• 제목/요약/키워드: $\b{flat\wire}$

검색결과 20건 처리시간 0.022초

다단계 냉간 압연된 고탄소강 와이어의 미세조직 및 기계적 특성에 미치는 패스스케줄의 영향 (Effect of Pass Schedule on the Microstructures and Mechanical Properties of Multi-step Cold Rolled High Carbon Steel Wires)

  • 우동혁;이욱진;박익민;박용호
    • 한국재료학회지
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    • 제21권6호
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    • pp.320-326
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    • 2011
  • Flat rolling of wire is an industrial process used to manufacture electrical flat wire, medical catheters, springs, piston segments and automobile parts, among other products. In a multi-step wire flat rolling process, a wire with a circular crosssection is rolled at room temperature between two flat rolls in several passes to achieve the desired thickness to width ratio. To manufacture a flat wire with a homogeneous microstructure, mechanical and metallurgical properties with an appropriate pass schedule, this study investigated the effect of each pass schedule (1stand ~ 4stand) on the microstructures, mechanical properties and widths of cold rolled high carbon steel wires using four-pass flat rolling process. The evolutions of the microstructures and mechanical properties of the widths of cold rolled wires during three different pass schedules of the flat rolling process of high carbon wires were investigated, and the results were compared with those for a conventional eight-pass schedule. In the width of cold rolled wires, three different pass schedules are clearly distinguished and discussed. The experimental conditions were the same rolling speed, rolling force, roll size, tensile strength of the material and friction coefficient. The experimental results showed that the four-pass flat cold rolling process was feasible for production of designed wire without cracks when appropriate pass schedules were applied.

트리핑 와이어를 사용한 평판에서의 국소물질전달 특성에 관한 실험적 연구 (Experimental Study on Local Mass Transfer Characteristics of Flat Plate Using Tripping Wire)

  • 유성연;조웅선;조우식
    • 대한기계학회논문집B
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    • 제37권3호
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    • pp.285-292
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    • 2013
  • 본 연구의 목적은 평판의 선단에 설치된 트리핑 와이어에 의한 경계층 박리가 층류에서 난류로의 천이에 미치는 영향과 그 결과로 발생하는 물질전달에 미치는 영향을 규명하는 것이다. 나프탈렌승화법을 사용하여 평판에서의 국소물질전달계수를 측정하였으며, 유동 경계층의 효과를 평가하기 위해 발달된 유동과 발달하는 유동의 조건에서 트리핑 와이어가 설치된 평판에서의 국소물질전달계수를 설치되지 않은 평판에서의 값과 비교하였다. 발달하는 유동에서 국소물질전달계수가 변화하는 경향은 트리핑 와이어가 설치된 평판과 설치되지 않은 평판이 비슷하지만 발달된 유동에서는 상당히 다르게 나타났다. 평균 Sherwood 수는 경계층 박리로 인하여 트리핑와이어가 설치된 평판이 설치되지 않은 평판에 비해서 훨씬 높았다.

압출형 박판 히트파이프의 모세관력 향상을 위한 구조 개발 (Development of the Structure for Enhancing Capillary Force of the Thin Flat Heat Pipe Based on Extrusion Fabrication)

  • 문석환;박윤우
    • 대한기계학회논문집B
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    • 제40권11호
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    • pp.755-759
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    • 2016
  • 전자 통신 분야에서 히트파이프를 활용한 방열기술은 점차 늘어나고 있다. 특히 전자 패키지 응용에서는 원형 단면 히트파이프에 비해 평판 형상의 얇은 히트파이프가 보다 더 적용하기에 용이하다. 압출 공정에 기반한 평판 히트파이프는 내벽에 사각 단면 그루브들로 이루어진 단순한 모세관 윅 구조를 갖는다. 그루브 윅이 내벽에 다수 개 설치가 된다고 하더라도 상대적으로 높은 모세관력을 달성하기는 어렵다. 본 연구에서는 그루브 윅의 모세관력 향상을 위해 와이어 다발을 적용한 평판 히트파이프의 제작 및 성능평가 실험을 수행하였다. 실험을 통해 와이어 다발을 윅으로 갖는 평판 히트파이프의 열저항 및 열전달률이 그루브 윅 평판 히트파이프에 비해 각각 3.4배와 3.8배 가량 우수한 것으로 나타났다. 본 연구를 통해 와이어 다발을 통한 모세관력 향상 효과를 실험적으로 확인하였으며, 향후 상용화를 위한 연구를 진행할 계획이다.

충돌분류계에서 WIRE MESH를 이용한 열전달 증진에 관한 연구 (The Study on The Heat Transfer Enhancement Using Wire Mesh in Impinging Jet System)

  • 금성민;김동춘;유지오;이창언;임장순
    • 태양에너지
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    • 제17권1호
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    • pp.47-58
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    • 1997
  • 본 연구는 2차원 충돌공기분류계의 포텐셜코어 영역에서 열전달증진을 목적으로 노즐출구와 전열면사이에 메쉬를 설치한후 노즐출구 속도, 메쉬와 전열면사이의 간극, 노즐출구와 전열면사이의 거리를 변화시킬 때의 열전달특성을 메쉬를 설치하지 않은 경우와 비교 검토한 것으로 메쉬를 설치했을 때에는 분류가 전열면에 충돌하면서 소분류로 분할되어 발생하는 난류에 의해 충돌영역에서 열전달성능이 좋아지며, 또한 벽면분류영역으로 진행하면서 홀과 홀사이의 밑부분에서 일어나는 가속으로 인해 열전달성능이 향상된다. 특히 메쉬와 전열면사이의 간극을 변화시켰을 경우 정체점부근에서는 간극이 클수록, 벽면분류영역에서는 간극이 작을수록 전달성능은 향상되며 U=18m/s, H/B=2, C=1인 경우에는 메쉬를 설치하지 않은 평판보다 평균 약 44%의 열전달증진 효과과 있었다. 그리고 본 실험결과를 기존의 난류촉진체를 이용한 연구결과와도 비교 검토하였다.

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타원형 실린더에 의해 교란되어진 난류경계층에 관한 실험적 연구 (A Turbulent Boundary Layer Disturbed by an Elliptic Cylinder)

  • 최재호;조정원;이상준
    • 대한기계학회논문집B
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    • 제25권11호
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    • pp.1476-1482
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    • 2001
  • Turbulent boundary layer over a flat plate was disturbed by installing an elliptic cylinder with an axis ratio of AR=2. For comparison, the same experiment was carried out for a circular cylinder having the same vertical height. The surface pressure and the heat transfer coefficient on the flat plate were measured with varying the gap distance between the elliptic cylinder and the flat plate. The mean velocity and the turbulent intensity profile of the streamwise velocity component were measured using a hot-wire anemometry. As a result, the flow structure and the local heat transfer rate were modified by the interaction between the cylinder wake and the turbulent boundary layer as a function of the critical gap ratio where the regular vortices start to shed. For the elliptic cylinder, the critical gap ratio is increased and the surface pressure on the flat plate is recovered rapidly at downstream location, compared with the equivalent circular cylinder. The maximum heat transfer rate occurs at the gap ratio of G/B = 0.5, where the flow interaction between the lower shear layer of the cylinder wake and the turbulent boundary layer is strong.

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

  • 최재호;이상준
    • 대한기계학회논문집B
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    • 제24권7호
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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.

배플판 형상이 다른 Gun식 가스버너의 난류유동 특성치 고찰 (Investigation on the Turbulent Flow Characteristics of a Gun-Type Gas Burner with the Different Shape of Baffle Plate)

  • 김장권;정규조
    • 대한기계학회논문집B
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    • 제28권4호
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    • pp.475-485
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    • 2004
  • This paper was studied to investigate and compare the effects of inclined baffle plate on the turbulent flow characteristics of a gun-type gas burner through X-Y plane and Y-Z plane respectively by using X-probe from hot-wire anemometer system. For this purpose, two burner models with a cone-type baffle plate and a flat-type one respectively were used. The fast jet flow spurted from slits plays a role such as an air-curtain because it encircles rotational flow by swirl vanes and drives mixed main flow to axial direction regardless of the inclination of baffle plate. The inclined baffle plate causes axial mean velocity component and turbulent intensities etc. to be greatly concentrated towards the central part of a burner, and its effect especially appears in the range of about X/R=1.0-2.0. Also, it gives much larger size to axial mean velocity component and turbulent intensities etc formed near the slits in the range of X/R=1.4103. Especially the inclined baffle plate shifts more the Reynolds shear stress uw to the central region of a burner(Y/R=${\pm}$0.75) than the flat-type one, moreover it develops more strongly than uv.

자유유동 난류강도 변화에 따른 평판위 천이 경계층의 유동특성에 관한 실험적 연구 (Flow Characteristics of Transitional Boundary Layers on a Flat Plate Under the Influence of Freestream Turbulent Intensity)

  • 신성호;전우평;강신형
    • 대한기계학회논문집B
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    • 제22권9호
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    • pp.1335-1348
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    • 1998
  • Flow characteristics in transitional boundary layers on a flat plate were experimentally investigated under three different freestream conditions i. e. uniform flow with 0.1 % and 3.7% freestream turbulent intensity and cylinder-wake with 3.7% maximum turbulent intensity. Instantaneous streamwise velocities in laminar, transitional and turbulent boundary layers were measured by I-type hot-wire probe. For estimation of wall shear stresses on the flat plate, measured mean velocities near the wall were applied to the principle of Computational Preston Tube Method (CPM). Distributions of skin friction coefficients were reasonably predicted in all developed boundary layers. Intermittency profiles, which were estimated using Conditional Sampling Technique in transitional boundary layers, were also consistent with previously published data. It was predicted that the incoming turbulent intensity had more influence on transition onset point and transition process than freestream turbulent intensity existed just over the transition region. It was also confirmed that non-turbulent and turbulent profiles in transitional boundary layers could not be simply treated as Blasius and fully turbulent profiles.

메쉬 스크린을 이용한 충돌제트 열전달 제어에 관한 연구 (Control of Impinging Jet Heat Transfer Using Mesh Screens)

  • 조정원;이상준
    • 대한기계학회논문집B
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    • 제25권5호
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    • pp.722-730
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    • 2001
  • The local heat transfer of an axisymmetric submerged air jet impinging on a heated flat plate is investigated experimentally with the variation of mesh-screen solidity. The screen installed in front of the nozzle exit modifies the flow structure and local heat transfer characteristics. The mean velocity and turbulence intensity profiles of streamwise velocity component are measured using a hot-wire anemometry. The temperature distribution on the heated flat surface is measured with thermocouples. The smoke-wire flow visualization technique was employed to understand the near-field flow structure qualitatively for different mesh screens. Large-scale toroidal vortices and high turbulence intensity enhance the heat transfer rate in the stagnation region. For a higher solidity, turbulence intensity become higher which increases the local heat transfer at small nozzle-to-plate spacings such as L/D<6. The local and average Nusselt numbers of impinging jet from the $\sigma$(sub)s=0.83 screen at L/D=2 are about 5.6∼7.5% and 7.1% larger than those for the case of no screen, respectively. For the nozzle-to-plate spacings larger than 6, however, the turbulence intensities for all tested screens approach to an asymptotic curve and the mean velocity along the jet centerline decreases monotonically. As the nozzle-to-plat spacing increases for high solidity screens, the heat transfer rate decreases due to the reduction in turbulence intensity and jet momentum.

Design Optimization of Hybrid-Integrated 20-Gb/s Optical Receivers

  • Jung, Hyun-Yong;Youn, Jin-Sung;Choi, Woo-Young
    • JSTS:Journal of Semiconductor Technology and Science
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    • 제14권4호
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    • pp.443-450
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    • 2014
  • This paper presents a 20-Gb/s optical receiver circuit fabricated with standard 65-nm CMOS technology. Our receiver circuits are designed with consideration for parasitic inductance and capacitance due to bonding wires connecting the photodetector and the circuit realized separately. Such parasitic inductance and capacitance usually disturb the high-speed performance but, with careful circuit design, we achieve optimized wide and flat response. The receiver circuit is composed of a transimpedance amplifier (TIA) with a DC-balancing buffer, a post amplifier (PA), and an output buffer. The TIA is designed in the shunt-feedback configuration with inductive peaking. The PA is composed of a 6-stage differential amplifier having interleaved active feedback. The receiver circuit is mounted on a FR4 PCB and wire-bonded to an equivalent circuit that emulates a photodetector. The measured transimpedance gain and 3-dB bandwidth of our optical receiver circuit is 84 $dB{\Omega}$ and 12 GHz, respectively. 20-Gb/s $2^{31}-1$ electrical pseudo-random bit sequence data are successfully received with the bit-error rate less than $10^{-12}$. The receiver circuit has chip area of $0.5mm{\times}0.44mm$ and it consumes excluding the output buffer 84 mW with 1.2-V supply voltage.