ solution at $70^{\circ}C$. The phase evolution and texture caused by the nitrogen ion implantation were analyzed by an X-ray diffractometer. It was demonstrated that the samples implanted at lower bias voltages, i.e., 5 kV and 10 kV, showed an expanded austenite phase, ${\gamma}_N$, and strong (111) texture morphology. Those samples exhibited a better corrosion resistance.

마이크로캡슐화한 축전지용 수소저장합금 전극의 충·방전 특성 (Charge and Discharge Characteristics of Microencapsulated Hydrogen Storage Alloy Electrodes for Secondary Batteries)

  • 최성수;최병진;예병준;김대룡
    • 한국수소및신에너지학회논문집
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    • 제3권2호
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    • pp.45-54
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    • 1992
  • An applicability microencapsulation, using electroless copper plating, of hydrogen storage alloy powder as an anode material for nickel-hydrogen secondary batteries was investigated. Alloys employed were $LaNi_{4.7}Al_{0.3}$ and $MmNi_{4.5}Al_{0.5}$(Mm=mischmetal) which have an appropriate equilibrium pressure and capacity. The microencapsulation of the alloy powder was found to accelerate initial activation of electrodes and to increase capacity which is about 285mAh/g for $LaNi_{4.7}Al_{0.3}$. In addition, other charge and discharge characteristics, such as polarization and flatness of charge and discharge potential, were improved due to the role of copper layer as a microcurrent collector and an oxidation barrier of the alloy powder. $MmNi_{4.5}Al_{0.5}$ alloy showed lower capacity than $LaNi_{4.7}Al_{0.3}$ because of higher equilibrium pressure. Cyclic characteristics of both alloys were somewhat poor because of mainly shedding and partial oxidation of alloy powder during the cycling. However, it was considered that the microencapsulation method is effective to improve the performances of the hydrogen storage alloy electrodes.

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Solution 코팅횟수에 따른 PZT(80/20)후막의 특성 (Properties of PZT(80/20) Thick Films with the Variation of the Number of Solution Coatings)

  • 박상만;이성갑;이영희;배선기
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2006년도 제37회 하계학술대회 논문집 C
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    • pp.1418-1419
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    • 2006
  • PZT(80/20) powder was prepared by a sol-gel method and PZT thick films were fabricated by the screen-printing method on the alumina substrates. The coating and drying procedure was repeated 4 times. And then the PZT(20/80) precursor solution was spin-coated on the multilayered thick films. A concentration of a coating solution was 0.5 mol/L and the number of coating was repeated from 0 to 6. The porosity of the thick films was decreased with increasing the number of coatings and the PZT thick films with 6-times coated showed the dense microstructure and thickness of about 60-65 ${\mu}m$. All PZT thick films showed the typical XRD patterns of a typical perovskite polycrystalline structure. The relative dielectric constant and the dielectric loss of the PZT-6 thick film were 275 and 3.5, respectively. And the PZT-6 film shows the remanent polarization of 22.1 $C/cm^2$ and coercive field of 13.7 kV/cm.

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270-W 15-kHz MOPA System Based on Side-pumped Rod-type Nd:YAG Gain Modules

  • Cha, Yong-Ho;Yang, Myoung-Yerl;Ko, Kwang-Hoon;Lim, Gwon;Han, Jae-Min;Park, Hyun-Min;Kim, Taek-Soo;Roh, Si-Pyo;Jeong, Do-Young
    • Journal of the Optical Society of Korea
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    • 제12권4호
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    • pp.298-302
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    • 2008
  • We have developed a 270-W 15-kHz MOPA system based on side-pumped rod-type Nd:YAG gain modules. The master oscillator is a 3-W 15-kHz $TEM_{00}$ $Nd:YVO_4$ laser with a pulse duration of 30 ns. To preserve the high beam quality during the amplification, we use image relay and polarization rotation which can simultaneously compensate for thermal lensing and thermal birefringence generated in the rod-type gain modules. After the amplification to 270 W with six rod-type gain modules, the beam quality factor ($M^2$) of the amplified laser beam is 5-10, and the pulse duration is maintained at 30 ns.

Use of Capparis decidua Extract as a Green Inhibitor for Pure Aluminum Corrosion in Acidic Media

  • Al-Bataineh, Nezar;Al-Qudah, Mahmoud A.;Abu-Orabi, Sultan;Bataineh, Tareq;Hamaideh, Rasha S.;Al-Momani, Idrees F.;Hijazi, Ahmed K.
    • Corrosion Science and Technology
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    • 제21권1호
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    • pp.9-20
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    • 2022
  • The aim of this paper is to study corrosion inhibition of Aluminum with Capparis decidua extract. The study was performed in a 1.0 M solution of hydrochloric acid (HCl) and was monitored both by measuring mass loss and by using electrochemical and polarization methods. A scanning electron microscopy (SEM) technique was also applied for surface morphology analysis. The results revealed high inhibition efficiency of Capparis decidua extract. Our data also determined that efficiency is governed by temperature and concentration of extract. Optimum (88.2%) inhibitor efficiency was found with maximum extract concentration at 45 o C. The results also showed a slight diminution of aluminum dissolution when the temperature is low. Based on the Langmuir adsorption model, Capparis decidua adsorption on the aluminum surface shows a high regression coefficient value. From the results, the activation enthalpy (∆H#) and activation entropy (∆S#) were estimated and discussed. In conclusion, the study clearly shows that Capparis decidua extract acted against aluminum corrosion in acidic media by forming a protective film on top of the aluminum surface.

Enhance photoelectric efficiency of PV by optical-thermal management of nanofilm reflector

  • Liang, Huaxu;Wang, Baisheng;Su, Ronghua;Zhang, Ao;Wang, Fuqiang;Shuai, Yong
    • Advances in nano research
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    • 제13권5호
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    • pp.475-485
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    • 2022
  • Crystalline silicon photovoltaic cells have advantages of zero pollution, large scale and high reliability. A major challenge is that sunlight wavelength with photon energy lower than semiconductor band gap is converted into heat and increase its temperature and reduce its conversion efficiency. Traditional cooling PV method is using water flowing below the modules to cool down PV temperature. In this paper, the idea is proposed to reduce the temperature of the module and improve the energy conversion efficiency of the module through the modulation of the solar spectrum. A spectrally selective nanofilm reflector located directly on the surface of PV is designed, which can reflect sunlight wavelength with low photon energy, and even enhance absorption of sunlight wavelength with high photon energy. The results indicate that nanofilm reflector can reduce spectral reflectivity integral from 9.0% to 6.93% in 400~1100 nm wavelength range, and improve spectral reflectivity integral from 23.1% to 78.34% in long wavelength range. The nanofilm reflector can reduce temperature of PV by 4.51℃ and relatively improved energy conversion efficiency of PV by 1.25% when solar irradiance is 1000 W/m2. Furthermore, the nanofilm reflector is insensitive in sunlight's angle and polarization state, and be suitable for high irradiance environment.

이산화탄소 분리용 세라믹 중공사 접촉막 모듈 기술 개발 (Development of Ceramic Hollow Fiber Membrane Contactor Modules for Carbon Dioxide Separation)

  • 이홍주;채진웅;박정훈
    • 한국기후변화학회지
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    • 제7권3호
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    • pp.249-256
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    • 2016
  • Porous $Al_2O_3$ hollow fiber membranes were successfully prepared by dry-wet spinning/sintering method. The SEM image shows that the $Al_2O_3$ hollow fiber membrane consists mostly of sponge pore structure. The contact angle and the breakthrough pressure were $126^{\circ}$ and 1.91 bar, respectively. This results indicate that the $Al_2O_3$ hollow fiber membranes were successfully modified to hydrophobic surface. The hydrophobic modified $Al_2O_3$ hollow fiber membranes were assembled into a membrane contactor system to separate $CO_2$ from a model gas mixture of the flue gas at elevated gas velocity. The $CO_2$ absorption flux was enhanced when the gas velocity increased from $1{\times}10^{-3}$ to $6{\times}10^{-3}$ m/s. Whereas the $CO_2$ absorption flux was decreased with the number of hollow fiber membrane of a module because of the concentration polarization. Furthermore, we developed an lab-scale $Al_2O_3$ hollow fiber membrane contactor modules and their system (i.e., $CO_2$ absorption using the $Al_2O_3$ membrane and monoethanolamine (MEA)) that could dispose of over $0.02Nm^3/h$ mixture gas (15% $CO_2$) with the removal efficiency higher than 95%. The results can be useful in a field of the membrane contactor for $CO_2$ separation, helping to design and extend a equipment.

솔-젤법 및 급속열처리에 의한 $Sr_{0.9}4$Bi_{2.1}$$Ta_2$$O_9$ 박막의 저온형성에 관한 연구 (Study on Low Temperature Formation of Ferroelectric $Sr_{0.9}4$Bi_{2.1}$$Ta_2$$O_9$ Thin Films by Sol-Gel Process and Rapid Thermal Annealing)

  • 장현호;송석표;김병호
    • 한국전기전자재료학회논문지
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    • 제13권4호
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    • pp.312-317
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    • 2000
  • Ferroelectric S $r_{0.9}$/B $i_{2.1}$/T $a_{2}$/ $O_{9}$ solutions were synthesized using sol-gel process in which strontinum ethoxide bismuth ethoxide trantalum ethoxide were used a s startring materials. SBT thin films were coated on Pt/Ti/ $SiO_2$/Si substrates by spin-coating. rapid thermal annealing (RTA) was used to promote crystallization. Thin films were annealed at $700^{\circ}C$ for 1 hr in an oxygen atmosphere. This temperature is about 10$0^{\circ}C$ lower than the usual annealing temperature for SBT thin films. Pt top-electrode was deposited by sputtering and thin films were post-annealed at $700^{\circ}C$ for 30 min. to enhance electrical properties. As the RTA temperature increased the higher 2 $P_{r}$ values were obtained. At RTA temperature being 78$0^{\circ}C$ remanent polarization of S $r_{0.9}$/B $i_{2.1}$/T $a_{2}$/ $O_{9}$ thin film was 7.73 $\mu$C/cm $_2$ and the leakage current density was 1.14$\times$10$^{-7}$ A/c $m^2$ at 3 V. As RTA temperature increased the breakdown voltage was decreased. It is considered that the low-field breadown is caused by the rough surface of SBT films and forming bismuth metal in SBT thin films.films.lms.

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2축 회전판형 UF 모듈의 Oil Emulsion 분리 특성 연구 (Study of Two-shaft Rotary Disc UF Module for the Separation of Oil Emulsion)

  • 김제우;노수홍
    • 멤브레인
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    • 제6권4호
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    • pp.219-226
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    • 1996
  • 본 연구에서는 2축 회전판형 한외여과막 모듈의 순수투과율 예측모델과 1% 절삭유의 분리특성 및 투과율 예측모델을 유도하였다. 2축 RDM은 한외여과막(UOP사, 직경 0.22m)을 씌운 같은 크기의 회전판막 20개를 장착한 후 막간격과 각속도($\omega$)에 따른 분리특성을 조사하였다. 2축 RDM의 순수 투과율은 각속도가 41.89rad/s에서 9.95% 감소하여서 1축 RDM의 감소율 3.01%보다 높았다. 2축 RDM은 회전판막이 겹친 부분에서 난류의 발생으로 미끄럼 흐름에 의한 압력 강하는 $(2.5{\omega}r)^{2}$에 비례하였다. 회전판막 간격이 3mm인 $J/J_{o}$(절삭유의 투과율/순수 투과율)는 각속도가 31.42rad/s에서 2.62rad/s로 감소할 때 0.64에서 0.31로 감소하였고 간격이 7mm 일 때의 $J/J_{o}$는 0.64에서 0.27의 감소하여 비슷한 경향을 보였다. 1축 RDM에 사용된 투과율 예측모델식을 변형하여 유도된 2축 RDM의 모델식은 실험결과와 잘 일치하였다.

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고체전해질형 연료전지용 Pr1-xMxMnO3(M-Ca, Sr) 산소극 재료의 특성 (Characteristics of Pr1-xMxMnO3(M=Ca, Sr) as a Cathode Material of Solid Oxide Fuel Cell)

  • 임형렬;정순기;이주성
    • 공업화학
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    • 제7권6호
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    • pp.1125-1131
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    • 1996
  • 고체전해질형 연료전지의 산소극 재료로서 페롭스카이트 구조를 갖는 $PrMnO_3$에 Ca과 Sr을 도핑시켜 도핑량에 따른 전기전도도, 산소환원과전압 등의 전기화학적 특성과, 전해질인 yttria stabilized zirconia와의 반응성 그리고 열 팽창률 등을 살펴 보았다. 합성된 페롭스카이트 분말은 대략 $2{\sim}5{\mu}m$의 평균입자 크기를 나타내었는데 이때 입자크기 및 비표면적은 도핑량과 무관하였다. Ca이 30mo1% 도핑되었을 때 전기전도도는 $1000^{\circ}C$에서 $266S{\cdot}cm^{-1}$로 가장 높은 값을 나타내었고, 분극을 통해 살펴 본 산소환원특성도 Ca이 30mol% 도핑되었을 때 가장 우수한 특성을 나타내었다. 전극물질과 전해질인 YSZ를 $1200^{\circ}C$에서 100시간 동안 반응시킨 결과 $PrMnO_3$에 Sr을 도핑시켰을 때보다 Ca을 도핑시킨 것이 반응성이 훨씬 약한 결과를 나타내었다. $Pr_{0.7}Ca_{0.3}MnO_3$의 열팽창계수는 $300{\sim}1000^{\circ}C$의 영역에서 $1.19{\times}10^{-5}K^{-1}$로 측정되었고 이 값은 YSZ의 열팽창계수 $1.15{\times}10^{-5}K^{-1}$과 유사한 값이었다.

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