principles and applications of microearthquake networks
principles and applications of microearthquake networks
principles and applications of microearthquake networks
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152<br />
6. Methods <strong>of</strong> Data Analysis<br />
(6.38)<br />
fork = 1, 2, . . . ,rn, j = 1, 2, . . . ,n<br />
Equation (6.38) is a generalization <strong>of</strong> Eq. (6.19) for the simultaneous inversion<br />
problem.<br />
6.3.2. Numerical Solution <strong>of</strong> the Simultaneous Inverswn Problem<br />
In the previous subsection, we have shown that the simultaneous inversion<br />
problem may be formulated in a manner similar to Geiger’s method <strong>of</strong><br />
determining origin time <strong>and</strong> hypocenter. The computations involve the<br />
following steps:<br />
Guess a trial parameter vector t* as given by Eq. (6.25).<br />
Compute the theoretical travel time TJk <strong>and</strong> its spatial partial derivatives<br />
dT,,/dx, dTik/dy, <strong>and</strong> dTj,/t3z evaluated at (x?, yJ, zj”)<br />
for k = 1, 2, . . . , rn <strong>and</strong>j = 1, 2, . . . , n.<br />
Compute matrix B as given by Eqs. (6.31), (6.32), <strong>and</strong> (6.37), <strong>and</strong><br />
compute vector r as given by Eqs. (6.28) <strong>and</strong> (6.26).<br />
Solve the system <strong>of</strong> rnn linear equations as given by Eq. (6.30) for<br />
the adjustment vector 65 with (4n + L) elements. This may be<br />
accomplished via the normal equations approach, or the generalized<br />
inversion approach as discussed in Chapter 5.<br />
Replace the trial parameter vector (* by (e* + St).<br />
Repeat steps 2-5 until some cut<strong>of</strong>f criteria are met. At this point,<br />
we set 5 = 5” as our solution for the hypocenter <strong>and</strong> velocity<br />
parameters .<br />
Although numerical solution for the simultaneous inversion is computationally<br />
straightforward, the pitfalls discussed in Section 6.1.3 apply here<br />
also. The set <strong>of</strong> mn linear equations to be solved in step 4 can be very<br />
large. Typically a few thous<strong>and</strong> equations <strong>and</strong> several hundred unknowns<br />
are involved. Because <strong>of</strong> the positions <strong>of</strong> the zero elements in matrix B<br />
[Eq. (6.31)], the arrival time residuals <strong>of</strong> one earthquake are coupled to<br />
those <strong>of</strong> another earthquake only through the velocity coefficient matrix C<br />
in Eq. (6.30). Therefore, it is possible to decouple mathematically the<br />
hypocenter parameters from the velocity parameters in the inversion procedure<br />
as shown by Pavlis <strong>and</strong> Booker (1980) <strong>and</strong> Spencer <strong>and</strong> Gubbins<br />
(1980). Consequently, large amounts <strong>of</strong> arrival time data can be used in