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IUGG XXIV General Assembly July 2-13, 2007 Perugia, Italy<br />

(S) - <strong>IASPEI</strong> - International Association of Seismology and Physics of the Earth's<br />

Interior<br />

JSS011 Oral Presentation 2115<br />

Ridge jumps associated with plume-ridge interaction: Weakening of the<br />

lithosphere by upwelling asthenosphere<br />

Mr. Eric Mittelstaedt<br />

Geology and Geophysics University of Hawaii, Manoa <strong>IASPEI</strong><br />

Garrett Ito<br />

Interaction of mantle plumes and young lithosphere near mid-ocean ridges can lead to changes in<br />

spreading geometry by shifts of the ridge-axis toward the plume such as seen at Iceland and the<br />

Galapagos. Previous work has shown that, with a sufficient magma flux, magmatism alone may weaken<br />

the plate sufficiently to initiate a ridge jump, but the contribution of upwelling asthenosphere to plate<br />

weakening and ridge-jumps is poorly understood. Using the FLAC (Fast Lagrangian Analysis of<br />

Continua) algorithm, we solve the equations of continuity, momentum and energy to examine<br />

deformation in near-ridge lithosphere associated with relatively hot upwelling asthenosphere and<br />

seafloor spreading. The cold portion of the lithosphere is treated as an elastic-plastic material and<br />

experiences brittle failure while the lower lithosphere and asthenosphere obey a non-Newtonian viscous<br />

rheology. Combined with a freely deformable surface this allows for simulation of gravitational effects<br />

on topography and dynamic faulting. Using a new 2-D dual-grid method, we achieve better than 0.5 km<br />

resolution within the lithosphere over a domain 100 km wide and 50 km deep and 5 km resolution in<br />

the mantle over a domain 1200 km wide and 400 km deep. The upper region of the box is initially set to<br />

a square-root of age thermal profile while a hot patch is placed at the bottom to initiate a single<br />

asthenospheric upwelling. The effect of upwelling asthenosphere on ridge jumps is evaluated by varying<br />

three parameters; the plume excess temperature, the spreading rate and the lateral location of the hot<br />

patch relative to the ridge axis. Preliminary results show plume related thinning (i.e. weakening) of the<br />

lithosphere over a wide area (100s of kms) with the rate of thinning dependent upon the thermal excess<br />

temperature of the plume. Initially thinning occurs as the plume approaches the lithosphere and<br />

asthenospheric material is forced out of the way. As the plume material comes into contact with the<br />

lithosphere, thinning of the boundary layer occurs through thermal weakening and mechanical removal<br />

of material. Thinning of the lithosphere is one of two primary factors in achieving a ridge jump. The<br />

other is high stresses capable of initiating rifting at this weakened location. Model stresses induced by<br />

the buoyant asthenosphere are significant fractions of the lithospheric yield strength near the plume<br />

and reach a maximum at the center of plume upwelling. The stresses decrease with distance from the<br />

plume center and increase with increasing spreading rate. Ridge jumps induced by upwelling<br />

asthenosphere alone are not observed which suggests that additional effects, such as off-axis<br />

magmatism, are important to ridge jump formation.<br />

Keywords: hotspot, rifting, plume ridge

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