principles and applications of microearthquake networks
principles and applications of microearthquake networks
principles and applications of microearthquake networks
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112 5. Inversion <strong>and</strong> Optimization<br />
number <strong>of</strong> unknowns is infinite. But because geophysical data are limited,<br />
the number <strong>of</strong> observations is finite. In other words, we write a finite<br />
number <strong>of</strong> equations corresponding to our observations, but our unknown<br />
vector x is <strong>of</strong> infinite dimension. In order to obtain a unique answer, the<br />
solution chosen is the one which maximizes or minimizes a subsidiary<br />
integral. In actual practice, we minimize a sum <strong>of</strong> squares to produce a<br />
smooth solution. A typical mathematical formulation may look like<br />
(5.32)<br />
where the top block A represents the underdetermined constraint equations<br />
with the observed data vector b, the vector x contains the unknowns,<br />
<strong>and</strong> the bottom block is a b<strong>and</strong> matrix which specifies that some filtered<br />
version <strong>of</strong>x should vanish. As pointed out by Claerbout (1976, p. 120), the<br />
choice <strong>of</strong> a filter is highly subjective, <strong>and</strong> the solution is <strong>of</strong>ten very sensitive<br />
to the filter chosen. The Backus-Gilbert inversion is intended for<br />
analysis <strong>of</strong> systems in which the unknowns are functions, i.e., they are<br />
infinite-dimensional, as opposed to, say, hypocenter parameters in the<br />
earthquake location problem, which are four-dimensional. For an application<br />
<strong>of</strong> the Backus-Gilbert inversion to travel time data, readers may<br />
refer, for example, to Chou <strong>and</strong> Booker (1979).<br />
5.1.3.<br />
Analysis <strong>of</strong> an Overdetermined System<br />
Most scientists are modest in their data modeling <strong>and</strong> would have more<br />
observations than unknowns in their model. On the surface it may seem<br />
very safe, <strong>and</strong> one should not expect difficulties in obtaining a reasonable<br />
solution for an overdetermined system. However, an overdetermined system<br />
may in fact be underdetermined because some <strong>of</strong> the equations may<br />
be superfluous <strong>and</strong> do not add anything new to the system. For example, if<br />
we use only first P-arrivals to locate an earthquake which is coniiderably<br />
outside a <strong>microearthquake</strong> network, the problem Is underdetermined no<br />
matter how many observations we have. In other words, in many physical<br />
situations we do not have sufficient information to solve our problem<br />
uniquely. Unfortunately, many scientists overlook this difficulty. Therefore,<br />
it is instructive to quote the general principle given by Lanczos<br />
(1961, p. 132) that “a lack <strong>of</strong> information cannot be remedied by any<br />
mathematical trickery. ”<br />
Usually a given overdetermined system is mathematically incompatible,<br />
i.e., some equations are contradictory because <strong>of</strong> errors in the observations.<br />
This means that we cannot make all the components <strong>of</strong> the re-