• 대한기계학회:학술대회논문집
• /
• 대한기계학회 2000년도 추계학술대회논문집B
• /
• pp.726-731
• /
• 2000

This study was experimentally analyzed to improve the performance and to reduce exhaust emissions in a turbochaged D.I. diesel engine of the displacement 9.4L. In generally, the system of intake port, fuel injection and turbocharger are very important factors which have influence on the engine performance and exhaust emission because the properties in the injected fuel depend on the combustion characteristics. The optimum results which is tested as available factors fur better performance and emission are as follows; the swirl ratio is 2.43, compression ratio is 16, combustion bowl is $5^{\circ}$ re-entrant type, nozzle hole diameter is ${\phi}0.28*6$, injection timing is BTDC $13^{\circ}CA$ and turbocharger is GT40 model which are selected compressor A/R 0.58 and turbine A/R 1.19.

• 한국산학기술학회논문지
• /
• 제20권12호
• /
• pp.723-729
• /
• 2019

터보과급기는 엔진에 장착하여 연비를 개선하는 효과적인 장치로 디젤엔진과 가솔린엔진 모두에서 광범위하게 사용되고 있다. 본 연구에서는 승용차용 가솔린엔진에 사용되는 트윈스크롤 터보과급기에서 발생하는 맥동유동의 질량유량을 측정하였다. 자체 설계 제작한 맥동유동장치를 사용하여 맥동이 있는 비정상상태에서 유동의 질량유량을 측정하였고, 맥동이 없는 정상상태의 질량유량과 비교 분석하였다. 맥동유동장치는 회전하는 상판과 고정된 하판을 사용하여 변하는 엔진의 배기밸브 유효면적을 반영하였다. 맥동이 있는 비정상상태 질량유량을 측정하기 위하여 차압식 압력계를이용한 오리피스 유량계를 사용하였다. 이때 기체의 온도와 절대압력을 측정하여 기체 밀도 변화를 고려하였다. 터보과급기의 저속 성능을 분석하기 위하여 압축공기를 사용하여 터보과급기 회전속도 60,000rpm에서 100,000rpm의 범위에서 측정을 수행하였다. 비정상상태의 질량유량은 정상상태와 비교하여 크게 다른 결과를 보였다. 정상상태 질량유량 계수는 터빈 팽창비가 증가함에서 따라 증가하지만, 비정상상태 질량유량 계수는 정상상태 값 주변의 히스테리시스 루프를 형성하며 변화량은 정상유동 기준 최대 5.0배이다. 이것은 맥동유동에 의하여 터빈 볼류트 공간에서 충진과 방출이 일어나기 때문이다.

• International Journal of Aeronautical and Space Sciences
• /
• 제5권1호
• /
• pp.46-56
• /
• 2004

The verification and improvement of the measurement uncertainty have beenperformed in the altitude test facility for small gas turbine engines, which was built atthe Korea Aerospace Research Institute (KARI) in October 1999. This test is performedwith a single spool turbojet engine at several flight conditions. This paper discussesthe evaluation and validation process for the measurement uncertainty improvements usedin the altitude test facility. The evaluation process, defined as tests before the facilitymodification, shows that the major contnbutors to the measurement uncertainty are theflow meter discharge coefficient, the inlet static and total pressures, the cell pressureand the fuel flow rate. The measurement uncertainty is focused on the primary parametersof the engine performance such as airflow rate, thrust and specific fuel consumption (SFC).The validation process, defined as tests after the facility modification, shows that themeasurement uncertainty, in seal level condition, is tmproved to the acceptable level throughthe facility modification. In altitude test conditions, the measurement uncertainties arenot improved as much as the uncertainty in sea level condition.

• Journal of Biosystems Engineering
• /
• 제26권3호
• /
• pp.263-270
• /
• 2001

This study was conducted in order to develop wind-water heating system where frictional heat is creased between the rotor and working fluid when they are rotating in the cylindrical heat generator. The wind-water heating system is composed of rotor, stator, working fluid, motor, inverter and heat generation tank. Instead of wind turbine, we have used an electrical motor of 30㎾ to rotate the rotor in this system. Two working fluids and six levels of rotor rpm were tested to quantify heat amounts generated by the system. Generally, as motor rpm goes up heat amount increases that we have expected. At the same rpm, viscous fluid showed up better performance than the water, generating more heat by 10$\^{C}$ difference. The greatest heat amount of 31,500kJ/h was obtained when the system constantly drained out the hot water of at the flow rate of 500ℓ/h. Power consumption rate of the motor was measured by thee phase electric power meter where the largest power consumption rate was 14㎾ when motor rpm was 600 and gained heat was 31,500kJ/h, that indicated total thermal efficiency of the wind power water heating system was 62%.

• 수산해양교육연구
• /
• 제5권1호
• /
• pp.31-44
• /
• 1993

Through the early 1900's, the evolution of the surface condenser was closely tied to the development of steam engine and the turbine. As the chemical and petroleum industries evolved in the 1900's, the use of surface condensers in many different processes. Today, industry uses condensers in many shapes and sizes. The actual condensation process occurs on the outside surface of tubes. The nature of this surface geometry affects the condenser's heat transfer performance. The first condensers were built with plain tubes. As tube manufacturing techniques advanced, manufacturers started making tubes with integral fins. In the 1940's, fin densities were limited to about 600 to 700 fins per meter(fpm) because of manufacturing procedure. Today new manufacturing techniques allow production of tubes with fin densities ranging from 750 to 1600 fpm. The integral-fin tubes investigated in this paper are nominally 19 mm diameter. Eight tubes have been used with trapezodially shaped integral-fins having fin density from 748 to 1654 fpm and 10, 30 grooves. For comparison, tests are made using a plain tube having the same inside diameter and an outside diameter equal to that at the root of the fins for the finned tubes. Betty and Katz's theoretical modelis is used to predict the R-11 condensation coefficient on horizontal integral-fin tubes having 748, 1024 and 1299 fpm. Experiments are carried out using R-11 as working fluid. The refrigerant condensates at a saturation state of $30^{\circ}C$ on the outside tube surface cooled by coolant. The amount of noncondensable gases present in the test loop is reduced to a negligible value by repeated purging. For a given heat input to the boiler and given cooling water flow rate, all test data are taken at steady state. The observed heat transfer enhancement for the finned and grooved tubes significantly exceeded that to be expected on grounds of increased area. For the eight fin tubes and one plain tube tested, the best performance has been obtained with a tube having a fin density of 1299 fpm, and a fin bight of 1.2mm and 30 grooves.