Geophysics ( Electric Method )

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    GEOELCTERICALMETHODS

    BY

    DR. ESSAM A. MORSY

    CAIRO UNIVERSITY

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    Geophysical Surveys:

    Can be divided

    into

    two classes

    Active

    Versus

    Passive

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    Passive geophysical surveys

    Involving measurementsofnaturally occurringfields or propertiesof the earth.

    The naturally occurringfields are the:

    gravitational field,

    magnetic field, and

    EM field.

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    Active geophysical Surveys.

    A signal is injected intothe earth and

    we then measure how

    the earth responds tothis signal.

    DC resistivity andseismic refraction.

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    Electrical Methods Overview

    The electrical

    and

    electromagnetic methodsrepresent

    the largest class

    of all geophysical methodsDue to the wide field applications.

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    INTRODUCTION

    Several authors pointed out thatgeoelectrical resistivity method can beused in:

    Searching for water bearing formations,Stratigraphic correlation in oil fields,

    Prospecting for conductive bodies,

    Determining the depths of high or lowconductive-anomalous layers,

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    Determining the depths andapproximate shape of resistivity-

    anomalous ore bodies,

    Civil engineering and environmental

    investigations,

    Cavity detection, and

    Identifying the depth of sand andgravel deposits.

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    What are the electricalProperties of rocks depend on:-

    The electrical properties of mostrocks in the upper part of the Earthscrust are dependent primarily upon

    The amount of water in the rock,

    The salinity of the water, and

    The distribution of the water in therock.

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    Saturatedrocks have lowerresistivities

    than unsaturated and dry rocks.The higher theporosityof thesaturated rock, the lower its

    resistivity, and

    the higher thesalinityof thesaturating fluids, the lower the

    resistivity.

    The presence ofclays andconductive minerals also reduces

    the resistivity of the rock.

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    Properties are of primary concern inthe application of electrical methods

    Two properties are of primary concernin the application of electricalmethods:

    1. The ability of rocks to conduct anelectric current, and

    2. The polarization which occurs when anelectrical current is passed throughthem (induced polarization).

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    The resistivity method is used in thestudy ofhorizontal and vertical

    discontinuities in the electricalproperties of the ground.

    It utilizes direct currents or low

    frequency alternating currents toinvestigate the electrical properties(resistivity) of the subsurface.

    A resistivity contrastbetween thetarget and the background geologymust exist.

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    Common applications ofresistivity surveying

    Groundwater exploration

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    Mineral exploration,

    detection of cavities

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    Oil exploration

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    Waste site exploration

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    Electrical methods employa variety of measurements

    within the Earth.

    DC Resistivity

    Induced Polarization (IP)Self Potential (SP)

    Electromagnetic (EM)

    Magnetotelluric (MT)

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    BASICSCurrent Flow and Ohm's Law

    In 1827, Georg Ohmdefined an empiricalrelationship between

    the current flowingthrough a wire and

    the voltage potentialrequired to drive that

    current.

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    It's Resistivity, NOT Resistance

    In the case of a wire,resistivity is definedas the resistance inthe wire, times the

    cross-sectional area

    of the wire, divided bythe length of the wire.The units associated

    with resistivity arethus, ohm - m

    (ohm-meters).

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    Resistivity is one of the most variablephysical properties.

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    There is

    a large range of resistivities,not only between varying

    rocks and minerals

    butalso

    within rocks of the same type.

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    ResistivityIs the reciprocal ofconductivity

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    RESISTIVITY UNITS

    It is reasonable to expect that R is directly

    proportional to the length of the resistor andinversely proportional to the cross-sectionalarea of the resistor. The conductivity is definedas

    Dimensionally, the units of resistivity must be in

    ohm-m, and conductivity then is:

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    Dependencies of Earthresistivities:

    1. Water , r 2. Salinity , r 4. Porosity , r (water filled)5. Clays , r 6. Metallic minerals , r

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    Rock types and resistivity

    Igneous rocks highest resistivities

    Sedimentary rocks tend to bethe most conductive due to theirhigh fluid content

    Metamorphic rocks haveintermediate but overlappingresistivities

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    Most rock-forming minerals are insulators:

    1081016m

    However, measurement in situ: sedimentary rocks: 51000 m

    metamorphic/crystalline rocks: 100105m

    Reason: Rocks are usually porous and poresare filled with fluids, mainly water. As theresult, rocks are electrolytic conductors.Electrical current is carried through a rockmainly by the passage of ions in pore waters.

    Most rocks conduct electricity byelectrolytic rather than ohmic processes.

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    Schematic current flow insoil sample

    An increase in the number of ions in soilwater (groundwater contamination) linearlydecreases the soil resistivity.

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    The approximate resistivity

    values of common rock types

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    Age of the rock and Resistivity

    Age of the rock is also important forthe resistivity.

    For example:

    Young volcanic rock (Quaternary)

    10200 m

    Old volcanic rock (Precambrian)1002000 m

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    Current Densities andEquipotentials

    How does thecurrent flowthrough the Earth?

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    At any point in the medium, thecurrent densityis defined as theamount of current passing through a

    unit area of an equipotential surface.

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    A First Estimate of Resistivity

    Vis voltage,Iis current,ris resistivity,and ris the distance

    this expression is nothingmore than Ohm's law with theresistance, R equal to rover2pr.

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    If the Earth had a constant resistivity,

    C t Fl F T Cl l

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    Current Flow From Two CloselySpaced Electrodes

    A Practical Way of Measuring

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    A Practical Way of MeasuringResistivity

    r1, r2, r3, and r4, as shown in the figure.

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    El d fi i

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    Electrode configurations

    and general case

    General CaseThe general case is considered, where thecurrent sink is a finite distance from the

    source.

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    Principle of

    measurementand potentialfield for forgeoelectric

    DC surveys

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    ELECTRODE ARRAYS

    There are three commonlyused electrode arraysincluding

    1- Wenner array,

    2- Dipole-Dipole array, and3- Schlumberger array

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    Fig. (I-2): Electrode arrays in common use(a) Schlumberger, (b) Wenner, and (c) Dipole- dipole configurations.

    I

    V

    A M N B

    2 L

    2 l

    I V

    a a

    L

    ( c ) Dipole - Dipole

    ( a ) Schlumberger

    A B M N

    I

    V

    A M N B

    aaa

    ( b ) Wenner

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    Comparison Of Electrode Arrays

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    Comparison Of Electrode Arrays

    R l ti b t l t d

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    Relation between electrodespacing and depth penetration

    Depth of penetration

    is

    equal toone fifth

    of

    electrode spacing

    Factors affecting selection of

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    Factors affecting selection ofresistivity electrode arrays.

    Sensitivity to surface

    inhomogeneties

    Resolution of

    Steeply dippingstructures

    Resolution of

    Horizontalstructures

    Signal

    Response

    ProfilingSoundingArrayCBCAAenner

    CABABchlumberger

    BDDBEipole-Dipole

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    Generally

    The Schlumberger and Wennerarrays are the most common arrays

    used for different engineering,environmental, and groundwaterapplications. There are two

    essential differences between thesetwo types of electrode arrays:

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    In the Schlumberger array, the distance between thepotential electrodes MNis small and is always keptequal to, or smaller than, one-fifth the distance

    between the current electrodes AB; that is,AB5MN.In the Wenner array, on the other hand, AB is alwaysequal to 3MN,

    The potential electrodes in a Schlumberger soundingare moved only occasionally. In a Wennersounding,however, they and the four electrode are moved aftereach measurement.

    K i h l i f h f l d

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    Knowing the locations of the four electrodes,and by measuring the amount of current input

    into the

    ground, iand the voltage difference betweenthe two potential electrodes, DV, we can

    compute the

    resistivity of the medium, ra, using the

    following equation.

    In this particular case,

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    In this particular case,regardless of the location of the

    four electrodes, ra will be exactly

    equal to theresistivity of the medium. Theresistivity computed using the

    equation given above is referredto as the

    apparent resistivity.

    Depth of Current Penetration Versus Current

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    Depth of Current Penetration Versus CurrentElectrode Spacing

    Current Flow in Layered Media

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    Current Flow in Layered Media

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    Variation in Apparent Resistivity: Layered VersusHomogeneous

    Media

    Current Flow in Layered Media Versus Current

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    Current Flow in Layered Media Versus CurrentElectrode Spacing

    Consider the earthmodel shownbelow: a highresistivity layerover a lowerresistivity layer.

    Plotting the Resistivity Data

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    Plotting the Resistivity Data

    Thus, if we were to compute and plotapparent resistivity for a variety of currentelectrode spacings while holding thepotential electrodes fixed, we wouldgenerate a plot similar to that shownbelow.

    A Second Example of Current

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    A Second Example of CurrentFlow in Layered Media

    As another example of

    current flow in layeredmedia and howapparent resistivitycan vary with varying

    electrode spacing*,consider the earthmodel shown below.In this case, a low

    resistivity layeroverlies a

    higher resistivityhalfspace.

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    Survey Types Overview:

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    Survey Types Overview:Soundings and Profiles

    Resistivity Soundings

    Resistivity Profiling

    VES

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    VES

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    VES

    The relation between electrodespacing and depth penetration

    Resistivity Soundings

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    Resistivity Soundings

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    Electrode Spacings and Apparent

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    gResistivity Plots

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    Flow Diagram showing the basic Steps of Acquisition,

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    Processing and interpretation of VES data.

    Resistivity Profiling

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    Resistivity Profiling

    resistivity profiles are resistivity surveys inwhich the electrode spacing is fixed

    for all readings. Apparent resistivity is

    computed for different electrode centerpoints as the entire

    electrode spread is moved. Usually, thecenter point is moved along the line of the

    electrodes, although

    this does not have to be the case.

    Profiling is accomplished by fixing

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    Profiling is accomplished by fixingthe electrode spacing and movingthe entire array.

    The distance between stations D, isdictated by the lateral resolutiondesired

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    Geo-electric Layering

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    Geo electric Layering

    Often the earth can be

    simplified as consistingof a series ofhorizontal beds thatare infinite in extent.

    Goal of the resistivitysurvey is then todetermine thicknessand resistivity of thelayers.

    VES Data Plotting Convention

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    VES Data Plotting Convention

    Plot apparent resistivity as a functionof the log of some measure ofelectrode separation.

    Wennera spacing

    SchlumbergerAB/2

    Dipole-Dipolen spacing

    Future? Towed Array

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    Future? Towed Array

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    Measurement System

    TransmitterPower SupplyCan be DCAC more

    common

    AmmeterMetal electrodes

    Receiver

    Volt meterMetal electrodes

    Field Considerations for DC

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    Resistivity

    Good electrode contact with the earth.

    Wet electrode location

    Add NaCl solution or bentonite.Surveys should be conducted along astraight line whenever possible.

    Stay away from cultural featureswhenever possible (power lines, pipes,grounded metal fences,pumps, etc)