摘要
在准静态近似条件下,利用水平电偶源在均匀半空间表面激发电磁场的计算公式,讨论了可控源音频大地电磁法(CSAMT)水平电场y分量Ey的观测范围、特点和由其定义视电阻率的应用优势;Ey与常规标量CSAMT测量的Ex、Hy幅值范围不同,采集并利用Ey数据可以扩大CSAMT野外观测扇区,减少采集成本。依据电法及电磁法勘探中视电阻率定义的基本原则,提出了Ey视电阻率的定义,说明了其具备频率测深的意义;通过几种典型层状模型(均匀半空间,两层D、G,三层H、K以及四层KH、HK型)的数值计算,对比了Ey视电阻率和Ex、Hy、Zxy、Re(Zxy)等对应的波区视电阻率及Ex、Zxy等对应的全区视电阻率对地电断面电性特征的反映效果。结果表明:Ey视电阻率的求取仅需测点的坐标和一个方向的电场值,计算方便、不必迭代,并且在曲线低频端收敛于一稳定值,可以明显改善非波区的畸变效应。
Under the quasi-static conditions,the measurement sector,features and advantages of electric field y-direction（Ey） of controlled source audio-frequency magnetotelluric are discussed according to the formula of electromagnetic field data from horizontal electric dipole.The amplitude range of electric field y-direction is different from the common scalar CSAMT measurement.Ey component data can be gathered and uesed to expand the CSAMT field observation sector and reduce the acquisition costs.According to the basic principal for definition of apparent resistivity in electrical prospecting,a new apparent resistivity defined by Ey is put forward and the sounding significance by frequency of which is explained.Through numerical calculation of several typical layered models,such as homogeneous half-space,D,G,H,K,KH and HK typical models,Ey apparent resistivity is compared with wave-area apparent resistivities defined by Ex、Hy、Zxy、Re（Zxy） and full-wave apparent resistivities defined by Ex、Zxy.The results show that the derivation of Ey apparent resistivity only needs the coordinate of the sounding station and one direction E-field intensity and the iterative procedures are unnecessary.The new apparent resistivity easily calculated can satisfactorily eliminate the distortion effect of the near and transient area,because it can converge to a stable value at low frequency parts.
出处
《吉林大学学报（地球科学版）》
EI
CAS
CSCD
北大核心
2011年第2期552-558,共7页
Journal of Jilin University：Earth Science Edition
基金
国家公益性行业基金项目(SinoProbe-03)
关键词
电磁勘探
可控源音频大地电磁法
Ey视电阻率
波区视电阻率
全区视电阻率
electromagnetic prospecting； controlled source audio-frequency magnetotelluric； Ey apparent resistivity； far-field apparent resistivity； full-wave apparent resistivity；
