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ST-01 26°09.4489′N49°59.4567′E 0 931 Minerals 2022, 12, 1236 ST-05 26°08.6684′N49°53.4044′E 3 ST-06 26°07.0260′N49°47.6663′E 44 ST-07 26°06.8866′N49°47.5993′E 44 10,700 6 of 21 20,584 20,736 ST-02 26°09.4057′N49°59.3446′E 0 1005 ST-03 26°09.3652′N49°59.2511′E 0 1092 ST-04 26°09.2756′N49°59.0329′E 0 1357 Figure 3. The study area and the configuration of the MT/CSEM receivers (red circles) and the trans- Figure 3. The study area and the configuration of the MT/CSEM receivers (red circles) and the mitter (Tx-green square) are shown. (A) The transmitter geometry/length and the location of the transmitter (Tx-green square) are shown. (A) The transmitter geometry/length and the location of receivers for the near surface MT/CSEM configuration are presented. (B) The configuration of each the receivers for the near surface MT/CSEM configuration are presented. (B) The configuration of receiver acquiring MT/CSEM (including FSEM) data is shown. (C) The broader study area with all each receiver acquiring MT/CSEM (including FSEM) data is shown. (C) The broader study area with the installed (near- and far- field) receivers (ST#) and the used transmitter (Tx) are depicted. all the installed (near- and far- field) receivers (ST#) and the used transmitter (Tx) are depicted. Before applying any task or starting any measurements at the installed stations, the Table 1 lists the receiver coordinates and their distances from the transmitter for both ground resistance—using a digital multimeter for both Ex (north–south electrical field) the near Tx sites (ST-01 to ST-04) and the far from Tx sites (ST-05 to ST-07). The locations and Ey (east–west electrical field)—on each receiver station is measured to ensure good were selected to test the transmitter and the signal behavior at different distances. Figure 3B (1–3 k ohm) contact resistance between electrodes. When the measured resistance was shows the receivers’ setup at each site. For MT, we used four electric field electrodes (Ex1, Ex2, Ey1, and Ey2) and three magnetic coils (Hx, Hy, and Hz). For the CSEM survey, two different layouts were applied. The LOTEM (long offset transient electromagnetic method) uses the standard CSEM layout, and the Focused-Source Electromagnetic (FSEM-4 electric fields) with the airloop, an S20 coil, which measures the vertical time-derivative of the magnetic field and a fifth electrode in the center of the array. The FSEM method was introduced by Davydycheva et al. [43] and was first followed by Davydycheva and Rykhlinski [13]. The goal of the FSEM method is to obtain deep resistivity data by focusing the EM field vertically and eliminating the horizontal component of electric current density. FSEM improves the conventional CSEM method, which has significantly higher spatial resolution and provides deeper resistivity data [16].PDF Image | First High-Power CSEM
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