• 제목/요약/키워드: Gap times

검색결과 1,029건 처리시간 0.028초

표면 텍스쳐링 크기와 밀도가 후면 전극 실리콘 태양전지에 미치는 영향 (A effect of the back contact silicon solar cell with surface texturing size and density)

  • 장왕근;장윤석;박정호
    • 한국신재생에너지학회:학술대회논문집
    • /
    • 한국신재생에너지학회 2011년도 춘계학술대회 초록집
    • /
    • pp.112.1-112.1
    • /
    • 2011
  • The back contact solar cell (BCSC) has several advantages compared to the conventional solar cell since it can reduce grid shadowing loss and contact resistance between the electrode and the silicon substrate. This paper presents the effect of the surface texturing of the silicon BCSC by varying the texturing depth or the texturing gap in the commercially available simulation software, ATHENA and ATLAS of the company SILVACO. The texturing depth was varied from $5{\mu}m$ to $150{\mu}m$ and the texturing gap was varied from $1{\mu}m$ to $100{\mu}m$ in the simulation. The resulting efficiency of the silicon BCSC was evaluated depending on the texturing condition. The quantum efficiency and the I-V curve of the designed silicon BCSC was also obtained for the analysis since they are closely related with the solar cell efficiency. Other parameters of the simulated silicon BCSC are as follows. The substrate was an n-type silicon, which was doped with phosphorous at $6{\times}10^{15}cm^{-3}$, and its thickness was $180{\mu}m$, a typical thickness of commercial solar cell substrate thickness. The back surface field (BSF) was $1{\times}10^{20}\;cm^{-3}$ and the doping concentration of a boron doped emitter was $8.5{\times}10^{19}\;cm^{-3}$. The pitch of the silicon BCSC was $1250{\mu}m$ and the anti-reflection coating (ARC) SiN thickness was $0.079{\mu}m$. It was assumed that the texturing was anisotropic etching of crystalline silicon, resulting in texturing angle of 54.7 degrees. The best efficiency was 25.6264% when texturing depth was $50{\mu}m$ with zero texturing gap in case of low texturing depth (< $100{\mu}m$).

  • PDF

Studies on the Ability to Detect Lesions According to the Changes in the MR Diffusion Weighted Images

  • Kim, Chang-Bok;Cho, Jae-Hwan;Dong, Kyung-Rae;Chung, Woon-Kwan
    • Journal of Magnetics
    • /
    • 제17권2호
    • /
    • pp.153-157
    • /
    • 2012
  • This study evaluated the ability of Diffusion-Weight Image (DWI), which is one of pulse sequences used in MRI based on the T2 weighted images, to detect samples placed within phantoms according to their size. Two identically sized phantoms, which could be inserted into the breast coil bilaterally, were prepared. Five samples with different sizes were placed in the phantoms, and the T2 weighted images and DWI were obtained. The Breast 2 channel coil of SIEMENS MAGNETOM Avanto 1.5 Tesla equipment was used for the experiments. 2D T2 weighted images were obtained using the following parameters: TR/TE = 6700/74 msec, Thickness/gap = 5/1 mm, Inversion Time (TI) = 130 ms, and matrix = $224{\times}448$. The parameters of DWI were that TR/TE = 8100/90 msec, Thickness/gap = 5/1 mm, matrix = $128{\times}128$, Inversion Time = 185 ms, and b-value = 0, 100, 300, 600, 1000 s/mm. The ratio of the sample volume on DWI compared to the T2 weighted images, which show excellent ability to detect lesions on MR images, was presented as the mean b-value. The measured b-value of the samples was obtained: 0.5${\times}$0.5 cm=0.33/0.34 square ${\times}$ cm (103%), 1${\times}$1 cm=1.28/1.25 square ${\times}$ cm (102.4%), 1.5${\times}$1.5 cm = 2.28/2.67 square ${\times}$ cm (85.39%), 2${\times}$2 cm=3.56/4.08 square ${\times}$ cm (87.25%), and 2.5${\times}$2.5 cm=7.53/8.77 square ${\times}$ cm (85.86%). In conclusion, the detection ability by the size of a sample was measured to be over 85% compared to T2 weighted image, but the detection ability of DWI was relatively lower than that of T2 weighted image.

전기분해에 의한 고농도 유기물질 제거 특성 (Removing High Concentration Organic Matters by Using Electrolysis)

  • 길대수;이병헌;이제근
    • 대한환경공학회지
    • /
    • 제22권2호
    • /
    • pp.251-264
    • /
    • 2000
  • 합성폐수의 전기분해에 의한 전류밀도, 체류시간, 전극간격 및 $Cl^-/COD_{Cr}$ 비에 대한 유기물질 제거 특성을 조사하기 위한 실험을 수행하였다. 양극판은 티타늄에 이산화이리듐을 전착한 $Ti/IrO_2$ 극판으로 하였으며, 음극판은 스테인리스 스틸판을 사용하였다. 판형태와 망형태의 전극을 사용한 경우 $COD_{Cr}$ 제거율은 비슷하게 나타났으나, 전력비는 판형태보다 망형태의 전극에서 저렴한 것으로 나타났다. $COD_{Cr}$ 제거율 70 %를 얻는데 소요되는 $Cl^-/COD_{Cr}$ 비는 약 $1.3kgCl^-/kgCOD_{Cr}$으로 나타났으며, $COD_{Cr}$을 완전히 제거하는데 약 $2.2kgCl^-/kgCOD_{Cr}$이 필요하였다. 유기물질의 제거는 전류밀도, 체류시간 및 $Cl^-/COD_{Cr}$ 비에 따라 높게 나타났고, 전극간격에는 반비례하였으며, 운전인자와 제거율과의 관계는 아래와 같이 나타났다. $$COD_{Cr}(%)=80.0360(Current\;density)^{0.4451}{\times}(HRT)^{0.8102}{\times}(Gap)^{-0.4915}{\times}(Cl^-/COD_{Cr})^{0.5805}$$ 유기물질과 질소를 동시에 전기분해할 경우 두 물질의 산화는 경쟁관계에 있으며, 암모니아성 질소를 산화하는데 우선적으로 작용하여 유기물질의 제거는 낮아지지만, 알칼리도 첨가에 의해 유기물질 제거가 증가하였다.

  • PDF

Optical energy band gap of the conductive $AgGaSe_2$ layers

  • You, Sang-Ha;Hong, Kwang-Joon
    • 한국전기전자재료학회:학술대회논문집
    • /
    • 한국전기전자재료학회 2009년도 추계학술대회 논문집
    • /
    • pp.46-46
    • /
    • 2009
  • The photoconductive $AgGaSe_2$(AGS) layers were grown by the hot wall epitaxy method. The AGS layer was confirmed to be the epitaxially grown layer along the <112> direction onto the GaAs(100) substrate. The band-gap variation as a function of temperature on AGS was well fitted by $E_8(T)=1.9501-8.37{\times}10^{-4}T^2/(T+224)$. The band-gap energy of AGS obtained at 293 K was determined to be 1.8111 eV.

  • PDF

이동 벽면에 의한 원형 실린더의 비대칭적 공력 발달에 관한 전산연구 (A COMPUTATIONAL STUDY ABOUT THE ASYMMETRIC AERODYNAMIC EVOLUTION AROUND A CIRCULAR CYLINDER CAUSED BY A MOVING WALL)

  • 정재윤;장조원
    • 한국전산유체공학회지
    • /
    • 제11권3호
    • /
    • pp.64-70
    • /
    • 2006
  • A Computational study was carried out in order to investigate the moving wall effect of a circular cylinder at a Reynolds number of $2.0{\times}10^4$. The viscous-incompressible Navier-Stokes equations and Spalart-Almaras turbulent model of the commercial CFD code were adopted for this numerical analysis. The moving wall was set parallel with the freestream, and moving speed was equal to the freestream velocity. The gap ratio is defined as the distance ratio between the circular cylinder diameter and the height from the moving wall. The results show that there is vortex shedding over the critical gap ratio and aerodynamic loads including amplitude and the Strouhal number change according to the gap ratio.

철근콘크리트 골조공사의 프로세스 및 공정 공백 산출 시뮬레이션 모형 개발 (Development of Computing Model for the Process and Operation Interval of Reinforced Concrete Work using Web-CYCLONE)

  • 박상민;손창백;이동은
    • 한국건축시공학회:학술대회논문집
    • /
    • 한국건축시공학회 2012년도 춘계 학술논문 발표대회
    • /
    • pp.341-343
    • /
    • 2012
  • This study introduces a method for computation of process and operation gap in the specific construction operation(i.e., RC frame construction applying a block-grouping scheme) using CYCLONE-based simulation modeling and analysis technique. Since uncertainty of construction environment exists, a thoughtful production planning is required to effectively deal with a risk resulting in schedule delay in advance. This study presents the concepts of a time delay occurred in a process level and operation level in a operation model, and a method of measuring gap-times in each level while the simulation progresses. It helps a site manager to decide how many segmentation in a construction block is suitable for eliminating unproductive time-delays under the constrained resources (e.g., laborer, equipment). A case study presents a network model representing a three segmented RC frame work, and result obtained from the simulation experiment.

  • PDF

Magneto-Optical Effect of One-Dimentional Magnetophotonic Crystal Utilizing the Second Photonic Band Gap

  • Uchida, H.;Tanizaki, K.;Khanikaev, A.B.;Fedyanin, A.A.;Lim, P.B.;Inoue, M.
    • Journal of Magnetics
    • /
    • 제11권3호
    • /
    • pp.139-142
    • /
    • 2006
  • We fabricated new one-dimensional magnetophotonic crystal (1D-MPC) utilizing the second and third photonic band gaps where localized modes existed. Structure of the 1D-MPC was $(Ta_{2}O_{5}/SiO_{2})_{5}/Bi:YIG/(SiO_{2}/Ta_{2}O_{5})_{5}$ with optical thicknesses of 3$\lambda$ /4 for $Ta_{2}O_{5} and $SiO_2$ dielectric layers and $\lambda$ /2 for Bi:YIG defect layer, where $\lambda$ is a wavelength of a localized mode in the second photonic band gap. Faraday rotation at the localized mode in the second photonic band gap was enhanced, which was confirmed by calculation using 4${\times}$4 matrix method.

Pool Boiling Heat Transfer in Annuli with Closed Bottom

  • Kang, Myeong-Gie;Han, Young-Hwan
    • Nuclear Engineering and Technology
    • /
    • 제34권2호
    • /
    • pp.165-175
    • /
    • 2002
  • Effects of gap sizes (3.9-44.3 mm) of vertical annuli on nucleate pool boiling heat transfer of water at atmospheric pressure have been obtained experimentally. Through the study, tubes of the closed bottom have been investigated and results are compared with those of a single unconfined tube. According to the results, the annular condition gives much increase in heat transfer coefficient at moderate heat fluxes. The increase is much enhanced 3s the gap size decreases. At the same tube wall superheat (about 3.1 K) the heat transfer coefficient for the least gap size (i.e., 3.9 mm) is more than three times greater than that of the unconfined tube. However, deterioration of heat transfer occurs at high heat flux for confined boiling.

Simulation of Low Temperature Plasmas for an Ultra Violet Light Source using Coplanar Micro Dielectric Barrier Discharges

  • Bae, Hyowon;Lee, Ho-Jun;Lee, Hae June
    • Applied Science and Convergence Technology
    • /
    • 제25권6호
    • /
    • pp.138-144
    • /
    • 2016
  • The discharge characteristics of pulse-driven coplanar micro barrier discharges for an ultraviolet (UV) light source using Ne-Xe mixture have been investigated using a two-dimensional fluid simulation at near-atmospheric pressure. The densities of electrons, the radiative excited states, the metastable excited states, and the power loss are investigated with the variations of gas pressure and the gap distance. With a fixed gap distance, the number of the radiative states $Xe^*(^3P_1)$ increases with the increasing driving voltage, but this number shows weak dependency on the gas when that pressure is over 400 Torr. However, the number of the radiative states increases with the increase of the gap distance at a fixed voltage, while the power loss decreases. Therefore, a long gap discharge has higher efficiency for UV generation than does a short gap discharge. A slight change in the electrode tilt angle enhances the number of radiative species 2 or 3 times with the same operation conditions. Therefore, the intensity and efficiency of the UV light source can be controlled independently by changing the gap distance and the electrode structure.

맥동전자장이 불완전 척수손상 흰쥐의 기능회복과 GAP-43의 발현에 미치는 영향 (The Effects of Pulsed Electromagnetic Field on Functional Recovery and Expression of GAP-43 after Incomplete Spinal Cord Injury in Rats)

  • 방현수
    • 대한물리의학회지
    • /
    • 제7권3호
    • /
    • pp.349-356
    • /
    • 2012
  • Purpose : This study was designed to investigate the effects of pulsed electromagnetic field on functional recovery and expression of GAP-43 after incomplete spinal cord injury (SCI) in rats. Methods : To confirm the damage of SCI and effects of pulsed electromagnetic field, 20 Sprague-Dawley male rats were used and divided randomly 2groups (SCI, PEMF). Incomplete SCI was induced by using modified NYU drop model. After operation, functional recovery test, immunohistochemistry and western blot analysis were measured at 1, 2, 3 weeks. Pulsed electromagnetic field were apply three weeks (one times a day, five days a week and twenty minutes a session). Results : In the this study, applications of pulsed electromagnetic field after incomplete SCI induced the significant improvement in functional recovery and expression of neurotrophic factor. The results were as follows; Foot print test, PEMF were significantly decreased than the SCI (p<.05). Expression of GAP-43, PEMF were significantly increased than the SCI at 2 and 3 weeks (p<.05). Conclusion : In conclusion, pulsed electromagnetic field were positive effect in functional recovery and expression of GAP-43 after incomplete SCI in rats.