• 대한기계학회논문집B
• /
• 제21권1호
• /
• pp.1-14
• /
• 1997

Natural convection cooling of discrete heaters located in a two-dimensional vertical open top cavity is investigated experimentally. The five discrete heaters with same heat generation are located on the wall of the cavity. The heaters are arranged in two configurations; flush-mounted on a vertical wall and protruding from the wall about 4.5 mm. The materials used for the vertical walls are copper and epoxy-resin, and air is used as the cooling fluid. The temperature and flow fields in the cavity were visualized by means of Mach-Zehnder interferometer and smoke-method. Also, local temperature measurements are made along the vertical wall. Results are obtained for cavity aspect ratios of 4.6, 7.5 and 9.5 and modified Rayleigh numbers ranging from 10$^{3}$ to 10$^{6}$ . Results indicate that the cooling efficiency for the copper wall is superior to that of the epoxy-resin. For the epoxy-resin wall, the protrusion of the heaters plays a role in decreasing the heat transfer performance. The location of maximum temperature is significantly influenced by the wall materials and heater configurations. Correlations relating the Nusselt number to the modified Rayleigh number are proposed.

• 한국통신학회논문지
• /
• 제22권6호
• /
• pp.1251-1258
• /
• 1997

Generally, it is very important to study selective coupling between cavities of the filter structure using multimode cavity resonator. In this paper, we have manufactured 5-pole bandpass filter(BPF) using dual and triple-mode cavity resonator. To do so, we have derived the formulas for coupling coefficient about coupling between TE-modes from TM/TE-mode's tangential and lognitudinal field intensities each other. To implement the Chebyshev response, the intercabity slot combining dual-mode and triple-mode is designed to couple one H-field of TE-mode parallel to slot plate. In this paper, specially it is derived the formulas for T $E_{11p}$-mode from TE-modes, and determined after obtaining location and size of intercabity slot from the equation. In this ppaer, based on this result, we designed and implmented teh bandpass filter operated at the center frequency of 14.5GHz with a Chebyshev response. For the manufactured cavity filter, dual-mode and triple-mode cavity are resonted by two orthogonal T $E_{113}$-modes, and by two orthogonal T $E_{113}$-modes and one T $M_{012}$-mode, respecitively. The 2-stage 5-pole BPF proposed in this paper has the insertion loss of -2.32dB, the reflection loss of -15dB in the passband, and the out-or-rejection of -67dB.

• 한국전자파학회논문지
• /
• 제23권4호
• /
• pp.507-514
• /
• 2012

본 논문에서는 함체 내부의 PCB에 있는 트레이스 파원에 의한 함체의 공진 특성 해석법을 제안하고 있다. 함체 내부의 전자계를 계산하기 위해 PCB 트레이스에 형성되는 전류 분포 및 PCB 유전체의 경계면에서 만족하는 경계면 전계 분포에 관한 연립 적분방정식을 유도하였으며, 연립 적분방정식의 해는 Galerkin의 모멘트 법으로 구하고 있다. 그 결과, 함체의 공진 특성은 실험 결과 및 HFSS 툴에 의한 시뮬레이션 결과와도 잘 일치하고 있으며, 함체의 공진 주파수는 PCB 트레이스의 위치에 의해 달라진다는 것을 확인하고 있다. 이론 해석의 타당성을 검증하기 위해 반사 계수의 이론치를 측정치와도 비교하고 있다.

• 소성∙가공
• /
• 제20권5호
• /
• pp.377-386
• /
• 2011

During stamping processes, the air trapped between sheet metal and the die cavity can be highly compressed and ultimately reduce the shape accuracy of formed panels. To prevent this problem, vent holes and passages are sometimes drilled into the based on expert experience and know-how. CAE can be also used for analyzing the air behavior in die cavity during stamping process, incorporating both elasto-plastic behavior of sheet metal and the fluid dynamic behavior of air. This study presents sheet metal forming simulation combined simultaneously with simulation of air behavior in the die cavity. There are three approaches in modeling of air behavior. One is a simple assumption of the bulk modulus having a constant pressure depending on volume change. The next is the use of the ideal gas law having uniform pressure and temperature in air domain. The third is FPM (Finite point method) having non-uniform pressure in air domain. This approach enables direct coupling of mechanical behavior of solid sheet metal and the fluid behavior of air in sheet metal forming simulation, and its result provides the first-hand idea for the location, size and number of the vent holes. In this study, commercial software, PAM-$STAMP^{TM}$ and PAM-$SAFE^{TM}$, were used.

• 한국발생생물학회지:발생과생식
• /
• 제15권4호
• /
• pp.291-299
• /
• 2011

The membranous adhesions could induce implantation failure despite transplantation of high quality of embryo. Clinically, of the patients who have membranous filmy adhesions, endometrial polyps have been found in not infrequently. Thus this study was tried to evaluate the features of endometrial polyps and the effect of endometrial polyps on formation and extents of membranous adhesions in uterine cavity of infertile patients under hysteroscopy. A retrospective study was conducted on 34 infertile patients who were diagnosed as endometrial polyps with membranous adhesions during hysteroscopy from July 2008 to July 2011. Number, size, location and morophologic type of endometrial polyps were investigated. If needed, methylene blue solution was instillated to endometrial cavity to identify membranous adhesions. Then, associations between membranous adhesions with features of endometrial polyps were evaluated. Mean size of endometrial polyp was $1.6{\pm}0.6$ cm, the bigger of endometrial polyps was, the larger of extents of membranous adhesions. (p<0.05). Endometrial polyps were locate evenly in endometrial cavity as follows: anterior uterine wall, 39.1%; posterior uterine wall, 34.8%; lateral uterine wall, 26.1%; upper: 29.4%, middle: 32.4%, lower segment, 35.3%. Mean number of endometrial polyps was $2.26{\pm}1.3$. The pedunculated type was 37.7% and sessile type was 32.4%. There was no statistically significant association of location, number and morphologic type of endometrial polyps with membranous adhesions. In conclusion, hysteroscopy before in vitro fertilization on infertile patients was worthy because of removing of endometrial polyps and membranous adhesions.

• 한국지반환경공학회 논문집
• /
• 제14권12호
• /
• pp.61-69
• /
• 2013

도로 및 철도의 터널 공사가 증가함에 따라 공사 시에 다양한 지반조건에서 터널 공사 단계를 진행하고 있다. 특히, 석회암 지역에서 터널 공사를 진행하게 되는 경우에는 대부분의 공동이 터널 계획구간에 존재하고 있는 실정이다. 하나 또는 그 이상의 공동은 터널의 안정성을 저하하는 것으로 예상된다. 따라서, 본 연구에서는 터널과 공동과의 상호 영향을 알아보고자 실내 모형 축소실험과 수치해석을 시행하였다. 실내모형실험은 터널과 공동 간의 거리에 따른 모형지반의 파괴하중을 확인하였고, 공동의 형상에 따른 파괴하중을 확인하였다. 실내모형실험결과 파괴하중은 공동과 터널 간의 거리가 0.5D 이내로 감소함에 따라서 파괴하중 역시 감소하는 것으로 나타났다. 수치해석은 모형실험의 검증을 위해 시행하였으며, 실내모형실험과 동일하게 터널과 공동 간의 거리가 0.5D 이내로 근접하는 경우 터널의 안정성이 저하되는 것으로 확인되었다.

• 지구물리와물리탐사
• /
• 제12권4호
• /
• pp.338-346
• /
• 2009

콘크리트의 배면에 위치하는 공동을 탐지하기 위해 실제 구조물과 같은 스케일의 모형을 제작하여 비파괴 검사로 널리 사용되는 GPR (ground penetrating radar)탐사와 충격반향기법(IE; impact echo), 충격응답기법(IR; impulse response)을 복합적으로 적용하였다. 콘크리트 모형은 철근 및 공동의 유무에 따라 다양한 반응을 관찰할 수 있도록 설계 하였다. GPR 탐사결과 공동의 유무에 따라 반응의 차이가 나타났지만 정확하게 공동의 존재를 파악하기 어려웠으며, 주로 건전도 측정을 위해 지반조사에 활용되었던 IE 및 IR 기법은 공동의 유무를 구분할 수 있는 반응을 보여주었다. 각 탐사의 적용 결과 철근의 존재에 따라 각 방법별로 배면의 공동을 탐지하는데 반응의 변화가 나타나긴 했지만, 세 가지 방법을 복합적으로 적용하였을 때 단일 탐사를 이용한 결과보다 정확하게 배면 공동의 위치를 파악할 수 있었다.

• 한국소음진동공학회논문집
• /
• 제21권11호
• /
• pp.983-990
• /
• 2011

This paper investigates active noise control(ANC) of a rectangular cavity using single channel filtered-x least mean square(FXLMS) algorithms to globally reduce the interior noise. To obtain the global reduction of the interior noise, multichannel active control should be incorporated in general. We, however, examined firstly the optimal location of the secondary source that produces a global reduction of the interior noise field using single channel control. We then investigated the frequency characteristics of the reduction to yield the effective frequency band of the active control system. It follows that the secondary source should be located as close to the primary source as possible in order to obtain the global reduction.

• 한국안전학회지
• /
• 제15권2호
• /
• pp.111-117
• /
• 2000

In this study, the bearing capacity behavior of strip footing located above a continuous cavity in sand was investigated experimentally. The model footing test was performed in a model box made by using raining method in sand. The model footing test results were compared with those obtained from theoretically proposed equations. The results of the analysis indicate that there is a critical region under the footing. For strip footing, there exists a critical depth below which the presence of the cavity has negligible influence on the footing performance. Only when the cavity is located within this region will the footing performance be significantly affected by the presence of the cavity. The size of the critical region depends on several factors such as footing shape, soil property, cavity size and cavity shape. When the cavity is located within the critical region, the bearing capacity of the footing varies with various factors, such as the size and location of the cavity and the depth of foundation. Based on the experimental study, the following conclusions were induced. 1. The ultimate bearing capacity due to the eccentricity of a underground cavity increases at the rate of the small rather than that due to the depth of a underground cavity. This indicates that the bearing capacity of a strip footing is influenced on the depth rather than the eccentricity of a underground cavity. 2. The critical $depth(D/B)_{cr}$, by underground cavity in sand soil ground that is made by the relative density($D_r$)=55%, 65%, 75%, approaches a range of about 8~10 in case of W/B=1, and about 11~13 in case of W/B=2. 3. In case of the relative density($D_r$) 75%, the most outstanding differential settlement trend is shown in the depth of 4~8cm regardless of the size of cavity, namely, when the value of D/B is 1~2. Therefore, a underground cavity influences on not only the decrease of the bearing capacity but also the differential settlement of a strip footing.

• 한국추진공학회지
• /
• 제24권5호
• /
• pp.13-20
• /
• 2020

초음속 연소기에서 공동 사이의 상대적인 거리가 연소 성능에 미치는 영향을 실험적으로 연구하였다. 사각형 단면 형상에서 마주보는 두 면에 각각 공동형 보염기가 1개씩 있고, 공동 사이의 거리가 135 mm, 220 mm 인 두 가지 형상을 사용하였고, 연료 당량비는 0.16과 0.38로 변경하였다. 직결형 시험 장치를 사용하여 마하 2.0 유동 조건을 조성하였다. 시험 결과 공동 사이의 거리가 가까운 경우에 연소 압력이 더 높았다. 그러나 연료 유량 변화에 의한 연소 압력 변화는 크지 않았다. 추가적인 연소 압력 상승을 얻기 위해서는 보염기 사이의 거리를 더욱 좁히거나 동일면에 보염기를 설치하는 등의 다른 연소기 형상 변화가 있어야 함을 판단하였다.