Me. Belardinelli et al., Redistribution of dynamic stress during coseismic ruptures: Evidence for fault interaction and earthquake triggering, J GEO R-SOL, 104(B7), 1999, pp. 14925-14945
We investigate the spatiotemporal evolution of dynamic stress outside a rup
turing extended fault. The dynamic stress variations caused by a coseismic
rupture in a half space are computed by using the discrete wavenumber and r
eflectivity methods. After a transient phase, the stress time history evolv
es to the final static stress value. We compare the static stress changes r
esulting from this model with those computed from a static dislocation mode
l. We have applied this method to study the interactions between the first
two normal faults which ruptured during the 1980 (M-S 6.9) Irpinia earthqua
ke. These two subevents are separated in time by nearly 20 s, while the thi
rd (and last) subevent occurred 40 s after the rupture onset. We compute th
e dynamic stress changes caused by the rupture of the first subevent. Our m
odeling results show that the dynamic stress peak on the second subevent fa
ult plane is reached between 7 s and 8 s after the rupture initiation on th
e main fault. On the average the static stress level on the second subevent
(20 s) fault plane is reached nearly after 14 s. The dynamic rupture did n
ot jump from a rupturing segment to the adjacent one immediately, but the t
riggering of the 20 s subevent is delayed by roughly 10 s with respect to t
he instant of occurrence of the dynamic stress peak induced by the 0 s even
t. The dynamic stress pulse propagates along the strike direction of the se
cond subevent fault plane at an average velocity of nearly 3.4 km/s. The de
layed triggering of the second subevent can be interpreted in terms of the
frictional properties of the faults. In particular, rate- and state-depende
nt frictional law can explain a delayed instability after a sudden change i
n stress. Using the estimated values of the subevent triggering delay and t
he shear stress change, we attempt to constrain the parameter A sigma on th
e 20 s fault. The values here inferred agree well with those resulting from
previous studies.