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首页> 外文期刊>The Journal of Experimental Biology >WINGBEAT FREQUENCY AND THE BODY DRAG ANOMALY: WIND-TUNNEL OBSERVATIONS ON A THRUSH NIGHTINGALE (LUSCINIA LUSCtNfA) AND A TEAL (ANAS CRECCA)
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WINGBEAT FREQUENCY AND THE BODY DRAG ANOMALY: WIND-TUNNEL OBSERVATIONS ON A THRUSH NIGHTINGALE (LUSCINIA LUSCtNfA) AND A TEAL (ANAS CRECCA)

机译:温贝吉特频率和身体拖拉异常:在夜莺(LUSCINIA LUSCtNfA)和小鸭(ANAS CRECCA)上的风洞观测

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A teal (Anas crecca) and a thrush nightingale (Lusdnia luscinia) were trained to fly in the Lund wind tunnel for periods of up to 3 and 16 h respectively. Both birds flew in steady flapping flight, with such regularity that their wingbeat frequenciescould be determined by viewing them through a shutter stroboscope. When flying at a constant air speed, the teal's wingbeat frequency varied with the 0.364 power of the body mass and the thrush nightingale's varied with the 0.430 power. Both exponents differed from zero, but neither differed from the predicted value (0.5) at the 1 % level of significance. The teal continued to flap steadily as the tunnel tilt angle was varied from -1 ° (climb) to +6° (descent), while the wingbeat frequency declined progressively by about 11%. In both birds, the plot of wingbeat frequency against air speed in level flight was U-shaped, with small but statistically significant curvature. We identified the minima of these curves with the minimum power speed (V_(mp)) andfound that the values predicted for Vmp, using previously published default values for the required variables, were only about two-thirds of the observed minimum-frequency speeds. The discrepancy could be resolved If the body drag coefficients (C_(Db))of both birds were near 0.08, rather than near 0.40 as previously assumed. The previously published high values for hody drag coefficients were derived from wind-tunnel measurements on frozen bird bodies, from which the wings had been removed, and had long been regarded as anomalous, as values below 0.01 are given in the engineering literature for streamlined bodies. Ve suggest that birds of any size that have well-streamlined bodies can achieve minimum body drag coefficients uf around 0.05 if the feetcan be fully retracted under the flank feathers. In such birds, field observations of flight speeds may need to be reinterpreted in the light of higher estimates of V_(mp) Estimates of the effective lift:drag ratio and range can alsn be revised upwards.Birds that have large feet or trailing legs may have higher body drag .coefficients. The original estimates of aroand C_(Db)=0.4 could be correct for species, such as pelicans and large herons, that also have prominent heads. We see no evidence for anyprogressive reduction of body drag coefficient in the Reynolds number range covered by our experiments, that is 21 600--215 000 on the basis of body cross-sectional diameter.
机译:训练了小野鸭(Anas crecca)和画眉夜莺(Lusdnia luscinia)在隆德风洞中飞行的时间分别为3小时和16小时。两只鸟以稳定的拍动飞行,规律性可以通过百叶窗频闪仪观察它们的翅膀频率。当以恒定的风速飞行时,蓝绿色的翼拍频率随质量的0.364倍而变化,而画眉夜莺的变化随0.430倍而变化。两个指数均不为零,但均与1%显着性水平的预测值(0.5)相同。当通道倾斜角从-1°(爬升)到+6°(下降)变化时,蓝绿色继续稳定拍打,而机翼拍频率逐渐下降约11%。在两只鸟类中,水平飞行中机翼频率与风速的关系图呈U形,曲率较小,但在统计上显着。我们用最小功率速度(V_(mp))识别了这些曲线的最小值,并发现使用先前发布的所需变量的默认值为Vmp预测的值仅约为观察到的最小频率速度的三分之二。如果两只鸟的身体阻力系数(C_(Db))都接近0.08,而不是先前假设的0.40,则可以解决差异。先前发布的霍迪风阻系数的高值来自冷冻鸟体的风洞测量,该翼体已被移除,并且长期以来一直被认为是反常的,因为流线形体的工程文献中给出的值低于0.01 。 Ve建议,如果脚可以完全缩回侧面的羽毛下,则任何具有良好流线形体形的鸟都可以实现最小的体阻力系数uf,约为0.05。在此类鸟类中,可能需要根据更高的V_(mp)估计值重新解释对飞行速度的野外观察结果,即对有效升力:阻力比和范围的估计值也可以向上修改。具有更高的车身阻力系数。 aroand C_(Db)= 0.4的原始估计值对于诸如鹈鹕和大苍鹭等也具有突出头部的物种可能是正确的。我们没有证据表明在我们的实验覆盖的雷诺数范围内,即身体横截面直径为21600--215 000时,身体阻力系数有任何逐步降低的证据。

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