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裴建国, 张新军. 基于瞬变电磁法发射线框通电时刻选取的研究[J]. 煤炭科学技术, 2021, 49(11): 169-173.
引用本文: 裴建国, 张新军. 基于瞬变电磁法发射线框通电时刻选取的研究[J]. 煤炭科学技术, 2021, 49(11): 169-173.
PEI Jianguo, ZHANG Xinjun. Study on electrifying time selection of transmit-loop for transient electromagnetic method[J]. COAL SCIENCE AND TECHNOLOGY, 2021, 49(11): 169-173.
Citation: PEI Jianguo, ZHANG Xinjun. Study on electrifying time selection of transmit-loop for transient electromagnetic method[J]. COAL SCIENCE AND TECHNOLOGY, 2021, 49(11): 169-173.

基于瞬变电磁法发射线框通电时刻选取的研究

Study on electrifying time selection of transmit-loop for transient electromagnetic method

  • 摘要: 对于瞬变电磁法,关心较多的是关断时间,通电时刻(建场时间)的重要性往往被忽略,常规采样方式是在设定足够观测时窗的采样频率下,赋予相同的激发建场时间,即对于正负极性观测时窗来说,正、负极性观测采样时窗和建场时间分别为固定的1/4周期。为研究并建立非对称式“发射-观测”时窗序列,以提高瞬变电磁法探测精度。 从瞬变电磁法激发场电信号的傅里叶变换入手,通过对不同建场时间下的电磁信号频率组分进行大量理论推导和计算,并进行统计分析,并且绘制了不同建场时间的频谱平剖图 ,得出了不同建场时间条件下信号频率组分(频谱)的变化规律。研究结果表明:建场时间越长信号频率组分中高频成分缺失越多,进而影响了浅层信息,以高频信号反演深度不超过盲区为宜;而建场时间越短信号频率组分中低频成分集中越多,有利于深部信号强度,当然受限于探测能力(极限探测深度),更短的建场时间也是不必的。然后又对该规律进行公式推导,得出了不同时刻建场电磁信号极大频率与时间的关联公式,进而得出了特定时刻的建场信号的频谱,最终提出了给瞬变电磁法设定若干非固定建场时间的设想,并将常规瞬变电磁法观测的合理建场时间范围锁定在发射线框通电后61.0 μs~12.7 ms ,更为合理地满足常规800 m以浅的瞬变电磁探测任务,进一步建立占空比由1∶1向1∶8过度的若干个非对称式“发射-观测”时窗序列,实现800 m以浅针对不同深度区的探测任务更为优化时窗序列。

     

    Abstract: As for transient electromagnetic method(TEM), turn-off time got so much concern that the importance of electrifying time (excited-field build-up time)for transmit-loop is always neglected. Normally,setting certain sampling frequency which has enough observation time window, same build-up time is set. This thesis has been studying about building asymmetry “transmitting-observing” time window array, for improving accuracy of TEM. As for positive or negative polar observation time window, observation time window or build-up time was a quarter of period. This thesis mainly proceeds with Fourier transform of electric signal, then frequency spectrum of different build-up time was calculated accurately. Influence of build-up time to frequency spectrum was concluded by theoretical derivation and numerical calculation. The results suggest that high frequency components lost much with build-up time getting more, then shallow information was influenced, inversion depth of high frequency signal should not be more than shallow layer shadow depth definitely. Meanwhile, low frequency components gather much with build-up time getting shorter. limited by detection depth, shorter build-up time was unnecessary. Eventually, by quantized calculation, reasonable build-up time interval was concluded, that is build-up time of TEM should be limited between 61.0 μs-12.7 ms, and asymmetric building-observation time window between 1∶1 from 1∶8 were built.Then, more appropriate time window was built for detecting different depth-no deeper than 800 m.

     

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