• Title/Summary/Keyword: Surface plate

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Heat Transfer Characteristics by the Right Angled Triangle Rod Array in Impinging Air Jet System (충돌공기제트시스템에서 직삼각형로드에 의한 열전달특성)

  • Kum, Sung-Min
    • Journal of ILASS-Korea
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    • v.13 no.1
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    • pp.9-15
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    • 2008
  • This experimental study was carried out to examine the heat transfer characteristics of impinging air jet on a flat plate with a set of right angled triangle rods. Each right angled triangle rod in the array was positioned normal to the flow direction and parallel to the flat plate surface. The clearances from a right angled triangle rod to flat plate surface (C=1, 2 and 4 mm) and the distance from nozzle exit to flat plate (H=100 and 500 mm) were changed for the pitch between each right angled triangle rods (P=40 mm). As a result, heat transfer shows best performance at the clearance of C=1 mm, in case clearance changed, and the average heat transfer enhancement rate increased up to 47% compared to the result of a flat plate without a right angled triangle rod.

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Effect of Periodic Passing Wake on the Flow Field of a Film-Cooled Flat Plate(I) (주기적인 통과후류가 막냉각되는 평판의 유동장에 미치는 영향(1);압력면과 흡입면에 대한 영향(1))

  • Kuk, Keon;Lee, Joon-Sik;Kauh, Sang-Ken
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.20 no.6
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    • pp.1931-1940
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    • 1996
  • The effect of periodic passing wake on the film-coolant flow issuing normally from a flat plate was investigated experimentally. The passing wake was generated by rotating thin circular bars. Depending on the rotational direction the test plate could be simulated as a pressure surface or a suction surface of a gas turbine blade. The phase-averaged velocity components were measured using an X-type hot-wire probe. The Reynolds number based on the free-stream velocity and injection hole diameter was 23, 500 and the velocity ratio which is the ratio of film coolant velocity to free-stream velocity was 0.5. The velocity-triangle induced by the wake was similar to that induced by the one generated at the blade trailing edge. The vertical velocity component induced by the passing wake, which approaches to the suction surface and moves away from the pressure surface, played a dominant role in the variation of the flow field. The variation in the phase-averaged velocity on the pressure surface was greater than on the suction surface, but the turbulence kinetic energy variation on the suction surface appeared larger than on the pressure surface.

Interaction between Turbulent Boundary Layer and Wake Behind an Elliptic Cylinder at Incidence (앙각을 가진 타원형 실린더 후류와 평판경계층의 상호작용에 대한 연구)

  • Choi, Jae-Ho;Lee, Sang-Joon
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.24 no.7
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    • pp.976-983
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    • 2000
  • The flow characteristics around an elliptic cylinder with axis ratio of AR=2 located near a flat plate were investigated experimentally to study the interaction between the cylinder wake and the turbulent boundary layer. The pressure distributions on the cylinder surface and on the flat plate were measured with varying the angle of attack of the cylinder. In addition, the velocity profiles of wake behind the cylinder were measured using a hot-wire anemometry As the angle of attack increases, the location of peak pressure on the windward and leeward surfaces of the cylinder moves toward the rear and front of the cylinder, respectively. At positive angles of attack, the position of the minimum pressure on the flat plate surface is moved downstream, but it is moved upstream at negative angles of attack. With increasing the angle of attack, the vortex shedding frequency is gradually decreased and the critical angle of attack exists in terms of the gap ratio. By installing the elliptic cylinder at negative angle of attack, the turbulent boundary layer over the flat plate is disturbed more than that at positive incidence. This may be attributed to the shift of separation point on the lower surface of the cylinder due to the presence of a ground plate nearby.

The Influence of the Surface Roughness on the Natural Convection on a Vertical Flat Plate (수직평판의 거칠기가 자연대류 열전달에 미치는 영향)

  • Ohk, Seung-Min;Chung, Bum-Jin
    • Journal of Energy Engineering
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    • v.23 no.2
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    • pp.21-27
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    • 2014
  • The influence of the surface roughness on the natural convection heat transfers of a vertical plate were measured experimently. Mass transfer experiments instead of heat transfer experiment were performed based on the analogy. The piecewise electrodes were adopted to measure the local-average Nusselt number. Prandtl number was 2,014 and height of the plate was 0.154m The test results for a smooth surface showed similar heat transfer rate with the Le Fevre heat transfer correlation for a vertical plate. The Nusselt number increased with the roughness Rz $0.5{\sim}14.1{\mu}m$. The test results were presented by a simple correlation.

A New Algorithm to Determine Heating Lines for Plate Forming by Line Heating Method (선상가열법에 의한 강판 가공의 가열선 결정 알고리즘)

  • Chang-Doo Jang;Sung-Choon Moon
    • Journal of the Society of Naval Architects of Korea
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    • v.35 no.2
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    • pp.104-113
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    • 1998
  • The line heating method is a popular technique used to form ship hull in shipyards. In order to promote shipbuilding productivity, some researchers have made progress in their studies on automatic fabrication system for plate forming. These researches have, however, focused on heat-induced plate deformation with particular mechanical modelings, and do not yet propose the heating paths applicable to actual plate forming process. In this paper, a new algorithm to determine heating lines is developed to simulate the line heating process. The important feature of this algorithm is that it calculates principal curvatures of deflection difference surface which represents difference between target surface and surface in fabrication. Several trials to typical surface types show its usefulness and good applicability to tactical use.

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Heat Transfer Measurements by a Round Impinging Jet on a Rib-Roughened Flat Plate (표면조도를 가진 평판에서 원형충돌제트에 의한 열전달 측정)

  • Lee, Dae-Hee;Kim, Yun-Taek;Chung, Seung-Hun;Chung, Young-Suk
    • Proceedings of the KSME Conference
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    • 2000.11b
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    • pp.87-92
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    • 2000
  • This study is to investigate the heat transfer characteristics the for a round turbulent jet impinging on the flat plate with and without rib. Liquid crystal/transient method was used to determine the Nusselt number distributions along the surface. The temperature on the surface was measured using liquid crystal and a digital color image processing system. The experiments were made fur the jet Reynolds number (Re) 23,000, the dimensionless nozzle-to-surface distance (L/d) from 2 to 10, and the rib type [height ($d_1$) 2mm, pitch (p) from 12 to 36mm]. It was found that for $L/d{\ge}6$ the average Nusselt numbers on the flat plate with rib type C ($p/d_1=16$) are higher than those without rib, mainly due to an increase in the turbulent intensity caused by flow separation, recirculation and reattachment on the wall surface.

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Jet Impingement Heat Transfer on a Pedestal Encountered in Chip Cooling (충돌제트를 이용한 pedestal 형상의 칩 냉각연구)

  • Lee, Dae-Hee;Chung, Seung-Hoon;Chung, Young-Suk;Lee, Joon-Sik
    • Proceedings of the KSME Conference
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    • 2001.11b
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    • pp.124-130
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    • 2001
  • The heat transfer and flow measurements were made on a cylindrical pedestal mounted on a flat plate with a turbulent impinging air jet. The heat transfer coefficient distributions on the flat plate were measured using the shroud-transient technique and liquid crystal was used to measure the surface temperature. The jet Reynolds number (Re) is 23,000, the dimensionless nozzle-to-surface distance (L/d) from 2 to 10, the dimensionless pedestal diameter-to-height (H/D) from 0 to 1.5, the dimensionless 2nd pedestal diameter-to-height ($H/D_2$) from 0 to 0.4 and the distance from the stagnation point to 2nd pedestal (p/D). The results show that for H/D = 0.5 to 1.5, the Nusselt number distributions on the plate surface exhibit a maximum between $r/d\;{\cong}\;1.0$ and 1.5. The presence of the pedestal appears to cause the flow separation and reattachment on the plate surface, which results in the maximum heal transfer coefficient. Also, for p/D = 2.5 and $H/D_2$ = 0.3, the local Nusselt number in the region corresponding to $r/d\;{\cong}\;1.1$ was increased up to 50% compared to that for $H/D_2=0$.

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Effect of Atmospheric Pressure Flame Plasma Treatment on Surface and Adhesive Bonding Properties between Steel Plate and Rubber (대기압 화염 플라즈마 처리가 강판의 표면 및 고무와의 접착특성에 미치는 영향)

  • Ryu, Sang-Ryeoul;Lee, Dong-Joo
    • Composites Research
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    • v.23 no.5
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    • pp.1-7
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    • 2010
  • To increase the adhesive strength of acrylonitrile butadiene rubber(NBR) and steel plate, the atmospheric pressure flame plasma(APFP) treatment device is applied. The effect of various conditions(processing velocity and distance) is experimentally investigated to ascertain the optimum conditions to yield the best adhesive properties. It is found that the optimum distance between burner port and steel plate is 40mm and the optimum processing velocity is 50m/min at given condition. When the surface is coated twice with the bonding agent, the adhesion strength of APFP treated steel plate is increased to about 20.5%. It suggests that the surface modification of steel by flame plasma treatment at atmospheric pressure is a proper and applicable method to improve the adhesion strength between steel and rubber.

Corrosion Image Monitoring of steel plate by using k-means clustering (k-means 클러스터링을 이용한 강판의 부식 이미지 모니터링)

  • Kim, Beomsoo;Kwon, Jaesung;Choi, Sungwoong;Noh, Jungpil;Lee, Kyunghwang;Yang, Jeonghyeon
    • Journal of the Korean institute of surface engineering
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    • v.54 no.5
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    • pp.278-284
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    • 2021
  • Corrosion of steel plate is common phenomenon which results in the gradual destruction caused by a wide variety of environments. Corrosion monitoring is the tracking of the degradation progress for a long period of time. Corrosion on steel plate appears as a discoloration and any irregularities on the surface. In this study, we developed a quantitative evaluation method of the rust formed on steel plate by using k-means clustering from the corroded area in a given image. The k-means clustering for automated corrosion detection was based on the GrabCut segmentation and Gaussian mixture model(GMM). Image color of the corroded surface at cut-edge area was analyzed quantitatively based on HSV(Hue, Saturation, Value) color space.

Chemical Evaluation of Corrosion Resistance for Stainless-Steel Plate Wet-Coated by Alumina-Fluoro Composite Coatings (알루미나-불소 복합 코팅제로 습식코팅된 스텐레스 강판의 화학 내식성 평가)

  • Jung, Ha-Young;Kim, Dae Sung;Lee, Seung-Ho;Lim, Hyung Mi;Kim, Kun;Jung, Min-Kyu
    • Korean Journal of Materials Research
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    • v.22 no.12
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    • pp.643-649
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    • 2012
  • Coatings composited with alumina and Perfluoro alkoxyalkane (PFA) resin were deposited on stainless steel plate (SUS304) to further improve corrosion resistance. Plate (ca. $10{\mu}m$) and/or nanosize (27~43 nm) alumina used as inorganic additives were mixed in PFA resin to make alumina-fluoro composite coatings. These coatings were deposited on SUS304 plate with wet spray coating and then the film was cured thermally. According to the amount and ratio of the two kinds of alumina having plate morphology and nano size, corrosion resistance of the film was evaluated under strong acids (HF, HCl) and a strong base (NaOH). The film prepared with the addition of 5~10 wt% alumina powders in PFA resin showed corrosion resistance superior to that of pure PFA resin film. However, for the film prepared with alumina content above 10 wt%, the corrosion resistance did not improve with the physical properties, such as surface hardness and adhesion. The film prepared with plate/nanosize (weight ratio = 1/2) alumina especially enhanced the surface hardness and corrosion resistance. This can be explained as showing that the plate and the nanosize alumina dispersed in PFA resin effectively suppressed the penetration of cations and anions due to the long penetration length and fewer defects that accompany the improved surface hardness under a serious environment of 10% HF solution for over 120 hrs.