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Archaeoseismology and Palaeoseismology in the Alpine ... - Tierra

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Fault system with<strong>in</strong> Central segment is presented by<br />

sequences of shear, extension, <strong>and</strong> thrust structures<br />

compos<strong>in</strong>g zone of left‐lateral strike‐slip, <strong>in</strong> which vertical<br />

offsets could be found fragmentary (Solonenko et al.,<br />

1966). There are contradictory <strong>in</strong>terpretations of vertical<br />

offset character. Amplitude of vertical offset does not<br />

exceed 3.3 m, of horizontal slip – 1 m (Kurush<strong>in</strong> et al.,<br />

2007).<br />

Eastern segment is located at <strong>the</strong> pediment of Udokan<br />

Range <strong>and</strong> is composed by extension structures (grabens).<br />

Observed steep dipp<strong>in</strong>g of <strong>the</strong> fault to <strong>the</strong> North is<br />

evidence of normal fault<strong>in</strong>g (Kurush<strong>in</strong> et al., 2007).<br />

Amplitude of <strong>the</strong> offset varies along <strong>the</strong> fault from 0 to<br />

1.5 m. There are no traces of horizontal slip at this fault<br />

segment (Kurush<strong>in</strong>, 1963; Solonenko et al., 1966).<br />

Total length of def<strong>in</strong>itely proved surface fault<strong>in</strong>g is ca. 20<br />

km. But <strong>in</strong> some publications po<strong>in</strong>ted out that Eastern<br />

segment might be extended for ano<strong>the</strong>r 5 km (e.g.<br />

Solonanko et al., 1985).<br />

Macroseismic <strong>in</strong>formation is summarized <strong>in</strong> Fig. 6, based<br />

on questionnaires collected <strong>in</strong> <strong>the</strong> Institute of <strong>the</strong> Physics<br />

of <strong>the</strong> Earth, RAS <strong>in</strong> 1958 <strong>and</strong> data from (Solonenko et al.,<br />

1958). Though <strong>the</strong> data spatial coverage is unfavourable<br />

for compilation of a reliable isoseismal map (unpopulated<br />

epicentral area <strong>and</strong> eastern part) we can draw a very<br />

large felt area (over 700 km from surface fault<strong>in</strong>g zone).<br />

DISCUSSION<br />

Fig. 6: Isoseismal map of <strong>the</strong> Muya earthquake.<br />

Epicentral <strong>in</strong>tensity (Io) of <strong>the</strong> Muya earthquake can be<br />

assessed based on <strong>the</strong> total length of <strong>the</strong> surface fault<strong>in</strong>g.<br />

Its well‐documented length is 20 km plus 5 km of doubtful<br />

piece. Accord<strong>in</strong>g to <strong>the</strong> ESI2007 scale (Michetti et al.,<br />

2007) epicentral <strong>in</strong>tensity X corresponds to 20‐25 km total<br />

rupture length. Maximum vertical offset is 3.3 m. For<br />

normal fault<strong>in</strong>g this value is also <strong>in</strong> agreement with<br />

<strong>in</strong>tensity X 1 . Therefore, both assessments give consistent<br />

result, which from one h<strong>and</strong> proves existence of<br />

correlation between SRL <strong>and</strong> offset along it, from <strong>the</strong><br />

o<strong>the</strong>r h<strong>and</strong> is evidence of accurate evaluation of Io be<strong>in</strong>g<br />

1 To avoid confusion Roman letters are used for ESI2007 scale<br />

<strong>and</strong> Arabic numbers are for macroseismic <strong>in</strong>tensities<br />

1 st INQUA‐IGCP‐567 International Workshop on Earthquake Archaeology <strong>and</strong> <strong>Palaeoseismology</strong><br />

158<br />

X degrees. Nearest to <strong>the</strong> surface fault<strong>in</strong>g zone localities<br />

are at 50 km distance from it. This large distance can<br />

expla<strong>in</strong> why maximum observed macroseismic <strong>in</strong>tensity is<br />

much lower than Io <strong>and</strong> does not exceed 8 degrees.<br />

Absence of localities <strong>in</strong> <strong>the</strong> epicentral area expla<strong>in</strong>s also<br />

<strong>the</strong> anomalously large size of 7 degree isoseismal<br />

compared to lower value isoseismals: certa<strong>in</strong>ly with<strong>in</strong> <strong>the</strong><br />

isoseismal 7 has to be higher <strong>in</strong>tensities. If for epicentral<br />

<strong>in</strong>tensity assessment of <strong>the</strong> Muya earthquake we<br />

considered only macroseismic effects <strong>in</strong> localities, as it is<br />

suggested by EMS98 (European Macroseismic Scale,<br />

1998), Io would be underestimated at least by two<br />

degrees.<br />

Epicenter <strong>in</strong>strumental location differs more than 100 km<br />

accord<strong>in</strong>g to different seismological agencies <strong>and</strong><br />

publications. Closest locations to <strong>the</strong> surface fault<strong>in</strong>g zone<br />

are solutions by Vvedenskaya <strong>and</strong> Balak<strong>in</strong>a (1960) <strong>and</strong> by<br />

Balak<strong>in</strong>a et al. (1960) (Fig. 5a). But it is very possible that,<br />

deriv<strong>in</strong>g it <strong>the</strong>y used also position of surface fault<strong>in</strong>g,<br />

<strong>the</strong>refore, it is not completely <strong>in</strong>strumental. Hypocentre<br />

depth given by (Kondorskaya <strong>and</strong> Shebal<strong>in</strong>, 1977) is 15<br />

km, by Doser (1991) – 10 km; <strong>the</strong> deepest solution (22<br />

km) gives Balak<strong>in</strong>a et al. (1972). Macroseismic data is<br />

consistent with 20 km depth. First of all, this depth<br />

toge<strong>the</strong>r with M=7.6 is <strong>in</strong> agreement with 700 km of felt<br />

radius. Second, isometric form of isoseismals (Fig. 6) is<br />

characteristic to relatively deep source. Relatively short<br />

surface fault<strong>in</strong>g zone (20‐25 km) also agrees with deeper<br />

source. For comparison, we could mention two<br />

earthquakes with M=7.4: <strong>the</strong> Neftegorsk, 1995, which<br />

accompanied by 46 km of SRL <strong>and</strong> Altai, 2003, ‐ by 70 km<br />

of SRL. Accord<strong>in</strong>g to Wells <strong>and</strong> Coppersmith (1994) 20‐25<br />

km of SRL corresponds to M=6.6, which is 1 unit less, than<br />

<strong>the</strong> magnitude of Muya earthquake. It is clear, that only<br />

small part of <strong>the</strong> rupture <strong>in</strong> <strong>the</strong> source of Muya<br />

earthquake was exposed on surface. Possibly it is<br />

characteristic to <strong>the</strong> regional seismicity. This hypo<strong>the</strong>sis<br />

can expla<strong>in</strong> why <strong>the</strong> reported PSS lengths are < 45 km (see<br />

Fig. 2).<br />

First motion mechanism (Vvedenskaya, Balak<strong>in</strong>a, 1960)<br />

corresponds to normal fault<strong>in</strong>g with left‐lateral strike‐slip<br />

component along a WNW plane, <strong>and</strong> steeply dipp<strong>in</strong>g to<br />

<strong>the</strong> South (Fig. 5a). In general, this solution is consistent<br />

with <strong>the</strong> geometry of surface faults <strong>and</strong> k<strong>in</strong>ematics of<br />

fault<strong>in</strong>g. But body wave‐form <strong>in</strong>version at teleseismic<br />

distances gives different solution (Doser, 1991): three<br />

sub‐events are recognized, each almost pure strike‐slip<br />

with negligible normal fault component. Data quality does<br />

not permit spatial resolution of sub‐events. Solution with<br />

sub‐events is <strong>in</strong> much better accordance with observed<br />

segmentation of surface fault zone, but is <strong>in</strong> contradiction<br />

with <strong>the</strong> fact, that vertical offset everywhere larger than<br />

horizontal slip. A possible reason might be <strong>the</strong> follow<strong>in</strong>g.<br />

Under extension stresses, strike‐slip movement along en<br />

echelon sub‐parallel faults, which are not co‐axial,<br />

requires normal fault<strong>in</strong>g at surface to accommodate shear<br />

deformation. Accord<strong>in</strong>g to this hypo<strong>the</strong>sis, normal fault<br />

component is not representative for <strong>the</strong> source <strong>in</strong> general<br />

<strong>and</strong> its amplitude can be anomalously large, compared to<br />

<strong>the</strong> surface fault length (as it was noted <strong>in</strong> Fig. 2).

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