SlideShare a Scribd company logo
5
Most read
6
Most read
8
Most read
Subject 14: Survey design and procedure
Lecturer: Dr. Bakhtiar Q. Aziz
Objective: The student will learn how to make a complete scientific plan for a
resistivity survey in the field and how to select a suitable field design for a certain
problem. Two field procedures are explain to the students, profiling mode and
sounding mode.
Scientific contents
1- Vertical electrical sounding.

1- lateral profiling.

3- Profiling-sounding mode.

References

    1.   Applied and environmental geophysics, 1999, Sharma,V.,P.
    2.   Introduction to geophysical prospecting, 1988, Durbin, M. B.
    3.   www.Geophysics.net
    4.   www.hager-richter.com/resistivity.htm
    5.   www.geovision.com/PDF/M_Resistivity.pdf
Electrode Spread (Array type)
C1   P1          P2                        C2
6- Gradient Array                  a                                Surface




                                               P0
                         C1        P1                   P2          C2
                                          ½a ½a
7- Lee-partition Array         a                                a   Surface



                                     C2                    P2
                                                    a
                              C1 a                  P1 a
                                          a
8- Square Array
Advantages and Disadvantages of Wenner and Schlumberger Arrays
     The following table lists some of the strengths and weaknesses of
     Schlumberger and Wenner sounding methods.

                     Schlumberger                                                        Wenner
      Advantage                     Disadvantage                  Advantage                       Disadvantage
Need to move the two
potential electrodes only
for most readings. This                                                                All four electrodes, two current and
can          significantly                                                             two potential must be moved to
decrease      the    time                                                              acquire each reading.
required to acquire a
sounding.

                              Because      the    potential   Potential   electrode
                              electrode spacing is small      spacing increases as
                              compared to the current         current     electrode
                              electrode spacing, for large    spacing    increases.
                              current electrode spacings      Less         sensitive
                              very sensitive voltmeters are   voltmeters         are
                              required.                       required.

                                                                                       Because all electrodes are moved for
Because the potential
                                                                                       each reading, this method can be more
electrodes remain in
                                                                                       susceptible to near-surface, lateral,
fixed     location,    the
                                                                                       variations in resistivity. These near-
effects of near-surface
                                                                                       surface    lateral   variations     could
lateral    variations    in
                                                                                       potentially be misinterpreted in terms
resistivity are reduced.
                                                                                       of depth variations in resistivity.

                              In general, interpretations
                              based on DC soundings will                               In general, interpretations based on
                              be    limited to    simple,                              DC soundings will be limited to simple,
                              horizontally        layered                              horizontally layered structures.
                              structures.
Survey Design and Procedure
Survey design depends on the specific characteristics of the site and the objective of the
survey. The three most common modes of electrical resistivity surveying are profiling,
sounding, and profiling-sounding, each having its own specific purpose. If the purpose of
the survey is to map the depths and thickness of stratigraphic units, then the electrical
resistivity data should be collected in the sounding mode. Lateral electrical resistivity
contrasts, such as lithologic contacts, can best be mapped in the profiling mode. In
cases where the electrical resistivity is expected to vary both vertically and horizontally,
such as in contaminant plume mapping, the preferred mode is profile sounding.
1- Sounding Mode
As we've already shown, the resistivity method can detect variations in resistivity that
occur solely in depth. In fact, this method is most commonly applied to look for variations
in resistivity with depth. Surveys that are designed to determine resistivity variations with
depth above some fixed surface location are referred to as resistivity soundings. In these
experiments, electrode spacing is varied for each measurement. The center of the
electrode array, where the electrical potential is measured, however, remains fixed. An
example of a problem for which one might employ resistivity soundings is the
determination of the depth to water table
The two most common arrays for electrical resistivity surveying in the sounding mode
are the Schlumberger and Wenner arrays. Electrode geometry for both arrays is shown
in Figure below.
Increasing the separation of the outer current electrodes, thereby driving the currents
deeper into the subsurface increases the depth of exploration.
Wenner Sounding                              Schlumberger Sounding
                       VES-1                                                VES-1
a=1m                                    AB/2=1.5, MN/2=0.5

a=2m                                    AB/2=2, MN/2=0.5


a=3m                                    AB/2=3, MN/2=0.5


a=4m                                    AB/2=4, MN/2=0.5

a=5m                                    AB/2=5, MN/2=0.5

                                        AB/2=5, MN/2=1
             Data Table
                                                             Data Table
        a,m        R       ρa
                                                           AB/2         R       ρa
         1
                                                            1.5
         2
                                                             2
         3
                                                             3
         4
                                                             4
       ρa Field Curve                                 ρa         Field Curve




                                  a,m                                                AB/2
2- Profiling Mode
The two most common arrays for electrical resistivity surveying in the profiling mode are
the Wenner and dipole-dipole arrays. The electrode geometry for the Wenner array is
the same as the sounding mode — the difference is that in profiling mode the entire
array is moved laterally along the profile while maintaining the potential and current
electrode separation distances.

The electrode geometry for the dipole-dipole array is shown in Figure below. In the
profiling mode, the distance between the potential and current dipoles (a dipole consists
of a pair of like electrodes) is maintained while the array is moved along the profile.
As was mentioned on the previous page, the data collected from resistivity soundings is
usually interpretable only for horizontally stratified structures. If you are employing
resistivity methods to find vertical structures, one would typically use resistivity profiles
instead of resistivity soundings.
As described previously, resistivity profiles are resistivity surveys in which the electrode
spacing is fixed for all readings. Apparent resistivity is computed for different electrode
center points as the electrode spread is moved. Usually the center point is moved along
the line of the electrodes, although this does not have to be the case. Shown below is a
geological structure involving a vertical boundary between a higher resistivity material to
the left and a lower resistivity material to the right. Below the geological model is the
apparent resistivity you would observe using a Wenner array as the array is moved from
left to right. Note that the distance shown along the bottom of this plot is the distance
between the vertical fault and the current electrode farthest to the left of the array.
Profiling by Wenner array



                                                                a= 5 m
            1           2           3           4           5           6 Profile-1
    1           2           3           4           5           6 Profile-2
1       2           3           4           5           6
                                                            Profile-3


                            Data Table
                St.             R           ρa
                 1
                    2
                    3
                    4
             ρa Field Curve




                                                            St. (Distance ,m)
3- Profiling-Sounding Mode
As in the profiling mode, the Wenner and dipole-dipole arrays are the most common
arrays used in the profiling sounding mode. As the name implies, this mode is a
combination of the profiling and sounding modes.
In the Wenner array the typical field procedure is to collect the data in a succession of
profiles, each having a different electrode separation. The resulting data therefore
contains information about the lateral and vertical electrical resistivity variations.
                       (3)                            (2)                           (1)

More Related Content

PDF
Resistivity Survey
PPTX
Flood Management
PPTX
Role of Seismic Attributes in Petroleum Exploration_30May22.pptx
PPT
Resistivity method
PDF
Global Trend PPT week 1&2-converted.pdf
PPTX
Groundwater management strategy by Dr S K Jain, CGWB
PDF
Geophysics Labs
PPTX
Gravity and magmetic method
Resistivity Survey
Flood Management
Role of Seismic Attributes in Petroleum Exploration_30May22.pptx
Resistivity method
Global Trend PPT week 1&2-converted.pdf
Groundwater management strategy by Dr S K Jain, CGWB
Geophysics Labs
Gravity and magmetic method

What's hot (20)

PPTX
Reflecting method of seismic prospecting
PPT
Magnetic prospecting
PPTX
EM .method.pptx
PDF
Geophysics
PPTX
ELECTRICAL METHODS OF GEOPHYSICAL EXPLORATION OF MINERAL DEPOSITS.pptx
PDF
Induced Polarization (IP)
PPTX
Gravity Survey Method
PDF
Application of vertical electrical sounding and horizontal profiling methods ...
PPTX
Introduction to Seismic Method
PDF
Subsurface geophysical methods
PPTX
Geology of cambay basin
PPT
Biochemical anomolies
PPTX
Gravity anomaly across reagional structures
PPT
Ground Geophysical Survey
PPTX
Electrical method
PPTX
Radioactive Survey
PPTX
Introduction to diagenesis
PPTX
Geothermometry in economic geology
PPTX
SEISMIC METHOD
Reflecting method of seismic prospecting
Magnetic prospecting
EM .method.pptx
Geophysics
ELECTRICAL METHODS OF GEOPHYSICAL EXPLORATION OF MINERAL DEPOSITS.pptx
Induced Polarization (IP)
Gravity Survey Method
Application of vertical electrical sounding and horizontal profiling methods ...
Introduction to Seismic Method
Subsurface geophysical methods
Geology of cambay basin
Biochemical anomolies
Gravity anomaly across reagional structures
Ground Geophysical Survey
Electrical method
Radioactive Survey
Introduction to diagenesis
Geothermometry in economic geology
SEISMIC METHOD
Ad

Similar to Lecture 13-electrical method -field procedure (20)

PDF
ECE2708 Microwave Engineering Lab Joournal
PDF
LECT_Chap2_AntPar1.pdf
PDF
Optical fiber communication Part 1 Optical Fiber Fundamentals
PDF
N 5-antenna fandamentals-f13
PPTX
Electron spin resonance spectroscopy
PDF
DOCX
Mobile detection
DOCX
Electric field detector
PPTX
Basic Electronics
PPTX
.Electron diffraction for m.sc, student complete unit
PPT
Electro-optic modulators
PDF
Radar system components and system design
PDF
Electromagnetic Soundings Aa Kaufman And P Hoekstra Eds
PPTX
Electrodes and montages lectures for all
PPT
Grounding System Presentation for Engineering
PDF
MSc Experimental Research on FinFETs
PPT
transmission-lines
DOC
Lmece407
DOC
lmece407
PPTX
Drainage pattern means formation of surface and subsurface characteristic. If...
ECE2708 Microwave Engineering Lab Joournal
LECT_Chap2_AntPar1.pdf
Optical fiber communication Part 1 Optical Fiber Fundamentals
N 5-antenna fandamentals-f13
Electron spin resonance spectroscopy
Mobile detection
Electric field detector
Basic Electronics
.Electron diffraction for m.sc, student complete unit
Electro-optic modulators
Radar system components and system design
Electromagnetic Soundings Aa Kaufman And P Hoekstra Eds
Electrodes and montages lectures for all
Grounding System Presentation for Engineering
MSc Experimental Research on FinFETs
transmission-lines
Lmece407
lmece407
Drainage pattern means formation of surface and subsurface characteristic. If...
Ad

More from Kosygin Leishangthem (15)

PPTX
Steel structure vs rcc (concrete)
PDF
Utilizing drone in land development
PPTX
PDF
Pier n abutment
DOCX
Friction full
PPTX
DOCX
environmental
DOCX
What is the water cycle or hydrological cycle
PPTX
Lecture 2 kosygin
PPTX
Lecture 1 kosygin
PDF
CIVIL ENGINEERING
PDF
Guidelines for naac financial assistance final 28 02-2015
DOCX
STUDENT Handbook final zz
Steel structure vs rcc (concrete)
Utilizing drone in land development
Pier n abutment
Friction full
environmental
What is the water cycle or hydrological cycle
Lecture 2 kosygin
Lecture 1 kosygin
CIVIL ENGINEERING
Guidelines for naac financial assistance final 28 02-2015
STUDENT Handbook final zz

Lecture 13-electrical method -field procedure

  • 1. Subject 14: Survey design and procedure Lecturer: Dr. Bakhtiar Q. Aziz Objective: The student will learn how to make a complete scientific plan for a resistivity survey in the field and how to select a suitable field design for a certain problem. Two field procedures are explain to the students, profiling mode and sounding mode. Scientific contents 1- Vertical electrical sounding. 1- lateral profiling. 3- Profiling-sounding mode. References 1. Applied and environmental geophysics, 1999, Sharma,V.,P. 2. Introduction to geophysical prospecting, 1988, Durbin, M. B. 3. www.Geophysics.net 4. www.hager-richter.com/resistivity.htm 5. www.geovision.com/PDF/M_Resistivity.pdf
  • 3. C1 P1 P2 C2 6- Gradient Array a Surface P0 C1 P1 P2 C2 ½a ½a 7- Lee-partition Array a a Surface C2 P2 a C1 a P1 a a 8- Square Array
  • 4. Advantages and Disadvantages of Wenner and Schlumberger Arrays The following table lists some of the strengths and weaknesses of Schlumberger and Wenner sounding methods. Schlumberger Wenner Advantage Disadvantage Advantage Disadvantage Need to move the two potential electrodes only for most readings. This All four electrodes, two current and can significantly two potential must be moved to decrease the time acquire each reading. required to acquire a sounding. Because the potential Potential electrode electrode spacing is small spacing increases as compared to the current current electrode electrode spacing, for large spacing increases. current electrode spacings Less sensitive very sensitive voltmeters are voltmeters are required. required. Because all electrodes are moved for Because the potential each reading, this method can be more electrodes remain in susceptible to near-surface, lateral, fixed location, the variations in resistivity. These near- effects of near-surface surface lateral variations could lateral variations in potentially be misinterpreted in terms resistivity are reduced. of depth variations in resistivity. In general, interpretations based on DC soundings will In general, interpretations based on be limited to simple, DC soundings will be limited to simple, horizontally layered horizontally layered structures. structures.
  • 5. Survey Design and Procedure Survey design depends on the specific characteristics of the site and the objective of the survey. The three most common modes of electrical resistivity surveying are profiling, sounding, and profiling-sounding, each having its own specific purpose. If the purpose of the survey is to map the depths and thickness of stratigraphic units, then the electrical resistivity data should be collected in the sounding mode. Lateral electrical resistivity contrasts, such as lithologic contacts, can best be mapped in the profiling mode. In cases where the electrical resistivity is expected to vary both vertically and horizontally, such as in contaminant plume mapping, the preferred mode is profile sounding. 1- Sounding Mode As we've already shown, the resistivity method can detect variations in resistivity that occur solely in depth. In fact, this method is most commonly applied to look for variations in resistivity with depth. Surveys that are designed to determine resistivity variations with depth above some fixed surface location are referred to as resistivity soundings. In these experiments, electrode spacing is varied for each measurement. The center of the electrode array, where the electrical potential is measured, however, remains fixed. An example of a problem for which one might employ resistivity soundings is the determination of the depth to water table The two most common arrays for electrical resistivity surveying in the sounding mode are the Schlumberger and Wenner arrays. Electrode geometry for both arrays is shown in Figure below. Increasing the separation of the outer current electrodes, thereby driving the currents deeper into the subsurface increases the depth of exploration.
  • 6. Wenner Sounding Schlumberger Sounding VES-1 VES-1 a=1m AB/2=1.5, MN/2=0.5 a=2m AB/2=2, MN/2=0.5 a=3m AB/2=3, MN/2=0.5 a=4m AB/2=4, MN/2=0.5 a=5m AB/2=5, MN/2=0.5 AB/2=5, MN/2=1 Data Table Data Table a,m R ρa AB/2 R ρa 1 1.5 2 2 3 3 4 4 ρa Field Curve ρa Field Curve a,m AB/2
  • 7. 2- Profiling Mode The two most common arrays for electrical resistivity surveying in the profiling mode are the Wenner and dipole-dipole arrays. The electrode geometry for the Wenner array is the same as the sounding mode — the difference is that in profiling mode the entire array is moved laterally along the profile while maintaining the potential and current electrode separation distances. The electrode geometry for the dipole-dipole array is shown in Figure below. In the profiling mode, the distance between the potential and current dipoles (a dipole consists of a pair of like electrodes) is maintained while the array is moved along the profile. As was mentioned on the previous page, the data collected from resistivity soundings is usually interpretable only for horizontally stratified structures. If you are employing resistivity methods to find vertical structures, one would typically use resistivity profiles instead of resistivity soundings. As described previously, resistivity profiles are resistivity surveys in which the electrode spacing is fixed for all readings. Apparent resistivity is computed for different electrode center points as the electrode spread is moved. Usually the center point is moved along the line of the electrodes, although this does not have to be the case. Shown below is a geological structure involving a vertical boundary between a higher resistivity material to the left and a lower resistivity material to the right. Below the geological model is the apparent resistivity you would observe using a Wenner array as the array is moved from left to right. Note that the distance shown along the bottom of this plot is the distance between the vertical fault and the current electrode farthest to the left of the array.
  • 8. Profiling by Wenner array a= 5 m 1 2 3 4 5 6 Profile-1 1 2 3 4 5 6 Profile-2 1 2 3 4 5 6 Profile-3 Data Table St. R ρa 1 2 3 4 ρa Field Curve St. (Distance ,m)
  • 9. 3- Profiling-Sounding Mode As in the profiling mode, the Wenner and dipole-dipole arrays are the most common arrays used in the profiling sounding mode. As the name implies, this mode is a combination of the profiling and sounding modes. In the Wenner array the typical field procedure is to collect the data in a succession of profiles, each having a different electrode separation. The resulting data therefore contains information about the lateral and vertical electrical resistivity variations. (3) (2) (1)