首页> 外文会议>SPWLA Annual Logging Symposium >IDENTIFICATION OF MIXED ACOUSTIC MODES IN THE DIPOLE FULL WAVEFORM DATA USING INSTANTANEOUS FREQUENCY-SLOWNESS METHOD
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IDENTIFICATION OF MIXED ACOUSTIC MODES IN THE DIPOLE FULL WAVEFORM DATA USING INSTANTANEOUS FREQUENCY-SLOWNESS METHOD

机译:瞬时频率-慢度法识别双极全波形数据中的混合声模

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Dipole full waveform acoustic tools are used to estimate shear wave velocities, especially in soft and poorly consolidated formations. Under ideal conditions dipole source employed by those tools excites only borehole flexural wave that is propagating along fluidsolid interface This frequency dispersed flexural wave is used to estimate the velocity of the formation shear wave. In very soft formations, the dipole source may also excite a phase reversed compressional mode, sometimes referred to as a slow compressional wave (primarily due to its dispersed character). The above scenario is frequently complicated by the presence of other acoustic modes: e.g. Stoneley waves, tool mode flexural waves, and multiple flexural modes due to shear wave anisotropy. Stoneley waves are generated either due to the tool decentralization, borehole ovality, or due to the dipole source malfunction. Tool mode flexural waves are observed when acoustic isolator underperforms and frequently in highly deviated holes. The Stoneley wave is particularly difficult to identify and suppress during data processing. Like the flexural wave, it propagates along the fluid-solid interface, albeit with the velocity that is affected by formation shear wave slowness and borehole parameters. Very often both waves overlay each other in time and frequency domain (especially at near receiver levels) thus making it difficult to compute flexural wave slowness using conventional processing methods. Instantaneous Frequency-Slowness Method, derived from complex waveform analysis, is particularly well suited for processing contaminated dipole data sets. The absence of mixed acoustic modes in a dipole excitation creates unique signatures of instantaneous frequency and slowness curves that are characterized by non-linear increases of frequency and slowness as a function of travel time due to dispersive effects. On the other hand, the presence of multiple modes within a processing window modifies the instantaneous frequency and slowness curves in such a way that the presence of competing modes can be detected and under certain conditions identified. Therefore, by analyzing instantaneous frequency and slowness signatures, it is possible to avoid many processing errors resulting from the improper identification of acoustic modes, thus avoiding a mistake frequently made when processing these datasets with other methods. The Instantaneous Frequency-Slowness Method is presented and discussed. Corresponding examples of field data further validates proposed processing methodology.
机译:偶极全波形声学工具用于估计剪切波速度,尤其是在软弱和固结不良的地层中。在理想条件下,那些工具使用的偶极子源仅激发沿流固界面传播的井眼挠曲波。这种频率分散的挠曲波用于估算地层剪切波的速度。在非常软的地层中,偶极子源也可能激发一种反相的压缩模式,有时被称为慢压缩波(主要是由于其分散特性)。由于存在其他声音模式,上述情况通常会变得很复杂:斯通利波,工具模态弯曲波和剪切波各向异性导致的多种弯曲模态。斯通利波是由于工具分散,井孔椭圆度或偶极子源故障而产生的。当隔音器的性能不佳且经常出现在高度偏斜的孔中时,会观察到工具模式的弯曲波。斯通利波在数据处理期间尤其难以识别和抑制。像弯曲波一样,它沿流固界面传播,尽管其速度受地层剪切波慢度和井眼参数的影响。通常,两个波在时域和频域上会相互重叠(尤其是在接收器级别附近),因此很难使用常规处理方法来计算弯曲波的慢度。从复杂波形分析中得出的瞬时频率慢度方法特别适合处理受污染的偶极子数据集。偶极子激发中不存在混合声模,会产生瞬时频率和慢度曲线的独特特征,其特征是由于频散效应,频率和慢度随行进时间的非线性增加。另一方面,在处理窗口内多个模式的存在以这样的方式修改了瞬时频率和慢度曲线,使得可以检测到竞争模式的存在并在某些条件下进行识别。因此,通过分析瞬时频率和慢度签名,可以避免由于声学模式识别不当而导致的许多处理错误,从而避免了在用其他方法处理这些数据集时经常犯的错误。提出并讨论了瞬时频率慢度方法。现场数据的相应示例进一步验证了所提出的处理方法。

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