• 제목/요약/키워드: Thermal Contact

검색결과 1,208건 처리시간 0.028초

1-propanol 첨가에 따른 이산화타이타늄(TiO2) 광 촉매의 비표면적 향상 및 이산화탄소 환원 효율 향상 (Improvement of Carbon Dioxide Reduction Efficiency of Titanium Dioxide Photocatalyst Using 1-propanol)

  • 하윤태;권진범;안희경;정대웅
    • 센서학회지
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    • 제31권5호
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    • pp.343-347
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    • 2022
  • Recently, the problem of global warming caused by greenhouse gases is getting serious due to the development of industry and the increase in transportation means. Accordingly, the need for a technology to reduce carbon dioxide, which accounts for most of the greenhouse gas, is increasing. Among them, a catalyst for converting carbon dioxide into fuel is being actively studied. Catalysts for reducing carbon dioxide are classified into thermal catalysts and photocatalysts. In particular, the photocatalyst has the advantage that carbon dioxide can be reduced only by irradiating ultraviolet rays at room temperature without high temperature or additional gas. TiO2 is widely used as a photocatalyst because it is non-toxic and has high stability, but has a disadvantage of low carbon dioxide reduction efficiency. To increase the reduction efficiency, 1-propanol was used in the synthesis process. This prevents agglomeration of the catalyst and increases the specific surface area and pores of TiO2, thereby increasing the surface area in contact with carbon dioxide. As a result of measuring the CO2 reduction efficiency, it was confirmed that the efficiency of TiO2 with 1-propanol and TiO2 without 1-propanol was 19% and 12.3%, respectively, and the former showed a 1.5 times improved efficiency.

볼 밀링 조건이 TiH2 분말의 미세조직과 탈수소화 거동에 미치는 영향 (Effect of Ball Milling Conditions on the Microstructure and Dehydrogenation Behavior of TiH2 Powder)

  • 김지영;이의선;최지원;김영민;오승탁
    • 한국분말재료학회지
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    • 제31권2호
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    • pp.132-136
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    • 2024
  • This study investigated the effects of revolution speed and ball size in planetary milling on the microstructure and dehydrogenation behavior of TiH2 powder. The particle size analysis showed that the large particles present in the raw powder were effectively refined as the revolution speed increased, and when milled at 500 rpm, the median particle size was 1.47 ㎛. Milling with a mixture of balls of two or three sizes was more effective in refining the raw powder than milling with balls of a single size. A mixture of 3 mm and 5 mm diameter balls was the optimal condition for particle refinement, and the measured median particle size was 0.71 ㎛. The dependence of particle size on revolution speed and ball size was explained by changes in input energy and the number of contact points of the balls. In the milled powder, the endothermic peak measured using differential thermal analysis was observed at a relatively low temperature. This finding was interpreted as the activation of a dehydrogenation reaction, mainly due to the increase in the specific surface area and the concentration of lattice defects.

Numerical and experimental analysis on the axial compression performance of T-shaped concrete-filled thin-walled steel

  • Xuetao Lyu;Weiwei Wang;Huan Li;Jiehong Li;Yang Yu
    • Steel and Composite Structures
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    • 제50권4호
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    • pp.383-401
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    • 2024
  • The research comprehensively studies the axial compression performance of T-shaped concrete-filled thin-walled steel tubular (CTST) long columns after fire exposure. Initially, a series of tests investigate the effects of heating time, load eccentricity, and stiffeners on the column's performance. Furthermore, Finite Element (FE) analysis is employed to establish temperature and mechanical field models for the T-shaped CTST long column with stiffeners after fire exposure, using carefully determined key parameters such as thermal parameters, constitutive relations, and contact models. In addition, a parametric analysis based on the numerical models is conducted to explore the effects of heating time, section diameter, material strength, and steel ratio on the axial compressive bearing capacity, bending bearing capacity under normal temperature, as well as residual bearing capacity after fire exposure. The results reveal that the maximum lateral deformation occurs near the middle of the span, with bending increasing as heating time and eccentricity rise. Despite a decrease in axial compressive load and bending capacity after fire exposure, the columns still exhibit desirable bearing capacity and deformability. Moreover, the obtained FE results align closely with experimental findings, validating the reliability of the developed numerical models. Additionally, this study proposes a simplified design method to calculate these mechanical property parameters, satisfying the ISO-834 standard. The relative errors between the proposed simplified formulas and FE models remain within 10%, indicating their capability to provide a theoretical reference for practical engineering applications.

Overview of separate effect and integral system tests on the passive containment cooling system of SMART100

  • Jin-Hwa Yang;Tae-Hwan Ahn;Hong Hyun Son;Jin Su Kwon;Hwang Bae;Hyun-Sik Park;Kyoung-Ho Kang
    • Nuclear Engineering and Technology
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    • 제56권3호
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    • pp.1066-1080
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    • 2024
  • SMART100 has a containment pressure and radioactivity suppression system (CPRSS) for passive containment cooling system (PCCS). This prevents overheating and over-pressurization of a containment through direct contact condensation in an in-containment refueling water storage tank (IRWST) and wall condensation in a CPRSS heat exchanger (CHX) in an emergency cool-down tank (ECT). The Korea Atomic Energy Research Institute (KAERI) constructed scaled-down test facilities, SISTA1 and SISTA2, for the thermal-hydraulic validation of the SMART100 CPRSS. Three separate effect tests were performed using SISTA1 to confirm the heat removal characteristics of SMART100 CPRSS. When the low mass flux steam with or without non-condensable gas is released into an IRWST, the conditions for mitigation of the chugging phenomenon were identified, and the physical variables were quantified by the 3D reconstruction method. The local behavior of the non-condensable gas was measured after condensation inside heat exchanger using a traverse system. Stratification of non-condensable gas occurred in large tank of the natural circulation loop. SISTA2 was used to simulate a small break loss-of-coolant accident (SBLCOA) transient. Since the test apparatus was a metal tank, compensations of initial heat transfer to the material and effect of heat loss during long-term operation were important for simulating cooling performance of SMART100 CPRSS. The pressure of SMART100 CPRSS was maintained below the design limit for 3 days even under sufficiently conservative conditions of an SBLOCA transient.

열화상카메라를 이용한 정상안과 건성안의 서모그래피 비교 (Thermographic Assessment in Dry Eye Syndrome, Compared with Normal Eyes by Using Thermography)

  • 박창원;이옥진;이승원
    • 한국안광학회지
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    • 제20권2호
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    • pp.247-253
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    • 2015
  • 목적: 열화상카메라를 이용하여 정상안 군과 건성안 군의 검결막과 안구표면의 서모그래피를 객관적으로 알아보고자 하였다. 방법: 각막질환, 안외상, 누도이상자, 안과수술 병력 등 안구표면의 눈물막에 영향을 주는 질환이 없고 콘택트렌즈를 사용하지 않는 대학생 72명(144안)을 대상으로 하였다. TBUT, Schirmer I test, McMonnies test를 시행하여 정상안 군과 건성안 군으로 분류하고 열화상카메라(Cox CX series, Answer co., Korea)를 이용하여 안구표면과 검결막의 온도변화를 분석하였다. 결과: 정상안 군에서 안구표면 눈물막의 중심부, 코방향, 귀방향, 위, 아래방향에서 온도변화량은 $-0.13{\pm}0.08$, $-0.14{\pm}0.08$, $-0.12{\pm}0.08$, $-0.14{\pm}0.08$, $-0.10{\pm}0.09(^{\circ}C/sec)$이었고 건성안군에서는 $-0.17{\pm}0.08$, $-0.16{\pm}0.07$, $-0.16{\pm}0.08$, $-0.17{\pm}0.09$, $-0.15{\pm}0.08(^{\circ}C/sec)$로 중심부, 귀방향, 아래방향에서 유의성을 띠었다(p<0.05). 정상안 군으로 분류된 대상자의 중심부, 코방향, 귀방향의 검결막 온도는 $34.36{\pm}1.12$, $34.17{\pm}1.10$, $34.07{\pm}1.12^{\circ}C$였고, 건성안 군은 $34.17{\pm}1.10$, $33.43{\pm}0.97$, $33.51{\pm}1.06^{\circ}C$로 중심부에서 유의한 차이를 보였다(p=0.05). 결론: 건성안 군에서 정상안 군보다 안구표면의 온도 감소가 빠르게 나타났고 검결막의 온도도 낮은 것으로 관찰되었다. 열화상카메라를 활용한 안구표면의 온도변화는 눈물막의 안정성을 평가하는데 객관적이었으며 건성안 연구에 유용할 것으로 기대된다.

폭염 시 어린이공원의 온열환경 (Thermal Environments of Children's Parks during Heat Wave Period)

  • 류남형;이춘석
    • 한국조경학회지
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    • 제44권6호
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    • pp.84-97
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    • 2016
  • 본 연구는 폭염 시 어린이공원 내 포장 및 차양의 유형에 따른 온열환경을 규명하고자 하였다. 이를 위해 진주기상대에서 측정한 일 최고기온이 $35.9{\sim}36.8^{\circ}C$를 나타낸 2016년 8월 11일부터 8월 13일까지 3일간 진주시내 어린이공원 2곳(칠암어린이공원: $N\;35^{\circ}11^{\prime}1.4{^{\prime}^{\prim}}$, $E\;128^{\circ}531.7{^{\prime}^{\prime}}$, 표고: 38m; 가호제12어린이공원: $N\;35^{\circ}09^{\prime}56.8{^{\prime}^{\prime}}$, $E\;128^{\circ}6^{\prime}41.1{^{\prime}^{\prime}}$, 표고: 24m)의 모래밭, 고무칩포장지, 쉘터, 녹음지를 대상으로 미기상을 측정하였다. 미기상환경으로서 지상 60cm 높이에서 기온, 흑구온도, 상대습도, 풍속, 6방향의 장파 및 단파 복사를 측정하였고, 이를 바탕으로 열스트레스 지수인 WBGT와 UTCI를 산정 및 분석하였다. 또한 열화상카메라로 포장면과 놀이시설의 표면온도를 측정하였으며, 이를 바탕으로 단시간 피부접촉시 화상의 위험을 평가하였다. 연구결과는 다음과 같다. 어린이공원의 3일 시간 평균 최고 기온은 $36.6{\sim}39.4^{\circ}C$였으며, 모래밭에 비해 녹음에서 $2.8^{\circ}C$, 쉘터에서 $1.0^{\circ}C$$2.3^{\circ}C$ 낮게 나타났다. 시간 평균 최저 습도는 44~50%였으며, 모래밭이나 고무칩포장지에 비해 녹음에서 6%, 쉘터에서 4% 및 6% 높게 나타났다. 열사병위험지수 WBGT 값에 근거하면 폭염 시 어린이공원의 주간의 열사병 위험도는 높은 또는 극심한 정도로 나타났다. 3일 30분 평균 최고 WBGT 값은 $31.2{\sim}33.6^{\circ}C$였으며, 모래밭에 비해 녹음에서 $2.8^{\circ}C$, 쉘터에서 $2.3^{\circ}C$$1.0^{\circ}C$ 낮게 나타났으나, 차양에 의해서도 열사병 위험을 피할 수는 없었다. 체감더위지수 UTCI 값에 근거하면 폭염 시 어린이공원의 주간의 온열 스트레스의 범주는 매우 강한 또는 극심한 정도로 나타났다. 3일 30분 평균 최고 UTCI 값은 $39.9{\sim}48.1^{\circ}C$였으며, 모래밭에 비해 녹음에서 $7.8^{\circ}C$, 쉘터에서 $8.2^{\circ}C$$4.1^{\circ}C$ 낮게 나타났으나, 차양에 의해서도 극심한 또는 매우 강한 온열 스트레스를 강한 또는 적정한 온열 스트레스로 낮출 수는 없었다. 단시간 피부접촉에 의한 화상 온도 기준에 따르면, 놀이시설 및 포장면의 최고 표면온도가 스텐레스 스틸($70.8^{\circ}C$)은 무도장 철재 3초 $60^{\circ}C$, 고무칩포장($76.5^{\circ}C$)은 플라스틱 5초 $74^{\circ}C$, 청색 플라스틱 미끄럼판($68.5^{\circ}C$)과 앉음판($71.0^{\circ}C$)은 플라스틱 1분 $60^{\circ}C$ 기준을 초과한 것으로 나타났다. 하지만 그늘이 진 놀이시설의 표면온도는 햇빛에 노출된 놀이시설의 표면온도에 비해 $20^{\circ}C$ 내외로 낮게 나타나, 차양에 의해 화상의 위험을 현저하게 개선할 수 있을 것으로 판단된다. 폭염 시에는 어린이공원의 온열환경은 어린이들에게 높거나 극심한 열사병 위험에 빠지게 하고, 매우 강한 또는 극심한 온열 스트레스를 주기 때문에 보호자나 관리자가 어린이들의 어린이공원 이용을 제한해야 한다. 그리고 폭염시에는 어린이공원의 포장면 또는 놀이시설에 의한 화상의 위험이 매우 높으므로 이용 시 주의를 해야 하며, 화상의 예방을 위해서는 차양시설을 적극적으로 도입해야 한다.

The Development of an Electroconductive SiC-ZrB2 Composite through Spark Plasma Sintering under Argon Atmosphere

  • Lee, Jung-Hoon;Ju, Jin-Young;Kim, Cheol-Ho;Park, Jin-Hyoung;Lee, Hee-Seung;Shin, Yong-Deok
    • Journal of Electrical Engineering and Technology
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    • 제5권2호
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    • pp.342-351
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    • 2010
  • The SiC-$ZrB_2$ composites were fabricated by combining 30, 35, 40, 45 and 50 vol. % of zirconium diboride ($ZrB_2$) powders with silicon carbide (SiC) matrix. The SiC-$ZrB_2$ composites and the sintered compacts were produced through spark plasma sintering (SPS) under argon atmosphere, and its physical, electrical, and mechanical properties were examined. Also, the thermal image analysis of the SiC-$ZrB_2$ composites was examined. Reactions between $\beta$-SiC and $ZrB_2$ were not observed via x-ray diffraction (XRD) analysis. The apparent porosity of the SiC+30vol.%$ZrB_2$, SiC+35vol.%$ZrB_2$, SiC+40vol.%$ZrB_2$, SiC+45vol.%$ZrB_2$ and SiC+50vol.%$ZrB_2$ composites were 7.2546, 0.8920, 0.6038, 1.0981, and 10.0108%, respectively. The XRD phase analysis of the sintered compacts demonstrated a high phase of SiC and $ZrB_2$. Among the $SiC+ZrB_2$ composites, the SiC+50vol.%$ZrB_2$ composite had the lowest flexural strength, 290.54MPa, the other composites had more than 980MPa flexural strength except the SiC+30vol.%$ZrB_2$ composite; the SiC+40vol.%$ZrB_2$ composite had the highest flexural strength, 1011.34MPa, at room temperature. The electrical properties of the SiC-$ZrB_2$ composites had positive temperature coefficient resistance (PTCR). The V-I characteristics of the SiC-$ZrB_2$ composites had a linear shape in the temperature range from room to $500^{\circ}C$. The electrical resistivities of the SiC+30vol.%$ZrB_2$, SiC+35vol.%$ZrB_2$, SiC+40vol.%$ZrB_2$ SiC+45vol.%$ZrB_2$ and SiC+50vol.%$ZrB_2$ composites were $4.573\times10^{-3}$, $1.554\times10^{-3}$, $9.365\times10^{-4}$, $6.999\times10^{-4}$, and $6.069\times10^{-4}\Omega{\cdot}cm$, respectively, at room temperature, and their resistance temperature coefficients were $1.896\times10^{-3}$, $3.064\times10^{-3}$, $3.169\times10^{-3}$, $3.097\times10^{-3}$, and $3.418\times10^{-3}/^{\circ}C$ in the temperature range from room to $500^{\circ}C$, respectively. Therefore, it is considered that among the sintered compacts the SiC+35vol.%$ZrB_2$, SiC+40vol.%$ZrB_2$ and SiC+45vol.%$ZrB_2$ composites containing the most outstanding mechanical properties as well as PTCR and V-I characteristics can be used as an energy friendly ceramic heater or ohmic-contact electrode material through SPS.

Perfluoropolymer Membranes of Tetrafluoroethylene and 2,2,4Trifluofo- 5Trifluorometoxy- 1,3Dioxole.

  • Arcella, V.;Colaianna, P.;Brinati, G.;Gordano, A.;Clarizia, G.;Tocci, E.;Drioli, E.
    • 한국막학회:학술대회논문집
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    • 한국막학회 1999년도 The 7th Summer Workshop of the Membrane Society of Korea
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    • pp.39-42
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    • 1999
  • Perfluoropolymers represent the ultimate resistance to hostile chemical environments and high service temperature, attributed to the presence of fluorine in the polymer backbone, i.e. to the high bond energy of C-F and C-C bonds of fluorocarbons. Copolymers of Tetrafluoroethylene (TEE) and 2, 2, 4Trifluoro-5Trifluorometoxy- 1, 3Dioxole (TTD), commercially known as HYFLON AD, are amorphous perfluoropolymers with glass transition temperature (Tg)higher than room temperature, showing a thermal decomposition temperature exceeding 40$0^{\circ}C$. These polymer systems are highly soluble in fluorinated solvents, with low solution viscosities. This property allows the preparation of self-supported and composite membranes with desired membrane thickness. Symmetric and asymmetric perfluoropolymer membranes, made with HYFLON AD, have been prepared and evaluated. Porous and not porous symmetric membranes have been obtained by solvent evaporation with various processing conditions. Asymmetric membranes have been prepared by th wet phase inversion method. Measure of contact angle to distilled water have been carried out. Figure 1 compares experimental results with those of other commercial membranes. Contact angles of about 120$^{\circ}$for our amorphous perfluoropolymer membranes demonstrate that they posses a high hydrophobic character. Measure of contact angles to hexandecane have been also carried out to evaluate the organophobic character. Rsults are reported in Figure 2. The observed strong organophobicity leads to excellent fouling resistance and inertness. Porous membranes with pore size between 30 and 80 nanometers have shown no permeation to water at pressures as high as 10 bars. However high permeation to gases, such as O2, N2 and CO2, and no selectivities were observed. Considering the porous structure of the membrane, this behavior was expected. In consideration of the above properties, possible useful uses in th field of gas- liquid separations are envisaged for these membranes. A particularly promising application is in the field of membrane contactors, equipments in which membranes are used to improve mass transfer coefficients in respect to traditional extraction and absorption processes. Gas permeation properties have been evaluated for asymmetric membranes and composite symmetric ones. Experimental permselectivity values, obtained at different pressure differences, to various single gases are reported in Tab. 1, 2 and 3. Experimental data have been compared with literature data obtained with membranes made with different amorphous perfluoropolymer systems, such as copolymers of Perfluoro2, 2dimethyl dioxole (PDD) and Tetrafluorethylene, commercialized by the Du Pont Company with the trade name of Teflon AF. An interesting linear relationship between permeability and the glass transition temperature of the polymer constituting the membrane has been observed. Results are descussed in terms of polymer chain structure, which affects the presence of voids at molecular scale and their size distribution. Molecular Dyanmics studies are in progress in order to support the understanding of these results. A modified Theodoru- Suter method provided by the Amorphous Cell module of InsightII/Discover was used to determine the chain packing. A completely amorphous polymer box of about 3.5 nm was considered. Last but not least the use of amorphous perfluoropolymer membranes appears to be ideal when separation processes have to be performed in hostile environments, i.e. high temperatures and aggressive non-aqueous media, such as chemicals and solvents. In these cases Hyflon AD membranes can exploit the outstanding resistance of perfluoropolymers.

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백내장수술 안에서 열화상카메라를 이용한 안구표면 온도의 변화 (Thermographic Assessment on Temperature Change of Eye Surface in Cataract Surgery Observation)

  • 박창원;안영주;김효진
    • 대한시과학회지
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    • 제20권4호
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    • pp.497-504
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    • 2018
  • 목적 : 백내장 환자를 대상으로 수술 전과 후의 안구표면의 온도변화 양상을 열화상카메라의 서모그래피를 이용하여 연구 하고자 하였다. 방법 : 본 연구는 백내장 수술을 받은 환자 50-79세까지 75명 75안의 환자 군을 대상으로 하였다. 과거에 굴절교정수술, 각막관련 수술을 받은 자와 콘택트렌즈를 사용하는 자, 눈물관 이상자, 전신질환 치료 약물을 복용하는 자 등 눈물분비와 눈물막에 영향을 줄 수 있는 자는 연구 대상자에서 제외하였고 눈물막파괴시간 검사(Tear Break Up Time, BUT), 쉬르머 검사(Schirmer's Test), 맥모니테스트(Mcmonnies questionnaire)를 시행한 후 열화상카메라(Cox CX series, Answer., Korea)를 이용하여 안구표면의 온도변화를 실시간으로 측정하였다. 결과 : 전체 대상자의 술 전 안구표면 온도는 $35.20{\pm}0.54^{\circ}C$이었고 술 후에는 $35.30{\pm}0.53^{\circ}C$로 표면온도가 상승하였으나 유의한 차이를 보이지 않았다. 안구표면 온도변화는 술전에서 $-0.12{\pm}0.08{\Delta}$ ($^{\circ}C/sec$)에서 술 후 $-0.18{\pm}0.07{\Delta}$ ($^{\circ}C/sec$)로 통계학적으로 유의한 결과를 나타냈다. 연령 별 비교에서는, 50 대군은 백내장 술 전 대상자의 안구표면 온도변화가 $-0.14{\pm}0.09{\Delta}$ ($^{\circ}C/sec$)에서 $-0.19{\pm}0.05{\Delta}$ ($^{\circ}C/sec$)으로 나타났고 60 대군에서는 $-0.12{\pm}0.08{\Delta}$ ($^{\circ}C/sec$)에서 $-0.15{\pm}0.07{\Delta}$ ($^{\circ}C/sec$)으로 나타났으며 70 대군에서는 술 전 대상자의 안구표면 온도변화는 $-0.12{\pm}0.08{\Delta}$($^{\circ}C/sec$)에서 $-0.18{\pm}0.07{\Delta}$($^{\circ}C/sec$)으로 전 연령에서 모두 유의한 안구표면 온도변화를 보였다. 결론 : 백내장 술 후에는 안구건조증 평가지표가 모두 감소하였고 안구표면 온도변화가 유의함을 보였다. 안구표면의 서모그래피 기술은 비침습적으로 안구건조증을 평가하는데 용이하였고 객관적으로 수치화할 수 있는 장점이 있어 다양한 안구건조증 연구에 활용 될 것으로 기대된다.

S확산에 의한 $n^+-p^+$ InP 태양전지의 제작 (The Fabrication of $n^+-p^+$ InP Solar Cells by the Diffusion of Sulphur)

  • 정기웅;김선태;문동찬
    • 태양에너지
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    • 제10권3호
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    • pp.60-65
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    • 1990
  • [ $p^+$ ]형의 InP 기판($p=4{\times}10^{18}cm^{-3}$)에 일정 온도에서 S를 열 확산시켜 $n^+-p^+$ 접합을 형성하고, $n^+$형 측에 사진식각법으로 폭 $20{\mu}m$의 표면 격자상 전극을 $300{\mu}m$ 간격으로 형성한 후, 반사방지(AR) 막으로 $600{\AA}$ 두께의 SiO 박막을 증착시켜 크기 $5{\times}5{\times}0.3mm^3$$n^+-p^+$ InP 동종접합 태양전지를 제작하였다. S의 접합깊이는 약 $0.4{\mu}m$이었으며, 제작된 태양전지는 확산시간이 증가함에 따라 단락전류($J_{sc}$)가 증가하였고, 충진율(F.F)이 감소하였으며, 직렬저항($R_s$)과 에너지 변환효율(${\eta}$)이 증가하는 경향을 나타냈다. $5,000-9,000{\AA}$의 파장 영역에서 양호한 분광감도 특성을 나타냈으며, 단락전류, 개방전압($V_{oc}$), 충진율, 에너지 변환효율이 각각 $13.16mA/cm^2$, 0.38V, 53.74%, 10.1%인 태양전지를 제작하였다.

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