• 제목/요약/키워드: 미립화 및 액적분열모델

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난류 횡단류에 수직 분사 되는 액주의 분열 및 기화 특성에 관한 LES (LES of Breakup and Atomization Characteristics of a Liquid Jet into Cross Turbulent Flow)

  • 양승준;구자예;성홍계
    • 한국추진공학회지
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    • 제14권2호
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    • pp.1-9
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    • 2010
  • 난류 유동장으로 분사되는 액체 제트의 액주 분열과 액적 미립화 현상에 관한 LES를 수행하였다. 기체상태의 공기 유동해석에 Eulerian 해법을 사용하고, 액적 추적을 위하여 Lagrangian 해법을 사용하여 기체-액체간 이상유동(two phase flow) 해석을 수행하였다. 액적 분열 과정 모사에 blob-KH 분열 모델을 적용하여 액주와 액적의 분열이 관찰되었다. 일정한 공기 유동 조건에서 액체 분사 속도 변화를 통한 액체-기체 운동량 플럭스 비의 변화에 따른 액체 제트의 침투깊이를 조사하였으며 실험결과와 유사함을 알 수 있었다. 분사 제트의 분열에 따라 유동장에 존재하는 액적의 분포를 Sauter 평균 입경(SMD)의 분석을 통해 수행하였다.

사각 덕트내 난류 횡단류 유동장에 분사되는 액체 제트의 분열과 미립화에 관한 LES 해석 (LES on breakup and atomization of a liquid jet into cross turbulent flow in a rectangular duct)

  • 유영린;한두희;성홍계;전혁수;박철현
    • 한국항공우주학회지
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    • 제44권4호
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    • pp.290-297
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    • 2016
  • 사각덕트에서 난류 유동장으로 분사되는 액체 제트의 액주 분열과 미립화 현상에 관한 LES를 수행하였다. 기체상태의 공기 유동 해석에 오일러리안 해법을 사용하고, 액적 추적을 위하여 라그랑지안 해법을 사용하여 기체-액체간 이상유동(two phase flow) 해석을 수행하였다. 액적 분열 모델, 아격자 스케일 모델 및 공간 차분법에 따른 액적 분열을 조사하였다. 액체 제트의 침투깊이를 경험식과 비교하였으며 경험식보다 약간 높음을 알 수 있었다. 제트 후류에서 사우터 평균직경에 대한 분석을 수행하였다.

디젤분무에서 미립화 및 액적분열모델의 예측능력평가 (Assessment of Prediction Ability of Atomization and Droplet Breakup Models on Diesel Spray Dynamic)

  • 김정일;노수영
    • 한국분무공학회지
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    • 제5권2호
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    • pp.35-42
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    • 2000
  • A number of atomization and droplet breakup models have been developed and used to predict the diesel spray characteristics. Of the many atomization and droplet breakup models based on the breakup mechanism due to aerodynamic liquid and gas interaction, four models classified as mathematical models, such as TAB, modified TAB, DDB, WB and one of the hybrid model based on WB and TAB models were selected for the assessment of prediction ability of diesel spray dynamics. The assessment of these models by using KIVA-II code was performed by comparing with the experimental data of spray tip penetration and sauter mean diameter(SMD) from the literature. It is found that the prediction of spray tip penetration and SMD by the hybrid model was only influenced by the initial parcel number. All the atomization and droplet breakup models considered here was strongly dependent on the grid resolution. Therefore it is important to check the grid resolution to get an acceptable results in selecting the models. At low injection pressure, modified TAB model could only give the good agreement with experimental data of spray tip penetration and both of modified TAB and DDB models were recommendable for the prediction of SMD. At high injection pressure, hybrid model could only give the good agreement with the experimental data of spray tip penetration and the prediction of all of the selected models did not match the experimental data. Spray tip penetration was increased with the increase the $B_1$ and the increase of $B_1$ did not affected the prediction of SMD.

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디젤분무의 모사를 위한 혼합 모델의 개발 (Development of Hybrid Model for Simulating of Diesel Spary Dynamics)

  • 김정일;노수영
    • 한국자동차공학회논문집
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    • 제9권1호
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    • pp.8-19
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    • 2001
  • A number of atomization and droplet breakup models have been developed and used to predict the diesel spray characteristic. Most of these models could not provide reasonable computational result of the diesel spray characteristic because they have only considered the primary breakup. A hybrid model is, therefore, required to develop by considering the primary and secondary breakup of liquid jet. according to this approach, wave breakup(WB) model was used compute the primary breakup of the liquid jet and droplet deformation and breakup(DDB) model was used for the secondary breakup of droplet. Development of hybrid model by using KIVA-II code was performed by comparing with the experimental data of spray tip penetration and SMD from the literature. A hybrid model developed in this study could provide the good agreement with the experimental data of spray tip penetration. The prediction results of SMD were in good agreement between 0.5 and 1.0 ms after the start of injection. Numerical results obtained by the present hybrid model have the good agreement with the experimental data with the breakup time constant in WB model of 30, and DDB model constant Ck of 1.0 when the droplet becomes less than 95% of maximum droplet diameter injected.

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