• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2011년도 제36회 춘계학술대회논문집
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• pp.196-199
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• 2011

고압관, 가압관, 발사관으로 구성된 2단식 경가스 총을 사용하는 축소형 초고압 분사 시스템은 액체 제트를 초음속으로 생성할 수 있다. 이러한 초음속 액체 제트는 전방에 발생하는 충격파로 인한 액적 미립화를 촉진 시킬 수 있다. 본 연구에서는 초음속 액체 제트의 미립화 특성을 파악하기 위해 직선 원추형 노즐을 사용하여 기하학적인 형상 변화에 따른 실험을 진행하였다. 미립화 특성을 나타내는 SMD는 L/d가 증가할수록 $151.2{\mu}m$에서 $52.25{\mu}m$로 감소하는 경향을 나타내었다.

• 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.

• 한국기계가공학회지
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• 제14권1호
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• pp.98-104
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• 2015

This experiment was a study of a Vortex nozzle designed to produce micro-bubbles due To investigate air self-suction and the generation of micro-bubble by the Vortex nozzle, the dimensions of air intake region, the nozzle shape, and the nozzle exit diameter ($d_n=5,7,9.2,12.3mm$)werevaried. The air self-suction rate was ~1,000 to 2,000 cc/min at the orifice nozzle (7 mm), and ~100 and ~22 cc/min at the sector nozzles (9.2 and 12.3 mm, respectively). The most bubbles were detected in the orifice nozzle, but bubbles less than $50{\mu}m$ were found in the 12.3-mm sector nozzle. The dissolved oxygen in the tank water was much greater in Case 2 than in Case 1, at both the orifice and sector nozzles. Moreover, the reduction rate of dissolved oxygen was found to be less at the sector nozzles, than at the orifice nozzle.

• 한국안전학회지
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• 제18권4호
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• pp.51-56
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• 2003

The goal of this study is to show the way to decrease the noise from air nozzles. The variables of this test are the shapes of air nozzles, air flow rate and the distance between a reflection plate and a nozzle tip. This experiment is aimed to find the most appropriate condition to minimize the noise. These are the results. If diameter ratio is more than 12:8, noise level increases by over 10 dB(A) regradless of the distance between a reflection plate and a nozzle and the existence of a reflection plate. And when $L_2$ of a nozzle is 5mm long, noise level rise relatively highly. So, it is strongly recommended that $L_2$ should be manufactured more than 10mm. The reason for a high intensity noise is that when diameter ratio is more than 12:8, the diameter of a nozzle tip($D_2$) turns small drastically, which increases the air velocity. It is assumed that when the vortes is great around the spots where a nozzle hole is suddenly smaller, great turbulent flow increases much noise.

• 한국추진공학회지
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• 제21권5호
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• pp.19-28
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• 2017

본 연구에서는 원형 노즐과 타원형 노즐을 이용하여 공동현상과 수력튀김 현상이 유동특성에 어떠한 영향을 미치는지 파악하고자 하였다. 이를 위해 오리피스 길이 대 직경비(L/d)와 타원형 노즐의 종횡비(a/b)가 서로 다른 분사기들을 제작하여 분무실험을 수행하였다. 분사압력 증가에 따라 공동현상이 발생할 경우 유량계수가 서서히 감소하였으나 수력튀김 영역에서는 유량계수가 급격히 떨어진 후 일정한 값을 유지함을 확인하였다. 하지만 타원형 노즐에서 장축지름(a)과 단축지름(b) 대비 오리피스 길이의 비인 L/b가 8 이상, L/a가 8 이하인 경우, 유량계수 및 액체제트 형상은 기존의 원형 노즐과는 상당히 다른 결과를 나타내었다. 정상유동 상태인 경우 타원형 노즐에서 분사된 액주는 원형 노즐과는 달리 하류로 가면서 장축에서는 분무각이 감소하였으며 단축에서는 분무각이 커지는 모습을 보였다.

• 대한기계학회논문집B
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• 제30권12호
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• pp.1164-1172
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• 2006

Measurements of the local heat transfer coefficients on hemispherical convex and concave surfaces with a turbulent impinging jet were made. The Reynolds number used was 11000, 23000, 50000 and the nozzle- to- surface distance was L/d=2, 4, 6, 8, and 10 and the jet angle was a = $0^{\circ}$, $15^{\circ}$, $30^{\circ}$ and $40^{\circ}$. In case of concave surface, 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 $0^{\circ}$ $\leq$ a $\leq$ $15^{\circ}$, L/d $\leq$ 4 for X/d<0(upstream) and at $0^{\circ}$ $\leq$ a $\leq$ $40^{\circ}$, L/d $\leq$ 4 and at $30^{\circ}$ $\leq$ a $\leq$ $40^{\circ}$, 4 < L/d $\leq$ 6 for X/d<0(downstream). The secondary maximum occurs at long distance from the stagnation point as the jet angle increases or the nozzle-to-surface distance decreases. In case of convex, correlations of the stagnation point Nusselt number according to Reynolds number, jet-to-surface distance ratio and dimensionless surface angle are presented. In the stagnation point, in term of Ren, n ranges from 0.43 in case of 2 $\leq$ L/d $\leq$ 6 to 0.45 in case of 6 < L/d $\leq$ 10, there agrees roughly appears to be laminar boundary layer result. The maximum Nusselt number, in this experiment, occurred in the direction of upstream. The displacement of the maximum Nusselt number from the stagnation point increases with increasing surface angle or decreasing nozzle-to-surface distance. On this condition about surface curvature D/d=10, the maximum displacement is about 0.7 times of the jet nozzle diameter. The ratio of the maximum Nusselt number to the stagnation Nusselt number increases as the jet angle increases.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2000년도 추계학술대회논문집B
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• pp.267-271
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• 2000

The local heat transfer rate of an axisymmetric submerged air jet impinging on normal to a heated flat plate was investigated experimentally with varying solidity of mesh screen. The mean velocity and turbulent Intensity profiles of streamwise velocity component were measured using a hot-wire anemometry. The temperature distribution on the heated flat surface was measured with thermocouples. The screen installed in front of the nozzle exit(behind of 35mm) modify the jet flow structure and local heat transfer characteristics. For higher solidity screen, turbulence intensity at core lesion is high and increases the local heat transfer rate at nozzle-to-plate spacings(L/D<6). For larger nozzle-to-plate spacings(L/D>6), however, the turbulent Intensities of all screens tested in this study approach to an asymptotic curve, but the small mean velocity at the core region reduces the local heat transfer rate for high solidity screens.

• 한국수산과학회지
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• 제22권4호
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• pp.201-213
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• 1989

본 연구는 유체분사식형망의 분사류의 저질에 대한 굴삭성능을 파악하고자 노즐의 크기별로 원형과 반원형노즐을 제작하여 수조실험을 통해서 노즐끝에서의 동압, 노즐과 판과의 거리, 노즐의 구경, 저질 등의 변화에 따른 저질의 굴삭형상변화를 측정하여 다음과 같은 결과를 얻었다. 1. 분사류의 운동량은 동압을 $100\~500gf/cm^2$로 변화시킴에 따라 4mm 원형노즐에서 $43\~114gf$, 6mm에서 $52\~227gf$. 8mm에서 $114\~506gf$. 10mm에서 $137\~769gf$로 각각 증가하였으나, 50cm이내의 거리에서는 거리에 대한 운동량의 변화는 거의 없었다. 2. 굴삭깊이는 노즐의 구경과 동압이 커짐에 따라, 그리고 노즐높이가 낮아짐에 따라 일정한 기울기로 직선적으로 증가하였으며, 저질 I과 II에 대해 다음과 같은 관계식을 얻었다. $$L_I=[0.01(H/r-100) -0.43\cdot\iota+11.78]{\cdot}D/4$$ $$L_{II}=[0.03(H/r-100) -0.34\cdot\iota+6.39]{\cdot}D/4$$ 단, $L_I,\;L_{II}$; 저질 I, II에 대한 굴삭깊이 H: 노즐동압($gf/cm^2$) r: 물의 단위체적당 중량($1gf/cm^2$) $\iota$: 노즐높이 (cm) D: 노즐구경 (mm)

• 대한기계학회논문집
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• 제16권8호
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• pp.1566-1574
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• 1992

본 연구에서는 원형수직 충돌분류에 의한 가열평판의 전열특성을 해석하기 위 하여 최근 표면온도 측정에 많이 사용되고 있는 liquid crystal을 이용하였다. 즉 liquid crystal의 감온특성과 영상처리 기법을 이용하여 레이놀즈수 및 노즐과 충돌판 사이의 거리(L/D) 변화에 따른 전열면의 온도장 변화를 측정하였다.

• 한국분무공학회지
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• 제13권3호
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• pp.134-142
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• 2008

In the case of heavy duty diesel engines, the Urea-SCR system is currently considered to reduce the NOx emission as a proved technology, and it is widely studied to get the high performance and durability. However, the nozzles to inject the urea-water solution into the exhaust pipe occur some problems, including the nozzle clogging, deposition of urea-water solution on the inner wall of the exhaust pipe, resulting in the production of urea salt. In this study, a swirl-type twin-fluid nozzle to produce more fine droplets was used as a method to solve the problems. The effect of the nozzle cap geometry, including the length to diameter ratio ($l_o/d_o$) and chamfer, on the spray characteristics were investigated experimentally. The length to diameter ratio of nozzle cap were varied from 0.25 to 1.125. The chamfer angle of the nozzle cap was constant at 90o. The mean velocity and droplet size distributions of the spray were measured using a 2-D PDA (phase Doppler analyzer) system, and the spray half-width, AMD (arithmetic mean diameter) and SMD (Sauter mean diameter) were analyzed. At result, The larger length to diameter ratio of nozzle cap were more small SMD and AMD. The effect of the chamfer did increase the radial velocity, while it did not affect the atomization effect.