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Semblance response to a ground-penetrating radar wavelet and resulting errors in velocity analysis

机译:对探地雷达小波的相似响应以及速度分析中的误差

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The propagation velocity of a ground-penetrating radar (GPR) wavelet may be used to derive physical subsurface properties, including layer thickness, porosity and water content. We describe a systematic error in semblance analysis of GPR common-midpoint (CMP) data, arising from the response of the statistic to the waveform of the GPR pulse. Only the first-breaks of GPR wavelets express true velocities and traveltimes but these cannot deliver a semblance response since they have zero amplitude; instead, this response derives from subsequent wavelet half-cycles, delayed from the first-break. This delay causes semblance picks to express slower velocity and later traveltime with respect to true quantities, even for simple cases of reflectivity. For a two-layer synthetic CMP data set, in which the GPR source pulse via a 500 MHz Berlage wavelet, semblance picks underestimate interval velocities of 0.135 ms and 0.060 ms by 10.0% and 2.0%, respectively. Velocity biases are corrected using the coherence statistic to simulate first-break traveltimes from a set of velocity picks, in a process termed `backshifting'. A t 2–x2 linear regression of simulated first-breaks yields smaller errors in the same interval velocities of –2.2% and –1.0%. A first real-data example considers a reflection from the base of a 3.39 m thick air-gap. Semblance analysis estimates the air-wave velocity' as 0.289 ms (-3.6% error) and the air-gap thickness as 3.59 m (+6.1% error); backshifting yields equivalent estimates of 0.302 ms (+0.9% error) and 3.35 m (-1.2% error). In a second example, semblance- and backshifting-derived velocity models overestimate the thickness of clay-rich archaeological deposits by 19.0% and 3.1%, respectively. Backshifting is a simple modification to conventional practice and is recommended for any analysis where physical subsurface properties are to be derived from the output GPR velocity.
机译:探地雷达(GPR)小波的传播速度可用于得出物理地下属性,包括层厚度,孔隙率和水含量。我们描述了GPR共中点(CMP)数据的相似度分析中的系统误差,这是由于统计数据对GPR脉冲波形的响应引起的。只有GPR小波的第一个爆发才表示真实的速度和传播时间,但由于振幅为零,因此无法提供相似的响应。取而代之的是,该响应来自随后的小波半周期,该周期从第一个中断开始延迟。这种延迟会导致相似的镐在相对于真实量的情况下表现出较慢的速度和较慢的传播时间,即使对于简单的反射率情况也是如此。对于两层合成CMP数据集(其中GPR源脉冲通过500 MHz Berlage小波),相似度分别将低估的间隔速度0.135 m / ns和0.060 m / ns降低了10.0%和2.0%。使用相干统计量来校正速度偏差,以模拟来自一组速度拾取的首个破折行程时间,此过程称为“后移”。在相同的间隔速度(–2.2%和–1.0%)下,t 2–x2线性回归的模拟初值产生的误差较小。第一个真实数据示例考虑了3.39 m厚气隙底部的反射。相似性分析估计气波速度为0.289 m / ns(-3.6%误差),气隙厚度为3.59 m(+ 6.1%误差);回移产生的等效估计值为0.302 m / ns(+ 0.9%误差)和3.35 m(-1.2%误差)。在第二个示例中,由相似性和后移产生的速度模型分别高估了富含粘土的考古沉积物的厚度19.0%和3.1%。回移是对传统实践的简单修改,建议用于从输出GPR速度导出物理地下属性的任何分析中。

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