SEISMIC STRUCTURE OF THE UPPER-MANTLE BENEATH THE SOUTHERN KENYA RIFTFROM WIDE-ANGLE DATA

Citation
Gf. Byrne et al., SEISMIC STRUCTURE OF THE UPPER-MANTLE BENEATH THE SOUTHERN KENYA RIFTFROM WIDE-ANGLE DATA, Tectonophysics, 278(1-4), 1997, pp. 243-260
Citations number
35
Categorie Soggetti
Geochemitry & Geophysics
Journal title
ISSN journal
00401951
Volume
278
Issue
1-4
Year of publication
1997
Pages
243 - 260
Database
ISI
SICI code
0040-1951(1997)278:1-4<243:SSOTUB>2.0.ZU;2-7
Abstract
In February 1994, the Kenya Rift International Seismic Project carried out two wide-angle reflection and refraction seismic profiles between Lake Victoria and Mombasa across southern Kenya. Our investigation of the data has revealed evidence for the presence of two upper mantle r eflectors beneath southwestern Kenya, sometimes at short range, from s even shotpoints. Two-dimensional forward modelling of these reflectors using a pre-existing two-dimensional velocity-depth model for the cru st [Birt, C.S., Maguire, P.H.K., Khan, M.A., Thybo, H., Keller, G.R., Patel, J., 1997. The influence of pre-existing structures on the evolu tion of the Southern Kenya Rift Valley - evidence from seismic and gra vity studies. Tectonophysics 278, 211-242], has shown them to lie at d epths of approximately 51 and 63 km. The upper reflector, denoted d(1) , shallows by about 5-10 km in the area beneath Lake Magadi, situated in the rift itself. Correlations for the deeper reflector, denoted d(2 ), are sparse and more difficult to determine, so it was not possible to define any shallowing corresponding to the surface expression of th e rift. Only limited control exists over the upper mantle velocities u sed in the modelling. Immediately beneath the Moho we use a value of P -n calculated from the crustal model, and constraints from previous re fraction, teleseismic and gravity studies, to determine the velocity a t depth. At the d(1) reflector a reasonable velocity contrast was intr oduced to produce a reflector for modelling purposes. Beneath the d(1) reflector the velocity decreases to the average value over 3 km. Bene ath the rift the velocity also rises across d(1) and again, decreases to the average value over the next 3 km. At the d(2) reflector a simil ar model is used. This model accounts for the presence of the mantle r eflectors seen in the data by using layers of thin higher velocity in a lower background velocity. Due to the uncertainty in the velocities the absolute position of both d(1) and d(2) could vary, but the relati ve upwelling beneath the rift is reasonably well constrained and data from four different shotpoints which indicate the shallowing show good agreement. A significant result of this study is that the continuity of the d(1) reflector indicates that the sub-Moho lithosphere has not been substantially disrupted by mantle upwelling, even though probably thinned and stretched.