29.03.2013 Views

IN WESTERN AUSTRALIA - Department of Mines and Petroleum

IN WESTERN AUSTRALIA - Department of Mines and Petroleum

IN WESTERN AUSTRALIA - Department of Mines and Petroleum

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

24<br />

PWA April Edition - Magnetotelluric Surveys<br />

Peter Kirk, <strong>Petroleum</strong> Geophysicist<br />

Peter Kirk Geophysical Consultancy Pty Ltd<br />

Of all the geophysical techniques used in<br />

petroleum exploration in Australia over the last 50<br />

years or more, the magnetotelluric or MT method<br />

has been used the least frequently <strong>and</strong> is probably<br />

the least familiar method to explorationists. There<br />

have, in fact, been five MT surveys conducted in<br />

WA, one conventional MT survey <strong>and</strong> four audio<br />

frequency MT (AMT) surveys, all <strong>of</strong> which have<br />

been conducted onshore.<br />

Although to date the technique has not resulted in<br />

any major discoveries, it has produced some<br />

interesting results <strong>and</strong> in the case <strong>of</strong> one survey it<br />

accurately predicted the results <strong>of</strong> two<br />

unsuccessful wells. It deserves to be used more<br />

frequently, particularly in areas where the seismic<br />

technique has significant problems (mainly due to<br />

shallow limestone) or where seismic acquisition is<br />

restricted due to environmental problems.<br />

The Magnetotelluric Method<br />

Magnetotellurics (MT) is a division <strong>of</strong> geophysics<br />

which studies the earth’s naturally occurring<br />

electromagnetic field <strong>and</strong> the telluric (from the<br />

Greek Tellus meaning earth) currents caused by<br />

fluctuations therein. Many researchers say that this<br />

source is “many orders <strong>of</strong> magnitude greater than<br />

the strengths <strong>of</strong> fields that can be generated with<br />

man-made sources on the surface <strong>of</strong> the earth”.<br />

The primary energy source is naturally occurring<br />

electromagnetic waves that are confined to the<br />

space between the ionosphere <strong>and</strong> the earth’s<br />

surface, these circumnavigate the globe <strong>and</strong> are<br />

consequently known as ‘spherics’. The frequencies<br />

<strong>of</strong> these waves cover a spectrum from 10 -3 Hz to<br />

10 4 Hz (about 22 octaves). The low to mid<br />

frequencies are caused by the interaction <strong>of</strong> the<br />

natural solar wind with the earth’s magnetic field,<br />

whilst the higher frequencies are generally<br />

Magnetotelluric Surveys for <strong>Petroleum</strong><br />

Exploration in Western Australia<br />

attributed to distant lightning strikes. Nearby<br />

lightning strikes, powerful man-made transmitters<br />

<strong>and</strong> highly irregular solar activity due to solar flares<br />

all produce levels <strong>of</strong> unwanted noise that prevent the<br />

recording <strong>of</strong> useful signal <strong>and</strong> also introduce<br />

spurious ‘static’ delays or depth shifts. Constant<br />

monitoring <strong>of</strong> sunspot activity or ‘space weather’ is<br />

necessary but this is greatly facilitated by the<br />

availability <strong>of</strong> reliable online data compiled by solar<br />

observatories, including the one at Learmonth in WA.<br />

Since the bulk <strong>of</strong> the useful energy is generated by<br />

the interaction with the solar wind, it is normally only<br />

possible to record during daylight hours.<br />

The primary energy source induces telluric currents<br />

just below the earth’s surface in large sheets,<br />

preferentially through conducting layers such as<br />

brine filled sedimentary rocks <strong>and</strong> certain mineral<br />

deposits. These currents flow more slowly through<br />

resistive layers such as dense limestone, volcanics<br />

such as basalt, tight non-porous rocks <strong>and</strong><br />

evaporites including salt (although salt in solution is<br />

highly conductive, solid salt is highly resistive). The<br />

currents can be readily measured as a result <strong>of</strong> the<br />

horizontal potential gradients <strong>and</strong> the horizontal <strong>and</strong><br />

vertical magnetic gradients that they produce at the<br />

surface. A modern recording instrument normally<br />

incorporates two electrical antennae horizontally at<br />

right angles <strong>and</strong> three magnetic coiled antennae<br />

horizontally <strong>and</strong> vertically at right angles. These<br />

signals may be recorded separately or the magnetic<br />

<strong>and</strong> electrical signal may be combined <strong>and</strong> recorded<br />

in stereo on digital magnetic tape. A high sampling<br />

rate is required for the higher frequency<br />

components <strong>and</strong> this is provided by modern DAT<br />

recorders, principally used by the music industry.<br />

The depth <strong>of</strong> penetration <strong>of</strong> the induced currents<br />

within the earth depends upon the frequency <strong>of</strong> the<br />

primary source with lower frequencies necessary to<br />

induce currents at greater depths. In order to<br />

measure currents kilometres below the surface, we<br />

need frequencies with periods <strong>of</strong> several minutes.<br />

Typically the length <strong>of</strong> each individual recording is<br />

20 minutes for petroleum exploration. The digitally<br />

recorded signals, which contain information for all<br />

depths, are demodulated by analogue or digital<br />

computer to final form for analysis. The recorded<br />

signal contains frequency-phase vs. amplitude<br />

information relating to the incoming field at the<br />

surface, the decaying earth carrier field, <strong>and</strong> the<br />

modulation resulting from the earth’s resistivity<br />

reflection coefficients. The former two fields are<br />

extracted using least square methods. Only the<br />

earth’s resistivity pr<strong>of</strong>ile remains as a function <strong>of</strong><br />

frequencies. The depth <strong>of</strong> investigation is a result <strong>of</strong><br />

the frequency <strong>of</strong> the data <strong>and</strong> the resistivity, <strong>and</strong> this<br />

is approximately described by the well known ‘skin<br />

depth equation’ - skin depth (m) = 500 p/f.<br />

Simplification <strong>of</strong> the “skin depth” equation is used to<br />

convert the pr<strong>of</strong>iles to depth. The result <strong>of</strong> this<br />

process is a series <strong>of</strong> electric <strong>and</strong> magnetic<br />

reflection coefficients. These are then combined to<br />

form the apparent resistivity series defined by<br />

Z = E/H as a function <strong>of</strong> depth. In addition phase<br />

values with depth are also obtained. The depths<br />

derived from the skin depth equation can then be<br />

corrected at a calibration well within the survey<br />

area. However, changes in the overburden<br />

composition, irregular variations in the earth’s<br />

magnetic field <strong>and</strong> accelerated solar activity can<br />

affect the depth accuracy. This can occur from dayto-day<br />

or from one survey area to another. These<br />

inaccuracies can be reduced by recording at a<br />

known calibration point at least every day <strong>and</strong><br />

sometimes continuously throughout the day.<br />

Sophisticated inversion algorithms can also be used<br />

to produce 2D <strong>and</strong> even 3D plots <strong>of</strong> apparent<br />

resistivity using all 5 recorded signals at each

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!