INTRODUCTION
There are two main reasons for making the separation. One is simply to locate or highlight anomalous areas. The other is to isolate just the local anomaly in a form suitable for quantitative modeling.
There are many ways to accomplish the separation. There is no best or unique procedure; only ones that are convenient and reasonable in a given context. Here are some common methods.
DO NOTHING METHOD
SMOOTH PROFILING
Smooth contouring is a similar process applied to gravity maps (Bothner, 1974).
SMOOTH PROFILING WITH GEOLOGICAL CONSTRAINTS
A benefit of such a scheme is that only non-anomalous points are used to define the regional field.
DIGITAL FILTERING
Digital filters can be designed to include or exclude any given range of wavelengths of gravity (or period of seismic waves for example). This method is objective in the sense that the procedure is cut-and-dried once the particular filter coefficients (weights) are chosen.
The basic limitation is that sources at any depth have spectra composed of all possible wavelengths. Thus, a perfect spectral separation is not possible.
As we saw in class, digital filtering tends to produce equal positive and negative anomalies. That could be geologically unreasonable in many situations. Filtering can also produce spurious anomalies of no geological significance.
From another point of view, we see that the residual is not entirely "pure" because anomalous local points are used in determination of the regional.
LEAST-SQUARES POLYNOMIALS
The great advantage of polynomials is that the procedure is entirely objective once the degree of polynomial is selected (a very subjective step!). If the degree is too low, the regional will be too simple and will not describe a reasonable regional trend. If the degree is too high, the residual will mainly be random noise and the significant anomaly values taken away as part of the regional.
As with polynomials, the least squares regional values are contaminated by local anomalous points.
Another problem with a very complex regional is it can not correspond to a uniform background density against which to define density contrasts in a model: quantitative modeling becomes impossible.
SUMMARY AND CONCLUSIONS
REFERENCES AND READINGS
Birch, 1970, Deep Sea Research, 17, 847-.
Birch, 1982, Geophysics, 47, 1185-.
Bothner, 1974, Geological Society of America Bulletin, 85, 51-.
Fuller, 1966, in "Mining Geophysics II", Society of Exploration Geophysicists, Tulsa
Gupta and Romani, 1980, Geophysics, 45, 1412-.