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    Geophysical Exploration forGeophysical Exploration forEngineering InvestigationsEngineering Investigations

    Dr. Adly AlDr. Adly Al--SaafinSaafin

    20112011

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    OUTLINEOUTLINE

    GEOLOGY OF ARABIAGEOLOGY OF ARABIA PHASES OF SITE INVETIGATIONPHASES OF SITE INVETIGATION EXPLORATIONEXPLORATION ROLE OF GEOPHYSICAL TECHNIQUES ONROLE OF GEOPHYSICAL TECHNIQUES ONENGINEERING WORKSENGINEERING WORKS FACTRORS INFLUENCING GEOPHYSICALFACTRORS INFLUENCING GEOPHYSICALINVESTIGATIONINVESTIGATION

    GEOPHYSICAL METHODSGEOPHYSICAL METHODS

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    GEOLOGY OF ARABIAGEOLOGY OF ARABIA

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    For Detailed Information

    Read Attachment # 1

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    PHASES OF SITE INVESTIGATIONPHASES OF SITE INVESTIGATION

    DESK STUDY

    RECONNAISSANCE FIELD TRIP

    PRLEMINARY SITE INVESTIGATION SITE EXPLORATION

    Surface Exploration

    Sub-surface Exploration

    LAB / IN-SITU TESTING

    ENGINEERING GEOLGICAL ASPECTSENGINEERING GEOLGICAL ASPECTS

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    EXPLORATIONEXPLORATION

    SURFACE EXPLORATION

    UBUB-SURFACE EXPLORATIONURFACE EXPLORATION

    Destructive Techniques

    Trenching Drilling

    Non-destructive Techniques:Geophysical InvestigationGeophysical Investigation

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    FACTRORS INFLUENCINGFACTRORS INFLUENCING

    GEOPHYSICAL INVESTIGATIONGEOPHYSICAL INVESTIGATION

    Geophysical exploration methods provide an indirect source ofinformation about subsurface setting.

    Geophysical techniques depend on the variations of physical /

    chemical properties of soil and rock:

    Mineralogical composition

    Water content

    Clay content

    Porosity / fractures

    Salinity

    Magnetic susceptibility

    Density

    Elastic moduli

    Velocity

    Resistivity

    xxxx

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    ROLE OF GEOPHYSICAL TECHNIQUESROLE OF GEOPHYSICAL TECHNIQUES

    ON ENGINEERING WORKSON ENGINEERING WORKS

    StratificationStratification Depth to water tableDepth to water table Groundwater qualityGroundwater quality Depth to bedrock,Depth to bedrock,

    Thickness of weathering zoneThickness of weathering zone

    Underground cavities detectionUnderground cavities detection Faults, Shear zones allocationFaults, Shear zones allocation

    Corrosion susceptibilityCorrosion susceptibility

    Rock Quality determinationRock Quality determination Rock RippabilityRock Rippability Physical characteristicsPhysical characteristics xxxxxxxx

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    GEOPHYSICAL METHODSGEOPHYSICAL METHODS

    Passive MethodsPassive Methods::

    Gravity field Magnetic field

    Seismic arrival

    (EQs) Active MethodsActive Methods::

    Seismic

    Electric Resistivity Electromagnetic

    GPR

    EM

    Surface MethodsSurface Methods::GravityMagnetic

    Seismic

    Electric ResistivityElectromagnetic

    Borehole MethodsBorehole Methods::

    Crosshole Test (CHT)

    Downhole Test (DHT)

    Logging

    xxx

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    Contrasts in physical properties from different geological targets give rise to

    geophysical target.

    Wet rock Wet rock

    Which MethodWhich Method.?.?

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    Usefulness of engineering geophysical methods

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    Usefulness of engineering geophysical methods (continued)

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    SEISMIC METHODSSEISMIC METHODS

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    SEISMIC METHODS

    1.1. IntroductionIntroduction

    2.2. Seismic wavesSeismic waves

    3.3. Seismic methodsSeismic methods

    4.4. SEISMIC REFRACTION METHODSEISMIC REFRACTION METHODi.i. Seismic waves propagation in theSeismic waves propagation in the

    groundgroundii.ii. Data acquisition & InstrumentsData acquisition & Instruments

    iii.iii. Data processing & InterpretationData processing & Interpretation

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    1.1. IntroductionIntroduction

    Seismic methods developed based on

    the fact that the elastic properties of soiland rock determine the velocities ofwave propagation through them.

    Vp and Vs are the P and S wavevelocities of the medium is a

    function of , and k.Whereas

    is the density of the medium,and

    and k are referred to as the shear

    and bulkmodules of the media.

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    2.2. Seismic WavesSeismic Waves Seismic waves; transfer of energy by

    way of particle motion. Seismic wavefront

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    Elastic WavesElastic Waves

    .

    .

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    Seismic WavesBody wavesBody waves - These are elastic waves that propagate through

    the Earth's interior. In reflection and refraction prospecting, bodywaves are the source of information used to image the Earth's

    interior.P Waves

    - P waves are also called primary waves, because they

    propagate through the medium faster than the other wavetypes.

    S Waves

    - S waves are sometimes called secondary waves,

    because they propagate through the medium slower than Pwaves.

    Surface WavesSurface Waves - that propagate along the Earth's surface.Their amplitude at the surface of the Earth can be very large, butthis amplitude decays exponentially with depth. Surface wavespropagate at speeds that are slower than S waves.

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    Types of WavesTypes of Waves

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    Types of Body WavesTypes of Body Waves

    Compressional waves (P), which travelin any medium (solid, water and airsolid, water and air).

    Shear waves (S), which travels only in

    solidsolid.

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    Compressional (P) Wave

    Identical to sound wave particle

    motion is parallel to wave propagation

    direction.

    Animation courtesy Larry Braile, Purdue University

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    Shear (S) Wave

    Particle motion is perpendicular

    to propagation direction.

    Animation courtesy Larry Braile, Purdue University

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    Mechanical of Body Waves

    SourceReceiver (Geophone)

    Oscilloscope

    P

    S R

    Time

    AmplitudeAmplitude

    R S P

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    Vp values forSelected Earths

    Materials

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    Seismic WavesSeismic Waves

    Body waves

    Surface waves

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    3.3. SEISMIC METHODSSEISMIC METHODS

    1.1. Reflection methodReflection method2.2. Refraction MethodRefraction Method

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    44 -- SEISMIC REFRACTION METHODSEISMIC REFRACTION METHODi.i. Seismic waves propagation in theSeismic waves propagation in the

    groundground

    ii.ii.Data acquisition & InstrumentsData acquisition & Instruments

    iii.iii.Data processing & InterpretationData processing & Interpretation

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    4.i4.i-- Seismic Refraction Waves PropagationSeismic Refraction Waves Propagation

    in the Groundin the Ground Refraction Seismology-A program to map geologic structure by using head

    waves.

    Head waves involve energy that enters a high-velocity medium (refractor)near the critical angle and travels in the high-velocity medium nearly parallel

    to the refractor surface.

    The change in curvature of the wave front as the wave passes through theinterface implies that the ray-paths describing the direction of propagationof the wave change direction through the boundary. This change in direction

    of the ray-path as it crosses a boundary is described by a well-known lawknown as Snell's Law.

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    Wave PropagationWave Propagation

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    Wave propagation (Two Layers)Wave propagation (Two Layers)

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    Wave Propagation (Multiple Layers)Wave Propagation (Multiple Layers)

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    What causes refraction?

    Notice.

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    layer Model-Waves propagation in a two

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    Travel TimeTravel Time

    ii4 ii D A i i i ID A i i i & I

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    4.ii4.ii-- Data Acquisition & InstrumentData Acquisition & Instrument

    Seismic Source, Geophones, Recording System

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    Field Survey

    Data Acquisition:

    Geophones

    Connection cable

    Other connections

    Generate sufficient energy

    Seismic record

    See Movie # 1See Movie # 1

    http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/http://seismic%20training%201-0%20%28field%20setup%29.flv/
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    Seismic Waves Record

    Oscilloscope

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    Seismic Refraction

    Vertical GeophonesSource

    (Plate)

    Rock: Vp2

    ASTM D 5777

    Soil: Vp1

    x1x2x3x4

    t1 t2t3t4

    Note: Vp1

    < Vp2

    zR

    Determine depthto rock layer, zR?

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    4.iii4.iii-- Data InterpretationData InterpretationDetermination of X ThicknessDetermination of X Thickness

    1

    2

    1. Intercept time

    value.

    2. Critical distance

    value.

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    Example.

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    Multiple LayersMultiple Layers

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    Hidden Layer CaseHidden Layer Case!......!......

    Comments & Suggestions?..omments & Suggestions?..

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    Dipping Layer CaseDipping Layer Case!......!......

    By acquiring refraction seismic observations in two directions, we can immediately determine

    whether or not subsurface layers are dipping.If dipping layers are present, the travel-time curves obtained in the two directions are no longermirror images of each other.

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    Using Seismic Refraction to

    Map the Subsurface

    Depth{

    For layer parallel tosurface

    12

    12

    2 VV

    VVXcDepth

    )cos(sin22

    11

    1

    VV

    VTi

    V2 > V1

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    50 Seismic refraction in three layer system

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    Seismic Refraction and Fault Detection

    D P & I i

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    Data Process & Interpretation

    Using Computer.

    Rippability of In-place Rock by Caterpillar Dozer Evaluate by P-Wave Velocity.

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    pp y p y p y y(After Franklin and Dusseault, 1989)

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    ELECTRIC RESISTIVITYELECTRIC RESISTIVITY

    METHODSMETHODS

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    Electric Resistivity MethodElectric Resistivity Method

    1.1. IntroductionIntroduction

    2.2. Current flow in the groundCurrent flow in the ground

    3.3. Electrode configurationElectrode configuration

    4.4. Field method and instrumentationField method and instrumentation

    5.5. Data interpretationData interpretation

    6.6. Case studiesCase studies

    11 I t d tiI t d ti

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    1.1. IntroductionIntroduction

    Electric Resistivity Methods developed based on somefactors that effect the resistance of earth material to electriccurrent flow.

    Seismic techniques depend on the physical properties ofearth materials.

    Electric resistivity methods depend on combination of (i)

    conductivity of the fluid present in porosity and (ii) earthmaterial itself as:

    Variations in mineralogy,Variations in mineralogy,

    Porosity / fractures,Porosity / fractures,

    Water contentWater content

    Clay contentClay content

    Salt contentSalt content

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    Introducing current to the earth through two

    electrodes that are pushed into the ground surface.The Resistance of earth material to current flow is

    obtained from (Ohms law) by measuring the

    potential drop between two electrodes that arepositioned with the field of the current electrodes.

    V = I. R

    Depth of investigation is proportional to the currentelectrode separation.

    Introducing current to the earth through twoelectrodes that are pushed into the ground surface.

    The Resistance of earth material to current flow is

    obtained from (Ohms law) by measuring the

    potential drop between two electrodes that arepositioned with the field of the current electrodes.

    V = I. R

    Depth of investigation is proportional to the currentelectrode separation.

    Basic ConceptsBasic Concepts

    )) and Resistivity (RResistance (

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    )) and Resistivity (RResistance (

    El i l R i i i MEl t i l R i ti it M t

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    Electrical Resistivity MeasurementsElectrical Resistivity Measurements

    1 10 100 1000 10000

    Bulk Resistivity,

    (ohm-meters)

    Clay

    Loam

    Loose Sands

    Sands & Gravels

    Glacial Till

    Weathered Rocks

    Resistivity Values (ConeTec & GeoProbe, 1997)

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    C d ti it (1/C d ti it (1/ ) f diff t il) f diff t il

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    Conductivity (1/Conductivity (1/) for different soils) for different soils

    2 C fl i h d

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    2.2. Current flow in the groundCurrent flow in the ground

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    Current flow in the ground

    Current flow in the ground

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    Current flow in the ground

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    Apparent Resistivity (a)

    El d C fi i

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    Electrodes Configuration

    33 El t d C fi tiEl t d C fi ti

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    3.3. Electrodes ConfigurationElectrodes Configuration

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    4 D t A i iti (Fi ld A ti it )

    44 Data Acquisition (Field Activity)Data Acquisition (Field Activity)

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    4. Data Acquisition (Field Activity)

    Instrumentation: Current Source, Ammeter, Voltmeter, Electrodes, Cables.

    4.4. Data Acquisition (Field Activity)Data Acquisition (Field Activity)

    InstrumentationInstrumentation: Current Source, Ammeter, Voltmeter, Electrodes, Cables.

    VES-1AB/2=1 5 MN/2=0 5

    Schlumberger SoundingVES-1

    Wenner Sounding

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    AB/2=1.5, MN/2=0.5

    AB/2=2, MN/2=0.5

    AB/2=3, MN/2=0.5

    AB/2=4, MN/2=0.5

    AB/2=5, MN/2=0.5

    AB/2=5, MN/2=1

    AB/2 R a1.5

    2

    3

    4a

    AB/2

    a=1m

    a=2m

    a=3m

    a=4m

    a=5m

    a,m R a

    1

    2

    3

    4

    a

    a,m

    Data Table

    Field Curve

    Data Table

    Field Curve

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    Electrode spacing & current penetration

    Arrangement for the Wenner Test

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    Arrangement for the Wenner Test

    Recommended probe spacing/depths for soil

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    Recommended probe spacing/depths for soilresistivity tests

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    Data Acquisition:

    1.

    2.

    3.4.

    5.

    6.

    http://www.fluke.eu/comx/products/demos/geox2_en.swf

    http://www.fluke.eu/comx/products/demos/geox2_en.swfhttp://www.fluke.eu/comx/products/demos/geox2_en.swf
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    Gulf Consult Vertical Electric sounding

    Normal profiling

    Environmental applications

    Others

    5.5. Data processing & InterpretationData processing & Interpretation

    VES-1

    a 1m

    Wenner Sounding

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    a=1m

    a=2m

    a=3m

    a=4m

    a=5m

    a,m R a

    1

    2

    3

    4

    a

    a,m

    Data Table

    Field Curve

    s Expertises Expertise

    Gulf ConsultGulf Consult

    Gulf Consult RequirementsGulf Consult Requirements

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    Gulf Consult RequirementsGulf Consult Requirements

    Apparent resistivity

    (a) = 2aR (ohm-m)Resistance (R)

    [V/I] (ohm)Spacing (a)

    (m)SN

    11/121/2

    41/361/4

    81/5101/6

    1/n

    Typical Soil Resistivity Plot

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    Typical Soil Resistivity Plot

    VES & Normal ProfilingVES & Normal Profiling

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    VES & Normal ProfilingVES & Normal Profiling

    Vertical Electric Soundings (VES): theresistivity method carried out to detect

    vertical variations in resistivity thatoccur solely with depth.

    Resistivity Profiles: the resistivity

    survey employed to detect lateralvariations in resistivity (NormalProfiling).

    Vertical Electric Soundings (VES): theresistivity method carried out to detect

    vertical variations in resistivity thatoccur solely with depth.

    Resistivity Profiles: the resistivity

    survey employed to detect lateralvariations in resistivity (NormalProfiling).

    S

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    Vertical Electric Sounding(VES)

    Vertical Electric Sounding(VES)

    Electrode Spacing and Apparent Resistivity Plots

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    p g pp y

    AB/2, of 0.25, 0.5, 0.75, 1.0, 1.25, 1.5, 1.75, 2.0, 2.25, 5.0, 7.5, 10.0, 12.5, 15.0, 17.5, 20.0, 22.5,

    50.0, 75.0, 100.0, 125.0, 150.0, 175.0, 200.0, and 250.0 meters were taken.

    Apparent Resistivity Curves for

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    Apparent Resistivity Curves forSoundings Over One-Layered Media

    Apparent Resistivity Curves in

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    Apparent Resistivity Curves in

    Two-Layered Media

    P ibl I t t ti f ERPossible Interpretation of ER survey

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    Possible Interpretation of ER surveyPossible Interpretation of ER survey

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    VES & GeoVES & Geo--electrical Profileelectrical Profile

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    VES & GeoVES & Geo--electrical Profileelectrical Profile

    VES & GeoVES & Geo--electrical Profileelectrical Profile

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    VES & GeoS & Geo electrical Profilee ect ca o e