80
Field course and methodology in geology and geophysics Geophysical Methods GEL2150

Field course and methodology in geology and geophysics

  • Upload
    bary

  • View
    58

  • Download
    2

Embed Size (px)

DESCRIPTION

GEL2150. Field course and methodology in geology and geophysics. Geophysical Methods. About this part of the course. Purpose: Introduction to geological/geophysical field methods used in hydrocarbon exploration Working Plan: Lecture: Introduction to the principles (27.3) Practical: - PowerPoint PPT Presentation

Citation preview

Page 1: Field course and methodology in geology and geophysics

Field course and methodology in geology and geophysics

Geophysical Methods

GEL2150

Page 2: Field course and methodology in geology and geophysics

About this part of the course

• Purpose: Introduction to geological/geophysical field methods used in hydrocarbon exploration

• Working Plan:– Lecture: Introduction to the principles (27.3)– Practical:

• Introduction to excercise (29.3, 14.15-14.30)• Seismic Interpretation excercise (29.3 14.30-17.00 & 31.3

13.15-16.00)• Field course

– Field based synthetic seismics (week 18)

– Tectonics and sedimentation (week 20)

Page 3: Field course and methodology in geology and geophysics

Lecture Contents

• Geophysical Methods

• Theory / Principles

• Acquisition and Prosessing

• Advantages and pitfalls

Page 4: Field course and methodology in geology and geophysics

Geophysical methods

• Passive:Method using the natural fields of the Earth, e.g. gravity and magnetic

• Active:Method that requires the input of artificially generated energy, e.g. seismic reflection

• The objective of geophysicsis to locate or detect the presence of subsurface structures or bodies and determine their size, shape, depth, and physical properties (density, velocity, porosity…) + fluid content

Page 5: Field course and methodology in geology and geophysics

Geophysical methods

Method Measured parameter “Operative” physical property

Application

Gravity Spatial variations in the strength of the gravitational field of the Earth

Density Fossil fuelsBulk mineral depositsConstruction

Magnetic Spatial variations in the strength of the geomagnetic field

Magnetic susceptibilityand remanence

Fossil fuelsMetalliferous mineral depositsConstruction

Seismic Travel times of reflected/refractedseismic waves

Seismic velocity (and density) Fossil fuelsBulk mineral depositsConstruction

Electromagnetic(SeaBed Logging)

Response to electromagnetic radiation

Electric conductivity/resistivityand inductance

Fossil fuelsMetalliferous mineral deposits

Electrical-Resistivity-Self potential

Earth resistanceElectrical potentials

Electrical conductivityElectrical conductivity

Widely used

Radar Travel times of reflected radar pulses

Dielectric constant EnvironmentalConstruction

Page 6: Field course and methodology in geology and geophysics

Further reading

• Keary, P. & Brooks, M. (1991) An Introduction to Geophysical Exploration. Blackwell Scientific Publications.

• Mussett, A.E. & Khan, M. (2000) Looking into the Earth – An Introduction to Geological Geophysics. Cambridge University Press.

http://www.learninggeoscience.net/modules.php

Page 7: Field course and methodology in geology and geophysics

Gravity

• Gravity surveying measures spatial variations in the Earth’s gravitational field caused by differences in the density of sub-surface rocks

• In fact, it measures the variation in the accelaration due to gravity

• It is expressed in so called gravity anomalies (in milligal, 10-5 ms-2), measured in respect to a reference level, usually the geoid

• Gravity is a scalar

Page 8: Field course and methodology in geology and geophysics

Gravity: Newton’s Law of Gravitation

• Newton’s Universal Law of Gravitation for small masses, m1 and m2 separated by a distance r, at the earth surface:

– With G (’big gee’) is the Universal Gravitational Constant: 6.67x10-11 m3/kg1·s2

2

21

r

mmGF,forceAttractive

m1 m2

rforce force

Page 9: Field course and methodology in geology and geophysics

Gravity: Earth

2

E

E

s2

E

sE

E R

MGggm

R

mMGF

• Spherical• Non-rotating• Homogeneous g (’little gee’) is constant!

Page 10: Field course and methodology in geology and geophysics

Gravity

• Non-spherical Ellipse of rotation• Rotating Centrifugal forces• Non-homogeneous

– Subsurface heterogeneities– Lateral density differences in the Earth

g (’little gee’) is NOT constant

Page 11: Field course and methodology in geology and geophysics

Gravity units

• An object dropped at C falls with a little greater acceleration than at P

• Difference in acceleration can be measured:

• Here: dg = 1.048·10-6 m/s2

• Small values, therefore we measure gravity anomalies in milliGals (mGal), or gravity units, g.u.

• 1 mGal = 10 g.u. = 10-5 m/s2 ~ 10-6·g

d =

100

m

r = 50m

C P

= 0.3 kg/m3

3

22r

3

4

d

G

d

mGg

Page 12: Field course and methodology in geology and geophysics

Gravity anomalies

The Gravity anomaly is positive if the body is more dense than its surroundings, negative if less

Gravity is a scalar: the combined pull has approx. The

same direction as the Earth pull; we measure therefore

only the size, or magnitude, of g

Page 13: Field course and methodology in geology and geophysics

Gravity anomalies of specific bodies

Page 14: Field course and methodology in geology and geophysics

Gravity anomalies of specific bodies

Page 15: Field course and methodology in geology and geophysics

Measurements of Gravity

• Spring or Beam

• Corrections– Instrumental drift– Latitude (due to Earth

rotation)– Elevation

• Free-air correction• Bouguer correction• Terrain correction

– Tidal– Eötvös (due to

measurements on moving vehicles)

mm

m·g m·(g+g)

extension

Page 16: Field course and methodology in geology and geophysics

NGU, 1992

Page 17: Field course and methodology in geology and geophysics

Magnetics

• Magnetic surveying aims to investigate the subsurface geology by measuring the strength or intensity of the Earth’s magnetic field.

• Lateral variation in magnetic susceptibility and remanence give rise to spatial variations in the magnetic field

• It is expressed in so called magnetic anomalies, i.e. deviations from the Earth’s magnetic field.

• The unit of measurement is the tesla (T) which is volts·s·m-2 In magnetic surveying the nanotesla is used (1nT = 10-9 T)

• The magnetic field is a vector• Natural magnetic elements: iron, cobalt, nickel, gadolinium• Ferromagnetic minerals: magnetite, ilmenite, hematite,

pyrrhotite

Page 18: Field course and methodology in geology and geophysics
Page 19: Field course and methodology in geology and geophysics
Page 20: Field course and methodology in geology and geophysics
Page 21: Field course and methodology in geology and geophysics
Page 22: Field course and methodology in geology and geophysics
Page 23: Field course and methodology in geology and geophysics
Page 24: Field course and methodology in geology and geophysics
Page 25: Field course and methodology in geology and geophysics

NGU, 1992

Page 26: Field course and methodology in geology and geophysics

Electromagnetics

Electromagnetic methods use the response of the ground to the propagation of incident alternating electromagnetic waves, made up of two orthogonal vector components, an electrical intensity (E) and a magnetizing force (H) in a plane perpendicular to the direction of travel

Page 27: Field course and methodology in geology and geophysics

Electromagnetics

Transmitter Receiver

Primary field Secondary field

Conductor

Primary field

Electromagnetic anomaly = Primary Field – Secondary Field

Page 28: Field course and methodology in geology and geophysics

Electromagnetics – Sea Bed Logging

SBL is a marine electromagnetic method that has the ability to map the subsurface resistivity remotely from the seafloor.The basis of SBL is the use of a mobile horizontal electric dipole (HED) source transmitting a low frequency electromagnetic signal and an array of seafloor electric field receivers. A hydrocarbon filled reservoir will typically have high resistivity compared with shale and a water filled reservoirs.SBL therefore has the unique potential of distinguishing between a hydrocarbon filled and a water filled reservoir

Page 29: Field course and methodology in geology and geophysics

Reflection Seismology

• Principle of reflection seismology– What is reflection seismology– Seismic wave propagation– Acquisition – collecting seismic data– Prosessing

• Limitations and Pitfalls– Resolution (Horizontal and Vertical)– Velocity Effects (Seismic velocities – Depth

Conversion– Geometrical Effects (Migration)– Seismic Modelling (Synthetic seismograms)

• 2D vs. 3D seismic reflection

Page 30: Field course and methodology in geology and geophysics

Reflection Seismology

Page 31: Field course and methodology in geology and geophysics

Reflection Seismology

Page 32: Field course and methodology in geology and geophysics

Reflection Seismology

Page 33: Field course and methodology in geology and geophysics

Reflection Seismology

• Spherical spreading• Absorption• Transmission/conversion

Page 34: Field course and methodology in geology and geophysics

Reflection Seismology

12

12

1122

1122

ZZ

ZZ

vv

vvR

Incident rayAmplitude: A0

Reflected rayAmplitude: A1

Transmitted rayAmplitude: A2

1, v1

2, v2

2, v2 1, v1

Acoustic Impedance: Z = ·v

Reflection Coefficient: R = A1/A0

R = 0 All incident energy transmitted (Z1=Z2) no reflectionR = -1 or +1 All incident energy reflected strong reflectionR < 0 Phase change (180°) in reflected wave

Layer 1

Layer 2Transmission Coefficient: T = A2/A0

1122

112

vv

vT

-1 ≤ R ≤ 1

Page 35: Field course and methodology in geology and geophysics

Reflection Seismology

Page 36: Field course and methodology in geology and geophysics

Reflection Seismology

Page 37: Field course and methodology in geology and geophysics

Reflection Seismology

Page 38: Field course and methodology in geology and geophysics
Page 39: Field course and methodology in geology and geophysics
Page 40: Field course and methodology in geology and geophysics

Reflection Seismology

• Shotpoint interval 60 seconds

• 25-120 receivers• Sampling rate 4

milliseconds• Normal seismic line

ca. 8 sTWT

Page 41: Field course and methodology in geology and geophysics

Reflection Seismology

Page 42: Field course and methodology in geology and geophysics
Page 43: Field course and methodology in geology and geophysics
Page 44: Field course and methodology in geology and geophysics
Page 45: Field course and methodology in geology and geophysics
Page 46: Field course and methodology in geology and geophysics
Page 47: Field course and methodology in geology and geophysics

Reflection Seismology

• SEISMIC PROSESSING– The objective of seismic prosessing is to

enhance the signal-to-noise ration by means of e.g. filtering

Page 48: Field course and methodology in geology and geophysics

Reflection Seismology

• Limitations and Pitfalls– Interference– Horizontal and Vertical Resolution– Velocity Effects– Geometrical Effects– Multiples

Page 49: Field course and methodology in geology and geophysics

INTERFERENCE

Page 50: Field course and methodology in geology and geophysics

Reflection Seismology

Interference

Page 51: Field course and methodology in geology and geophysics

Reflection SeismologyInterference

Page 52: Field course and methodology in geology and geophysics

VERTICAL RESOLUTION

Page 53: Field course and methodology in geology and geophysics

Reflection Seismology

100 Hz

67 Hz

40 Hz

Wavelength increases with depthFrequency decreases

Reduced vertical resolution

f v z

100 Hz 2 km/s 20 m 5 m ~250 m

40 Hz 4 km/s 100 m 25 m ~2250 m

Page 54: Field course and methodology in geology and geophysics

Reflection Seismology

(Brown 1999)

Page 55: Field course and methodology in geology and geophysics

Reflection Seismology

(Brown 1999)

Page 56: Field course and methodology in geology and geophysics

Reflection Seismology

Page 57: Field course and methodology in geology and geophysics

HORIZONTAL RESOLUTION

Page 58: Field course and methodology in geology and geophysics

Reflection Seismology

Page 59: Field course and methodology in geology and geophysics

Reflection Seismology

~25 m

~690 m

~2500 m

Page 60: Field course and methodology in geology and geophysics

Reflection Seismology

Page 61: Field course and methodology in geology and geophysics

Reflection Seismology

Page 62: Field course and methodology in geology and geophysics

GEOMETRICAL EFFECTS

Page 63: Field course and methodology in geology and geophysics

Reflection Seismology

Page 64: Field course and methodology in geology and geophysics

Reflection Seismology

Page 65: Field course and methodology in geology and geophysics
Page 66: Field course and methodology in geology and geophysics
Page 67: Field course and methodology in geology and geophysics
Page 68: Field course and methodology in geology and geophysics
Page 69: Field course and methodology in geology and geophysics

VELOCITY EFFECTS

Page 70: Field course and methodology in geology and geophysics
Page 71: Field course and methodology in geology and geophysics
Page 72: Field course and methodology in geology and geophysics
Page 73: Field course and methodology in geology and geophysics
Page 74: Field course and methodology in geology and geophysics
Page 75: Field course and methodology in geology and geophysics

MULTIPLES

Page 76: Field course and methodology in geology and geophysics
Page 77: Field course and methodology in geology and geophysics
Page 78: Field course and methodology in geology and geophysics
Page 79: Field course and methodology in geology and geophysics

Magnetics

• Magnetic susceptibility

a dimensionless property which in essence is a measure of how susceptible a material is to becoming magnetized

• Sedimentary Rocks– Limestone: 10-25.000– Sandstone: 0-21.000– Shale: 60-18.600

• Igneous Rocks– Granite: 10-65– Peridotite: 95.500-196.000

• Minerals– Quartz: -15– Magnetite: 70.000-2x107

Page 80: Field course and methodology in geology and geophysics

Magnetics

• Induced and remanent magnetization

• Intensity of magnetization, J

• Magnetic anomaly = regional - residual

HJi

JresJr