Geoscience Reference
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SISMALP NETWORK
28.03.2006 05:33
Conand aftershocks
CNDSZ
CNDSN
CNDSE
05:34
5
10
15
20
25
Fig. 4
Aftershock doublet felt at Conand (
M
L
= - 0.2 and - 0.7), 25-s time window, 200-Hz
sampling rate. Amplitude window for each component is
ms
−
1
. Note that the maximum
amplitude is here reached on the E-W component, whereas it is observed on the N-S component
for Fig. 3. It indicates either a slight difference in the position of the epicentre or a difference in
source mechanism
±
30
However, a very large uncertainty on magnitude values computed here is brought
by the conversion from
M
0
to
M
L
. Kanamori's (1977) relation does not apply here
because it addresses great earthquakes and involves the so-called moment magni-
tude. (Were it applied, it would provide a 1.3 value for the magnitude of the 10-Feb.
event.) Other empirical relations similar to Bakun's have been proposed, for instance
by Hainzl and Fischer (2002) in their study of an earthquake swarm with magnitudes
between
−
.
0
5 and 3.2:
log
10
M
0
=
1
.
05
M
L
+
11
.
3
.
This relation would provide an
M
L
= - 0.35 value for the 10-Feb. event, still smaller
than the 0.75 value computed with Bakun's relation. This conversion problem set
aside, it seems anyway rather clear that the two 28-Mar. events had very small, most
probably negative magnitudes.
4 The Upthrow of Rocks
Documented observations of upthrown rocks and boulders are relatively scarce.
They include the
M
= 6.9 1984 Western Nagano, Japan, earthquake (Umeda et al.
1987), the
M
= 7.8 1990 Philippine earthquake (Umeda 1992), the
M
= 6.0 1997
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