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Airborne Gravity 2010 - Geoscience Australia

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

Figure 3. Inversion starting model<br />

location (green) and inversion data<br />

segment (orange).<br />

Calculated Tensor vs Measured Tensor<br />

180<br />

Figure 4. Solution using joint inversion<br />

of all tensor elements.<br />

At present, the full tensor gravity instruments are large and heavy and are not routinely used for<br />

exploration surveys. It is possible to mathematically calculate a full tensor from a grid of any<br />

component or tensor element. So is it worth persevering with the search for a full tensor instrument<br />

that can be used for exploration?<br />

To investigate this, the vertical component (Gz) along each line was gridded and then used to<br />

calculate the full tensor. It can be seen that the peak response has moved from beside the line to a<br />

position on the line, and that the amplitude of the peak has been reduced (Figure 5 and Figure 6).<br />

Figure 5. Gz gridded from line data<br />

showing peak offset from the source<br />

body (magenta).<br />

Figure 6. East-West line over the anomaly<br />

peak showing directly modelled data in red and<br />

gridded data in blue.

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