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Airborne Gravity 2010 - Geoscience Australia

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<strong>Airborne</strong> <strong>Gravity</strong> <strong>2010</strong><br />

error on Gzz crosses the geological signal at a wavelength around 0.5 – 1 km showing that for this<br />

model, anomaly wavelengths down to this level can be recovered in grids of the processed data.<br />

PSD [Em]<br />

10 3<br />

10 2<br />

10 1<br />

10 0<br />

10 -1<br />

10 -1<br />

Gzz equiv source error<br />

Gzz signal<br />

Gzz terrain corrected<br />

Figure 5. Gridded data radial wavenumber PSDs.<br />

26<br />

10 0<br />

Inverse wavelength [km -1 ]<br />

To demonstrate how well the linear drift model was able to track the low frequency noise, Figure 6<br />

shows the fit for one of the FTG output channels over 4 survey lines. The noise series was low pass<br />

filtered to 0.01 Hz to show more clearly the low order correlated noise. One can see that the shifts in<br />

bias levels dominate and only small linear trends are apparent along these relatively short survey<br />

lines. Both are well fitted by the drift model solution.<br />

Figure 6. Red: low pass filtered noise data, Blue: linear drift model solution. Four survey lines<br />

shown.<br />

10 1

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