Baddoo P J, Ayton L J
Department of Applied Mathematics and Theoretical Physics, Wilberforce Road, Cambridge CB3 0WA, UK.
Proc Math Phys Eng Sci. 2018 Sep;474(2217):20180065. doi: 10.1098/rspa.2018.0065. Epub 2018 Sep 12.
The potential flow through an infinite cascade of aerofoils is considered as both a direct and inverse problem. In each case, a perturbation expansion about a background uniform flow is assumed where the size of the perturbation is comparable to the aspect ratio of the aerofoils. This perturbation must decay far upstream and also satisfy particular edge conditions, including the Kutta condition at each trailing edge. In the direct problem, the flow field through a cascade of aerofoils of known geometry is calculated. This is solved analytically by recasting the situation as a Riemann-Hilbert problem with only imaginary values prescribed on the chords. As the distance between aerofoils is taken to infinity, the solution is seen to converge to a known analytic expression for a single aerofoil. Analytic expressions for the surface velocity, lift and deflection angle are presented as functions of aerofoil geometry, angle of attack and stagger angle; these show good agreement with numerical results. In the inverse problem, the aerofoil geometry is calculated from a prescribed tangential surface velocity along the chords and upstream angle of attack. This is found via the solution of a singular integral equation prescribed on the chords of the aerofoils.
通过无限翼型叶栅的势流被视为一个正问题和一个反问题。在每种情况下,都假设围绕背景均匀流进行微扰展开,其中微扰的大小与翼型的展弦比相当。这种微扰必须在远上游衰减,并且还需满足特定的边界条件,包括每个后缘处的库塔条件。在正问题中,计算通过已知几何形状的叶栅的流场。通过将该情况重新表述为仅在弦上规定虚数值的黎曼 - 希尔伯特问题来解析求解。当叶栅中翼型之间的距离趋于无穷大时,解收敛到单个翼型的已知解析表达式。给出了表面速度、升力和偏转角的解析表达式,它们是翼型几何形状、攻角和 stagger 角的函数;这些结果与数值结果显示出良好的一致性。在反问题中,根据沿弦规定的切向表面速度和上游攻角来计算翼型几何形状。这是通过在翼型弦上规定的奇异积分方程的解来找到的。