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Bubble-induced skin-friction drag reduction and the abrupt transition to air-layer drag reduction

机译:气泡引起的皮肤摩擦减阻作用和突然过渡到空气层减阻作用

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摘要

To investigate the phenomena of skin-friction drag reduction in a turbulent boundary layer (TBL) at large scales and high Reynolds numbers, a set of experiments has been conducted at the US Navy's William B. Morgan Large Cavitation Channel (LCC). Drag reduction was achieved by injecting gas (air) from a line source through the wall of a nearly zero-pressure-gradient TBL that formed on a flat-plate test model that was either hydraulically smooth or fully rough. Two distinct drag-reduction phenomena were investigated; bubble drag reduction (BDR) and air-layer drag reduction (ALDR). The streamwise distribution of skin-friction drag reduction was monitored with six skin-friction balances at downstream-distance-based Reynolds numbers to 220 million and at test speeds to 20.0 m s(-1). Near-wall bulk void fraction was measured at twelve streamwise locations with impedance probes, and near-wall (0 < Y < 5 mm) bubble populations were estimated with a bubble imaging system. The instrument suite was used to investigate the scaling of BDR and the requirements necessary to achieve ALDR. Results from the BDR experiments indicate that: significant drag reduction (>25%) is limited to the first few metres downstream of injection; marginal improvement was possible with a porous-plate versus an open-slot injector design; BDR has negligible sensitivity to surface tension; bubble size is independent of surface tension downstream of injection; BDR is insensitive to boundary-layer thickness at the injection location; and no synergetic effect is observed with compound injection. Using these data, previous BDR scaling methods are investigated, but data collapse is observed only with the 'initial zone' scaling, which provides little information on downstream persistence of BDR. ALDR was investigated with a series of experiments that included a slow increase in the volumetric flux of air injected at free-stream speeds to 15.3 m s(-1). These results indicated that there are three distinct regions associated with drag reduction with air injection: Region 1, BDR; Region 11, transition between BDR and ALDR; and Region 111, ALDR. In addition, once ALDR was established: friction drag reduction in excess of 80% was observed over the entire smooth model for speeds to 15.3 m s(-1); the critical volumetric flux of air required to achieve ALDR was observed to be approximately proportional to the square of the free-stream speed; slightly higher injection rates were required for ALDR if the surface tension was decreased; stable air layers were formed at free-stream speeds to 12.5 m s(-1) with the surface fully roughened (though approximately 50% greater volumetric air flux was required); and ALDR was sensitive to the inflow conditions. The sensitivity to the inflow conditions can be mitigated by employing a small faired step (10 mm height in the experiment) that helps to create a fixed separation line.
机译:为了研究大尺度和高雷诺数的湍流边界层(TBL)中皮肤摩擦阻力减小的现象,在美国海军的William B. Morgan大型气蚀通道(LCC)上进行了一组实验。通过从管线源通过接近零压力梯度的TBL壁注入气体(空气)来实现减阻作用,该TBL壁是在液压光滑或完全粗糙的平板测试模型上形成的。研究了两种不同的减阻现象:气泡减阻(BDR)和空气层减阻(ALDR)。用六个皮肤摩擦天平监测皮肤摩擦阻力减少的流向分布,这些天平基于下游距离的雷诺数为2.2亿,测试速度为20.0 m s(-1)。使用阻抗探针在十二个流向位置测量近壁体积空隙率,并使用气泡成像系统估算近壁(0 25%)仅限于注入下游的前几米;与多孔板喷射器设计相比,多孔板有可能获得少量改进; BDR对表面张力的敏感性可以忽略不计;气泡大小与注入下游的表面张力无关; BDR对注入位置的边界层厚度不敏感;并且没有观察到化合物注射的协同作用。使用这些数据,对以前的BDR缩放方法进行了研究,但是只有使用“初始区域”缩放才能观察到数据崩溃,这几乎无法提供有关BDR下游持久性的信息。通过一系列实验研究了ALDR,其中包括以自由流速度将空气的体积通量缓慢增加至15.3 m s(-1)。这些结果表明存在三个与通过空气喷射减少阻力相关的不同区域:区域1,BDR;区域1,BDR。 11区,BDR和ALDR之间的过渡;和ALDR 111区。此外,一旦建立了ALDR:在整个光滑模型上,观察到摩擦阻力降低了80%以上,速度达到15.3 m s(-1);观察到达到ALDR所需的空气临界体积通量大约与自由流速度的平方成正比;如果表面张力降低,则ALDR需要稍高的注射速率;在表面完全粗糙的情况下,以自由流速度至12.5 m s(-1)形成稳定的空气层(尽管需要约50%的体积空气通量); ALDR对流入条件敏感。可以通过采用有助于形成固定分隔线的小的整流罩台阶(实验中为10毫米高度)来减轻对流入条件的敏感度。

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