Nachtigall W, Hanauer-Thieser U
Arbeitsgruppe Nachtigall, Zoologisches Institut, Universität des Saarlandes, FRG.
J Comp Physiol B. 1992;162(3):267-77. doi: 10.1007/BF00357534.
Drag forces and lift forces acting on honeybee trunks were measured by using specially built sensitive mechanical balances. Measurements were made on prepared bodies in 'good' and in 'bad' flight position, with and without legs, at velocities between 0.5 and 5 m.s-1 (Reynolds numbers between 4.10(2) and 4.10(3)) and at angles of attack between -20 degrees and +20 degrees. From the forces drag coefficients and lift coefficients were calculated. The drag coefficient measured with a zero angle of attack was 0.45 at 3 less than or equal to v less than or equal to 5 m.s-1, 0.6 at 2 m.s-1, 0.9 at 1 m.s-1 and 1.35 at 0.5 m.s-1, thus demonstrating a pronounced effect of Reynolds number on drag. These values are about 2 times lower (better) than those of a "drag disc" with the same diameter and attacked at the same velocity. The drag coefficient (related to constant minimal frontal area) was minimal at zero angle of attack, rising symmetrically to larger (+) and smaller (-) angles of attack in a non-linear fashion. The absolute value is higher and the rise is steeper at lower speeds or Reynolds numbers, but the incremental factors are independent of Reynolds number. For example, the drag coefficient is 1.44 +/- 0.05 times higher at an angle of attack of 20 degrees than at one of 0 degrees. On a double-logarithmic scale the slope of the drag versus Reynolds number plot was 1.5: with decreasing Reynolds number the relationship between drag and velocity changes from quadratic (Newton's law) to linear (viscous flow). Trunk drag was not systematically increased by the legs at any velocity or Reynolds number or any angle of attack. The legs appear to shape the trunk "aerodynamically", to form a relatively low-drag trunk-leg system. The body is able to generate dynamic lift. Highly significant positive linear correlations between lift coefficient and angle of attack were determined for the trunk-leg system in the typical flight position. Lift coefficient was +0.05 at zero angle of attack (possibly attained during very fast flight), +0.1 at 5 degrees (attained during fast flight), +0.25 at +20 degrees (attained during slow flight) and +0.55 at 45 degrees (attained whilst changing over to hovering). Average slope delta cL/delta alpha was 0.66 +/- 0.07, and average profile efficiency was 0.10. Non-wing lift contribution due to body form and banking only accounts for a few percent of body weight during fast flight.(ABSTRACT TRUNCATED AT 400 WORDS)
通过使用专门制造的灵敏机械天平来测量作用在蜜蜂躯干上的阻力和升力。在“良好”和“不佳”飞行姿态下,对有腿和无腿的准备好的躯体进行测量,速度范围为0.5至5米/秒(雷诺数在4×10²至4×10³之间),攻角范围为-20度至+20度。根据这些力计算出阻力系数和升力系数。在攻角为零时测量的阻力系数,在3≤v≤5米/秒时为0.45,在2米/秒时为0.6,在1米/秒时为0.9,在0.5米/秒时为1.35,这表明雷诺数对阻力有显著影响。这些值比相同直径且以相同速度攻击的“阻力圆盘”的值低约2倍(更好)。阻力系数(与恒定的最小正面面积相关)在零攻角时最小,以非线性方式对称地向更大(+)和更小(-)攻角增加。在较低速度或雷诺数时绝对值更高且增加更陡,但增加因子与雷诺数无关。例如,在攻角为20度时的阻力系数比在0度时高1.44±0.05倍。在双对数尺度上,阻力与雷诺数关系图的斜率为1.5:随着雷诺数减小,阻力与速度的关系从二次方(牛顿定律)变为线性(粘性流)。在任何速度、雷诺数或攻角下,腿部都不会系统性地增加躯干阻力。腿部似乎在“空气动力学上”塑造了躯干,形成了一个相对低阻力的躯干-腿部系统。躯体能够产生动态升力。对于处于典型飞行姿态的躯干-腿部系统,确定了升力系数与攻角之间高度显著的正线性相关性。攻角为零时升力系数为+0.05(可能在非常快速飞行时达到),5度时为+0.1(快速飞行时达到),+20度时为+0.25(慢速飞行时达到),45度时为+0.55(转换为悬停时达到)。平均斜率ΔcL/Δα为0.66±0.07,平均剖面效率为0.10。在快速飞行期间,由于身体形状和倾斜产生的非翼升力贡献仅占体重的百分之几。