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Ultrasonic contact pulse transmission for elastic wave velocity and stiffness determination: Influence of specimen geometry and porosity

机译:超声接触脉冲传输,用于确定弹性波的速度和刚度:试样几何形状和孔隙率的影响

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Elasticity determination by means of ultrasonic pulse transmission requires experimental realization of non-dispersive, i.e. frequency-independent, wave propagation, be it in form of bulk waves propagating in an (approximately) infinite medium, or of extensional waves propagating through a 1D bar system. While it is conceptually known that wavelengths need to tend towards zero (as compared to the specimen dimensions perpendicular to the pulse propagation direction) in the 3D case, and towards infinity in the 1D case, we here report on a new systematic experimental assessment of the influence of the sample geometry on wave type: tests on solid isotropic aluminum samples reveal that the extensional (or bar) wave propagation mode requires transmission of truly slender samples (required slendemess ratio of 20 or larger for wavelengths equal to the wave travel distance; this minimum slenderness ratio is increasing with increasing travel distance-over-wavelength ratio). After a transition zone with dispersive wave propagation, non-dispersive bulk waves are detected once the slenderness ratio is reduced to 5 or lower (at wavelengths equal to the wave travel distance; this maximum slenderness ratio is increasing with increasing travel distance-over-wavelength ratio). On the other hand, it is conceptually known from continuum mechanics that the wavelength needs to be larger than the investigated material volume or representative volume element (RVE), as to reveal the material's elastic properties, while corresponding quantitative data are rare. As a remedy, we here report on new experiments on transversely isotropic, porous aluminum samples, which reveal that minimum pore dimension-over-wavelength ratios of 1 and 10, respectively, relate to detection of normal and shear stiffnesses, respectively, of the solid material between the pores, while these ratios need to be smaller than 0.01 and 0.1, as to detect the normal and shear stiffnesses of the overall porous materials. The latter can be quantified through various homogeni-zation techniques.
机译:通过超声波脉冲传输来确定弹性需要实验性地实现非分散(即与频率无关)的波传播,无论是在(近似)无限大的介质中传播的体波形式,还是通过一维条形系统传播的扩展波形式。虽然从概念上讲,在3D情况下波长需要趋向于零(与垂直于脉冲传播方向的标本尺寸相比),在1D情况下趋向于无穷大,但我们在此报告了一种新的系统实验评估样品几何形状对波类型的影响:对固态各向同性铝样品的测试表明,扩展(或条形)波传播模式需要传输真正细长的样品(对于等于波传播距离的波长,要求的朗姆比为20或更大;最小纤细率随行进距离与波长之比的增加而增加)。在具有色散波传播的过渡区之后,一旦细长比减小到5或更低(在等于波传播距离的波长下,则检测到非色散体波);随着行波距离随波长的增加,最大细长比正在增加比)。另一方面,从连续力学上概念上知道,波长必须大于所研​​究的材料体积或代表体积元素(RVE),以显示材料的弹性,而相应的定量数据却很少。作为补救措施,我们在这里报告了关于横观各向同性的多孔铝样品的新实验,该实验表明,最小孔尺寸与波长之比分别为1和10与检测固体的法向刚度和剪切刚度有关。这些比率必须小于0.01和0.1,以检测整个多孔材料的法向刚度和剪切刚度。后者可以通过各种均质化技术进行量化。

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