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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

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