地震地质 ›› 2004, Vol. 26 ›› Issue (3): 484-491.

• 构造物理实验 • 上一篇    下一篇

周期性层状介质中超声波传播的实验研究

杨晓松, 马瑾, 刘力强   

  1. 中国地震局地质研究所, 地震动力学国家重点实验室, 北京, 100029
  • 收稿日期:2004-02-27 修回日期:2004-07-13 出版日期:2004-09-02 发布日期:2009-10-26
  • 作者简介:杨晓松,男,生于1959年,1999年在中国地质大学(武汉)获博士学位,研究员,主要从事实验岩石物理学、实验岩石学和构造地质学研究,E-mail:xsyang@ies.ac.cn.
  • 基金资助:
    地震科学联合基金(103057)、国家自然科学基金(40072063)、国家重点基础研究发展规划项目(1998040700)与中国博士后科学基金项目共同资助。中国地震局地质研究所论著200480045。

EXPERIMENTAL STUDY ON THE PROPAGATION OF ACOUSTIC WAVES THROUGH PERIODICALLY LAYERED MEDIA

YANG Xiao-song, MA Jin, LIU Li-qiang   

  1. State Key Laboratory of Earthquake Dynamics, Institute of Geology, China Earthquake Administration, Beijing 100029, China
  • Received:2004-02-27 Revised:2004-07-13 Online:2004-09-02 Published:2009-10-26

摘要: 实验研究了韵律层结构和超声波探测频率对弹性波波速和波形的影响。实验中所使用的超声波频率为240kHz,韵律层由不同厚度的钢板和有机玻璃板构成。研究表明,当λi/di<4(i=1,2)(λi为超声波在介质i中传播时的波长,di为韵律层中介质i的厚度)时,韵律层的波速近似等于2种介质的时间平均速度;当λi/di>5(i=1,2)时,其速度开始显著地降低,并趋向于有效介质波速的Reuss下限(VpR)。韵律层的结构对于透射波的波形有显著的影响。特别是当λi/di接近于6时,透射波波形非常简单,并且其透射波的振幅显著地降低。因此波形简单并不一定对应着简单的介质结构。由于弹性波在韵律层中的传播速度以及波形与探测频率有关,因此在利用地震测深结果分析岩石圈结构,推断其物质组成时应该充分考虑地震测深频率和地壳结构对分析结果的影响。

关键词: 周期性层状介质, 超声波地震实验, 长波近似, 地壳结构

Abstract: The propagation of acoustic waves through periodically layered media (PLM) is experimentally investigated for the purpose of determining how the velocities and waveforms depend on periodical structures and detection frequency. In our experiments the PLM were made of stacks of plastic and steel plates with different periodical spacing. The acoustic wave frequency used in our experiments was 240MHz. Velocities and waveforms were measured by Digitization Wave Meter with 12-bit resolution and 40MHz sampling rate. The results show that the velocity transition from the time averaged relation to the long-wave approximation (LWA) is related to the critical ratio of λi/di(i=1,2) (λi-the wavelength of wave going through medium i; di-the thickness of medium i in PLM) rather than to λ/d (the ratio of wavelength to the thickness of rhythmic layer). The LWA occurs when λi/di>5(i=1,2),and the velocities (V) approach to the Reuss bound (VR),whereas the time averaged velocities hold when λi/di<4(i=1,2). We attribute the behavior of V→VR to "softer shape" distribution of different rigid components in PLM. The waveforms are also frequency dependent. With larger thickness of rhythmic layer,the attenuation of the first arrival is low and the multiple waves reflected from interfaces can be observed. In the case of LWA,however,the transmitted waves tend to have relatively simple waveforms. This behavior implies that simple waveform does not always reflect simple medium structure through which the wave propagates. As λi/di~6 (i=1,2),the transmitted wave is obviously attenuated,and consequently it is equivalent to a shield layer for the wave. Therefore,the influences of medium structures on velocities and waveforms should be taken into account when interpreting deep structures and compositions based on seismic data. Tectonic nature of intracrustal low velocity zones is one of the hotly debated topics. An important implication of our experimental results is that PLM are potentially low velocity zones. If extremely reflective deep crust is caused by alternating layers,the relatively lower velocities observed in deep crust should probably be attributed to the rock properties that we wish to image,as well as to its structures,scales and detection frequencies.

Key words: periodically layered media, acoustic seismic experiments, long-wave approximation, effective medium velocity, time-averaged velocity

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