• Title/Summary/Keyword: arc energy

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The research of porous Si for crystalline silicon solar cells (다공성 실리콘을 적용한 결정질 실리콘 태양전지에 관한 연구)

  • Lee, Jae-Doo;Kim, Min-Jeong;Lee, Soo-Hong
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.06a
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    • pp.235-235
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    • 2010
  • The Anti-reflection coating(ARC) properties can be formed on silicon substrate using a simple electrochemical etching technique. This etching step can be improve solar cell efficiency for a solar cell manufacturing process. This paper is based on the removal of silicon atoms from the surface a layer of porous silicon(PSi). Porous silicon is form by anodization and can be obtained in an electrolyte with hydrofluoric. It have demonstrated the feasibility of a very efficient porous Si layer, prepared by a simple, cost effective, electrochemical etching method. We expect our research can results approaching to lower than 10% of reflectance by optimization of process parametaer.

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The Study on the Self-Flow Generation Phenomena in a Gas Circuit Breaker (대전류 영역에서의 가스차단기 내의 아크의 자발적인 흐름현상에 따른 에너지 전달의 수치적 해석)

  • Choi, Jae-Won;Choi, Seung-Kil;Kang, Hyung-Boo
    • Proceedings of the KIEE Conference
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    • 1997.07e
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    • pp.1837-1839
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    • 1997
  • This study presents the energy transfer of thermal arc in the circuit breaker with self-generation flow without puffer action. The phenomenon of pressure increase in the cylinder which encloses fixed contact was focused on and rising current stage was considered. Temperature and velocity of arc plasma were calculated by using energy balance equation and the amount of energy transfer due to convective flow was calculated.

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Investigation of Amorphous Carbon Film Deposition by Molecular Dynamic Simulation (분자 동역학 전산모사에 의한 비정질 탄소 필름의 합성거동 연구)

  • 이승협;이승철;이규환;이광렬
    • Journal of the Korean Vacuum Society
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    • v.12 no.1
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    • pp.25-34
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    • 2003
  • Deposition behavior of hard amorphous carbon film was investigated by molecular dynamic simulation using Tersoff potential which was suggested for the interaction potential between carbon atoms. When high energy carbon atoms were collided on diamond (100) surface, dense amorphous carbon film could be obtained. Physical properties of the simulated carbon film were compared with those of the film deposited by filtered cathodic arc process. As in the experimental result, the most diamond-like film was obtained at an optimum kinetic energy of the incident carbon atoms. The optimum kinetic energy was 50 eV, which is comparable to the experimental observation. The simulated film was amorphous with short range order of diamond lattice. At the optimum kinetic energy condition, we found that significant amount of carbon atom were placed at a metastable site of distance 2.1 $\AA$. By melting and quenching simulation of diamond lattice, it was shown that this metastatic peak is Proportional to the quenching rate. These results show that the hard and dense diamond-like film could be obtained when the localized thermal spike due to the collision of high energy carbon atom can be effectively dissipated to the lattice.

Effect of the Slag Former on the Metal Melting and Radionuclides Distribution in an Electric Arc Furnace

  • Song Song-Pyung;Min Byung-Youn;Choi Wang-Kyu;Chung Chong-Hun;Oh Won-zin
    • Proceedings of the Korean Radioactive Waste Society Conference
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    • 2005.11a
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    • pp.32-37
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    • 2005
  • The characteristics of the metal melting and radionuclide distribution of the radioactive has been investigated in a lab-scale arc furnace. The slag former based on the constituents of silica, calcium oxide, aluminum oxide, borate and calcium fluoride additions was used for melting of the stainless and carbon steel. In the melting of the stainless steel, the amount of slag formation increased with an increase of the concentration of the slag former. But the effects of the slag basicity on the amount of stag formation showed a local maximum value of the slag formation with an increase of the basicity index in the melting of the stainless steel as well as in the melting of the carbon steel. With an increase of the amount of slag former addition, the trends of the cobalt distribution into the ingot and the stag depended on the kind of slag former used in the melting of the stainless steel while the effect of the slag basicity on the distribution of the cobalt was not clarified in the melting of carbon steel. Tn the melting of the carbon steel, the strontium was captured at up to $50\%$ into the slag phase. Cesium was completely eliminated from the melt of the stainless steel as well as the carbon steel and distributed to the dust phase.

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Depositon of Transparent Conductive Films by a DC arc Plasmatron

  • Penkov, O.V.;Plaksin, V. Yu.;Joa, S.B.;Kim, J.H.;LEE, H.J.
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.02a
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    • pp.480-480
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    • 2010
  • In the present work, we studied effect of the deposition parameters on the structure and properties of ZnO films deposited by DC arc plasmatron. The varied parameters were gas flow rates, precursor composition, substrate temperature and post-deposition annealing temperature. Vapor of Zinc acetylacetone was used as source materials, oxygen was used as working gas and argon was used as the cathode protective gas and a transport gas for the vapor. The plasmatron power was varied in the range of 700-1,500 watts. Flow rate of the gases and substrate temperature rate were varied in the wide range to optimize the properties of the deposited coatings. After deposition films were annealed in the hydrogen atmosphere in the wide range of temperatures. Structure of coatings was investigated using XRD and SEM. Chemical composition was analyzed using x-ray photo-electron spectroscopy. Sheet conductivity was measured by 4-point probe method. Optical properties of the transparent ZnO-based coatings were studied by the spectroscopy. It was shown that deposition by a DC Arc plasmatron can be used for low-cost production of zinc oxide films with good optical and electrical properties. Sheet resistance of 4 Ohms cm was achieved after the deposition and 30 min annealing in the hydrogen at $350^{\circ}C$. Elevation of the substrate temperature during the deposition process up to $350^{\circ}C$ leads to decreasing of the film's resistance due to rearrangement of the crystalline structure.

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Content Variation of Total Chromium and Hexavalent Chromium in Flux Cored Arc Welding (플럭스 코어드 아크 용접 중 발생하는 총 크롬 및 6가 크롬의 함량 변화)

  • Yoon, Chung Sik;Paik, Nam Won;Kim, Jeong Han;Park, Dong Uk;Ha, Kwon Chul;Cho, Sang Jun;Kim, Shin Bum;Chae, Hyun Byung
    • Journal of Korean Society of Occupational and Environmental Hygiene
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    • v.10 no.1
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    • pp.32-44
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    • 2000
  • The practice of welding stainless steel is known to produce various valance states of chromium. $CO_2$ flux cored arc welding on stainless was performed in fume collection chamber. Content of total chromium and hexavalent chromium in fumes, content of hexavalent chromium in total chromium, solubility of hexavalent chromium were investigated. Content of total chromium in fumes increases from 2~3% to 7~9% as a function of input energy, but hexavalent chromium, less than 1.2% in fumes, is not related to input energy. Hexavalent chromium in fumes exists as solubles up to 90%. Content of total chromium in flux cored arc welding fumes and solubility of hexavalent chromium are similar to shielded metal arc welding fumes, but content of hexavalent chromium is similar to metal inert gas welding fumes. These characteristics are relevant to flux of wires and $CO_2$ shielding gas.

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A Study on Behaviour and Characteristics of Spark Discharge in Spark Ignition System (스파크 점화 시스템의 방전 거동 및 특성에 관한 연구)

  • Lee Myung Jun;Hall Matt;Ezekoye Ofodike A.;Matthews Ron;Chung Sung Sik
    • Transactions of the Korean Society of Automotive Engineers
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    • v.14 no.1
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    • pp.100-108
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    • 2006
  • Time-resolved current and voltage measurements for an inductive automotive spark system were made. Also presented are measurements of the total energy delivered to the spark gap. The measurements were made in air for a range of pressures from 1-18atm, at ambient temperatures. The measured voltage and current characteristics were found to be a function of many ignition parameters; some of these include: spark gap distance, internal resistance of the spark plug and high tension wire, and pressure. The voltages presented were measured either at the top of the spark plug or at the spark gap. The measurements were made at different time resolutions to more accurately resolve the voltage and current behavior throughout the discharge process. This was necessary because the breakdown event occurs on a time scale much shorter than the arc and glow phases. The breakdown, are, and glow voltages were found to be functions of spark plug resistance, gas density, and spark plug gap as expected from the literature. Spark duration was found to decrease as either pressure or gap was increased. The transition from the arc to glow phase is usually distinguished by a sudden rise in the voltage across the gap. At pressures above about 7atm this transition was not observed suggesting that a glow phase was not present. Energy delivered to the gap increased with increasing pressure. The effective resistance of the spark gap during discharge was about twice as large for the glow phase as the arc phase.

Basic Performance Test of a Three Phase AC Arc Plasma Torch System for Plasma Gas Reforming (플라즈마 가스 개질 응용을 위한 3상 아크 플라즈마 토치 시스템 특성 실험)

  • DONG-HYUN LEE;DARIAN FIGUERA-MICHAL;HAE-WON PARK;NAM-KI LEE;SANG-YUN PAEK;SHIYOUNG YANG;JUN-HO SEO
    • Journal of Hydrogen and New Energy
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    • v.34 no.1
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    • pp.8-16
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    • 2023
  • In this work, we report basic performance test results of a lab-scale three phase alternative current (AC) arc plasma torch system for plasma gas reforming applications. The suggested system primarily consists of three graphite electrodes inclined at 12.5° to the central axis, a 𝞥 150 mm cylindrical gas path and a three phase-60 Hz AC power supply. At air flow rate of 50 Lpm and arc currents of 100-175 A, test results revealed that plasma resistances were decreasing from 1.08 Ω to 0.53 Ω with the increase of plasma power from 9.3 kW to 13.8 kW, causing the decrease of power factor and increase of the line voltages. However, the injected air can be heated quickly up to the temperatures of >1,200℃ when injecting AC arc plasma powers of >10 kW.