The Climate chamber system is an essential facility for aerodynamic performance development of commercial vehicles to investigate air flow field characteristics in different climatic conditions. In particular, the analysis of airflow fields within the chamber system is an essential consideration for optimal design. In this study, the pressure characteristics and velocity uniformity in the test section area were predicted with blower impeller rotational speed using CFD. The velocity uniformity is affected by the distance from the blower nozzle outlet, reaching up to 72.7% at 695 RPM. The pressure differential between 300 RPM and 740 RPM shows an approximate difference of 2651 Pa, with a high-pressure distribution observed along the right side wall of the blower. These results are expected to be used as design data applicable for improving the performance of environmental chamber systems.

본 연구는 이탈리안 라이그라스 원형베일 사일리지 조제에 있어서 원료작물의 수분함량과 베일러 챔버의 압력에 따른 사일리지의 사료가치와 발효품질의 변화를 구명하기 위하여 수행되었다. 수확 후 1일(고수분), 2일(중수분) 및 4일간(저수분) 각각 예건하여 서로 다른 수분함량의 이탈리안 라이그라스를 베일러 챔버 압력이 115, 130 및 145 bar로 설정된 베일러로 원형베일 사일리지를 조제하여 60일간 저장하였다. 베일 사일리지의 무게는 고수분 처리구에서 높게 나타났고, 건물중은 저수분 처리구가 유의적으로 높게 나타났다. 베일러 압력에 따른 사일리지의 무게는 유의적인 차이는 없었으나, 압력이 증가할수록 건물중은 증가하였다. 수분함량과 베일러 압력에 따른 사일리지의 NDF, ADF, CP 및 CF는 처리 간에 유의적인 차이가 없었으며, RFV (relative feed value)는 고수분 저압력 처리구에서 가장 높게 나타났다. Lactic acid는 고수분-고압력 처리구가 가장 높았으며, 저수분-중압력 처리구에서 가장 낮게 나타내었다. Butyric acid는 베일러 압력에 따른 유의적인 차이는 없었으나, 예건기간이 길어질수록 감소하였다. 사일리지 pH는 고수분 처리구가 중수분과 저수분 처리구에 비해 낮게 나타났으나, 베일러 압력에 따른 차이는 없었다. 이러한 결과는 이탈리안 라이그라스 원형베일 사일리지 조제 시 조사료의 수분함량과 베일러 챔버의 압력이 사일리지의 발효품질에 영향을 미치는 중요한 요인임을 나타내는 것이다.

This paper presents the approach of design parameters optimization based on Taguchi method for the uniformity of outlet pressure in a plasma discharge chamber. The key issue of a plasma discharge chamber is to have the uniformity of outlet pressure which can make a high performance of surface treatment. To extend the length of a outlet from 60mm to 250mm with the uniformity, This study optimally designed the middle holes, outlet width and height, and diameter of the second chamber by using SolidWorks and flow simulation tool. Simulation results demonstrate the validity of the proposed approach.

In the present work, bismuth nanopowders with various particle size distributions were synthesized by controlling argon (Ar) gas flow rate and chamber pressure of a gas condensation (GC) apparatus. From the analyses of transmission electron microscopy (TEM) images and nitrogen gas adsorption results, it was found that as Ar gas flow rate increased, the specific surface area of bismuth increased and the average particles size decreased. On the other hand, as the chamber pressure increased, the specific surface area of bismuth decreased and the average particles size increased. The optimum gas flow rate and chamber pressure for the maximized electrochemical active surface area were determined to be 8 L/min and 50 torr, respectively. The bismuth nanopowders synthesized at the above condition exhibit 13.47 of specific surface area and 45.6 nm of average particles diameter.

MgTiO3 thin films were prepared by r.f. magnetron sputtering in order to prepare miniaturized NPO type MLCCs.MgTiO3 films showed a polycrystalline structure of ilmenite characterized by the appearance of (110) and (202) peaks. Theintensity of the peaks decreased with an increase in the chamber pressure due to the decrease of crystallinity which resultedfrom the decrease of kinetic energy of the sputtered atoms. The films annealed at 600oC for 60min. showed a fine grainedmicrostructure without micro-cracks. The grain size and roughness of the MgTiO3 films decreased with the increase of chamberpressure. The average surface roughness was 1.425~0.313nm for MgTiO3 films prepared at 10~70mTorr. MgTiO3 films showeda dielectric constant of 17~19.7 and a dissipation factor of 2.1~4.9% at 1MHz. The dielectric constant of the films is similarto that of bulk ceramics. The dielectric constant and the dissipation factor decreased with the increase of the chamber pressuredue to the decrease of grain size and crystallinity. The leakage current density was 10−5~10−7A/cm2 at 200kV/cm and this valuedecreased with the increase of the chamber pressure. The small grain size and smooth surface microstructure of the filmsdeposited at high chamber pressure resulted in a low leakage current density. MgTiO3 films showed a near zero temperaturecoefficient and satisfied the specifications for NPO type materials. The dielectric properties of the MgTiO3 thin films preparedby sputtering suggest the feasibility of their application for MLCCs.

This study was conducted to analyze the variations of air temperature, relative humidity and pressure in a low pressure chamber for plant growth. The low pressure chamber was composed of an acrylic cylinder, a stainless plate, a mass flow controller, an elastomer pressure controller, a read-out-box, a vacuum pump, and sensors of air temperature, relative humidity, and pressure. The pressure leakage in the low pressure chamber was greatly affected by the material and connection method of tubes. The leakage rate in the low pressure chamber with the welding of the stainless tubes and a plate decreased by 0.21kPa·h-1, whereas the leakage in the low pressure chamber with teflon tube and rubber O-ring was given by 1.03kPa·h-1. Pressure in the low pressure chamber was sensitively fluctuated by the air temperature inside the chamber. An elastomer pressure controller was installed to keep the pressure in the low pressure chamber at a setting value. However, inside relative humidity at dark period increased to saturation level.. Two levels (25 and 50kPa) of pressure and two levels (500 and 1,000sccm) of mass flow rate were provided to investigate the effect of low pressure and mass flow rate on relative humidity inside the chamber. It was concluded that low setting value of pressure and high mass flow rate of mixed gas were the effective methods to control the pressure and to suppress the excessive rise of relative humidity inside the chamber.

Fe nanopowders were successfully synthesized by plasma arc discharge (PAD) process using Fe rod. The influence of chamber pressure on the microstructure was investigated by means of X-ray Diffraction (XRD), Field Emission Scanning Electron Microscope (FE-SEM), Transmission Electron Microscopy (TEM) and X-ray Photoelectron Spectroscopy (XPS). The prepared particles had nearly spherical shapes and consisted of metallic cores (a-Fe) and oxide shells (FeO), The powder size increased with increasing chamber pressure due to the higher dissolution and ejection rate of H and gas density in the molten metal.

Experimental studies on the characteristics of annular jet pump were carried out in this paper. Jet pump can be used widely for the transportation of solid materials, farm produce and fishes. The effects of high pressure chamber on the characteristics of annular jet pump were sought in this paper. Experiments were done for three shapes of high pressure chamber, and for several lengths of the high pressure chamber. Three types of the high pressure chamber's entrances(90˚ single inflow, 45˚single inflow, and 45˚ double inflow) were tested. Water was used for both the primary fluid and secondary fluid. The results obtained in this study are as follows; 45˚double inflow type is the most effective among the tested three types of the high pressure chamber's entrances. The efficiency of jet pump with 400mm of high pressure chamber length is the highest among the chamber lengths tested in this study, thus indicating appropriate chamber length is required to get an efficient.

멀티 앤빌 프레스(multi-anvil press)는 일반적으로 5-25 GPa의 압력범위와 ~2,300℃의 온도범위를 구현할 수 있는 고압 기기로, 지구과학에서는 상부맨틀-맨틀전이대까지의 지구 구성물질의 구조를 연구하는 데 도움이 된다. 본 연구에서는 광물의 상전이를 이용한 멀티 앤빌 프레스에 대한 압력- 부하 보정(pressure-load calibration) 과정을 소개하고, 시료실(sample chamber) 내에 존재할 수 있는 온도구배에 대해서 논의하였다. 압력-부하 보정은 14/8 G2, 14/8 step, 14/8 HT 조립세트(assembly set)와 18/12 조립세트에 대해 1,100톤 멀티 앤빌 프레스를 이용하여 수행했다. 초기 물질로 석영, 규회석 구조의 CaGeO₃, 포르스테라이트를 사용했고, 고압상의 동정은 XRD 분석을 통해 수행하였다. 광물의 상전이를 통해 1,200℃에서 시료에 가해지는 압력을 유추할 수 있었으며, α-석영에서 코에사이트로의 상전이는 3.1 GPa, 석류석 구조의 CaGeO₃에서 페로브스카이트 구조의 CaGeO₃로의 상전이는 5.9 GPa, 코에사이트에서 스티쇼바이트로의 상전이는 9.2 GPa, 포르스테라이트에서 와즐리아이트로의 상전이는 13.6 GPa의 압력 확인에 이용했다. XRD 결과로 획득한 압력-부하 보정 곡선은 기존에 보고된 유사한 기기의 압력-부하 보정 곡선에 비해 동일 압력을 구현하기 위해 50톤 가량의 유압이 더 필요한 것으로 확인됐다. 이러한 차이는 시료실의 크기 및 조립세트의 압력 매체(pressure medium)와 이차 앤빌 사이의 마찰력으로부터 기인한 유압 손실에 의한 것으로 생각된다. 또한 본 연구에서는 14/8 HT 조립세트에서의 시료실 내의 온도구배를 확인했다. 특히 열전대(thermocouple)의 위치 변화에 따라 시료실 높이에 평행한 방향으로 약 ~200 ℃/mm에 해당하는 온도구배가 존재한다. 본 연구로부터 구한 멀티 앤빌 프레스의 압력-부하 보정 곡선과 시료실 내의 온도구배 값은 앞으로 맨틀 내에서의 다양한 비정질 및 결정질의 지구물질에 대한 원자 구조의 변화와 그에 따른 물성 변화를 설명하는 데 적용할 수 있다.

Pressure chamber(DIC-PC-40형) technique에 의한 대두재배품종 Williams와 금강대립의 경엽에 대한 수분특성의 결과는 다음과 같다. 1. 최대포수시의 삼투압(~Pip) 은 Williams 9.0bar, 금강대립은 10.4bar였다. 3. 초기원형질분리점에서의 상대함수율(PWC*)4 은 금강대립이 86.0%, Williams가 92.6%였다. 4. 삼투수의 총량에 대한 원형질분리점에서의 침출량비(Vp/Vo) 는 Williams가 94.0%, 금강대립이 83.4%였다. 5. 최대함수량에 대한 삼투수의 총량의 비(Vp/w5) 는 금강대립이 84.3%, Williams가 77.5%였다. 7. 탄성계수는 금강대립이 1.6105bar 이었으며 Williams는 8.5 102bar로 현저한 차이를 보였다.