横流中射流的自发拉特曼散射实验研究

B. Leo
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引用次数: 0

摘要

目的:对三维气体流的实验研究。数据处理需要大量的数据访问,而数据处理需要大量的数据访问,数据处理需要大量的数据访问,数据处理需要大量的数据访问。这就满足了这些要求。其中之一就是利用降雨散射技术来精确测量风洞中的空气密度。在混合过程中,我要把混合物的浓度降到最低,然后仔细地测量。维尔吗?用激光束刺激粒子的合理频率。环境拉曼频移与分子种类有关。散射在Stokes谱线上的光强与探针体积内的分子浓度密切相关。探针体积的直径在0。它的长度在0.6到0.8英寸之间。“最快速度”是每秒100到1000个发明。自发的雷曼散射是tisetl的。ISI。研究了一个从R圆核进入超音速横流的令人激动的超涡旋射流问题。风洞内主要气流内部的马赫数为2.06。这架喷气式飞机的速度是2马赫。实验研究包括了三聚乙烷和三聚乙烷的部分密度,包括了沿模型的整个电场和壁面压力的变化。在经典的流体动力学假设下,密度测量被转换成第一部分B - 1的压力值。. 我们得到了壁面压强场。这些结果与壁面压力分析结果吻合较好。通过对模型的积分,估计了影响模型相互作用的升力系数和空气动力学系数;这是一个压力场。
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Experimental investigation of a jet in a cross-flow by spontaneous Ratman scatter
Ahsfruct The experimental itivcstigatioii of' threedimensional gas flc.rws requircs ircrn-int rrisive ant1 qua si po i n t I i k e mea s 11 remen t s. The re a re s t i I I few techniques for quanti t a t ivc nieasiirenients. which iiieei these demands. One nf them i.c spniitaiienws Rainan scattering which allnws to nicasure tlie tleiisity in wincl tunnels. I n a mixing I'low the par t i a l clenrily is measured. Vil?rational frequencies of niolecrilcs arc stimulatecl by a laser beam. The vilmtional Raman frcqriericy shift depends on the molccular species. The light intensity scattered iii Stokes lines is pmlmrtinnal to the molecular concentratinn in llie probe voluiiie. 'I'he probe volume has a diameter hetween 0. I a n d 0.3 inn1 aiicl a length between 0.6 ant1 0.8 ni i i i . 'flic (lata ratc is 100 to 1000 inenwreinents per second. The spontaneous Ramnn ccattering is tisetl. at ISI,. to investigate an irnpiiiging supers(-rnic jet issuecl from R circular nutlet into a supcrsonic cross-stream. The Mach ni in iber of the main flow in tlie wind tunnel i y 2.06. The inipinging jet ir n incthane jet a t Mach 2. l 'he experimental investigatinn inclutlex iiicthane ancl a i r partial dcnsities ineawrcnients i n (lic iiiipinging jc t inclucetl f l h v field arid wall pressure incasiirenrc~its along the model. On classical f luid dynamics assumptions, clensit ies ineasurcmenta are converted i 11 to part i B I p ressii res. 011 these ass ii in pt io 11 c; . we o 11 t a i t i lhe wall pressure field. 'These rerult$ are in good agreement with wall presslire nieasrii~cnieiits. Tlic lift and nioineirt cnefficients intlucccl hy t l i e jct intcraction are estimated hy tlie integration rrf the \v; iI l pressure f ie ld.
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