• 설비공학논문집
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• 제11권6호
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• pp.846-854
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• 1999

Measurements of the local heat transfer coefficients were made on a hemispherically convex surface with a round oblique impinging jet. The liquid crystal transient method was used for these measurements. This method, which is a variation on the transient method, suddenly exposes a preheated wall to an impinging jet while video recording the response of liquid crystal for the surface temperature measurements. The Reynolds number used was 23000 and the nozzle-to-surface distance was L/d=2, 4, 6, 8, and 10 and the jet angle was $\alpha$=$0^{\circ}\; 15^{\circ}\;30^{\circ}C\; and \;40^{\circ}C$. In the experiment, the Nusselt number at the stagnation point decreases as the jet angle increases and has the maximum value for L/d=6. The X-axis Nusselt number distributions exhibit Secondary maxima at $0^{\circ}C\re $\alpha$\re 15^{\circ}C, L/d\le6$ for X/d＜0(upstream) and at $0^{\circ}C\re $\alpha$40^{\circ}C,\;L/d\le4\;and\; at\; 30^{\circ}C\re $\alpha$$\leq$40^{\circ}C,\;L/d\le 6 $for X/d＞0(downstream). The secondary maxima occurs at long distance from the stagnation point as the jet angle increases or the nozzle-to-surface distance decreases. The Y-axis Nusselt number distributions exhibit secondary maxima at Y/d=$\pm$2 for $0^{\circ}C\le a\le30^{\circ}C\; and\; L/d\le4, and \;for\;$\alpha$=40^{\circ}C$and L/d=2. The displacement of the maximum Nusselt number from the stagnation point increases as the jet angle increases or the nozzle-to-surface distance decreases and the maximum distance is about 0.67 times of the nozzle diameter. The ratio of the maximum Nusselt number to the stagnation Nusselt number increases as the jet angle increases.

• 수산해양기술연구
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• 제27권4호
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• pp.255-265
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• 1991

분사류의 굴삭성능을 이용하여 해저의 모래속에서 서식하고 있는 패류를 어획할 목적으로 원형과 직사각형의 모형노즐을 제작하여 수조에서 분사노즐의 모래면에 대한 굴삭실험을 한 결과를 요약하면 다음과 같다. 1. 분사노즐에 의한 모래면의 최대 굴삭깊이와 폭은 분사속도와 노즐의 단면적의 크기에 비례하여 직선적으로 증가하며, 노즐의 분사거리에 대해서는 굴삭깊이는 직선적으로 감소하나, 굴삭폭은 직선적으로 증가한다. 2. 직사각형 노즐(폭 1mm)은 단면적이 같은 원형 노즐보다 굴삭성능이 다소 우수하였다. 3. 노즐별 분사각도와 분사속도, 분사거리에 따른 최대 굴삭깊이와 폭에 관한 실험식은 직선식으로 나타나며, 분사각도 45$^{\circ}$에서 직사각형노즐(폭 1mm)의 분사속도와 분사거리에 따른 실험식은 다음과 같다. D=0.0093V 하(0)-0.23H+5.7. W=0.0147V 하(0)+1.06H+10.2. 단, D: 최대 굴삭깊이(cm), V 하(0): 노즐의 분사속도(cm/sec) 926$\leq$V 하(0)$\leq$1504, W: 최대굴삭폭(cm), H: 노즐구멍에서 모래면까지의 거리(cm).

• 한국군사과학기술학회지
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• 제4권2호
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• pp.256-262
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• 2001

Viscous solutions of supersonic side jet nozzle and supersonic jet impinging on a flat plate are simulated using three-dimensional Navier-Stokes solver. For rapid and abrupt control of a missile in supersonic flight, side jet on a missile body is found to be a useful devise as evidenced by recent missile development at several nations. The magnitude of the side jet and the duration of it decide the level of control of such a missile system. The aerodynamic characteristics of the side jet devise itself are examined in terms of key parameters such as the side jet nozzle geometry, the chamber pressure and temperature. On the other hand, the jet impinging flow structure exhibits such complex nature as shock shell, plate shock and Mach disk depending on the flow parameters. Among others, the dominant parameters are the ratio of the nozzle exit pressure to the ambient pressure and the distance between the nozzle exit plane and the impinging plane. As the plate is placed close to the nozzle, the computed wall pressure at or near the jet center oscillates with large amplitude with respect to the mean value. The amplitude of wall pressure fluctuations subsides as the plate/nozzle distance increases, and the frequency of the wall pressure is estimated on the order of 10.0 KHz. Objectives of this paper are to show accurate simulation of nozzle flow itself and to demonstrate the jet flow structure when the jet interacts with a wall at a close range.

• 농업과학연구
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• 제11권2호
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• pp.284-294
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• 1984

동력분무기용(動力噴霧機用) 3분두(噴頭) 분공(噴孔)의 크기, 살포각도(撒布角度) 및 와실(渦室)의 간격을 변화(變化)시키면서 최대(最大) 분무유효거리(噴霧有效距離)의 구명(究明)과 살포도(撒布度)의 개선(改善)을 위(爲)한 분두배열(噴頭配列) 방법(方法)의 분석결과(分析結果)는 다음과 같다. 1. 분공(噴孔) 직경(直徑)이 커짐에 따라 분무량(噴霧量)은 증가(增加)하였고 1번구(番口)는 2차(次) 곡선(曲線)으로 II번구(番口), III번구(番口)는 1차(次) 함수관계(關係)를 나타냈다. 2. 최대(最大) 유효거리(有效距離)는 살포각도(撒布角度)가 $15^{\circ}$일때 최대(最大) 값을 나타냈고 분공(噴孔)의 크기가 3.0mm일때 약17m, 2.5mm 및 2.0mm 일때 각각 약 14m, 약 13m로 나타났다. 3. 살포도(撒布度)의 균등개선(均等改善)을 위(爲)한 분두배열(噴頭配列)(表 6참조(參照))은 I번구(番口)의 분공(噴孔)크기에 따라 다르지만 균등계수(均等係數)는 약 6%정도(程度) 개선(改善)시킬 수 있었다. 4. 살포거리(撒布距離) 6m의 최저(最低) 살포량(撒布量)을 II번구(番口)의 와실(渦室) 간격 조절(調節)로서 개선(改善)시킬 수 있었다.

• 한국신재생에너지학회:학술대회논문집
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• 한국신재생에너지학회 2010년도 춘계학술대회 초록집
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• pp.58.2-58.2
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• 2010

This paper deals with the simulation of solid particle coating technology via supersonic nozzle in vacuum environment to devote as an aerosol-deposition device. In order to improve efficiencies of nozzle and coating process, effects of shockwave, nozzle geometry, and substrate location were studied computationally under a fixed chamber pressure of 0.01316 bar which is nearly vacuous. Shockwave is the important factor affect to entire flow because shockwave in the jet flow dissipates the kinetic energy of the flow in the supersonic condition. Results show that various nozzle geometries have significant effect on the supersonic flow and we know that the supersonic nozzle should be optimized to minimize the loss of the flow. Another parameter, the distance between substrate and nozzle tip, shows little effect in this study.

• Agricultural and Biosystems Engineering
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• 제3권1호
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• pp.29-34
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• 2002

Two charging methods of electrostatic nozzle, i.e. induction and ionized field corona charging, were designed and evaluated for orchard sprayer application. An artificial (metallic) target was constructed and used in this experiment. The charge-to-mass ratio for the induction electrode was measured by using the Faraday cage. Two conventional pressure-swirl nozzles have been employed with different orifice diameters under the same experimental operating conditions. A commercial pressure-swirl nozzle with orifice diameter of 1.0 was used for the conventional spray. The diameter of the electrostatic was 0.59 mm. The experiment was carried out for individual nozzle sprays at $0^{\circ}$, $20^{\circ}$ and $50^{\circ}$ oriented angles and three nozzles, sprayed simultaneously at a distance of 1.0 and 2.0 m from the nozzle tip to the target. The nozzles were mounted on a carriage with constant speed of 1.26 km/h with a blower attached. The weighing method was employed to evaluate for the spray deposition, ground loss and estimated drift. The results show more promising for the induction charging method, especially at $20^{\circ}$oriented angle at a distance of 1.0 m from the target for a single nozzle and when all three nozzles were operated simultaneously for spray deposition. The results of the induction charging method show promising with the developed electrostatic technique.

• 한국기계가공학회지
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• 제15권4호
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• pp.148-154
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• 2016

A study on the micro particle blasting was conducted to find the optimum conditions of the blasted surface of aluminum 6061. The particle type such as $Al_2O_3$ and SiC, nozzle diameter, pressure, standoff distance and injection time were used as blasting conditions. Statistical method of orthogonal arrays(ANOVA) was used to find optimum conditions of maximum depth and maximum diameter of blasted surface. Particle type, nozzle diameter, and pressure were found to be the main factors of maximum blasted depth and diameter. Maximum blasted diameter was affected by increasing pressure and nozzle diameter but saturated maximum diameter. Maximum blasted depth was affected by pressure and nozzle diameter when aluminum 6061 was blasted with $Al_2O_3$ particle. The value of surface roughness was increased as pressure and nozzle diameter increased when aluminum 6061 was blasted with SiC.

• 대한기계학회논문집B
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• 제24권4호
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• pp.519-525
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• 2000

The effect of nozzle diameter on the local Nusselt number distributions has been investigated for an axisymmetric turbulent jet impinging on the flat plate surface. The flow at the nozzle exit has a fully developed velocity profile. A uniform heat flux boundary condition at the plate surface was created using gold film Intrex. Liquid Crystal was used to measure the plate surface temperature. The experiments were made for the jet Reynolds number (Re) 23,000, the dimensionless nozzle to surface distance (L/d) from 2 to 14, and the nozzle diameter (d) from 1.36 to 3.40 cm. The results show that the Nusselt number at and near the stagnation point increase with an increasing value of the nozzle diameter.

• 대한기계학회논문집B
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• 제36권3호
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• pp.285-291
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• 2012

비예혼합 화염의 안정성에 관한 종래의 연구는 연료노즐이나 퀄의 형상에 초점을 많은 맞추어 왔으나 화염안정화에 중요한 연료의 후퇴거리 및 공기노즐의 홀 형상에 대한 연구는 상대적으로 부족하여 이에 관한 연구가 절실한 실정이다. 따라서, 본 연구에서는 메탄 분류 후퇴거리 및 2 차 공기의 홀 형상에 따른 연소특성을 관찰하기 위해 동축 삼중관 형태의 버너를 설계하였다. 1 차 공기는 스월러를 통하여 분류하였고, 2 차 공기는 홀 형상 및 슬릿 형상의 각 노즐로부터 분류되었다. 본 연구에 사용된 실험실 스케일 버너로부터 2 차 공기의 유속은 화염의 형태에 영향을 끼치는 것을 알 수 있었다. 후퇴거리의 경우 공급관외경의 절반에 해당하는 거리로 설정했을 때 화염이 안정적으로 존재하고, 휘도는 더욱 높아짐을 알 수 있었다.

• 대한기계학회논문집B
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• 제39권8호
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• pp.645-651
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• 2015

본 논문은 중앙구동 이젝터의 유량비에 미치는 설계변수의 영향에 대한 연구를 목적으로 한다. 중앙구동 이젝터의 설계변수는 구동노즐 출구 단면적 및 거리비, 디퓨저 출구 단면적비로 설정하였다. 실험장치는 가변노즐 이젝터, 전동 모터-펌프, 구동유체 저장수조, 제어판넬 그리고 고속 카메라 시스템으로 구성하였다. 유량비는 실험변수에 따라 측정되는 유입 공기량과 구동유체인 물의 유량을 이용하여 도출하였다. 유량비는 구동노즐 거리비와 혼합관 길이비가 커지면 증가하는 반면에, 구동노즐 면적비와 디퓨저 출구 면적비가 커지면 감소하였다.