三维复电阻率电磁场正演研究

将Cole—Cole模型表示的地下异常体各剖分单元复电阻率,引入到体积分方程求解均匀大地三维电磁场计算中,实现电偶源地面激发、接收复电阻率三维电磁场正演模拟。     

求地下极化体真柯尔-柯尔参数的研究

对求地下极化体真柯尔-柯尔参数的方法进行了研究。研究表明:诺模图校正法只在已知大地的电阻率分布并且极化体的电阻率与围岩接近时才可以使用;在大地电阻率分布未知的情况下,用反演单个测点视谱的方法不可能求得极化体的真柯尔-柯尔参数;对一些简单的大地模型可以用联合反演2个或多个测点视谱的方法求极化体的真柯尔-柯尔参数;先求大地模型的电阻率分布,再对单个测点的视谱进行反演也可能是1种求真柯尔-柯尔参数的合适的方法。     

Current and voltage source induced polarization transients: a comparative consideration

The article discusses the excitation of transient induced polarization responses using current and voltage sources. The first method has found a wide application in induced polarization surveys and—directly or indirectly—in the theory of the induced polarization method. Typically, rectangular current pulses are injected into the earth via grounding electrodes, and decaying induced polarization voltage is measured during the pauses between pulses. In this case, only the secondary field is recorded in the absence of the primary field, which is an important advantage of this method. On the other hand, since the current injected into the ground is fully controlled by the source, this method does not allow studying induced polarization by measuring the current in the transmitter line or associated magnetic field. When energising the earth with voltage pulses, the measured quantity is the transient induced polarization current. In principle, this method allows induced polarization studies to be done by recording the transmitter line current, the associated magnetic field, or its rate of change. The decay of current in a grounded transmitter line depends not only on the induced polarization of the earth but also on the polarization of the grounding electrodes. This problem does not occur when induced polarization transients in the earth are excited inductively. A grounded transmitter line is a mixed‐type source; hence, for a purely inductive excitation of induced polarization transients, one should use an ungrounded loop, which is coupled to the earth solely by electromagnetic induction.