EM
and IP METHODS FOR GEOLOGISTS
This course on electrical and induced polarisation
methods of geophysics is targetted for geologists in industry, and for
geophysicists who need an update in current practice.
The course presenter is Dr Michael Asten (Flagstaff
Geo-Consultants and Monash University). He has presented this popular course thirty times over the last decade, to exploration Companies and university
MSc students on four continents.
Dr Asten was formerly a Principal Geophysicist and
Snr Principal Research Scientist with BHP, who pioneered many innovations
in electrical methods into BHPs mineral exploration practice.
Course Duration: 2 days or 3 days (depending on Client
requirements).
Outline:
The course is a two-day workshop-style course aiming
to introduce geologists/ processors/technicians to current geophysical
exploration methodologies in ground, borehole and airborne electromagnetic
exploration, induced polarization and Controlled-Source Audio-magneto-telluric
(CSAMT) methods. This last method also has significant applications
in basin studies and petroleum exploration.
Issues covered include fixed-loop, moving-loop and
sounding methods for reconnaissance and detail surveys, borehole surveys
for target location and/or definition of geometry, and considerations where
conductive overburden is present. Emphasis is on time-domain EM methods,
but VLF and ground FEM (Max-Min) methods can be included. The course
incorporates ground and airborne (GEOTEM) case histories from vms, sedex,
copper-gold and porphyry-copper prospects, plus examples where electrical
methods have complemented seismic methods in basin studies. Participants
have an opportunity to perform basic interpretations on ground, borehole
and airborne data.
Where available, local exploration geophysicists
contribute case-history material relevant to participants' projects.
All course participants receive a comprehensive Course
Manual. Click here to view Contents.
Michael Asten
Flagstaff GeoConsultants,
ph 61 3 8420 6200 fax 61
3 8420 6299
email michaelasten@flagstaff-geoconsultants.com.au
COURSE CONTENTS
CHAPTER 1.
Introduction to transient EM and induction
Why are we here – a few examples.
Rocks as conductors
-
define resistivity, conductivity, conductance
-
effect of weathering, saline water, clay, metallic minerals,
graphite
-
effect of mineral texture: py vs po/cpy
-
The Electromagnetic spectrum
-
radar RIM TEM Res/IP
-
an elementary EM system and response
-
real and imaginary
-
in-phase and quadrature
-
decay constants
-
Time-domain EM and "smoke rings"
-
induction (vortex) currents
-
channelled (galvanic) currents
CHAPTER 2
Fixed and moving-transmitter loop surveys
Fixed transmitter-loop surveys (FL)
-
roving receiver
-
why z-component
-
profile shapes
-
target pick, interpretation rules
-
coupling diagrams
-
blind spots, pairs of loops
-
typical loop sizes and profile spacing
-
example
-
current channelling example
Moving transmitter surveys (ML)
-
coincident-loop receiver
-
separated loop receiver (why)
-
in-loop receiver
-
profile shapes
-
target pick, interpretation rules
-
example
-
when twin peaks generate; into one peak (the usual!)
Case histories
-
FL – Thalanga, Eloise
-
ML - Mt Bulga, Teutonic Bore
-
Frequency-Domain EM techniques
-
horizontal loop EM systems – Max-Min
-
field set-up
-
presentation of HLEM data
-
HLEM interpretation
CHAPTER 3
WORKSHOP 1
-
ML over conductor
-
pick conductor, design follow-up survey
-
WORKSHOP 2
-
FL follow up over conductor
-
pick conductor
-
site drill hole
CHAPTER 4
-
Effect of conductive overburden on profiles
-
FL vs ML (Time Domain) & HLEM
-
Different EM instruments
-
Sirotem, Protem, Crone, UTEM
-
transmitter power and loop size- comparison
-
Time Domain vs Frequency Domain systems
-
Logistics
-
gridding requirements – FL vs ML
-
cost per station or line km
-
production rate
-
Reconnaissance vs Detail surveys
-
Uniformity of illumination
-
Relative coupling with horizontal and vertical targets
-
Case History – Hellyer (UTEM)
-
Case History – HLEM
-
Discrimination between targets
-
thin/thick
-
shallow/deep
-
mineralogical assemblage
CHAPTER 5
Conductivity – depth images and parasections
TEM on a layered earth
-
apparent conductance
-
apparent conductivity
-
conductance-depth parasection
-
conductivity-depth parasection
-
alternative algorithms available
Application to non-layered earth
CHAPTER 6
Examples of parasections and EM response maps
-
parasections over vertical orebody
-
stripping
-
transforms
-
images
Examples – Eloise, Ernest Henry
CHAPTER 7
Down-hole EM
-
positioning of loops (primary field)
-
elementary profile shapes
-
current elements and EM signatures
-
graphical interpretation procedures
-
intersected plates
Examples - Eloise, Hellyer
WORKSHOP 3
Plot conductor off hole and site new drill hole
WORKSHOP 4
Assess whether follow-up hole intersected best mineralisation
Conductor beyond end of hole
Migration of currents in thick conductor - Hellyer
example
Case histories on
-
plot vertical extent of intersected conductor
-
dip of a conductor
-
strike extent of conductor
-
3 component borehole TEM
Example – Balcooma
Computer demonstration eg. Filament
Graphical interpretation tools
CHAPTER 8
Other borehole EM methods
MMR (magnetometric method)
Anomaly shapes in boreholes
Examples –
Pinnacles Lead MVT, Thalanga VMS, Broken Hill
BHT
RIM (radio imaging method)
borehole to borehole
Eloise eg
CHAPTER 9
Airborne EM
Helicopter AEM– eg Dighem
-
Geometry
-
Anomaly shapes
-
parasections
-
Examples – Bathurst mining camp,
Fixed wing – Geotem, Questem
-
transmitter waveform
-
anomaly signatures
Case histories
Freddy Well, HYC, Flying Doctor, kimberlites
Data integration – mag & conductivity
AEM mapping
-
example Lady Loretta
-
lag effects – example Bushman
-
AEM depth penetration
AEM image enhancement
-
time constants
-
principal components
-
horizontal derivatives
-
discrimination between classes of conductors
CHAPTER 10
Transient EM Surroundings
-
diffusion of EM current in layered earth ("smoke rings")
-
apparent resistivity curves
-
field procedure (in/out of loop readings)
Case histories – HYC, Sydney Basin coal
CHAPTER 11
Induced polarization method,
CSAMT and ISR
Electrode arrays
Pseudo-sections thick and thin conductors
Cause of IP effect
-
frequency and time domain, chargeability and and
phase anomalies
Case histories
Inversions - Century
Introduction to CSAMT and ISR
-
case histories in gold exploration
(Ohui, Temora)
CHAPTER 12
Open discussion
-
What "extra" information should a geologist supply to
a geophysicist to maximize usefulness of geophysical surveys
EM
METHODS FOR GEOLOGISTS / GEOPHYSICISTS
Course Notes for Industry Short Courses
Michael Asten
Flagstaff Geo-Consultants and Monash University
The courses cover air, ground and borehole electromagnetic
methods in exploration geophysics.
Courses for geologists use a descriptive approach,
plus discussion of case histories. Courses for geophysicists draw
on more detailed material in the Manual, plus specialist material as required.
All overhead transparencies and data used in discussions
will be supplied to participants as a set of paper copies. Simple
interpretation exercises are designed to illustrate principles, and can
be accomplished with pencil and graph paper.
Participants should provide colour highlighting pens
(red green blue), a calculator, A4/quarto or metric graph paper, pencil,
ruler, and protractor.
These course notes are copyright © Michael Asten
1999. Reproduction of any part of these notes is not permitted without
permission of the author.
For more details contact:-
Dr. Michael Asten:
Telephone: 61 3 8420 6200
Facsimile: 61 3 8420 6299
Suite 2, 337a Lennox St
Richmond, Victoria, 3121
Australia
PO Box 2236
ALSO AT
Department of Earth Sciences
Monash University
Clayton Vic 3169 Australia
masten@mail.earth.monash.edu.au
The Presenter
Dr Michael Asten is a consulting geophysicist and
Partner with Flagstaff Geo-Consultants in Melbourne, Australia, and
also holds a part-time academic position as Principal Research Fellow at
Monash University. He majored in Physics, Geology and Geophysics
at the University of Tasmania before entering post-graduate study at Macquarie
University in 1972. After excursions into magneto-tellurics and DC
electrical methods he gained a PhD in geophysics on the topic of
using micro-seismic waves as a tool for studying sedimentary basins.
In 1977 he took up a two-year appointment lecturing and coordinating an
MSc (geophysics) programme at Ahmadu Bello University in Nigeria. He then
joined BHP Minerals in 1979 and worked in coal and base-metal exploration
in Australia, East Africa and North America, with particular emphasis on
geophysical research issues. He has been active in EM research for a decade,
initiated the airborne gravity gradiometer project in BHP, and has conducted
numerous short Industry courses on EM Methods at various levels, for Geologists
and Geophysicists on four continents. He is a past Vice-President
of the ASEG, an Associate Editor for the SEG, and was Co-Chairman of the ASEG
Conference 1998.