• 제목/요약/키워드: fill buffer

검색결과 18건 처리시간 0.032초

고준위폐기물처분장 공학적방벽의 갭채움재 기술현황 (R&D Review on the Gap Fill of an Engineered Barrier for an HLW Repository)

  • 이재완;최영철;김진섭;최희주
    • 터널과지하공간
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    • 제24권6호
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    • pp.405-417
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    • 2014
  • 고준위폐기물처분장에서 갭채움재는 완충재와 뒷채움재의 성능을 좌우하는 중요한 공학적방벽의 구성요소이다. 본 논문에서는 갭채움재에 대한 해외 기술현황을 조사하고, 이를 통하여 갭채움재의 개념, 제조기술, 성형특성, 설치기술에 대한 연구결과들을 정리하였다. 갭채움재 개념은 처분방식과 처분개념에 따라서 나라마다 약간씩 차이가 있었다. 갭채움재 물질로는 대부분 벤토나이트를 사용하였고, 충전제로 점토를 사용하였다. 갭채움재는 펠렛, 과립상, 또는 펠렛-과립상 혼합물의 형태로 사용되었다. 갭채움재 펠렛 제조에는 정압축, 롤러압축, 압출-컷팅 방법 등이 사용되었으며, 이 중, 실험과 실제 현장에서의 펠렛 소요량을 감안하여 많은 나라들이 롤러압축방법과 압출-컷팅방법에 대한 기술 확보에 집중하였다. 펠렛 성형특성 실험결과, 펠렛의 건조밀도와 건전성은 수분함량, 구성물질, 제조방법, 펠렛 크기에 민감하였고, 제작 시 압축하중에는 상대적으로 덜 민감하였다. 갭채움재의 설치방법으로는 수직처분공 완충재 갭에서는 부어넣기(pouring) 방법, 붓고 다지기(pouring and tamping) 방법, 진동을 주며 부어넣기(pouring with vibration) 방법 등이 시도되었으며, 수평처분공 완충재와 처분터널의 뒷채움재 갭에서는 숏크리트 기술을 이용한 불어넣기(blowing by use of shotcrete technology) 방법과 오거를 이용한 정치 및 다지기(auger placement and compaction) 방법 등이 시도되었다. 그러나 이 방법들은 아직 기술적으로 초기단계에 있어 앞으로도 계속적인 연구가 이루어질 것으로 예상되었다.

The Characteristics of a Hydrogenated Amorphous Silicon Semitransparent Solar Cell When Applying n/i Buffer Layers

  • Lee, Da Jung;Yun, Sun Jin;Lee, Seong Hyun;Lim, Jung Wook
    • ETRI Journal
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    • 제35권4호
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    • pp.730-733
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    • 2013
  • In this work, buffer layers with various conditions are inserted at an n/i interface in hydrogenated amorphous silicon semitransparent solar cells. It is observed that the performance of a solar cell strongly depends on the arrangement and thickness of the buffer layer. When arranging buffer layers with various bandgaps in ascending order from the intrinsic layer to the n layer, a relatively high open circuit voltage and short circuit current are observed. In addition, the fill factors are improved, owing to an enhanced shunt resistance under every instance of the introduced n/i buffer layers. Among the various conditions during the arrangement of the buffer layers, a reverse V shape of the energy bandgap is found to be the most effective for high efficiency, which also exhibits intermediate transmittance among all samples. This is an inspiring result, enabling an independent control of the conversion efficiency and transmittance.

Effect of p-type a-SiO:H buffer layer at the interface of TCO and p-type layer in hydrogenated amorphous silicon solar cells

  • Kim, Youngkuk;Iftiquar, S.M.;Park, Jinjoo;Lee, Jeongchul;Yi, Junsin
    • Journal of Ceramic Processing Research
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    • 제13권spc2호
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    • pp.336-340
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    • 2012
  • Wide band gap p-type hydrogenated amorphous silicon oxide (a-SiO:H) buffer layer has been used at the interface of transparent conductive oxide (TCO) and hydrogenated amorphous silicon (a-Si:H) p-type layer of a p-i-n type a-Si:H solar cell. Introduction of 5 nm thick buffer layer improves in blue response of the cell along with 0.5% enhancement of photovoltaic conversion efficiency (η). The cells with buffer layer show higher open circuit voltage (Voc), fill factor (FF), short circuit current density (Jsc) and improved blue response with respect to the cell without buffer layer.

Flower like Buffer Layer to Improve Efficiency of Submicron-Thick CuIn1-xGaxSe2 Solar Cells

  • Park, Nae-Man;Cho, Dae-Hyung;Lee, Kyu-Seok
    • ETRI Journal
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    • 제37권6호
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    • pp.1129-1134
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    • 2015
  • In this article, a study of a flower like nanostructured CdS buffer layer for improving the performance of a submicron-thick $CuIn_{1-x}Ga_xSe_2$ (CIGS) solar cell (SC) is presented. Both its synthesis and properties are discussed in detail. The surface reflectance of the device is dramatically decreased. SCs with flower like nanostructured CdS buffer layers enhance short-circuit current density, fill factor, and open-circuit voltage. These enhancements contribute to an increase in power conversion efficiency of about 55% on average compared to SCs that don't have a flower like nanostructured CdS buffer layer, despite them both having the same CIGS light absorbing layer.

사출금형에서 균형충전을 위한 새로운 러너시스템 멜트버퍼 (A New Runner System Melt-Buffer for Filling Balance in Injection Mold)

  • 정영득;장민규
    • 소성∙가공
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    • 제18권2호
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    • pp.122-127
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    • 2009
  • The injection mold with multi-cavity is essential for mass production of plastic products. Multi-cavity molds are designed to geometrically balanced runner system to uniformly fill to each cavity. However, despite geometrical balanced runner system, filling imbalances between cavity to cavity have always been observed in injection molding. To solve these problems, many studies such as Melt Flipper, RC Pin, and others have been presented. The results of these studies have been an effect on filling balances in multi-cavity molds. But, those have had a limitation that additional insert parts must have existed in the mold. In this study, a new runner system is suggested for filling balance between cavity to cavity using "Melt-Buffer" with simple change of runner shape. A series of simulation to confirm feasibility of Melt-Buffer's effects was conducted using injection molding CAE program. Also, a series of injection molding experiment was conducted using plastic materials such as ABS and PP. As results of this study, feasibilities of filling balances by Melt-Buffer were confirmed.

Improved Carrier Tunneling and Recombination in Tandem Solar Cell with p-type Nanocrystalline Si Intermediate Layer

  • Park, Jinjoo;Kim, Sangho;Phong, Pham duy;Lee, Sunwha;Yi, Junsin
    • Current Photovoltaic Research
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    • 제8권1호
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    • pp.6-11
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    • 2020
  • The power conversion efficiency (PCE) of a two-terminal tandem solar cell depends upon the tunnel-recombination junction (TRJ) between the top and bottom sub-cells. An optimized TRJ in a tandem cell helps improve its open-circuit voltage (Voc), short-circuit current density (Jsc), fill factor (FF), and efficiency (PCE). One of the parameters that affect the TRJ is the buffer layer thickness. Therefore, we investigated various TRJs by varying the thickness of the buffer or intermediate layer (TRJ-buffer) in between the highly doped p-type and n-type layers of the TRJ. The TRJ-buffer layer was p-type nc-Si:H, with a doping of 0.06%, an activation energy (Ea) of 43 meV, an optical gap (Eg) of 2.04 eV, and its thickness was varied from 0 nm to 125 nm. The tandem solar cells we investigated were a combination of a heterojunction with intrinsic thin layer (HIT) bottom sub-cell and an a-Si:H (amorphous silicon) top sub-cell. The initial cell efficiency without the TRJ buffer was 7.65% while with an optimized buffer layer, its efficiency improved to 11.74%, i.e., an improvement in efficiency by a factor of 1.53.

Effect of MoO3 Thickness on the Electrical, Optical, and structural Properties of MoO3 Graded ITO Anodes for PEDOT:PSS-free Organic Solar Cells

  • Lee, Hye-Min;Kim, Seok-Soon;Chung, Kwun-Bum;Kim, Han-Ki
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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    • pp.478.1-478.1
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    • 2014
  • We investigated $MoO_3$ graded ITO electrodes for organic solar cells (OSCs) without PEDOT:PSS buffer layer. The effect of $MoO_3$ thickness on the electrical, optical, and structural properties of $MoO_3$ graded ITO anodes prepared by RF/DC magnetron co-sputtering system using $MoO_3$ and ITO targets was investigated. At optimized conditions, we obtained $MoO_3$ graded ITO electrodes with a low sheet resistance of 13 Ohm/square, a high optical transmittance of 83% and a work function of 4.92 eV, comparable to conventional ITO films. Due to the existence of $MoO_3$ on the ITO electrodes, OSCs fabricated on $MoO_3$ graded ITO electrode without buffer layer successfully operated. Although OSCs fabricated on ITO anode without buffer layer showed a low power conversion efficiency of 1.249%, OSCs fabricated on $MoO_3$ graded ITO electrode without buffer layer showed a outstanding cell performance of 2.545%. OSCs fabricated on the $MoO_3$ graded ITO electrodes exhibited a fill factor of 61.275%, a short circuit current of 7.439 mA/cm2, an open circuit voltage of 0.554 V, and a power conversion efficiency of 2.545%. Therefore, $MoO_3$ graded ITO electrodes can be considered a promising transparent electrode for cost efficient and reliable OSCs because it could eliminate the use of acidic PEDOT:PSS buffer layer.

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Co-sputtering법으로 제작한 ZnTe 태양전지의 특성 (Characteristics of the ZnTe solar cell by the co-sputtering methods)

  • 장유진;김성우;최혁환;이명교;권태하
    • 한국정보통신학회논문지
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    • 제8권2호
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    • pp.440-448
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    • 2004
  • 본 논문에서는 II-Vl족의 ZnTe 화합물반도체 태양전지를 제작하기 위하여 투명전극(AZO) 및 Buffer layer(ZnO)의 특성과 태양전지의 효율에 가장 큰 영향을 미치는 광흡수층의 에너지밴드갭을 줄이는 연구를 하였다. ZnTe박막은 Zn(Zinc)과 Te(Tellurium)를 co-sputtering법을 이용하여 증착하였다. ZnTe 박막은 Zn과 Te의 RF power를 각각 50W, 30W로 하여 10mTorr의 Ae 분위기에서 20$0^{\circ}C$의 기판온도로 제작되었으며, 이때의 에너지밴드갭은 1.73eV였다. 이렇게 제작된 박막을 진공상태에서 $400^{\circ}C$의 온도로 10초간 열처리하여 1.67eV의 에너지밴드갭을 얻을 수 있었고, 이때의 Zn과 Te의 비율은 32%:68%였다. 최적의 조건에서 태양전지는 6.85% (Voc:0.69V, Jsc:21.408㎃/$cm^2$, Fill Factor (FF):0.46)의 효율을 얻을 수 있었다.

인버티드 유기태양전지용 Ti-Zn-O 버퍼층 특성 평가 연구

  • 강신비;나석인;김한기
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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    • pp.534-534
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    • 2013
  • 본 연구에서는 RF/DC 마그네트론 스퍼터링 시스템을 이용하여 co-sputtering 방법으로 TiO2와 ZnO를 이용하여 인버티드 유기태양전지용 버퍼층을 제작하고 TiO2와 ZnO의 함량에 따른 인버티드 유기 태양전지 특성을 비교하였다. Ti-Zn-O 버퍼층은 기존의 버퍼층 제작에 사용되던 용액 공정 대신 스퍼터링 시스템을 이용하여 제작하였다. ITO 전극 상부에 곧바로 Ti-Zn-O를 성막하여 Anode와 버퍼층이 일체화된 투명 전극을 제작하고 ZnO와 TiO2 함량이 유기 태양전지의 특성에 미치는 영향을 연구하였다. 버퍼층의 TiO2와 ZnO 함량에 따른 광학적, 구조적특성을 UV/Vis spectrometry와 X-ray diffraction (XRD), TEM 등으로 분석하였으며, Ti-Zn-O 박막의 실제 버퍼 층으로서의 적용 가능성을 알아보기 위해 인버티드 유기태양전지로 제작하여 그 특성을 평가하였다. 기존의 인버티드 유기태양전지의 특성이 fill factor of 55.58%, short circuit current of 8.33 mA/cm2, open circuit voltage of 0.66 V, efficiency 3.06%인데 반해 최적 조건의 Ti-Zn-O 버퍼층을 적용했을 경우 fill factor of 52.05%, short circuit current of 8.81 mA/cm2, open circuit voltage of 0.66 V, efficiency 3.03%인 우수한 유기태양전지의 특성을 보임으로써 스퍼터링 공법으로 제작된 Ti-Zn-O 박막의 인버티드 유기태양전지용 버퍼 층으로서의 적용 가능성을 확인하였다.

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Effects as Plasma Treatments on CdS Buffer Layers in CIGS Thin Film Solar Cells

  • Jo, Hyun-Jun;Sung, Shi-Joon;Hwang, Dae-Kue;Bae, In-Ho;Kim, Dae-Hwan
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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    • pp.171-171
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    • 2012
  • We have studied the effects of plasma treatments on CdS buffer layers in CIGS thin film solar cells. The CdS layers were deposited on CIGS films by chemical bath deposition (CBD) method. The RF plasma treatments of the CdS thin films were performed with Ar, $O_2 and $N_2 gases, respectively. After plasma treatments, the solar cells with Al:ZnO/i-ZnO/CdS/CIGS structures were fabricated. The surface properties of the CdS/CIGS thin films after plasma treatments were investigated with SEM, EDX and AFM measurements. The electrical properties of manufactured solar cell were discussed with the results of current-voltage measurements. The plasma treatments have a strong influence on the open circuit voltage (VOC) and the fill factor of the solar cells. Finally, a correlation between the surface properties of CdS layer and the efficiencies of the CIGS thin film solar cells is discussed.

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