Background: We have hypothesized that, if a low resistant gravity-flow membrane oxygenator is used, then the twin blood sacs of TPLS can be located at downstream of the membrane oxyenator, which may ...double the pulse rate at a given pump rate and increase the pump output. The purpose of this study was to determine the optimal configuration for the ECLS circuits by using the concept of pulse energy and pump output. Material and Method: Animals were randomly assigned to 2 groups in a total cardiopulmonary bypass model. In the serial group, a conventional membrane oxygenator was located between the twin blood sacs. In the parallel group, the twin blood sacs were placed downstream of the gravity-flow membrane oxygenator. Energy equivalent pressure (EEP) and pump output were collected at pump-setting rates of 30, 40, and 50 BPM. Result: At the given pump-setting rate, the pulse rate was doubled in the parallel group. Percent changes of mean arterial pressure to EEP were $13.0\pm1.7,\; 12.0\pm1.9\;and\;7.6\pm0.9\%$ in the parallel group, and $22.5\pm2.4,\; 23.2\pm1.9,\;and\;21.8\pm1.4\%$ in the serial group at 30, 40, and 50 BPM of pump-setting rates. Pump output was higher in the parallel circuit at 40 and 50 BPM of pump-setting rates $(3.1\pm0.2,\;3.7\pm0.2L/min\;vs.\;2.2\pm0.1\;and\;2.5\pm0.1L/min,\;respectively,\;p=0.01)$. Conclusion: Either parallel or serial circuit configuration of the ECLS generates effective pulsatility. As for the pump out, the parallel circuit configuration provides higher flow than the serial circuit configuration. 배경: 체외순환장치 중 막형산화기를 사용하는 인공심폐기나 생명구조장치(Extra-corporeal Life Support System; ECLS)는 혈액이 통과하기 위해 막형산화기 전방에 구동점프가 요구된다. 국내에서 개발된 박동식 생명구조장치(T-PLS)의 경우는 막형산화기가 두 개의 혈액주머니 사이에 위치하여 액츄에이터가 번갈아 까내는 구조로 되어 있다 저자 등은, 만일 저항이 낮은 gravity-flow hollow fiber 막형산화기를 사용한다면 두 개의 혈액주머니와 박동점프를 막형산화기 후방에 설치하는 것이 가능하며, 이러한 구조는 같은 펌프박동 조건에서 2배의 맥박수를 보장하므로 펌프박출량이 증가될 것으로 가정하였다. 본 실험은 한국형 생명구조장치의 회로구성을 최적화하기 위해 계획되었으며, 기존의 막형산화기를 사용한 직렬회로구조와 gravity-flow hollow fiber 막형산화기를 이용한 병렬회로 구조를 박동에너지와 펌프박출량을 이용하여 비교하였다. 대상 및 방법: 실험은 $35\~45kg$의 돼지 12마리에서 심실세동혈 심정지 모델을 만들었으며, T-PLS 회로구성 형태에 따라 두 군으로 나누었다. 직렬군은 두 개의 혈액주머니 중간에 기존 막형산화기를 직렬로 설치하였으며, 병렬군은 gravity-flow hollow fiber막형산화기 후방에 이중구동점프를 병렬로 설치하였다. 펌프박출량은 대동맥 도관에서 직접 혈류를 측정하였고, 등가압력에너지(EEP)는 실시간으로 컴퓨터에 저장된 펌프박출곡선과 하행대동맥 혈압곡선에서 계산하였다. 각 지표는 점프속도 30, 40, 50 BPM에서 매번 측정하였다. 결과: 두 군 모두 박동에너지 측면에서 충분한 박동성을 보여주었다. 점프속도 30, 40, 50 BPM에서 EEP와 평균동맥압의 변화율은 병렬군의 경우 $13.0\pm.7\%,\;12.0\pm1.9\%,\;and\;7.6\pm0.9\%$였으며, 직렬군의 경우 $22.5\pm2.4\%,\;23.2\pm1.9\%,\;and\;21.8\pm1.4\%$였다. 점프박출량의 경우는 점프속도 40, 50 BPM에서 병렬군의 경우 $3.1\pm0.2\;and\;3.7\pm0.2L/min$였으며, 직렬군의 경우 $2.2\pm0.1\;and\;2.5\pm0.1\;L/min$였다(p<0.05). 결론: 혈류 저항이 낮은 gravity-flow 막형산화기를 사용하여 T-PLS 구동점프를 병렬회로로 배치할 경우 효과적인 박동성은 유지하면서, 기존의 막형산화기를 이용한 직렬회로 구조에 비해 점프박출량을 증가시켰다.
In this paper, the thermal buckling and postbuckling behaviour of composite beam with embedded shape memory alloy (SMA) wires are investigated experimentally and analytically. The results of thermal ...buckling tests on uniformly heated, clamped, composite beam embedded with SMA wire actuators are presented and discussed in consideration of geometric imperfections, slenderness ratio of beam and embedding position of SMA wire actuators. The shape recovery force can reduce the thermal expansion of composite laminated beam, which result in increment of the critical buckling temperature and reduction of the lateral deflection of postbuckling behaviours. It is presented quantitatively on the temperature-load-deflection behaviour records how the shape recovery force affects the thermal buckling. The cross tangential method is suggested to calculate the critical buckling temperature on the temperature-deflection plot. Based on the experimental analysis, the new formula is also proposed to describe the critical buckling temperature of a laminated composite beam with embedded SMA wire actuators. 형상기억합금 선을 삽입한 복합적층 보의 열좌굴 및 좌굴후 거동을 해석 및 실험적으로 고찰하였다. 균일한 온도분포, 양단고정 상태에서 형상기억합금 선을 삽입한 복합적층 보의 열좌굴 거동을 나타내었고 검토하였다. 삽입한 형상기억합금 선의 형상회복력은 복합적층 보의 열팽창 변형률을 감소시킴으로써 임계좌굴온도를 증가시키고 좌굴후 거동에서 횡방향 변형을 감소시키는 결과를 얻을 수 있었다. 형상회복력이 열좌굴에 미치는 영향을 온도-하중-횡방향 변위의 거동결과에서 세장비, 기하학적 초기결함, 형상기억합금 선의 삽입 위치 등의 설계변수를 고려하여 정량적으로 나타내었다. 온도-횡방향 변형의 결과로부터 임계좌굴온도를 구하는 접선교차점의 방법을 제안하였다. 열좌굴 및 좌굴후 거동에서 실험결과의 해석을 바탕으로 형상회복력이 임계좌굴온도에 미치는 영향을 나타내는 이론적인 식을 제시하였다.
In this paper, an experimental study on the buckling and postbuckling control of a laminated composite beam with eccentrically embedded SMA wire actuators is performed. For the purpose of enhancing ...the critical buckling load, buckling control is investigated through the use of reactive moment associated with the shape recovery force of SMA wire actuators. To improve the control authority for the buckling and postbuckling control of the SMA-composite beam, closed-loop control is used. The buckling and postbuckling control behaviours are presented and discussed qualitatively and quantitatively on loaddeflection plots considering the stacking sequence of the laminate, slenderness ratio of the beam and activation conditions of the SMA wire actuators. By maintaining the desired deflection shape with the proper reactive moment, buckling control can be extended to the postbuckling of the SMA-composite beam subjected to an external load. 본 연구에서는 형상기억합금 선을 편심하게 삽입한 복합적층 보의 좌굴 및 좌굴후 제어에 관한 실험결과를 나타내었다. 임계좌굴하중을 향상하기 위하여 형상회복모멘트의 특성을 활용하였다. 좌굴제어의 범위를 향상시키기 위해 페루프 제어를 사용하여 좌굴후 제어의 거동을 검토하였다. 이러한 좌굴제어 실험을 통하여, 임계좌굴하중을 증가시키고 좌굴모드가 반대방향으로 변화하는 거동을 보의 세장비 및 기하학적 초기결함, 형상기억합금 선의 삽입 위치 등을 고려하여 하중-변위의 결과로부터 정량적, 정성적으로 분석하였다. 적당한 형상회복모멘토를 이용하여 원하는 변형형상을 유지함으로써 외부하중을 받는 보의 좌굴후 제어에서도 적용할 수 있다.
This research has a purpose to achieve experimental data used for design of ventilation systems necessary for indoor air quality control and their operation and management. For the study, spatial ...concentration distribution of indoor air quality according to pollutant site in a simplified model chamber. In low flow ventilation, flow pattern of indoor air was mainly influenced by diffusion and additionally, spatial distribution was formed by convection. Distribution of ventilation efficiency according to each pattern of model chamber was evaluated. It was confirmed that diffusion patterns of a pollutant among sites were formed, centering around main stream areas of supply and exhaust outlets.
A Fourier transform infrared spectrophotometric method was described for the determination of quartz, mica(sericite) and feldspar(potassium feldspar) in respirable dust in Taebaek area. The results ...were as follows; 1) The concentration of minerals were determined from the intensity of absorption peak of quartz at $799cm^{-1}$, sericite at $539cm^{-1}$, and potassium feldspar at $648cm^{-1}$ respectively. 2) The precision(C. V. %) for the quartz determination was $7.70{\pm}2.68%$ from 10 to $200{\mu}g$ of quartz. 3) The precision for the sericite determination was $16.34{\pm}6.82%$ from 30 to $500{\mu}g$ of serictite. 4) The precision for the potassium feldspar determination was $5.28{\pm}1.74%$ from 30 to $500{\mu}g$ of potassium feldspar. 5) The concentration of respirable dust in Taebaek area was $4.90{\pm}3.29mg/m^3$ (0.4-93.7%), percent quartz was $1.80{\pm}4.14%$ (0.01-20.56%), percent sericite was $11.37{\pm}6.43%$ (0.00-29.69%), percent potassium feldspar was 8.15% (n=7, 3.41-19.70%). 6) The difference of respirable coal dust, quartz, and sericite concentrations in drilling, coal cutting, hauling and seperating was significant respectively (p<0.05).
The digital dust indicator (Sibata P-5), one of the direct·reading instruments was evaluated for the respirable dust in the underground coal mine environments. As a reference, respirable dust was ...determined using three cyclones and/or impactors. All the tests were performed on aerosol in twenty underground coal mines. The coefficients of mass-relative concentration were $0.067{\pm}0.054$ (Mean$\pm$Standard deviation) (range: 0.006-0.172). The relationship between relative concentration and temperature was not significant statistically. Also, the relationship of relative concentration and relative humidity was not significant. Mass concentration and relative concentration were $5.31{\pm}5.22mg/m^3$ and $162{\pm}163$ CPM ($Mean{\pm}Standard$ deviation) respectively. The range of mass concentration was $1.22-22.69mg/m^3$; relative concentration 16-628 CPM. The relationship of mass concentration and relative concentration was not significant in these ranges.
