• Title/Summary/Keyword: KIVA code

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Numerical Study for Spray Characteristics of Liquid Jet in Cross Flow with Variation of Injection Angle (분사각 변화에 따른 횡단류에 분사되는 액체제트의 분무특성에 대한 수치적 연구)

  • Lee Kwan-Hyung;Ko Jung-Bin;Koo Ja-Ye
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.30 no.2 s.245
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    • pp.161-169
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    • 2006
  • The spray characteristics of liquid jet in cross flow with variation of injection angle are numerically studied. Numerical analysis was carried out using KIVA code, which was modified to be suitable for simulating liquid jet ejected into cross flow. Wave model and Kelvin-Helmholtz(KH)/Rayleigh-Taylor(RT) hybrid model were used for the purpose of analyzing liquid column, ligament, and the breakup of droplet. Numerical results were compared with experimental data in order to verify the reliability of the physical model. Liquid jet penetration length, volume flux, droplet velocity profile and SMD were obtained. Penetration length increases as flow velocity decreases and injection velocity increases. From the bottom wall, the SMD increases as vertical distance increases. Also the SMD decreases as injection angle increases.

Characteristic of Liquid Jet in Subsonic Cross-flow (횡단가스 유동에 분사되는 액체제트의 분무특성)

  • Ko, Jung-Bin;Lee, Kwan-Hyung;Koo, Ja-Ye
    • Journal of ILASS-Korea
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    • v.10 no.1
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    • pp.35-42
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    • 2005
  • The present study has numerically and experimentally investigated the spray behavior of liquid jet injected in subsonic cross-flow. The corresponding spray characteristics are correlated with jet operating parameters. The spray dynamics are known to be distinctly different in the three regimes: the column, the ligament and the droplet regimes. The behaviors of column, penetration and breakup of liquid jet have been studied. Numerical and physical models are base on a modified KIVA code. The primary atomization is represented by a wave model base on the KH(Kelvin-Helmholtz) instability that is generated by a high interface relative velocity between the liquid and gas flows. In odor to capture the spray trajectory, CCD camera has been utilized. Numerical and experimental results indicate that the breakup point is delayed by increasing gas momentum ratio and the penetration decreases by increasing Weber number.

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CONDITIONAL MOMENT CLOSURE MODELING OF TURBULENT SPRAY COMBUSTION IN A DIRECT INJECTION DIESEL ENGINE

  • HAN I. S.;HUH K. Y.
    • International Journal of Automotive Technology
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    • v.6 no.6
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    • pp.571-577
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    • 2005
  • Combustion of turbulent sprays in a direct injection diesel engine is modeled by the conditional moment closure (CMC) model. The CMC routines are combined with the KIVA code to provide conditional flame structures to determine mean state variables, instead of mean reaction rates. An independent transport equation is solved for each flame group with equal mass of sequentially evaporating fuel vapor. CMC calculation begins as the fuel mass for each flame group begins to evaporate with corresponding initialization conditions. Comparison is made with measured pressure traces for four operating conditions at different rpm's and injection conditions. Results show that the CMC model with multiple flame histories can successfully be applied to ignition and mixing-controlled combustion phases of a diesel engine.

Modeling of a Gasoline Spray Impinging on a Wall (벽면충돌 가솔린 분무 모델)

  • 김태완;원영호;박정규
    • Transactions of the Korean Society of Automotive Engineers
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    • v.9 no.5
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    • pp.30-37
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    • 2001
  • Most gasoline engines employ a port injection system to achieve the better fuel-air mixing. A part of injected fuels adheres to the wall or intake valve and forms a film of liquid fuel. The other is secondarily atomized by the spray-wall interaction. A better understanding of this interaction will help in designing injection systems and controlling the strategies to improve engine performance and exhaust emissions. In the present research, the spray-wall interaction was investigated by a laser sheet visualization method. The shape of sprays was pictured at various impinging velocities and angles. The fuel dispersion was estimated by fluorescence light, and the atomization was evaluated by the enlarged images of droplets. The experimental results were compared with model predictions which are based on OPT method. The model has been modified to have the better agreement with the experimental result, and was implemented in the KIVA-II code.

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Prediction of Pressure Drop in Venturi Scrubber Using the Eulerian - Lagrangian Method (오일러-라그랑지 방법을 이용한 벤튜리 스크라버의 압력강하 계산)

  • Pak S, I.;Moon Y. W.;Chang K. S.
    • 한국전산유체공학회:학술대회논문집
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    • 2004.03a
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    • pp.190-195
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    • 2004
  • The pressure drop in a Venturi Scrubber is predicted using the Eulerian-Lagrangian Method, which is one of the numerical methods to solve the dispersed two-phase flow. KIVA-3V Code is modified to solve the coupled gas-liquid two-phase flow field. The liquid is assumed to be injected through the nozzles with the Rosin-Rammler drop size distribution. The computational results shows good agreement with the experimental data.

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The Effect of the Intake Port Configuration on the Flow and Combustion in a 4-Valve Pentroof Gasoline Engine

  • Kim, Hongsuk;Lee, Jeongmin;Nakwon Sung
    • Journal of Mechanical Science and Technology
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    • v.15 no.2
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    • pp.259-267
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    • 2001
  • The flow field in a cylinder of a 4-valve pentroof engine is studied using the KIVA-3V code. Turbulence is generated from the jet flow through valves and broken down to the small scale eddies in the compression process. It is known that the tumble effectively keeps turbulence during the compression process. In the combustion process, turbulence is known to enhance flame speed by increasing mass, momentum and heat transfer rates. The effects of the intake port angles on the flow and combustion characteristics are studied in this study. To study the effect of turbulence on the combustion process, Cantore combustion model is applied in this study.

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Numerical Simulation of Spray Behavior and Its Interaction with Air Flow in Oil Burner (오일 버너에 있어서 분무거동과 공기유동의 상호작용에 관한 수치해석)

  • 나가지마
    • Journal of Advanced Marine Engineering and Technology
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    • v.23 no.3
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    • pp.320-330
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    • 1999
  • A numerical study was performed to investigate spray behavior and its interaction with air flow in a flame holding region of an oil burner(0.1MW) using the KIVA3 code. The numerical results in shape of the recirculating flow and size of the recirculation zone under different conditions were compared to those experimental results. The numerical results in fuel droplet trajectory show that a droplet under 30${\mu}m$ can follow the air flow but a droplet over 50${\mu}m$ penetrates the recirculation zone due to large momentum and a droplet of 30-50${\mu}m$ can follow the recirculating flow or pene-trates the recirculation zone.

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A Study of the Propagation of Turbulent Premixed Flame Using the Flame Surface Density Model in a Constant Volume Combustion Chamber

  • Lee, Sangsu;Kyungwon Yun;Nakwon Sung
    • Journal of Mechanical Science and Technology
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    • v.16 no.4
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    • pp.564-571
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    • 2002
  • Three-dimensional numerical analysis of the turbulent premixed flame propagation in a constant volume combustion chamber is performed using the KIVA-3V code (Amsden et. al. 1997) by the flame surface density (FSD) model. A simple near-wall boundary condition is eaployed to describe the interaction between turbulent premixed flame and the wall. A mean stretch factor is introduced to include the stretch and curvature effects of turbulence. The results from the FSD model are compared with the experimental results of schlieren photos and pressure measurements. It is found that the burned mass rate and flame propagation by the FSD model are in reasonable agreement with the experimental results. The FSD combustion model proved to be effective for description of turbulent premixed flames.

Propose an Analysis Model of Evaporation Process in Multi-Component Fuel Spray (다성분연료 분무에 있어서 증발과정의 해석모델 제안)

  • Yeom, Jeong-Kuk;Tanaka, Tomoyuki
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.33 no.5
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    • pp.373-380
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    • 2009
  • The evaporation process of multi-component fuel is different from one of a single component, because the properties of each component affects among the components. In actual engine, the spatial distribution of fuel vapor concentration dominates auto-ignition and initial combustion, and depends on the volatility and diffusivity of each component fuel contained in the multi-component fuel. Then, this study proposes a simplified numerical scheme for analysis of evaporation process of multi-component fuel sprays. Evaporation process is calculated by KIVA-II code based on the simple two-phases region that is approximated by modified saturated liquid-vapor line, which was obtained by connecting the 50% distillation temperature for each component under several pressure fields. Consequently, it can be quantitatively simulated that vapor of low boiling fuel component mostly exists around nozzle and spray tip region, the high boiling duel component, on the other hand, mostly appears near the spray tip.

The Numerical Study of GDI Spray Behavior on Various Ambient Conditions (분위기 조건에 따른 GDI 분무거동의 수치적 연구)

  • Shim, Young-Sam;Hwang, Soon-Chul;Kim, Duck-Jool
    • Proceedings of the KSME Conference
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    • 2003.11a
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    • pp.466-471
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    • 2003
  • The purpose of this study is to obtain the accurate prediction for the atomization and vaporization processes of GDI spray. Atomization process is modeled using hybrid model that is composed of Linearized Instability Sheet Atomization (LISA) model and Aerodynamically Progressed TAB (APTAB) model. Vaporization process is modeled using Spalding model and Abramzon & Sirignano model. To obtain the experimental results for comparing with calculated results, the cross-sectional images of liquid and vapor phases and SMD distribution were acquired by exciplex fluorescence method and Phase Doppler Analyzer respectively. The experiment and computation was performed at the ambient pressure of 0.1 MPa, 0.5 MPa, 1.0 MPa and the ambient temperature of 293K, 473K. The calculated results by modified KIVA-II code show good agreement with experimental results.

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