• Title/Summary/Keyword: gas bubble

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독성가스 제거용 기포탑 반응기의 설계기법 (Design Parameters Estimations for Bubble Column Reactors to Remove Toxic Gases)

  • 오정환;홍민선
    • 한국위험물학회지
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    • 제6권2호
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    • pp.95-104
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    • 2018
  • Gas-liquid bubble column reactors are extensively used in industrial processes. A detailed knowledge of bubble size distribution is needed for determining the mass transfer in gas-liquid film. Experimental data on bubble size distribution and liquid-side mass transfer coefficient($k_L$) were used to calculate the estimated time to saturation in bubble column reactor. Also, the gas flux was evaluated to the liquid-side mass transfer coefficient($k_L$) and solubility data for hydrogen sulfide($H_2S$) and chlorine($Cl_2$) absorption into water. Simulation results show that $H_2S$ absorption time to 50 % of saturation concentrations are 611 sec and 1,329 sec when bubble diameters are 0.5 mm and 4.5 mm, while absorbing 1 % $H_2S$ gas. In case of $Cl_2$, absorption time range 657 to 1,400 sec when bubble size range 0.5 mm to 4.5 mm, while absorbing 1 % $Cl_2$ gas. Calculated simulation results can be used in the design of emergency relief bubble reactors.

영상기법을 이용한 수직상향 기포유동에 관한 연구 (A Study on the Vertical upward Bubble Flow using Image Processing Technique)

  • 서동표;오율권
    • Journal of Advanced Marine Engineering and Technology
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    • 제27권5호
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    • pp.617-623
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    • 2003
  • In the present study, the characteristics of upward bubble flow were experimentally investigated in a liquid bath. The velocity of upward bubble flow was calculated for two different experimental conditions:1) bubble flow without kinetic energy 2) bubble flow with kinetic energy. Bubble flow without kinetic energy starts to undergo the effect of buoyancy l0cm away from the nozzle. Whereas. kinetic energy is dominant before 30 cm away from the nozzle in bubble flow but after this point kinetic energy and inertial force are applied on bubble flow at the same time In addition, as the flow rate increases the maximum velocity point moves to the nozzle. The velocity Profiles near free surface is extremely irregular due to surface flow. Gas volume fraction is high near the nozzle due to gas concentration. but decreases with the increasement of axial position. Gas volume fraction does not vary after the axial position, z=60 in spite of the increasement of flow.

수직상향 기체주입시 기포거동에 관한 연구 (A Study on the Bubble Behavior in the Vertical-upward Gas Injection)

  • 서동표;오율권
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2003년도 추계학술대회
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    • pp.712-716
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    • 2003
  • In the present study, the gas injection system based on air-water model was designed to investigate the behavior characteristics of bubbles injected into a ladle. The parameters such as gas volume fraction and bubble rise velocity were exprementally measured in a gas-liquid flow region. To measure gas volume fraction, an electo-conductivity probe was used and bubble rise velocity was obtained by a high speed CCD camera. Gas volume fraction was symmetric to the axis of nozzle secured on the bottom of a ladle. The bubble rise velocity was calculated for two different experimental conditions. That is, gas flow conditions were following two case: 1) Q = $0.63{\times}10^{-4}$ $m^{3}/s$, 2) $1.26{\times}10^{-4}$ $m^{3}/s$. As a gas injected into the liquid ladle, the liquid-phase region is circulated by bubbles' behavior. The bubble rise velocity was influenced of the circulation flow of liquid phase. As a result, the bubble rise velocity was appeared higher middle region of ladle than near the nozzle.

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Gas Bubble Driven Circulation Systems에서의 이상유동 특성의 시뮬레이션 (A Simulation on the Two-Phase Flow Characteristics in Gas Bubble Driven Circulation Systems)

  • 최청렬
    • 한국시뮬레이션학회논문지
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    • 제7권2호
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    • pp.17-32
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    • 1998
  • The flow fields in Gas Bubble Driven Circulation Systems were numerically analyzed. In various gas flow rate and bubble size, the flow characteristics were predicted. Eulerian-Eulerian approach was used for the formulation of both the continuous and dispersed phases. The modification of the general purpose computer program PHOENICS code was employed to predict the mean flow fields, turbulent characteristics, gas dispersion, volume fraction. The predicted shows very satisfactory agreement with experimental results for all regions of ladle. The results are of interest in the design and operation of wide variety of material processing.

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Comparative Study of Mass Transfer and Bubble Hydrodynamic Parameters in Bubble Column Reactor: Physical Configurations and Operating Conditions

  • Sastaravet, Prajak;Chuenchaem, Chomthisa;Thaphet, Nawaporn;Chawaloesphonsiya, Nattawin;Painmanakul, Pisut
    • Environmental Engineering Research
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    • 제19권4호
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    • pp.345-354
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    • 2014
  • In this paper, effects of physical configurations and operating conditions on bubble column performance were analyzed in terms of bubble hydrodynamic and mass transfer parameters. Bubble column with 3 different dimensions and 7 gas diffusers (single / multiple orifice and rigid / flexible orifice) were applied. High speed camera and image analysis program were used for analyzing the bubble hydrodynamic parameters. The local liquid-side mass transfer coefficient ($k_L$) was estimated from the volumetric mass transfer coefficient ($k_La$) and the interfacial area (a), which was deduced from the bubble diameter ($D_B$) and the terminal bubble rising velocity ($U_B$). The result showed that the values of kLa and a increased with the superficial gas velocity (Vg) and the size of bubble column. Influences of gas diffuser physical property (orifice size, thickness and orifice number) can be proven on the generated bubble size and the mass transfer performance in bubble column. Concerning the variation of $k_L$ coefficients with bubble size, 3 zones (Zone A, B and C) can be observed. For Zone A and Zone C, a good agreement between the experimental and the predicted $K_L$ coefficients was obtained (average difference of ${\pm}15%$), whereas the inaccuracy result (of ${\pm}40%$) was found in Zone B. To enhance the high $k_La$ coefficient and absorption efficiency in bubble column, it was unnecessary to generate numerous fine bubbles at high superficial gas velocity since it causes high power consumption with the great decrease of $k_L$ coefficients.

마이크로 T자형 합류지점에서 기체 및 액체의 주입 방법이 기포 및 액체 슬러그 생성에 미치는 영향 (Effect of Gas- and Liquid-injection Methods on Formation of Bubble and Liquid Slug at Merging Micro T-junction)

  • 이준경;이치영
    • 대한기계학회논문집B
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    • 제40권4호
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    • pp.227-236
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    • 2016
  • 본 논문에서는 $600{\times}600{\mu}m$ 사각 마이크로 채널에서 T자형 합류지점에서의 기체 및 액체의 주입방법이 기포 및 액체 슬러그의 생성에 미치는 영향을 실험을 통해 살펴보았다. 실험 유체로는 질소와 물을 사용하였으며, 액체 및 기체 겉보기 속도는 각각 0.05 - 1 m/s, 0.1 - 1 m/s 의 범위로 테일러 유동이 나타나는 구간에서 데이터를 얻었다. 기포 길이, 액체 슬러그 길이, 기포 속도 그리고 기포 생성 빈도를 고속 카메라를 사용하여 이미지 분석을 통해 측정하였다. 유사한 입구 겉보기 속도 조건에서, T-자형 합류지점의 main channel에 기체를 주입하는 방법(T_gas-liquid)이 액체를 주입하는 방법(T_liquid-gas)보다 기포와 액체 슬러그의 길이가 길었고 기포 생성 빈도는 낮았다. 한편, 두 주입방법에서 기포 속도는 유사하게 나타났다. T_liquid-gas 주입방법의 기존 예측 상관식은 T_gas-liquid 주입방법의 기포 길이, 기포 속도, 액체 슬러그 길이, 기포 생성 빈도 실험데이터를 각각 ~24 %, ~9 %, ~39 %, ~55 %로 예측하였다.

Semiempirical model for wet scrubbing of bubble rising in liquid pool of sodium-cooled fast reactor

  • Pradeep, Arjun;Sharma, Anil Kumar
    • Nuclear Engineering and Technology
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    • 제50권6호
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    • pp.849-853
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    • 2018
  • Mechanistic calculations for wet scrubbing of aerosol/vapor from gas bubble rising in liquid pool are essential to safety of sodium-cooled fast reactor. Hence, scrubbing of volatile fission product from mixed gas bubble rising in sodium pool is presented in this study. To understand this phenomenon, a theoretical model has been setup based on classical theories of aerosol/vapor removal from bubble rising through liquid pools. The model simulates pool scrubbing of sodium iodide aerosol and cesium vapor from a rising mixed gas bubble containing xenon as the inert species. The scrubbing of aerosol and vapor are modeled based on deposition mechanisms and Fick's law of diffusion, respectively. Studies were performed to determine the effect of various key parameters on wet scrubbing. It is observed that for higher vapor diffusion coefficient in gas bubble, the scrubbing efficiency is higher. For aerosols, the cut-off size above which the scrubbing efficiency becomes significant was also determined. The study evaluates the retention capability of liquid sodium used in sodium-cooled fast reactor for its safe operation.

기포계수식 발효가스 발생량 계측시스템의 개발 (Development of Gas Production Measurement System by Bubble Counting during Fermentation)

  • 이영진;전재근
    • 한국식품과학회지
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    • 제26권3호
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    • pp.195-198
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    • 1994
  • Yeast 발효공정에서 발생되는 가스량을 전자적으로 monitoring 할 수 있는 새로운 기포수 계측 쎈서를 설계, 제작하였다. 본 기포쎈서는 기체를 발생하는 발효공정에 적용할 수 있으며 공정의 상태와 환경에 아무런 변화를 주지 않도록 설계하였다. 그 구조는 가스포집부, 기포형성부, 전자식 기포감지부와 컴퓨터 접속장치로 구성하였다. 기포 계측부는 photo-interrupter카 counter IC 등을 사용하였다. 제작된 쎈서와 컴퓨터 시스템은 효모 배양공정에 활용하여 발효진행과정을 자동적으로 monitoring 하는데 성공하였으며 발효공정에서 발생된 기포수의 값으로 작성된 가스발생량 곡선은 효모의 생육곡선의 양상과 매우 유사한 모양을 보였으며 배양액의 기질영양원이 달리한 발효공정을 monitering한 결과 기질이용 특성도 정확하게 표현할 수 있었다.

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점성슬러리 기포탑에서 작은 기포의 체류량 특성 (Holdup Characteristics of Small Bubbles in a Viscous Slurry Bubble Column)

  • 진해룡;송양호;강용;정헌;이호태
    • Korean Chemical Engineering Research
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    • 제49권1호
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    • pp.83-88
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    • 2011
  • 점성슬러리 기포탑에서 작은 기포의 체류량 특성에 대해 고찰하였다. 정압 강하방법(Static pressure drop method)에 의해 구한 기포탑 내부전체 기포체류량과 이중저항탐침법(dual resistivity probe method)에 의해 구한 큰 기포의 체류량으로부터 기포탑 내부에 체류하는 작은 기포의 체류량을 구할 수 있었다. 기체유속, 연속액상의 점도 그리고 슬러리 상중에 포함된 고체입자의 분율이 전체 기체체류량, 큰 기포의 체류량 그리고 작은 기포의 체류량에 미치는 영향을 검토하였다. 점성슬러리 기포탑에서 작은 기포의 체류량은 기체의 유속이 증가하면 증가하였으나 연속액상의 점도와 슬러리상에 포함된 고체입자의 분율이 증가하면 감소하였다. 기포탑 내부에 체류하는 전체 기포 체류량 중 작은 기포 체류량의 분율은 기체유속이 증가하면 증가하였으나 연속액상의 점도와 슬러리상에 포함된 고체입자의 분율이 증가하면 감소하였다. 기포탑 내부에 체류하는 작은 기포는 큰 기포의 상승속도에 영향을 미치지 못하였다.

사각 마이크로 채널 내 Taylor Flow의 기포 및 액체 슬러그 유동 특성에 대한 연구 (Study on the Characteristics of Bubble and Liquid Slugs for Gas-Liquid Taylor Flow in a Rectangular Micro-channel)

  • 이준경;이관근
    • 설비공학논문집
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    • 제27권10호
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    • pp.520-526
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    • 2015
  • The characteristics of gas-liquid Taylor (Slug) flow in a square micro-channel of $600{\sim}600{{\mu}m}$ were investigated experimentally in this paper. The test fluids were nitrogen and water. The liquid and gas superficial velocities were 0.01~3 m/s and 0.1~3 m/s, respectively. Bubble and liquid slug length, bubble velocity, and frequency were measured by analyzing optical images using a high speed camera. Bubble length decreased with higher liquid flow rate, which increased dramatically with higher gas flow rate. However, slug length did not vary with changes in inlet liquid conditions. Additionally, bubble velocities and frequencies increased with higher liquid and gas flow rates. It was found that measured bubble lengths were in good agreement with the empirical models in the existing literature, but slug lengths were not.