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1 Slide 1 Dr Elena Pasternak Petroleum Engineering Fundamentals PETR2510 Exploration methods Slide 2 Dr Elena Pasternak Literature Selley, R.C. 1998. Elements of Petroleum Geology, Academic press Jahn, F., M. Cook & M. Graham, 2007. Hydrocarbon Exploration and Production. Elsevier Hyne, N.J. 2001. Nontechnical Guide to Petroleum Geology, Exploration, and Production. Penn Well Corporation

Petr 2510 Lectures 2

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Page 1: Petr 2510 Lectures 2

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Slide 1Dr Elena Pasternak

Petroleum Engineering Fundamentals

PETR2510

Exploration methods

Slide 2Dr Elena Pasternak

Literature Selley, R.C. 1998. Elements of Petroleum

Geology, Academic press Jahn, F., M. Cook & M. Graham, 2007.

Hydrocarbon Exploration and Production. Elsevier

Hyne, N.J. 2001. Nontechnical Guide to Petroleum Geology, Exploration, and Production. Penn Well Corporation

Page 2: Petr 2510 Lectures 2

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Slide 3Dr Elena Pasternak

Plan

Aim

Geophysics

Borehole geophysics (logs)

(Pictures, if not indicated otherwise, are copied from Selley, 1998 )

Slide 4Dr Elena Pasternak

Aim Objective is to find new volumes of

hydrocarbons (at a low cost and in short period of time)

Two types of methods» Geophysics (exploration from the surface)» Borehole geophysics (logging)

Geochemistry» Detects surface anomalies caused by hydrocarbon

accumulation

Field studies (outcrops)» Vertical and lateral relationship of the different rock

types of a reservoir

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Slide 5Dr Elena Pasternak

Definition of a good reservoir

Now: How to find a reservoir (“good” or otherwise!)

» Find a basin (coarse scale)

– gravity surveys, magnetic surveys, macro-geology (in many cases today this data can be available in public domain)

» Within the basin (medium level of coarseness)

– coarse seismic 2D grid, covers a wide area to show a potential accumulation (plus regional geology)

» With prospects identified

– Fine scale seismic

– drill an exploration well (only drilling of an exploration well proves the validity of the concept)

Exploration Methods & Techniques

Slide 6Dr Elena Pasternak

Exploration activities are potentially damaging to the environment.» eg, cutting down of trees in preparation for an

onshore seismic survey may result in soil erosion in the future

» Offshore, fragile ecological systems (eg, reefs) can be permanently damaged by spills of crude or mud chemichals.

» Responsible companies have to carry out an Environmental Impact Assessment before the activity planning and draw up contingency plan in the case of an accident happening.

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Slide 7Dr Elena Pasternak

Timing of different exploration methods

Slide 8Dr Elena Pasternak

Geophysics

Gravity surveys

Magnetic surveys

Seismic surveys

3D and 4D surveys

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Slide 9Dr Elena Pasternak

Gravity surveys

r

F

M

m

Newton’s law

222

2

311

2

,,

10670.6

zyxr

zyx

skg

mG

rr

mMG

r

r

rF

Acceleration of mrr

MG

m

rFa

2

1

x

y

z

Slide 10Dr Elena Pasternak

Direct reconstruction of the density distribution

x

V

y

V

dVG 3

)()(

xy

xyyxa y

Solution of this integral equation is sensitive to errors –Difficult to solve

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Slide 11Dr Elena Pasternak

Corrections

Correction for latitude» Gravity varies with latitude

Free-air correction» Gravity varies with altitude

Bouguer anomaly correction» Influence of the mass of rock between the

survey station and a reference datum (usually sea level)

Slide 12Dr Elena Pasternak

Gravimeter (Gravity Meter)

Accuracy within 1 µGal.

L&R Aliod G MeterMass and spring gravity meterhttp://www.earthsci.unimelb.edu.au/ES304/MODULES/GRAV/NOTES/spring.html

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Slide 13Dr Elena Pasternak

The gravity method measures small (~10-6g) variations of the Earth’s gravity field caused by density variations in geological structures.

The sensing element is a spring balance. Variations in the Earth’s gravity field cause changes in the length of the spring which is measured (gravimeter).

The gal, sometimes called Galileo (Gal) is a unit of acceleration for a gravitational field. 1Gal=1cm/sec2=10-2m/sec2.

Slide 14Dr Elena Pasternak

Magnetic surveys Measure changes in the Earth magnetic field caused by

variations in the magnetic properties of rocks» Airborne - Both fluxgate and proton precession magnetometers

can be mounted within or towed behind aircraft, including helicopters. These so-called aeromagnetic surveys are rapid and cost effective. When relatively large areas are involved, the cost of acquiring 1 km of data from an aeromagnetic survey is about 40% less than the cost of acquiring the same data on the ground. In addition, data can be obtained from areas that are otherwise inaccessible. GPS is used to fix the positions of the aircraft.

» Shipborne - Magnetic surveys can also be completed over water by towing a magnetometer behind a ship. Marine magnetic surveying is slower than airborne surveying. Efficient together with other geophysical methods from the same ship.

» Ground Based - Like gravity surveys, magnetic surveys are also commonly conducted on foot or with a vehicle. Ground-based surveys may be necessary when the target of interest requires more closely-spaced readings than are possible to acquire from the air.

http://www.earthsci.unimelb.edu.au/ES304/MODULES/MAG/NOTES/fieldmodes.html

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Slide 15Dr Elena Pasternak

Example of magnetic survey

http://www.ga.gov.au/education/minerals/magsurv.html

Slide 16Dr Elena Pasternak

Example (cont)

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Slide 17Dr Elena Pasternak

Catalogue of typical

situations

Calculate the gravity and magnetic signatures of typical geological structures

Slide 18Dr Elena Pasternak

Seismic surveys Basics

» Types of stress waves

» Reflection of wave from the boundary

Surveys» Land

» Sea

Examples

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Slide 19Dr Elena Pasternak

Seismic surveys involve the generation of artificial shock waves which propagates through ‘overburden’rocks to the reservoir and beyond, reflects back to the receivers.

Receivers register waves as a pressure pulse (hydrophones – offshore) or as acceleration(geophones – onshore).

The objective of seismic surveying is to produce an (acoustic) image of the subsurface with as much resolution is possible, with all the reflections correctly positioned and the image is as close to the real geological picture as possible.» in exploration for determining structures and traps

to be drilled» in field appraisal and development for estimation

of reserves and plans of field development» during production for observing movement of

contacts, distribution of reservoir fluids and changes in pressures

Slide 20Dr Elena Pasternak

Basics

Types of stress waves» P-wave (pressure wave)

» S-wave (shear wave)

» Rayleigh wave (surface wave)

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Slide 21Dr Elena Pasternak

Wave equations. Planar wave

xz

y

uxuz

uy

Wave front

Direction of wave propagation

P-waveS-waves0

1

01

01

2

2

22

2

2

2

22

2

2

2

22

2

t

u

cx

u

t

u

cx

u

t

u

cx

u

z

S

z

y

S

y

x

P

x

∑/∑y=∑/∑z0

Slide 22Dr Elena Pasternak

Non-planar wave front

Locally the front can be replaced with a tangent plane

Plane waves

x

z

y

uxuz

uy

Wave front

Direction of wave propagation

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Slide 23Dr Elena Pasternak

Rayleigh wavesWaves near the boundary of a semi-

space

Direction of wave propagation

Direction of particle motion

Dec

ays

expo

nent

iall

y

Velocity

Slide 24Dr Elena Pasternak

Reflection of wave from the boundary

Depth(geophone at the source location)

21tv

D

v1 – average wave velocity in rockst – two-way (there and back) travel time

III

II

v2

v1

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Slide 25Dr Elena Pasternak

Velocity-density relationship for sedimentary rocks

Slide 26Dr Elena Pasternak

Arrays Bundles of geophones on a streamer

Energy source» Land

– Explosives

– Dropping heavy weight

– Vibrating plate

» Sea– Electric sparker (implosion, shallow depths)

– Air gun (bubble of compressed air, up to 5km)

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Slide 27Dr Elena Pasternak

Land (Hyne, 2001)

GeophoneVibrator truck

A geophone is a small, cheap instrument for measuring ground motion.

Slide 28Dr Elena Pasternak

Sea

6 km

Hydrophones on cable

(Hyne, 2001)

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Slide 29Dr Elena Pasternak

Marine Seismic Surveys

Slide 30Dr Elena Pasternak

Wave Source, Receiver and Recording Equipment

Survey vessel» Tows 12 to 16, 3000 to 8000 m long

hydrophone streamers spaced 50 to 100 m apart

» Survey speed 5 knots

» 68 crew members

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Slide 31Dr Elena Pasternak

Wave Source, Receiver and Recording Equipment

Airguns use compressed air to generate bubbles which emit sound as they expand

They are often used in an array to create the required amplitude and frequency range

Slide 32Dr Elena Pasternak

Wave Source, Receiver and Recording Equipment

Hydrophone arrays» Each streamer is made up of hundreds

of groups of 12 to 24 hydrophones» Streamers are towed at a depth of 6 to

10m

Streamer SteererStreamer Spool Hydrophone

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Slide 33Dr Elena Pasternak

Time Structure Map

Seismic Survey Lines and Times

X 1.205

X 1.205

X 1.205

X 1.205

X 1.205

X 1.505

X 1.505

X 1.485

X 1.485

X 1.215

X 1.215

X 1.215

X 1.215

X 1.215

X 1.225

X 1.225

X 1.225

X 1.225

X 1.225

X 1.225

X 1.505

X 1.485

Equal times are joined by contours

X 1.205

X 1.205

Time Structure Map

H

- Fault Edge

X 1.215

Slide 34Dr Elena Pasternak

Time Structure Map LEGENDRE

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Slide 35Dr Elena Pasternak

Time-Depth conversion

From the Time Structure map it is possible to create a Depth Structure map by utilising the velocity profile which was created during the data processing procedures

Slide 36Dr Elena Pasternak

Depth Structure Map

Time Structure Map

H

+ Velocity Profile

Increasin

g

Velocity

2.0 km/s

2.5 km/s

3.0 km/s

3.5 km/s

4.0 km/s

= Depth Structure Map

H

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Slide 37Dr Elena Pasternak

Depth Structure Map LEGENDRE

Slide 38Dr Elena Pasternak

LEGENDRE

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Slide 39Dr Elena Pasternak

Hydrophone

A hydrophone is a microphone designed to be used underwater for recording or listening to underwater sound. Most hydrophones are based on a piezoelectric transducer that generates electricity when subjected to a pressure change.

Slide 40Dr Elena Pasternak

Velocity determination

S

Velocity

21 Sv

22

v

DZ

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Slide 41Dr Elena Pasternak

Example

(Hyne, 2001)

Slide 42Dr Elena Pasternak

3D and 4D surveys

3D surveys» Combinations of 2D surveys into a 3D

picture

4D surveys» Succession of 2D and 3D surveys at

intervals of time during which it is expected that the variations in wave propagation can occur (eg, due to production)

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Slide 43Dr Elena Pasternak

Borehole geophysics

Boreholes» Exploration

» Production

Logging» Measurements in borehole

Slide 44Dr Elena Pasternak

Production boreholes

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Slide 45Dr Elena Pasternak

Logs

Sonic (acoustic) log

Electric logs

Radioactivity logs

Porosity logs in combination

Dielectric log » Dielectric constant

» Porosity and saturation

Dipmeter log and borehole imaging

Mud logs

Slide 46Dr Elena Pasternak

Sonic (acoustic) log

Used in open uncased boreholes

Determines rock porosity, , by measuring the wave velocities

maf

ma

tt

tt

log

Interval transit time from the log

Interval transit time of the rock

Interval transit time of the fluid

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Slide 47Dr Elena Pasternak

Typical wave velocities

Slide 48Dr Elena Pasternak

Electric logs

Spontaneous Potential (self potential, SP) logs» To delineate permeability

zones

Resistivity logs» Quantification of

hydrocarbon saturation

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Slide 49Dr Elena Pasternak

Basic arrangement for the SP log

Slide 50Dr Elena Pasternak

Spontaneous Potential (self potential, SP) logs

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Slide 51Dr Elena Pasternak

Resistivity logs

Slide 52Dr Elena Pasternak

Radioactivity logs Gamma-Ray log

» Uses scintillation counter to measure natural radioactivity of rocks (in API units)

» Lithological identification Neutron log

» Rock is bombarded by neutrons» As a result, gamma-rays are emitted in proportion to

hydrocarbon content (HC+neutron → -ray) Density log (gamma-gamma tool)

» Tool emits gamma-rays and measures gamma-rays returned from formation. This depends upon density. Knowing density of dry rock and density of fluid, the porosity can be recovered (HC+ -ray → attenuation of -rays)

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Slide 53Dr Elena Pasternak

Natural radioactivity of rocks

Slide 54Dr Elena Pasternak

Porosity logs in combination Sonic (acoustic) log → porosity Electric logs → porosity Radioactivity logs → porosity Dielectric logs (electromagnetic wave propagation,

salty water – bad dielectric, dielectric constant in salty water < than in fresh water < HC; cf. resistivity of salty water is low, higher in fresh water and HC)→porosity

Combination» The three types of porosity measurements are differently

influenced by factors:– Lithology– Clay content– Presence of gas

» Combination increases accuracy

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Slide 55Dr Elena Pasternak

Dipmeter log and borehole imaging

Dipmeter» Multi-arm micro-resistivity log» Measures direction of dip of beds adjacent

to borehole

Formation MicroImager» Large numbers of micro-resistivity probes » Imaging through statistical analysis

(synthesises an image of lithology of a borehole face by using dipmeter log)

Slide 56Dr Elena Pasternak

Dipmeter

4 pad 4 track dipmeter

Locations of a, b, c, d –peaks on resistivitycurves give location of bedding plane (boundary between different rocks. Boundary does not conduct electricity well – high resistivity.)

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Slide 57Dr Elena Pasternak

Formation MicroImager

Unrolled format Cylindrical format

Slide 58Dr Elena Pasternak

Mud Logs

Drilling rate» Information about lithology

» Qualitative indication of porosity

Investigation of cuttings lifted with mud» Traces of hydrocarbons

Gas detector

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Slide 59Dr Elena Pasternak

Mud logs

(Jahn et al., 2007)

Slide 60Dr Elena Pasternak

Summary of exploration objectives and methods

(Jahn et al., 2007)

Exploration requires integration of different techniques and disciplines

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Slide 61Dr Elena Pasternak

Exploration Methods & Techniques

Definition of a good reservoir Now: How to find a reservoir (“good” or

otherwise!!)» Find a basin (coarse scale)

– gravity surveys, magnetic surveys, macro-geology

» Within the basin (medium level of coarseness)

– coarse seismic

» Now, With prospects identified– drill an exploration well

drill an exploration wellmake well-bore measurements