• 제목/요약/키워드: Thermophoretic

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균일 층류유동중에 있는 원형 실린더 주위의 열영동에 의한 입자 부착 (Thermophoretic Particle Deposition Around a Circular Cylinder in a Uniform Laminar Air Dlow)

  • 홍기혁;강신형
    • 대한기계학회논문집B
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    • 제20권2호
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    • pp.641-648
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    • 1996
  • Thermophoretic particle deposition on a circular cylinder in a uniform laminar air flow was numerically investigated using a control volume method based on the generalized non-orthogonal coordinate system. Variation of air properties due to the change of temperature was taken into account. Effects of variable property on the distribution of heat transfer and deposition rates of particle were discussed. A new correlation of thermophoretic particle deposition on a circular cylinder was proposed in the present study.

정체점 입자유동에서 복사열전달을 고려한 열영동 입자부착 연구 (A study of thermophoretic particle deposition in a particle laden stagnation flow including the effect of radiative heat transfer)

  • 정창훈;이공훈;최만수;이준식
    • 대한기계학회논문집B
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    • 제20권5호
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    • pp.1624-1638
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    • 1996
  • A study of thermophoretic particle deposition has been carried out for a particle laden stagnation flow considering the effect of radiative heat transfer. Energy, concentration and radiative transfer equations are all coupled and have been solved iteratively assuming that absorption and scattering coefficients were proportional to the local concentration of particles. Radiative heat transfer was shown to strongly affect the profiles of temperature and particle concentration. e. g., radiation increases the thickness of thermal boundary layer and wall temperature gradients significantly. As the wall temperature gradients increase, the particle concentration at the wall decreases due to thermophoretic particle transport. The deposition rate that is thermophoretic velocity times particle concentration at the wall decreases as the effects of radiation increases. The effects of optical thickness, conduction to radiation parameter and wall emissivity have been determined. The effects of anisotropic scattering are shown as insignificant.

미세유체 채널 내에서 열영동에 의한 입자이동 제어 (Thermophoretic Control of Particle Transport in a Microfluidic Channel)

  • 소주희;구형준
    • Korean Chemical Engineering Research
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    • 제57권5호
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    • pp.730-734
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    • 2019
  • 열영동은 매질의 온도 구배에 의해 입자가 이동하는 현상이다. 본 논문에서는 미세유체 채널에서 입자의 열영동 현상에 대해서 논의한다. 흐름이 없는 비유동 채널에서 열원인 백금 와이어에 가해지는 전압에 비례해서 열영동에 의한 마이크로 입자의 이동이 더 크게 나타남을 확인하였다. 전압에 따른 백금 와이어 주변 온도 변화는 Callendar-van Dusen 식을 이용하여 예측하였다. 동일한 시스템에서 나노 입자의 열영동 현상을 관찰한 결과, 나노 입자도 마이크로 입자와 유사한 열영동 거동을 보임을 확인하였다. 마지막으로 Y 모양 미세유체 채널을 제작하고 백금 와이어 열원을 채널 내에 설치하여, 채널을 흐르는 현탁액 내의 입자의 열영동 현상을 구현하고, 이를 기반으로 현탁액의 흐름을 제어할 수 있음을 보인다.

디젤매연측정용 마이크로 희석터널의 희석챔버에서의 열유동 특성 (Characteristics of Thermo-Fluid Flow in Dilution Chamber of Micro-Dilution Tunnel for Diesel Particulate Measurement)

  • 김태권;김성훈;임문혁
    • 한국자동차공학회논문집
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    • 제10권6호
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    • pp.90-99
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    • 2002
  • The main purpose of this study lies on the development of micro dilution tunnel based on the Sierra Dilution chamber model. As a primary examination, characteristics of flow and temperature distributions during the steady dilution process in dilution chamber are observed with numerical analysis. The penetration of dilution air through porous tube as well as wall temperature and temperature gradient inside porous tube are examined. The thermophoretic velocity in terms of temperature behavior inside porous tube are defined and examined. Based on the ratio of penetration and thermophoretic velocities, all part of porous tube are shown to be safe from the particulate depositions. However, The inlet portion of porous tube in addition to the portion of impinging of dilution air are marginally safe from the particulate depositions. Generally the safer design against particulate deposition is required in provision f3r steady dilution process and for transient process as well.

외부증착공정에서의 열영동에 의한 입자부착에 관한 3차원 해석 (Three-dimensional analysis of the thermophoretic particle deposition in the OVD process)

  • 홍기혁;강신형
    • 대한기계학회논문집B
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    • 제21권3호
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    • pp.436-444
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    • 1997
  • Three-dimensional conjugate heat transfer and particle deposition on a circular cylinder in the OVD process are numerically investigated. Flow and temperature fields are obtained by an iterative method, and thermophoretic particle deposition is simulated. Effects of the heat conduction in the cylinder, the rotation speed of the cylinder, and the traversing speed of torch on the deposition are studied. Effects of variable properties are also included. As the conductivity of the cylinder decreases, particle deposition rate and deposition efficiency greatly decrease due to the reduced temperature gradient. The rotation of the cylinder has no significant effect on the deposition due to the small diameter of the cylinder and low speed of rotation. Since the increase of the torch speed keeps the surface low temperature, the particle deposition increases with the traversing speed.

미소중력환경에서의 고체벽면근방 층류확산염내 매연입자의 열영동 부착 (Thermophoretic deposition of soot particles in laminar diffusion flame along a solid wall in microgravity)

  • 최재혁;후지타오사무;정석호
    • 한국연소학회:학술대회논문집
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    • 한국연소학회 2007년도 제34회 KOSCO SYMPOSIUM 논문집
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    • pp.19-24
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    • 2007
  • The deposition behavior of soot particles in a diffusion flame along a solid wall was examined experimentally by getting rid of the effect of natural convection utilizing microgravity environment. The microgravity environment was realized by using a drop tower facility. The fuel for the flame was an ethylene ($C_2H_4$) and the surrounding oxygen concentration 35% with the surrounding air velocity of $V_a$=2.5, 5, and 10 cm/s. Laser extinction method was adopted to measure the soot volume fraction distribution between the flame and burner wall. The results show that observation of soot deposition in normal flame was difficult from buoyancy and the relative position of flame and solid surface changes with time. The soot particle distribution region moves closer to the surface of the wall as the surrounding air velocity is increased. And the experiments determined the trace of the maximum soot concentration line. It was found that the distance between soot line and flame line is around 5 mm. That is, the soot particle near the flame zone tends to move away from flame zone because of thermophoretic force and to concentrate at a certain narrow area inside of the flame, finally, to adhere the solid wall.

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버너의 벽면온도와 연소실내 주위공기온도에 따른 매연입자의 열영동 부착 특성에 관한 수치적 연구 (Numerical Study on the Thermophoretic Deposition Characteristics of Soot Particles for Wall Temperature of Burner and Surrounding Air Temperature in Combustion Duct)

  • 최재혁;한원희;윤두호;윤석훈;정석호
    • Journal of Advanced Marine Engineering and Technology
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    • 제32권1호
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    • pp.57-65
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    • 2008
  • The characteristics of soot deposition on the cold wall in laminar diffusion flames have been numerically analyzed with a two-dimension with the FDS (Fire Dynamics Simulator). In particular, the effects of surrounding air temperature and wall temperature have been discussed. The fuel for the flame is an ethylene ($C_2H_4$). The surrounding oxygen concentration is 35%. Surrounding air temperatures are 300K, 600K, 900K and 1200K. Wall temperatures are 300K, 600K and 1200K. The soot deposition length defined as the relative approach distance to the wall per a given axial distance is newly introduced as a parameter to evaluate the soot deposition tendency on the wall. The result shows that soot deposition length is increased with increasing the surrounding air temperatures and with decreasing the wall temperature. And the numerical results led to the conclusion that it is essential to consider the thermophoretic effect for understanding the soot deposition on the cold wall properly.

열영동력이 수평 웨이퍼상의 입자침착에 미치는 영향 (Thermophoretic Effect on Particle Deposition Toward a Horizontal Wafer)

  • 배귀남;박승오;이춘식
    • 대한기계학회논문집
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    • 제18권1호
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    • pp.175-183
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    • 1994
  • To investigate thermophoretic effect on particle deposition, average deposition velocity toward a horizontal wafer surface in vertical airflow is measured keeping the wafer surface temperature different from the surrounding air temperature. In the present measurement, the temperature difference is maintained in the range from -10 to $4^{\circ}$ C Polystyrene latex (PSL) spheres of diameter between 0.3 and 0.8 .mu.m are used for the experiment. The number of particles deposited on a wafer surface is estimated from the measurements using a wafer surface scanner (PMS SAS-3600). Experimental data are compared with prediction model results.

입자의 형상에 따른 열영동 영향에 대한 실험적 연구 (Experimental Study on Thermophoretic Particle Deposition for an Agglomerated and Non-Agglomerated Particles)

  • 최광열;윤진욱;안강호
    • 대한기계학회논문집B
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    • 제28권7호
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    • pp.741-746
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    • 2004
  • Agglomerated and non-agglomerated SiO$_2$ particles are synthesized in a furnace by oxidation of TEOS vapor. These polydispersed particles are classified with DMA to extract particles. Then these particles are introduced into a thermal precipitator through the ESP(Electrostatic Precipitator) to investigate the themophoretic particle deposition using CNCs(Condensation Nuclei Counter). The efficiency of themophoretic particle deposition according to agglomerated and non-agglomerated particles in the thermal precipitator has been studied as a function of particle size and TEOS mole concentration using monodisperse particles classified by DMA. The results show that the particle deposition efficiency decreases as TEOS mole concentration increases and particle size increases. Thereffre, it is concluded that the thermophoretic deposition efficiency is dependent of the particle morphology.

가열 또는 냉각되는 수평웨이퍼 표면으로의 입자침착에 관한 해석 (Analysis of Particle Deposition onto a Heated or Cooled, Horizontal Free-Standing Wafer Surface)

  • 유경훈;오명도;명현국
    • 대한기계학회논문집
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    • 제19권5호
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    • pp.1319-1332
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    • 1995
  • Numerical analysis was performed to characterize the particle deposition behavior on a horizontal free-standing wafer with thermophoretic effect under the turbulent flow field. A low Reynolds number k-.epsilon. turbulence model was used to analyze the turbulent flow field around the wafer, and the temperature field for the calculation of the thermophoretic effect was predicted from the energy equation introducing the eddy diffusivity concept. The deposition mechanisms considered were convection, diffusion, sedimentation, turbulence and thermophoresis. For both the upper and lower surfaces of the wafer, the averaged particle deposition velocities and their radial distributions were calculated and compared with the laminar flow results and available experimental data. It was shown by the calculated averaged particle deposition velocities on the upper surface of the wafer that the deposition-free zone, where the deposition velocite is lower than 10$^{-5}$ cm/s, exists between 0.096 .mu.m and 1.6 .mu.m through the influence of thermophoresis with positive temperature difference of 10 K between the wafer and the ambient air. As for the calsulated local deposition velocities, for small particle sizes d$_{p}$<0.05 .mu.m, the deposition velocity is higher at the center of the wafer than at the wafer edge, whereas for particle size of d$_{p}$ = 2.0 .mu.m the deposition takes place mainly on the inside area of the wafer. Finally, an approximate model for calculating the deposition velocities was recommended and the calculated deposition velocity results were compared with the present numerical solutions, those of Schmidt et al.'s model and the experimental data of Opiolka et al.. It is shown by the comparison that the results of the recommended model agree better with the numerical solutions and Opiolka et al.'s data than those of Schmidt's simple model.