EGU24-15344, updated on 09 Mar 2024
https://doi.org/10.5194/egusphere-egu24-15344
EGU General Assembly 2024
© Author(s) 2024. This work is distributed under
the Creative Commons Attribution 4.0 License.

Imaging the Electrical Resistivity Structure of a Locked Fault Segment: The Ganos Fault example

Bülent Tank1, Ruken Yazıcı2, Esra Doğukan3, Tunç Demir4, Gözde Taşseten4, Pınar Duran1, and Tannaz Assar3
Bülent Tank et al.
  • 1Bogazici University, Kandilli Observatory and E. R.I., Geophysics, Istanbul, Türkiye (bulent.tank@boun.edu.tr)
  • 2Bogazici University, Kandilli Obs. & E.R.I, Dept. of Earthquake Engineering, İstanbul, Türkiye (ruken.yazici@boun.edu.tr)
  • 3Istanbul Technical University, Faculty of Mines, Dept. Of Geophysical Engineering, İstanbul, Türkiye
  • 4Tekirdağ Metropolitan Municipality, Dept. Of Earthquake Risk Administration, Tekirdağ, Türkiye

The Ganos Fault, in the westernmost part of the North Anatolian Fault Zone (NAFZ), stayed quiet for approximately 146 years before two catastrophic events shook the area in the summer of 1912. The historical records point out that two devastating activities shook both sides of the Marmara Sea in 1766, too. Following the 1766 events, on August 9th, 1912, two blocks of the dextral Ganos Fault shifted one more time to create an Mw = 7.4 event near Mürefte in Tekirdağ. Nearly a month later, further to the west, the fault zone moved on September 13th, forcing another disastrous Mw= 6.8 earthquake. Almost 112 years have passed since then (leaving approximately 34 more years to complete the recurrence), and the Ganos Fault is again acting as a seismic gap. In brief, the Ganos Fault tends to generate another series of earthquakes in the region, and the fault zone characteristics of this locked segment are poorly known. In this study, magnetotellurics (MT) method is utilized to image the crustal electrical resistivity structure for deciphering the fault zone geometry. With this object in mind, simultaneous electric and magnetic observations were made at nearly 40 sites in two campaigns. For each observation point, the collected data were transferred to the frequency domain where the electromagnetic impedance tensor elements were calculated with robust processing algorithms (Birrp) for wideband frequencies. Following the dimensionality analyses performed with various tools such as Groom and Bailey decomposition, phase tensor analysis, etc., which eventually pointed out a geo-electric strike angle of nearly ~N60oE, numerical models based on two- and three-dimensional algorithms (such as MT2D and ModEM) were developed to image the fault zone properties of the Ganos Fault. Several numerical models were calculated to realize the influence of the coast-effect caused by the Marmara Sea. Pre-modeling analysis results and the final models suggest that (i) the geo-electric strike angle of ~N60oE agrees well with the earlier results, the geology and the fault’s geometry, (ii) the Ganos Fault acts as a geological boundary between the Eocene-aged Keşan Formation in the north and Miocene-aged Çengelli Formation in the south, (iii) while the Keşan Formation defines a continuous tubular highly resistive zone (~500- 800 Ωm) that may be acting as the seismogenic zone along the Ganos Fault, the Çengelli Formation appears to be less resistive in coherent with the ages of the formations highlighted earlier, (iv) the aforementioned resistive block reaches to a depth of nearly 15 - 18 km and this feature may mark the bottom of the seismogenic zone.          

How to cite: Tank, B., Yazıcı, R., Doğukan, E., Demir, T., Taşseten, G., Duran, P., and Assar, T.: Imaging the Electrical Resistivity Structure of a Locked Fault Segment: The Ganos Fault example, EGU General Assembly 2024, Vienna, Austria, 14–19 Apr 2024, EGU24-15344, https://doi.org/10.5194/egusphere-egu24-15344, 2024.