• 생물환경조절학회지
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• 제29권4호
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• pp.320-325
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• 2020

본 연구는 최근 신소재 단열재로 주목받고 있는 실리카 에어로겔을 이용하여 현재 사용되고 있는 다겹보온커튼의 단점을 보완하고 보온성을 유지 및 향상시킬 수 있는 새로운 조합의 다겹보온커튼을 제작 하여 현장에 설치함으로써 보온성과 경제성을 분석하고자 한다. 실험에 사용된 다겹보온커튼은 실리카 에어로겔이 함유된 부직포를 사용하여 2가지의 조합으로 제작하였으며 시중에 판매, 사용되고 있는 관행 다겹보온 커튼과의 차이에 따른 온습도변화와 연료소비량을 측정하여 비교분석하였다. 실험결과 단동온실과 연동온실에서 다겹보온커튼 차이에 따른 온습도변화는 미세하게 나타났으나, 거의 비슷한 온습도 값을 유지하였다. 이는 실리카 에어로겔을 이용한 다겹보온커튼이 관행 다겹보온커튼에 비해 온습도 제어 측면에서 문제가 없음을 나타냈다. 난방에너지 비교분석 결과, 실리카 에어로겔을 이용한 다겹보온커튼이 관행 다겹보온커튼에 비해 연료소비량은 단동온실에서 약 15%, 연동온실에서 약 20%의 연료소비량을 절감한 것으로 나타나 온실의 규모와 사용기간이 증가함에 따라 난방에너지는 절감될 것으로 판단된다. 실리카 에어로겔 이용 다겹보온커튼이 관행 다겹보온커튼에 비해 통기성과 보온성이 증가되는 것이 확인되었다. 그러나, 연동온실에서 사용된 다겹보온커튼은 관행 다겹보온커튼에 비해 무게가 증가하고 뻣뻣하여 시공성과 작동성이 떨어지는 것을 확인할 수 있었다. 이에 단동온실에서 사용된 다겹보온 커튼에서는 개선사항을 적용하였다. 내부단열재의 교체를 통해 두께를 감소시키고 뻣뻣함을 개선함으로써 농가가 사용하기에 충분한 가능성이 있다는 것을 확인하였다.

• Current Photovoltaic Research
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• 제11권2호
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• pp.44-48
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• 2023

In heterojunction technology (HJT) solar cells, low-temperature curing paste is used because the passivation layer deteriorates at high temperatures of 200℃ or higher. However, manufacturing HJT photovoltaic (PV) modules is challenging due to the weak peel strength between busbar electrodes and cells after soldering process. For this issue, the electrode thicknesses of the busbars of the HJT solar cell were analyzed, and the peel strengths between electrodes and wires were measured after soldering using an infrared (IR) lamp. As a result, the electrodes printed by the screen printing method had a difference in thickness due to screen mask. Also, as the thickness of the electrode increased, the peel strength of the wire increased.

• 마이크로전자및패키징학회지
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• 제18권4호
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• pp.71-77
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• 2011

표면실장형 수동소자인 0402, 0603, 1005 칩에 대한 인쇄 주요인자 결정 및 공정 최적화를 실험계획법을 통해 실시하였다. 실험에 사용된 솔더는 Sn-3.0Ag-0.5Cu와 Sn-0.7Cu이며, 공정변수로는 스텐실 두께, 스퀴지 각도, 인쇄 속도, 기판분리 속도, 스텐실과 기판간의 갭이며, 인쇄압력은 2 $kgf/cm^2$로 고정하였다. 분산분석을 통해 인쇄효율에 영향을 미치는 주요인자가 스텐실 두께와 스퀴지 각도임을 확인할 수 있었다. 주요인자인 스텐실 두께와 스퀴지 각도를 변화시켜 인쇄효율의 최적화 영역을 확인하였고, 0402, 0603, 1005 칩 모두 스퀴지 각도가 $45^{\circ}$ 이하일 경우 인쇄효율이 높았다. 스텐실 두께를 변화할 경우 칩 크기에 따라 인쇄효율이 다른 양상을 보였는데, 0402, 0603 칩에서는 스텐실 두께가 얇을수록 높은 인쇄효율을 보였으며, 1005 칩에서는 스텐실 두께가 두꺼울수록 높은 인쇄효율을 나타내었다.

• 한국전기전자재료학회논문지
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• 제19권7호
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• pp.667-672
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• 2006

Ferroelectric $Pb(Zr_{0.52}Ti_{0.48})O_3$ (PZT(52/48)) thick films were fabricated by the screen-Printing method on the alumina substrates, and $PbTiO_3$ (PT) Precursor solution, which prepared by sol-gel method, was spin-coated on the PZT(52/48) thick films to obtain a densification. Its structural and electrical properties of the PZT(52/48) thick films with the treatment of PT precursor solution coating were investigated. The particle size of the thick films was increased with increasing the number of coatings and the thickness of the PZT-6 (6: number of coatings) films was about $60{\mu}m$. The relative dielectric constant increased and the dielectric loss decreased with increasing the number of PT sol coatings. The relative dielectric constant and dielectric loss of the PZT-6 thick film were 475 and 2 %, respectively. The remanent polarization, coercive field and breakdown strength of the PZT-6 film were $32.6{\mu}C/cm^2$, 15 kV/cm and 60 kV/cm, respectively.

• 대한방사선기술학회지:방사선기술과학
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• 제22권1호
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• pp.43-47
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• 1999

In order to obtain effective utilization of intensifying screens[$CaWO_4(W),\;Gd_2O_2S:Tb(Gd)$, BaFCl : Eu(Ba)] over the diagnostic radiology range, we calculated absorption coefficient (${\mu}$), absorption efficiency (${\eta}_{\alpha}$) and absorbed energy ratio(R) and analyzed effects of these properties on X-ray image, finally concluded as below. Regardless of presence of contrast media, absorption coefficient of Gd the highest and decreased with increase of thickness and kVp. Absorption efficiency related with absorbance of fluorescent materials showed the highest value for the Gd, and discontinuous points exhibited at around $80{\sim}90\;kVp$ and $90{\sim}100kVp$ for the Ba and the Gd, respectively. Furthermore, the absorbed energy ratio(R) correspond to contrast of reflection showed the largest value for the W in the absence of contrast media, and for the Gd in the case of the existence of it, and the ratio was decreased with increasing of incident energy. Owing to these properties, we assumed that it was more preferable to use rare earth type intensifying screen for the radiography using in the C.M.(I, Ba), while in the general radiography, $CaWO_4$ intensifying screen was applicable.

• 대한전기학회논문지:전기물성ㆍ응용부문C
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• 제55권9호
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• pp.429-433
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• 2006

PZT(80/0) 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) precusor solution was spin-coated on the PZT thick films. A concentration of a coating solution was 0.5mol/L and the number of coating was varied from 0 to 6. The porosity decreased and the grain size increased with increasing the number of coatings. The thickness of the PZT-6(6: number of coatings) films was about $60{\mu}m$. The relative dielectric constant increased and the dielectric loss decreased with increasing the number of PZT(20/80) sol coatings. The relative dielectric constant and dielectric loss of the PZT-6 thick film were 275 and 3.5%, respectively. The remanent polarization, coercive field and breakdown strength of the PZT-6 film were $19.8{\mu}C/cm^2$, 13.7kV/cm and 130kV/cm, respectively.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2004년도 추계학술대회 논문집 Vol.17
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• pp.400-403
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• 2004

The dielectric properties of $BaTiO_3/SrTiO_3$ multilayered thick films with printing times were investigated. $BaTiO_3/SrTiO_3$ thick films were deposited by Screen-printing method on alumina substrates. The obtained films were sintered at $1400^{\circ}C$ with bottom electrode(Pt) for 2hours. The structural and the dielectric properties were investigated for various printing times. The BST phase appeared in all of the $BaTiO_3/SrTiO_3$ mutilayered thick films. The $BaTiO_3/SrTiO_3$ multilayered thick film thickness, obtained by one printings, was $50{\mu}m$. The dielectric constant and dielectric loss of the $BaTiO_3/SrTiO_3$ multilayered thick film, obtained by five printings, were about 266, 0.8% at 1Mhz, respectively.

• Transactions on Electrical and Electronic Materials
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• 제4권2호
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• pp.24-28
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• 2003

(Ba,Sr,Ca)TiO$_3$ powders, prepared by the sol-gel method, were mixed with organic binder and the BSCT thick films were fabricated by the screen printing techniques on alumina substrates. All the BSCT thick films, sintered at 1420$^{\circ}C$, showed the typical XRD patterns of a perovskite polycrystalline structure. The average grain sizes decreased with increasing amounts of ZrO$_2$, and the BSCT(40/40/20) thick films doped with 2wt% MnO$_2$ showed a value of 8$\mu\textrm{m}$. The thickness of thick films by four-cycle on printing/drying was approximately 951$\mu\textrm{m}$. The relative dielectric constant decreased with increasing Ca content and MnO$_2$ doping amount. The relative dielectric constant, dielectric loss and tunability of the BSCT(50/40/10) thick films doped with 2.0wt% ZrO$_2$ were 772, 0.184％ and 15.62%, respectively.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2005년도 추계학술대회 논문집 전기물성,응용부문
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• pp.71-73
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• 2005

Ferroelectric PZT heterolayered thick films were fabricated by the alkoxide-based sol-gel method. PZT(20/80) and PZT(80/20) paste were made and alternately screen-printed on the alumina substrates. The coating and drying procedure was repeated 4 times to form the heterolayered thick films. The thickness of the PZT heterolayered thick films was approximately 60 mm. All PZT thick films showed the typical XRD patterns of a perovskite polycrystalline structure. The relative dielectric constant and the dielectric loss of the PZT thick films sintered at $1050^{\circ}C$ were 1382 and 1.90%, respectively. The remanent polarization and coercive field of the PZT thick films sintered at $1050^{\circ}C$ were $14.15{\mu}C/cm^2$ and 19.13kV/cm, respectively.

• 한국전기전자재료학회논문지
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• 제19권11호
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• pp.1014-1019
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• 2006

The influence of the number of solution coatings on the densification of the PZT thick films was studied. PZT powder and PZT precursor solution was prepared by a sol-gel method and PZT thick films were fabricated by the screen-printing method on the alumina substrates. The powder and solution of composition were (A) PZT(80/20)/PZT(20/80), (B) PZT(70/30)/PZT(30/70) and (C) PZT(60/40)/PZT(40/60), (D) PZT(52/48)/PT. The coating and drying procedure was repeated 4 times. And then the PZT precursor solution was spin-coated on the PZT thick films. A concentration of a coating solution was 0.5 moth 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 $60{\mu}m$. A grain size was increased with increasing the coating number. All PZT thick films showed the typical XRD patterns of a typical perovskite polycrystalline structure. The relative dielectric constant of PZT thick films was improved 30-100% as the number of coatings.