Maurel Agnès, Pagneux Vincent, Barra Felipe, Lund Fernando
Laboratoire Ondes et Acoustique, UMR CNRS 7587, Ecole Supérieure de Physique et de Chimie Industrielles, 10 rue Vauquelin, 75005 Paris, France. agnes.maurel@ espci.fr
J Acoust Soc Am. 2007 Jun;121(6):3418-31. doi: 10.1121/1.2734488.
The attenuation of ultrasound in polycrystalline materials is modeled with grain boundaries considered as arrays of dislocation segments, a model valid for low angle mismatches. The polycrystal is thus studied as a continuous medium containing many dislocation "walls" of finite size randomly placed and oriented. Wave attenuation is blamed on the scattering by such objects, an effect that is studied using a multiple scattering formalism. This scattering also renormalizes the speed of sound, an effect that is also calculated. At low frequencies, meaning wavelengths that are long compared to grain boundary size, then attenuation is found to scale with frequency following a law that is a linear combination of quadratic and quartic terms, in agreement with the results of recent experiments performed in copper [Zhang et al., J. Acoust. Soc. Am. 116(1), 109-116 (2004)]. The prefactor of the quartic term can be obtained with reasonable values for the material under study, without adjustable parameters. The prefactor of the quadratic term can be fit assuming that the drag on the dynamics of the dislocations making up the wall is one to two orders of magnitude smaller than the value usually accepted for isolated dislocations. The quartic contribution is compared with the effect of the changes in the elastic constants from grain to grain that is usually considered as the source of attenuation in polycrystals. A complete model should include this scattering as well.
在多晶材料中,超声衰减的建模是将晶界视为位错段阵列,该模型适用于小角度失配情况。因此,多晶体被当作一种连续介质来研究,其中包含许多随机分布和取向的有限尺寸位错“壁”。波的衰减归因于这些物体的散射,这一效应通过多重散射形式理论进行研究。这种散射还会使声速重整化,这一效应也会被计算出来。在低频情况下,即波长与晶界尺寸相比很长时,发现衰减与频率的关系遵循一个定律,该定律是二次项和四次项的线性组合,这与最近在铜中进行的实验结果一致[Zhang等人,《美国声学学会杂志》116(1),109 - 116(2004)]。在不使用可调参数的情况下,对于所研究的材料,可以得到四次项的前置因子的合理值。假设构成壁的位错动力学上的阻力比孤立位错通常接受的值小一到两个数量级,就可以拟合出二次项的前置因子。将四次项贡献与通常被认为是多晶体中衰减来源的晶粒间弹性常数变化的效应进行了比较。一个完整的模型也应该包括这种散射。