程久龙, 姜国庆, 李垚, 田楚霄, 孟上, 梁沛元. 钻孔瞬变电磁法扫描探测磁芯线圈激励电磁场响应特征[J]. 煤炭学报, 2023, 48(3): 1302-1310.
引用本文: 程久龙, 姜国庆, 李垚, 田楚霄, 孟上, 梁沛元. 钻孔瞬变电磁法扫描探测磁芯线圈激励电磁场响应特征[J]. 煤炭学报, 2023, 48(3): 1302-1310.
CHENG Jiulong, JIANG Guoqing, LI Yao, TIAN Chuxiao, MENG Shang, LIANG Peiyuan. Electromagnetic field response characteristics excited by magnetic core coil for borehole TEM with scanning detection[J]. Journal of China Coal Society, 2023, 48(3): 1302-1310.
Citation: CHENG Jiulong, JIANG Guoqing, LI Yao, TIAN Chuxiao, MENG Shang, LIANG Peiyuan. Electromagnetic field response characteristics excited by magnetic core coil for borehole TEM with scanning detection[J]. Journal of China Coal Society, 2023, 48(3): 1302-1310.

钻孔瞬变电磁法扫描探测磁芯线圈激励电磁场响应特征

Electromagnetic field response characteristics excited by magnetic core coil for borehole TEM with scanning detection

  • 摘要: 瞬变电磁测井一般采用超小线圈作为发射装置,由于激励产生的瞬变电磁场强度较低,仅能进行钻孔孔壁岩层探测,无法实现钻孔外围径向远距离探测及地质异常体精确定位。基于全空间瞬变电磁场相关理论,提出钻孔瞬变电磁法(BTEM)扫描探测方法,利用磁芯线圈激励电磁场,增强发射磁矩,提高钻孔瞬变电磁法的径向探测距离。同时,通过灵活调整线圈方向,对钻孔孔壁进行360°扫描,实现钻孔径向方向全方位探测,提高钻孔瞬变电磁法对含水地质体的空间分辨率和定位精度。建立钻孔全空间三维地质-地球物理模型,提出优化的网格剖分策略,采用特殊网格结构对钻孔中磁芯线圈进行网格加密及规范化,提高数值模拟精度。采用有限单元法分别计算均匀介质条件下钻孔瞬变电磁法磁芯激励电磁场响应以及含有低阻地质异常体时钻孔瞬变电磁法不同装置探测的瞬变电磁场响应,分析了共面偶极装置及共轴偶极装置以及不同几何参数对应的瞬变电磁场响应特征,采用全空间全区视电阻率计算及时深转换算法进行全空间电阻率成像。研究表明,在钻孔瞬变电磁法超小线圈中加入磁芯可以显著增强电磁场强度,并且增强的幅度与磁芯的直径和长度成正比,相比较而言,增大磁芯长度对电磁场响应的增强作用更为显著;钻孔全空间磁芯线圈激励时探测结果可以较好地反映钻孔径向外围岩层中低阻地质体引起的瞬变电磁场异常,共面偶极装置和共轴偶极装置均可以获得较为理想的探测效果,全空间电阻率成像结果分辨率较高,相比较而言,共面偶极装置得到的异常幅度更大,并且对异常体中心的定位更为准确,而共轴偶极装置对异常体整体形态和边界的刻画更为准确。

     

    Abstract: Ultra-small coil is generally used by transient electromagnetic logging as the transmitting device. Due to the low intensity of excited transient electromagnetic field, only the rock layer near the borehole wall can be detected, but the remote radial detection of the outer borehole and the accurate location of geological anomalies cannot be realized. Based on the theory of transient electromagnetic field in whole space, the scanning detection method for borehole transient electromagnetic method(BTEM)is proposed. The magnetic core coil is used to excite the electromagnetic field, enhance the transmitting magnetic moment, and improve the radial detection distance of BTEM. At the same time, by flexibly adjusting the direction of the coils, the borehole wall can be scanned at 360° to realize all-round detection in the borehole radial direction, the spatial resolution and positioning accuracy of BTEM for the water-bearing geological body can be improved. Three-dimensional geological-geophysical model of borehole whole space is established, optimized mesh generation strategy is proposed, and special grid structure is used to encrypt and standardize the magnetic core coil in the borehole to improve the accuracy of numerical simulation. Using the finite element method, the electromagnetic field response of BTEM excited by magnetic core coil is calculated under the condition of uniform medium, and then the transient electromagnetic field response of different devices for the model of low resistivity geological anomaly is also calculated. The response characteristics of transient electromagnetic field with coplanar dipole device and coaxial dipole device and with different geometric parameters are analyzed. The whole space all-time apparent resistivity calculation and time to depth conversion algorithm are used to image the resistivity in whole space. The research shows that the electromagnetic field strength can be significantly enhanced by adding a magnetic core to the ultra-small coil of BTEM,and the amplitude of the enhancement is proportional to the diameter and length of the magnetic core. In comparison, the enhancement of the electromagnetic field response is more significant by increasing the length of the magnetic core. The detection result of BTEM with magnetic core coil in whole space can better reflect the transient electromagnetic field anomaly caused by low resistivity geological body in the surrounding rock layer of the borehole radial direction. Both the coplanar dipole device and the coaxial dipole device can obtain ideal detection effect, and the resolution of resistivity imaging in whole space is high, In comparison, the anomaly amplitude obtained by the coplanar dipole device is larger, and the positioning of the center of anomaly body is more accurate, while the description of the overall shape and boundary of the anomaly body by the coaxial dipole device is more accurate.

     

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