湖南大学学报(自然科学版)
湖南大學學報(自然科學版)
호남대학학보(자연과학판)
JOURNAL OF HUNAN UNIVERSITY(NATURAL SCIENCES EDITION)
2015年
5期
65-71
,共7页
王汉封%邹超%王启文%何旭辉
王漢封%鄒超%王啟文%何旭輝
왕한봉%추초%왕계문%하욱휘
钝体绕流%悬臂圆柱%气动力%雷诺数效应
鈍體繞流%懸臂圓柱%氣動力%雷諾數效應
둔체요류%현비원주%기동력%뢰낙수효응
flow around bluff body%cantilevered circular cylinder%aerodynamic forces%Reynolds number effects
通过风洞试验对均匀来流中长径比为5的悬臂圆柱体气动力进行了研究.试验中圆柱直径为200 mm,来流风速为5~45 m/s,对应的雷诺数为0.68×105~6.12×105,涵盖了亚临界、临界与超临界区间.研究表明,尽管悬臂圆柱处于均匀流中,但其气动力特性在不同高度上仍存在显著的差异,悬臂圆柱气动力也存在着明显的雷诺数效应.其从亚临界进入临界区所对应的临界雷诺数略大于二维圆柱.悬臂圆柱阻力系数在临界雷诺数范围内的减小幅度明显小于二维圆柱.在亚临界区内,悬臂圆柱阻力系数小于二维圆柱的对应值,而在超临界区则大于后者.尽管处于均匀流中,悬臂圆柱不同高度所对应的临界雷诺数并不相同,越接近自由端越早出现从亚临界向临界区的转变.
通過風洞試驗對均勻來流中長徑比為5的懸臂圓柱體氣動力進行瞭研究.試驗中圓柱直徑為200 mm,來流風速為5~45 m/s,對應的雷諾數為0.68×105~6.12×105,涵蓋瞭亞臨界、臨界與超臨界區間.研究錶明,儘管懸臂圓柱處于均勻流中,但其氣動力特性在不同高度上仍存在顯著的差異,懸臂圓柱氣動力也存在著明顯的雷諾數效應.其從亞臨界進入臨界區所對應的臨界雷諾數略大于二維圓柱.懸臂圓柱阻力繫數在臨界雷諾數範圍內的減小幅度明顯小于二維圓柱.在亞臨界區內,懸臂圓柱阻力繫數小于二維圓柱的對應值,而在超臨界區則大于後者.儘管處于均勻流中,懸臂圓柱不同高度所對應的臨界雷諾數併不相同,越接近自由耑越早齣現從亞臨界嚮臨界區的轉變.
통과풍동시험대균균래류중장경비위5적현비원주체기동력진행료연구.시험중원주직경위200 mm,래류풍속위5~45 m/s,대응적뢰낙수위0.68×105~6.12×105,함개료아림계、림계여초림계구간.연구표명,진관현비원주처우균균류중,단기기동력특성재불동고도상잉존재현저적차이,현비원주기동력야존재착명현적뢰낙수효응.기종아림계진입림계구소대응적림계뢰낙수략대우이유원주.현비원주조력계수재림계뢰낙수범위내적감소폭도명현소우이유원주.재아림계구내,현비원주조력계수소우이유원주적대응치,이재초림계구칙대우후자.진관처우균균류중,현비원주불동고도소대응적림계뢰낙수병불상동,월접근자유단월조출현종아림계향림계구적전변.
The aerodynamic forces on a cantilevered circular cylinder with an aspect ratio of 5 were ex-perimentally investigated in a wind tunnel.The diameter of the cylinder d was 200 mm.The oncoming flow velocity ranged from 5 m/s to 45 m/s,corresponding to Reynolds number of 0.68×10 5 ~6.12×10 5 , which covered subcritical,critical and transcritical regimes.It was found that,although the cantilevered cylinder is in uniform flow,its aerodynamic forces present significant differences at various spanwise posi-tions,indicating a strong three dimensionality.Reynolds number has profound effect on the aerodynamic forces on the cantilevered cylinder.The critical Reynolds number is smaller for the cantilevered cylinder relative to that of 2D cylinder.In the critical regime,reduction in the drag coefficient (C d )of the cantile-vered cylinder is relatively smaller compared with that of 2D cylinder.In subcritical regime,C d of the can-tilevered cylinder is smaller than that of 2D cylinder.On the other hand,C d of the former is larger in tran-scritical regime.The critical Reynolds number is different at various spanwise locations for the cantilevered cylinder.Transition from subcritical to critical regimes occurs earlier near the free end of the cantilevered cylinder.