2.6 Interpretation of gravity surveys - The Berkeley Course in ...
2.6 Interpretation of gravity surveys - The Berkeley Course in ...
2.6 Interpretation of gravity surveys - The Berkeley Course in ...
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from which the anomalies <strong>of</strong> adjacent bodies or structures have beensubtracted.<strong>The</strong> equivalent stratumA fundamental statement <strong>of</strong> non-uniqueness for <strong>gravity</strong> data is that anyobserved <strong>gravity</strong> field on the surface <strong>of</strong> the earth can be represented exactlyby a surface distribution <strong>of</strong> density given by the follow<strong>in</strong>g simple formula:g z (x, y) = 2π G σ (x, y)where σ(x, y) is a ‘surface density’ with the dimension gm cm -2 . Of coursethis is a mathematical relation that implies the existence <strong>of</strong> arbitrary, nonphysical,densities but the implications are obvious. A similar formula can bederived for a physical layer <strong>in</strong> which a lateral variation <strong>of</strong> volume density canrepresent the observed <strong>gravity</strong>. This is a sober<strong>in</strong>g statement about the validity<strong>of</strong> any <strong>gravity</strong> <strong>in</strong>terpretation and it illustrates better than any other model theimportance <strong>of</strong> a sound geological model <strong>in</strong> any <strong>in</strong>terpretation.<strong>The</strong> relative scales <strong>of</strong> <strong>gravity</strong> anomaliesIt is observed <strong>in</strong> field data that there is a roughly l<strong>in</strong>ear relationshipbetween the magnitude <strong>of</strong> an anomaly and its spatial extent or scale. <strong>The</strong>crust <strong>of</strong> the Earth is very <strong>in</strong>homogeneous and there are large-scale variationson the order <strong>of</strong> 100 mgals with scale lengths on the order <strong>of</strong> 100 km. Small2