天津大学学报
天津大學學報
천진대학학보
Journal of Tianjin University
2015年
10期
929-936
,共8页
刘伟光%张涛%徐英%白龙
劉偉光%張濤%徐英%白龍
류위광%장도%서영%백룡
锥形流量计%CFD仿真%PIV实验%锥体尾涡%湍流模型
錐形流量計%CFD倣真%PIV實驗%錐體尾渦%湍流模型
추형류량계%CFD방진%PIV실험%추체미와%단류모형
cone flowmeter%computational fluid dynamics simulation%particle image velocimetry(PIV) experi-ment%vortex in the cone wake flow field%turbulence model
锥形流量计尾流流场通过差压影响锥形流量计的流出系数,是影响锥形流量计性能的关键指标.为此,使用PIV实验的方法研究DN100口径,β为0.65,前后锥角分别为26.0°和67.5°的锥形流量计尾流流场的速度分布状况.通过 PIV 实验得到锥形流量计尾流中存在漩涡结构.对比 PIV 实验和 CFD 仿真得到的锥形流量计尾流漩涡处的速度分布、漩涡中心得出结论:SST k-ω湍流模型更适合锥形流量计的三维流场的仿真.利用校准后的CFD仿真得到2个规律:经过管道内径的无量纲化以后,锥形流量计尾涡的涡心、漩涡尺寸在4×104~3×105的入口雷诺数范围内仅与β相关;在此入口雷诺数范围内,同一锥形流量计的尾涡涡心的位置和漩涡长度保持稳定.
錐形流量計尾流流場通過差壓影響錐形流量計的流齣繫數,是影響錐形流量計性能的關鍵指標.為此,使用PIV實驗的方法研究DN100口徑,β為0.65,前後錐角分彆為26.0°和67.5°的錐形流量計尾流流場的速度分佈狀況.通過 PIV 實驗得到錐形流量計尾流中存在漩渦結構.對比 PIV 實驗和 CFD 倣真得到的錐形流量計尾流漩渦處的速度分佈、漩渦中心得齣結論:SST k-ω湍流模型更適閤錐形流量計的三維流場的倣真.利用校準後的CFD倣真得到2箇規律:經過管道內徑的無量綱化以後,錐形流量計尾渦的渦心、漩渦呎吋在4×104~3×105的入口雷諾數範圍內僅與β相關;在此入口雷諾數範圍內,同一錐形流量計的尾渦渦心的位置和漩渦長度保持穩定.
추형류량계미류류장통과차압영향추형류량계적류출계수,시영향추형류량계성능적관건지표.위차,사용PIV실험적방법연구DN100구경,β위0.65,전후추각분별위26.0°화67.5°적추형류량계미류류장적속도분포상황.통과 PIV 실험득도추형류량계미류중존재선와결구.대비 PIV 실험화 CFD 방진득도적추형류량계미류선와처적속도분포、선와중심득출결론:SST k-ω단류모형경괄합추형류량계적삼유류장적방진.이용교준후적CFD방진득도2개규률:경과관도내경적무량강화이후,추형류량계미와적와심、선와척촌재4×104~3×105적입구뢰낙수범위내부여β상관;재차입구뢰낙수범위내,동일추형류량계적미와와심적위치화선와장도보지은정.
Cone wake flow field is the key factor to the cone flowmeters’ performance because the field affects dis-charge coefficient through the differential pressure. The wake flow field’s velocity distribution of cone flowmeter with DN100,β value being 0.65,front cone’s angle being 26.0° and back cone’s angle being 67.5° was studied by PIV experimental method. Vortex structure was found in the wake flow field of cone flowmeter. By comparing the velocity distribution and vortex core of cone wake vortex between the PIV experimental data and CFD simulation data,the conclusion has been drawn that SSTk-ω turbulence model is more suitable for the three dimensional flow field simula-tion of cone flowmeter. Two laws have been deduced by CFD simulation:within Reynolds number range of 4×104—3×105 the vortex core’s position and vortex’s size of cone wake flow field are only affected byβ value after non-dimension disposal of the inner diameter of the meter’s tube;vortex core position and length of vortex in the cone wake flow field remain stable to the same cone flowmeter.