• 오토저널
• /
• 제8권4호
• /
• pp.43-55
• /
• 1986

소음저감에 대한 연구에서 소음언을 규명하기 위해서 소음의 발생 메카니즘을 안다는 것은 중요 하다. 구조물의 진동과 이로 인해서 발생되는 방사음과의 관계는 상당히 복잡하기 때문에 본 연 구에서는 음향인텐시티의 측정을 위하여 간단한 방사 모델을 대해 연구하였다. 소음원 규명의 첫 단계로서 본 연구에서는 음압측정에 의한 소음평가에 대해 알아 보았다. 두 번째 단계로서 음향 인텐시티법을 이용하여 음향 방사 모우드 패턴을 결정하였으며 음향인텐시티법이 소음원 검출에 유효함을 입증하였다. 또한 본 연구에서는 방진재 부착에 따른 음의 방사특성을 예측하고 방 진재 부착위치를 결정할 수 있었다.

• 태양에너지
• /
• 제12권2호
• /
• pp.9-17
• /
• 1992

This is an experimental work concerning about an application of a heat pipe to an evacuated-glass-tube solar collector system. A methanol heat pipe with length of 0.7 m and diameter of 8 mm was manufactured and tested to compare its performance with that of freon thermosyphon which was originally used in a solar collector system fabricated at Thermomax Co.. Then this methanol heat pipe was utilized to be one component, i.e. heat transfer element, of the present experimental model of a solar collector. This model was performed the operation test as its absorber plate was irradiated by infrared lamps. The following results were obtained. (1) The methanol heat pipe was showed a stable operation when the variation of axial heat transport was $0{\sim}40$ watts and that of inclination angle was $30{\sim}90^{\circ}$. (2) The heat transport capability of the heat pipe was proved to be higher than that of the thermosyphon, because the heat transport limitation of the latter was occured at about 30 watt. (3) The heat pipe in a solar collector was also showed good performance as it transmitted absorbed energy.

• 한국신재생에너지학회:학술대회논문집
• /
• 한국신재생에너지학회 2006년도 춘계학술대회
• /
• pp.222-224
• /
• 2006

A non-vacuum process for $Cu(In,Ga)Se_2$ (CIGS) thin film solar cells from nanoparticle precursors was described in this work CIGS nanoparticle precursors was prepared by a low temperature colloidal route by reacting the starting materials $(CuI,\;InI_3,\;GaI_3\;and\;Na_2Se)$ in organic solvents, by which fine CIGS nanoparticles of about 20nm in diameter were obtained. The nanoparticle precursors were mixed with organic binder material for the rheology of the mixture to be adjusted for the doctor blade method. After depositing the mixture of CIGS with binder on Mo/glass substrate, the samples were preheated on the hot plate in air to evaporate remaining solvents ud to burn the organic binder material. Subsequently, the resultant (porous) CIGS/Mo/glass simple was selenized in a two-zone Rapid Thermal Process (RTP) furnace in order to get a solar ceil applicable dense CIGS absorber layer. Complete solar cell structure was obtained by depositing. The other layers including CdS buffer layer, ZnO window layer and Al electrodes by conventional methods. The resultant solar cell showed a conversion efficiency of 0.5%.

• 태양에너지
• /
• 제20권1호
• /
• pp.21-29
• /
• 2000

본 연구에서는 하루중의 각 시간별로 서로 다른 경사각도별로 수광면에 입사하는 태양에너지의 강도를 실측을 통하여 정량적인 검토와 분석이 가능하도록 측정된 데이터를 기술자료화하고, 각각의 날별로 일사량 강도가 유사한 날들을 그룹화하기 위하여 시간별 일사량 변화에 따른 다항회귀모형을 일별로 산출하고, 각 날별로 서로 비교하기 위해 일별로 산출된 다항회귀모형의 두 그래프사이의 면적을 계산하여 면적의 차가 거의 없는 날들을 일사량 강도가 유사한 날들로 그룹화하는 기법을 개발하여, 월별 또는 전년을 통하여 이들 그룹을 모형별로 제시한다. 또한 다시 이들 모형별로 태양에너지 이용시스템의 효율을 최대화 할 수 있는 시스템 최적경사각도를 제시하여 해당 지역에 적합한 시스템의 최적 설계기준을 제시하고자 한다.

• 대한기계학회논문집A
• /
• 제21권8호
• /
• pp.1250-1258
• /
• 1997

This paper reports on the development of a new foot for a quadrupedal jointed-leg type walking robot. The foot has 2 toes, one at the front and the other at the rear side, for stable landing on uneven ground by point contact. The toes can move up and down independantly, guided by double-wishbone shaped parallel links which enable the lower leg to rotate with respect to a remote center on the ground surface. The motion of each toe is damped by a hydropneumatic shock absorber integrated in the foot in order to absorb the dynamic landing shock. Furthermore, the new foot can reduce the maximum hip joint drive torque by shortening the moment arm length between the hip joint and the landing force vector on the ground. Intensive experiments were carried out in this study by using a one-leg walking model to investigate the soft landing performance of the foot which could be hardly offered by conventional robot feet such as a flat plate with a gimbal type ankle joint. And it was confirmed that the hip joint torque of the leg walking on the flat surface could be reduced remarkably by using the new foot.

• 대한원격탐사학회:학술대회논문집
• /
• 대한원격탐사학회 2005년도 Proceedings of ISRS 2005
• /
• pp.538-541
• /
• 2005

Tidal flats develop along the south coast ofthe Korean peninsula. These areas are famous for sea farming. Specially, strong and coherent radar backscattering signals are observed over oyster sea farms that consist of artificial structures. Tide height in oyster farm is possible to measure by using interferometric phase and intensity of SAR data. It is assumed that the radar signals from oyster farm could be considered as double-bouncing returns by vertical and horizontal bars. But, detailed backscattering mechanism and polarimetric characteristics in oyster farm had not been well studied. We could not demonstrate whether the assumption is correct or not and exactly understand what the properties of back scattering were in oyster farm without full polarimetric data. The results of AIRSAR L-band POLSAR data, experiments in laboratory and JERS-l images are discussed. We carried out an experiment simulating a target structure using vector network analyser (Y.N.A.) in an anechoic chamber at Niigata University. Radar returns from vertical poles are stronger than those from horizontal poles by 10.5 dB. Single bounce components were as strong as double bounce components and more sensitive to antenna look direction. Double bounce components show quasi-linear relation with height of vertical poles. As black absorber replaced AI-plate in bottom surface, double bounce in vertical pole decreased. It is observed that not all oyster farms are characterized by double bounced scattering in AIRSAR data. The image intensity of the double bounce dominant oyster farm was investigated with respect to that of oyster farm dominated by single bounce in JERS-l SAR data. The image intensity model results in a correlation coefficient (R2 ) of 0.78 in double bounce dominant area while that of 0.54 in single bouncing dominant area. This shows that double bounce dominant area should be selected for water height measurement using In8AR technique.

• Journal of Advanced Marine Engineering and Technology
• /
• 제37권8호
• /
• pp.843-848
• /
• 2013

LNG 수요의 증가에 따라, LNG FPSO (부유식 생산저장 하역설비) 선박 및 LNG 선박의 건조도 지속적으로 증가하고 있고, 다양한 형태의 저장탱크 설계가 시도되고 있다. 본 논문에서는 LNG를 저장하는 선박 화물창 내부탱크의 방식으로 5~9% Ni강재를 적용하고, 단열재를 우레탄폼 블록 대신에 펄라이트 분말을 충전하는 새로운 선박 탱크 형식을 제안하였다. 펄라이트 단열재의 적용 가능성을 위하여 필수적으로 검토되어야 하는 펄라이트의 내부탱크 벽체에 가하는 압력, 압력 흡수를 위하여 적용되는 탄성 블랭킷의 특성, 블랭킷의 적정 설계두께, 내부탱크 설계압력 등 설계 인자들을 분석하였다. 연구결과로, 블랭킷의 두께설계 기준은 내부탱크 단열간격의 1/4~1/3 사이가 되어야 하고 적정 두께는 30% 정도가 되었으며, 탱크 설계압력 기준은 블랭킷 두께에 따라 1,500 Pa 이하가 되어야 하는 것으로 얻어졌다.

• 한국항공우주학회지
• /
• 제42권12호
• /
• pp.1037-1044
• /
• 2014

연구에서는 달환경을 고려한 달착륙선 충격흡수장치의 시험장치 구성 및 시험을 수행하였다. 달착륙선은 착륙 시 충격 완화를 위하여 토양이 있는 지역을 착륙지점으로 선정한다. 착륙 시 발생하는 달착륙선의 가속도는 착지면의 특성의 영향을 받아 결정된다. 달착륙선의 충격흡수장치의 시험에서 달 토양을 직접 사용할 수 없기 때문에, 복제토를 사용하여 착륙시험을 수행해야 한다. 본 연구에서는 NASA의 달탐사 프로젝트를 통해 획득된 달 토양의 정보를 기반으로 달 토양과 기계적 성질이 유사한 달 복제토 KAUMLS를 개발하여 달착륙선 충격흡수장치의 낙하시험을 수행하였으며, 지면특성에 따른 충격특성 분석을 위하여 단단한 철판과 건조된 모래위에서의 낙하시험을 수행하였다.

• 한국식품과학회지
• /
• 제11권1호
• /
• pp.8-12
• /
• 1979

알루미늄-아크릴 필림을 사용(使用)한 곡면식(曲面式) 태양열이용장치(太陽熱利用裝置)의 제작(製作)과 이의 한국적(韓國的) 기후조건하(氣候條件下)에서 효능(效能)을 시험(試驗)한 결과(結果) 다음과 같은 결과를 얻었다. 1. 반사집광판(反射集光板)으로 사용(使用)한 알루미늄-아크릴 필림의 반사율(反射率)은 66.1%이었으며 저렴(低廉)한 가격(價格)에 비(比)하여 볼 때 반사판(反射板)으로서 충분(充分)히 이용(利用)할 수 있었다. 2. 흡광부위(吸光部位) 에서의 열이용효율(熱利用?率)은 73%이었으며 2.82 cm/sec의 자연대류(自然對流)에 의(依)한 유속(流速)을 얻을수 있었다. 3. 태양열이용장치(太陽熱利用裝置)를 물의 가온(加溫)에 사용(使用)할 경우 최고(最高) 28.6%의 열이용효율(熱利用?率)을 얻을 수 있었다. 4. 태양열이용장치(太陽熱利用裝置)에 의해 가온(加溫)된 수온(水溫)의 온도차(溫度差)의 대수치(對數値)와 태양열복사(太陽熱輻射)에너지와의 관계는 선형적비례(線型的比例)관계가 성립(成立)되었고 열이용효율(熱利用?率)은 복사에너지량이 클수록 선형적 감소관계가 있었다.

• Journal of Biosystems Engineering
• /
• 제10권1호
• /
• pp.54-68
• /
• 1985

It is desirable to collect the solar thermal energy at relatively high temperature in order to minimize the size of thermal storage system and to enlarge the scope of solar thermal energy utilization. So far the concentrating solar collector has been developed to collect solar thermal energy at relatively high temperature, but it has some difficulties in maintaining the volumetric body of solar collector for long term utilization. On the other hand, the flat-plate solar collector has been developed to collect the solar thermal energy at low temperature, and it has advantages in maintaining the system for long term utilization, since it's thickness is thin and not volumetric. In this study, to develop a solar collector that has both advantages of collecting solar thermal energy at high temperature and fixing conveniently the collector system for long term period, a cylindrical parabolic concentrating solar collector was designed, which has two rows of parabolic reflectors and thin thickness such as the flat-plate solar collector, maintaining the optical form of concentrating solar collector. The characteristics of the concentrating parabolic solar collector newly designed was analysed and the results are summarized as follows; 1. The temperature of the air enclosed in solar collector was all the same as $50^{\circ}C$ in both cases of the open and closed loop, and when the heat transfer fluid was not circulated in tubular absorber, the maximum surface temperature of the absorber was $118-120^{\circ}C$, this results suggested that the heat transfer fluid could be heated up to $118^{\circ}C$. 2. In case of longitudinal installation of the solar collector, the temperature difference of heat transfer fluid between inlet and outlet was $4^{\circ}-6^{\circ}C$ at the flow rate of $110-130{\ell}/hr$, and the collected solar energy per unit area of collector was $300-465W/m^2$. 3. The collected solar energy per unit area for 7 hours was 1960 Kcal/$m^2$ for the open loop and 220 Kcal/$m^2$ for the closed loop. Therefore it is necessary to combine the open and closed loop of solar collectors to improve the thermal efficiency of solar collector. 4. The thermal efficiency of the solar collector (C.P.C.S.C.) was proportional to the density of solar radiation, indicating the maximum thermal efficiency ${\eta}_{max}=58%$ with longitudinal installation and ${\eta}_{max}=45%$ with lateral installation. 5. The thermal efficiency of the solar collector (C.P.C.S.C.) was increased in accordance with the increase of flow rate of heat transfer fluid, presenting the flow rate of $110{\ell}/hr$ was the value of turning point of the increasing rate of the collector efficiency, therefore the flow rate of $110{\ell}/hr$ was considered as optimum value for the test of the solar collector (C.P.C.S.C.) performance when the heat transfer fluid is a liquid. 6. In both cases of longitudinal and lateral installation of the solar collector (C.P.C.S.C.), the thermal efficiency was decreased linearly with an increase in the value of the term ($T_m-T_a$)/Ic and the increasing rate of the thermal efficiency was not effected by the installation method of solar collector.