Kergomard J, Guillemain P, Silva F, Karkar S
Laboratoire de Mécanique et d'Acoustique (LMA, Research Unit of CNRS 7051) Aix-Marseille University, Centrale Marseille, F-13453 Marseille Cedex 13, France.
Laboratory of Electromagnetics and Acoustics, École Polytechnique Fédérale de Lausanne, Station 11 Route Cantonale, CH-1015 Lausanne, Switzerland.
J Acoust Soc Am. 2016 Feb;139(2):927-37. doi: 10.1121/1.4942185.
Two models for the generation of self-oscillations of reed conical woodwinds are presented. The models use the fewest parameters (of either the resonator or the exciter), whose influence can be quickly explored. The formulation extends iterated maps obtained for lossless cylindrical pipes without reed dynamics. It uses spherical wave variables in idealized resonators, with one parameter more than for cylinders: the missing length of the cone. The mouthpiece volume equals that of the missing part of the cone, and is implemented as either a cylindrical pipe (first model) or a lumped element (second model). Only the first model adds a length parameter for the mouthpiece and leads to the solving of an implicit equation. For the second model, any shape of nonlinear characteristic can be directly considered. The complex characteristic impedance for spherical waves requires sampling times smaller than a round trip in the resonator. The convergence of the two models is shown when the length of the cylindrical mouthpiece tends to zero. The waveform is in semi-quantitative agreement with experiment. It is concluded that the oscillations of the positive episode of the mouthpiece pressure are related to the length of the missing part, not to the reed dynamics.
本文提出了两种用于簧片圆锥木管乐器自激振荡产生的模型。这些模型使用了最少的参数(无论是共鸣器还是激励器的参数),其影响可以快速探究。该公式扩展了从没有簧片动力学的无损圆柱形管道获得的迭代映射。它在理想化的共鸣器中使用球面波变量,比圆柱形管道多一个参数:圆锥体的缺失长度。吹嘴的体积等于圆锥体缺失部分的体积,并被实现为圆柱形管道(第一个模型)或集总元件(第二个模型)。只有第一个模型为吹嘴添加了一个长度参数,并导致求解一个隐式方程。对于第二个模型,可以直接考虑任何形状的非线性特性。球面波的复特性阻抗要求采样时间小于在共鸣器中的往返时间。当圆柱形吹嘴的长度趋于零时,显示了两种模型的收敛性。波形与实验结果在半定量上一致。得出的结论是,吹嘴压力正相位的振荡与缺失部分的长度有关,而与簧片动力学无关。