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【WGMD-4】Application of geological disaster landslide investigation
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Description
Ⅰ.Introduction
Geophysical exploration using two Dimensional (2D) electrical resistivity tomography (ERT) survey plays a significant role in determining the subsurface resistivity distribution by making measurements on the ground surface. From these measurements, apparent resistivities are recorded during the fieldwork, which are later converted to true resistivity using appropriate computer software. These true resistivities are then converted to subsurface geological condition. The 2D electrical resistivity profiling is capable of detecting boundaries between unconsolidated materials (overburden), rocks, identifying weathered rock from fresh rock and contact between rocks of different lithology.
The Kerunga landslide site is located about 14.3 km NW form Kawasoti, 24 km along gravel and earthen road connecting Mahindra highway from Daldale. The landslide located at Hupsekot V.D.C, ward -5, Kerungatol of Nawalparasi district. The location of project sites are shown in Figure.
Ⅱ.Objective of study
The main objective of the proposed study consists of mapping vertical as well as horizontal variations of electrical resistivity to enable detection of the boundaries between unconsolidated materials and rocks of the different resistivity. The objectives of the survey are as follows:
- Depth of various types of rock masses.
- Thickness of the overburdens colluvial /alluvial soil and river bed materials, if they are thick.
- Quality of the bedrocks occurring below the overburdens.
- Weak zones: Fractured zone, local fault zone, shears zones etc and propogation towards Ramche village.
- Ground water bearing formations etc.

Ⅲ.Investigation method
To fulfill these proposed objectives, this project uses Geotech’s WGMD-4 Distributed High-density Electrical Method System. Right flank of landslide areas was mapped by six 2D ERT profiles covering 1,400 m length. These ERT layout plan are shown in Figure 2. The field crew and ERT survey in operation are shown in Figure 3. The positions and lengths of the profiles were determined based on the geological and engineering geological condition of the present sites.
The depth of investigation depends on the length of the profile. To collect information from the depth of about 35 m, a full length of profile is required, which is 51 electrodes spacing times 5 m and is 250 m. If profile length is 200 m, there is length for only 41 electrodes instead of 51 electrodes. Such survey will give result from a depth of the order of 20-25m only. Hence to maintain depth of about 20-25 m from ground surface, survey was conducted using appropriate lengths of profile. The field work was started on 8th April 2018. The crew returned to Head Office Kathmandu on 16 April, 2018 after completing the data acquisition in the field. Total actual ERT coverage for sixteen profiles is 1,400 m. The details of 2D ERT coverage are tabulated in Table 1.

Ⅳ.Interpretation of electrical resistivity tomography
Electrical resistivitiy of rocks
Electrical resistivity of the rocks or sediments depends on the resistivity of the rock mineral matrix and the fluid contained in its pore spaces. Rocks are composed primarily of quartz, feldspar and mica or other silicate minerals, which are poor conductors. They contain water in the pores, which is usually a better conductor. Thus the resistivity of, say, sandstone, generally depends on geometry of its pore spaces and the resistivity (or salinity) of its contained fluid. As permeability and porosity decrease, resistivity usually increases, when there is no change in formation fluid. The resistivity also depends upon the age of the rock or sediment as, with age, they become compacted and/or weathered. Compacted rocks show very high resistivity compared to unconsolidated sediments like clays, sands, gravels and so on as there will be less fluid in it. The weathered rock shows low resistivity when there is presence of water in it. Dry rocks or sediments have very high resistivity (of the order of 10,000 to 100,000 Ohm-m), whereas water bearing rocks or saturated sediments become much less resistant (10 to 1,000 Ohm-m).
Resistivity tomography
The field data were filtered, processed and treated with the software, RES2DINV. The software inverts the field data and calculates the appropriate model in term of resistivity and provides output in the form of resistivity contours. This inversion data is used to draw up the lithological and geological information. The basic principle behind the relation between resistivity data and lithology/geology are already dealt with in above sections. In the conversion from resistivity data to lithology following table (Table 3) has been used. This correlation table has been prepared based on the local geological information and experience with similar works in other parts of the country. However, it should be noted that the resistivity of certain lithology has wide variation and the following table (Table 3) is just an approximation. These inversion results showing resistivity model of all six profiles are presented in Figure 6 to 11 and are attached. The sections are prepared as per topographic undulations, as the electrodes are fixed at each 5 m slope distance (not horizontal distance or plan distance). Hence though it looks more distance in section, they actually are shorter in plan. The maximum and minimum thickness of overburden in each profile is tabulated in Table 4.

ERT InterPretations
Altogether six ERT profiles were surveyed at right flank of Kerunga Landslide. These ERT profiles are shown in Figure 6 to Figure 11 in the following section. The 2D ERT results are discussed below for each profile.
Lithological section of ERT 1
This profile located at right flank of Kerunga landslide parallel to slide axis. ERT1 profile crosses ERT 2 profile at obtuse angle at chainage of 80 m and total run of this profile is 200 m have thickness of 37 m. The 2D ERT result and lithology are shown in Figure 6.
There is low resistivity contours which covers top part of the entire profile length, indicates presence of moist and saturated residual soil with fragments of shale, which may be due to presence of subsurface water channel and stream at chainage 145 m. The thickness of this saturated overburden layer ranges from 15 m to 37 m throughout the profile. The under laying second layer from chainage of 45 m to 200 m with medium resistivity value denotes presence of weathered shale and quartzite. Thickness of this layer ranges from 3 m to 18 m.
The existence of very high resistivity value from chainage 80 m to 180 m indicates presence of quartzite bed at the bottom part of the profile. Thickness of this profile ranges from 2 m to 18 m.
Lithological section of ERT 2
This profile located at right flank of Kerunga landslide perpendicular to slide axis. ERT2 profile crosses ERT 1 profile at acute angle at chainage of 120 m and total run of this profile is 250 m have thickness of 37 m. The 2D ERT result and lithology are shown in Figure 7.
There is low to medium resistivity contours at the top part of the profile indicates presence of water saturated to moist residual soil with fragments of shale from chainage 30 m to 250 m, thickness of this layer ranges from 1 m to 37 m. Low resistivity counters from chainage 10 m to 155 m underneath top layer indicates water saturated zone or subsurface water channel with thickness 20 m to 37 m. There is presence of stream at change 25 m chainage may have contributed.
Lithological section of ERT 3
This profile located at right flank of Kerunga landslide perpendicular to slide axis. ERT4 profile crosses ERT 3 profile at chainage of 85 m and total run of this profile is 200 m have thickness of 37 m. The 2D ERT result and lithology are shown in Figure 8.
There is low to medium resistivity contours which entirely covers profile run at the top part, indicates presence of water saturated to dry residual soil with fragments of shale and quartzite. Very low resistivity patches of resistivity value at chainages 0 m to 80 m and 160 to 200 m indicates water saturated zone as observed in field. Low resistivity patch at chaingae 85 m to 110 m indicates subsurface water channel which may have disintegrated surrounding bedrock. The thickness of this overburden layer ranges from 12 m to 37 m. The under laying second layer from chainage 0 m to 80 m and 90 m to 180 m with medium resistivity value denotes presence of weathered shale and quartzite, which envelopes fresh bedrock. Thickness of this layer ranges from 2 m to 10 m.
The third layer is marked by high resistivity contours form chainage 0 m to 75 m and 105 m to 150 m, suggests presence of hard, fresh quartzite and shale. Thickness of this layer ranges from 25 m to 23 m.
Lithological section of ERT 4
This profile located at right flank of Kerunga landslide parallel to slide axis. ERT3 profile crosses ERT4 profile at chainage of 120 m and total run of this profile is 250 m with thickness of 37 m. The 2D ERT result and lithology are shown in Figure 9.
There is low resistivity contours which covers profile length, indicating presence of moist and saturated to moist residual soil with fragments of shale. Bedrock may have been totally disintegrated in to soil with fragments of shale and quartzite as observed in field.
Lithological section of ERT 5
This profile located at right flank of Kerunga landslide perpendicular to slide axis. ERT6 profile crosses ERT5 profile at chainage of 80 m and total run of this profile is 250 m with thickness 37 m. The 2D ERT result and lithology are shown in Figure 10.
There is very low resistivity contours which covers top part of the entire profile length, indicates presence of saturated residual soil with fragments of shale from chainage 0 m to 70 m of profile length, which may be due to presence of nearby stream (Figure 2). Presence of moist residual soil from chainage 70 m to 250 m is demarked by low resistivity contour. The thickness of top overburden layer ranges from 8 m to 20 m throughout the profile. The under laying second layer with medium resistivity value denotes presence of weathered shale and quartzite throughout the profile. Thickness of this layer ranges from 17 m to 25 m.
Lithological section of ERT 6
This profile located at right flank of Kerunga landslide parallel to slide axis. ERT5 profile crosses ERT 6 profile at chainage of 60 m and total run of this profile is 250 m with thickness of 37 m. The 2D ERT result and lithology are shown in Figure 11.
There is low resistivity contours which covers top part of the entire profile length, indicates presence of moist and saturated residual soil with fragments of shale. The thickness of this top overburden layer ranges from 15 m to 37 m throughout the profile. The under laying second layer from cahinage of 0 m to 155 m and 160 m to 250 m with medium resistivity value denotes presence of weathered shale and quartzite. Thickness of this layer ranges from 18 m to 22 m.







Ⅴ.In conclusion
In total, 6 ERT profiles were surveyed at right flank of Kerunga landslide covering 1400 m. Thick to thin layer of residual soil with fragments of shale and quartzite blanketed over survey length. Moist to saturated overburden with subsurface stream channel is frequently observed in ERT profiles. The thickness of these overburden vary from few meters to 37 m. Rock is found to be very weak class and deeply weathered due to presence of water and low strength. The main conclusions are listed below:
(1)Rock and soil at left flank of Landslide found to be weak and disintegrated up to residual soil.
(2) Most of the surveyed area rarely consist of fresh rock up to ~ 40 m depth, covered by weathered zone.
(3)Water from surface and subsurface channel found to be main cause of disintegration of rock mass. Which may be the main cause of landslide propagation.
(4)ERT1 and ERT2 profiles shows that presence of subsurface water saturated zone and subsurface water channel.
(5) ERT3 profile shows gradual disintegration of bedrock due to water channel.
(6)ERT4 profile made up of totally weathered rock in-situ.
(7)The rock at the top part of landslide found to be totally weathered as indicated by ERT5 and ERT6.
These conclusions are obtained from indirect method and should be correlated with drilling results to arrive at the overall geological conclusions.
Further reading | Technical solutions related to this article
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FAQ
The double tap has a large current and can be used for IP testing to get more accurate data.
High-density apparent resistivity method is an array prospecting method, also known as automatic apparent resistivity system, which is developed from direct current method. Its function is equivalent to the combination of quadrupole sounding and electrical profiling method. The artificial electric field is formed by supplying electricity to the underground through electrodes. The distribution of the electric field is closely related to the distribution of the resistivity of the underground rock and soil medium. By measuring the artificial electric field at different parts of the surface, the distribution of the apparent resistivity of the underground medium is understood, and the underground geological structure is inferred and interpreted based on the distribution of the apparent resistivity of the rock and soil medium.
The principle of high-density electrical method is the same as that of traditional resistivity method. It is a combination method of multiple devices and multiple pole distances that integrates electrical depth sounding and electrical profiling method, which can obtain the conductivity characteristics of two-dimensional underground media. It has the characteristics of multi-device data acquisition in one pole arrangement, and highlighting abnormal information by obtaining ratio parameters, which greatly increases the amount of collected data, improves work efficiency, and ensures the accuracy and reliability of the pole running process.
This method is particularly sensitive to the water content of the surrounding rock. If the surrounding rock is broken and contains water, its apparent resistivity is significantly reduced. The apparent resistivity of intact and hard rock and soil is significantly higher than that of the surrounding rock in the fault zone or broken zone and water-rich zone. This method has a clear principle and intuitive images. It is a geophysical method with high resolution. In recent years, with the improvement of computer data acquisition technology, the exploration efficiency has been greatly improved, the coverage area and detection depth of the profile have been increased, reliable data can be obtained in a strong interference environment, the signal-to-noise ratio has been greatly improved, and the geological body can be accurately detected. This method has been widely and successfully applied in engineering and hydrogeological exploration and exploration of mineral and water resources.
(1) Application in coalfield and mine goaf detection
(2) Non-destructive detection of termite nests in dam foundations
(3) Karst and foundation surveys of railways, roads and tunnels
(4) Delineation of stratum lithology boundaries
(5) Survey of the leakage range of landfills
(6) Ancient tomb surveys
(7) Detection of sewage pipes
(8) Non-destructive testing of leakage in reservoirs and river dams
(9) Detection of bedrock fracture zones
(10) Soil salinity and water quality surveys
(11) Detection of ancient tunnels, air-raid shelters, metal burial sites, etc.
(1)The high-density resistivity method is based on the resistivity method, so it is suitable for all underground explorations with obvious conductivity differences;
(2)Any medium underground will have a weak polarization potential at the moment of power on and off, which will affect our measurement of the true potential difference. When the electrode distance is small, the loop current is large, which has little effect on the measurement results; when the electrode distance is too large, the interference potential is close to the effective potential, which has a greater impact on the measurement results. Therefore, due to the influence of the power supply electrode distance, the exploration depth cannot be too large, generally within 100m. When the conductivity of the soil medium is good, it can be appropriately increased, and the exploration depth in the soil medium with poor conductivity is appropriately smaller;
(3)It is generally less used in cities, near large transmission lines, etc. due to site restrictions and industrial stray current interference; 4. In areas such as concrete pavements and exposed bedrock surfaces, it is also less used due to the difficulty of electrode layout.
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