PDF file - Laboratoire de Géologie de l'Ecole normale supérieure - Ens
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VIGNY ET AL.: GEODETIC MEASUREMENTS MONITOR ASAL RIFT DEFORMATION<br />
smaller than estimated for the 1974 Krafla crisis in<br />
Iceland [Foulger et al.,1992]. The diffusivity measures<br />
the ratio of the length scale to the square root of the<br />
time scale. The time scale is the time between the<br />
rifting episo<strong>de</strong> and the second geo<strong>de</strong>tic survey, i.e. 19<br />
years at Asal and 11 years at Krafla. The length scale<br />
is the distance from the rift axis to the fastest-moving<br />
point, 3 km at Asal, consi<strong>de</strong>rably shorter than the 25<br />
km at Krafla. The diffusivity ratio for Asal with<br />
respect to Krafla is ~1/70, implying that the top elastic<br />
layer (crust ?) is at least an or<strong>de</strong>r of magnitu<strong>de</strong> thinner<br />
beneath Asal and/or that the viscosity of the<br />
un<strong>de</strong>rlying half-space (mantle ?) is at least an or<strong>de</strong>r of<br />
magnitu<strong>de</strong> higher at Asal than at Krafla. Although<br />
these differences are qualitatively consistent with the<br />
tectonic settings of Djibouti and Iceland, their stark<br />
quantitative contrast suggests that the 1-dimensional<br />
analysis oversimplifies the problem somewhat.<br />
In a subsequent paper [Cattin et al., 2005], we<br />
argue that the geometric consi<strong>de</strong>rations (multiple<br />
dipping, non-planar faults) and thermal effects (postrifting<br />
cooling increases viscosity) require a complete<br />
3-dimensional approach, using numerical mo<strong>de</strong>ling.<br />
Such a mo<strong>de</strong>l is required to explain the <strong>de</strong>tails of the<br />
inner rift <strong>de</strong>formation. For example, the geo<strong>de</strong>tic data<br />
suggest that the northern part of the rift zone<br />
accommodates more (some 70%) of the extension than<br />
the southern part.<br />
Consi<strong>de</strong>ring the amount of extension absorbed in<br />
the Asal rift during the 1978 sequence, the high postseismic<br />
velocity, and the present-day velocity, we<br />
infer that the opening rate across the Asal rift will<br />
have to <strong>de</strong>crease significantly before the next such<br />
seismo-volcanic crisis can occur. The <strong>de</strong>formation<br />
recor<strong>de</strong>d by the topography as well as the <strong>de</strong>formation<br />
recor<strong>de</strong>d by the lake Asal Holocene markers, suggest<br />
that the recurrence time of such a crisis is about 120 to<br />
300 yr [Ruegg et al., 1990; Stein et al., 1991;<br />
Manighetti et al., 1998]. However, the ongoing high<br />
rate and the fact that the whole system is being<br />
uplifted is an indication that magma injection still<br />
prevails over extension as the active process driving<br />
the rifting today.<br />
Acknowledgments<br />
We are grateful to many people who occasionally<br />
participated in measurement campaigns: in particular<br />
people from the “Observatoire d’Arta”, and especially<br />
to J.-C. Delmont who was director during the 1991<br />
campaign and participated in 1995 and 1999. The<br />
leveling line was surveyed by A. Coulomb from IGN.<br />
Very special thanks to Moumin in Djibouti. The Afar<br />
geo<strong>de</strong>tic program was sponsored by CNRS/INSU<br />
programs (Tectoscope-Positionnement, IDHYL, IT).<br />
We also appreciate the guidance of Peter Molnar,<br />
whose NSF grant (OCE8916680) boosted the 1991<br />
campaign.<br />
10<br />
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