HR: 1340h
AN: P13A-1035 [Abstracts]
TI: Assessment of the Role Played by Neutral Buoyancy on the Failure of Shallow Magma Reservoirs
AU: * Hochman, S
EM: steven.hochman@pomona.edu
AF: Pomona College, Geology Department
185 E. Sixth St, Rm 232, Claremont, CA 91711, United States
AU: Grosfils, E B
EM: egrosfils@pomona.edu
AF: Pomona College, Geology Department
185 E. Sixth St, Rm 232, Claremont, CA 91711, United States
AB:
During its ascent from the depth where it forms, magma often stalls at the horizon of neutral buoyancy (NB), i.e.
the depth at which the magma and immediate surrounding host rock have equal densities. If magma supply rate
and other conditions promote formation of a stable magma reservoir, then subsequent inflation, for instance in
response to periodic injection of magma from below, can cause the reservoir walls to fail in tension, leading to
lateral or vertical intrusion and the possibility of surface eruption.
Constraining the overpressure required to induce failure of an ellipsoidal reservoir, and identifying the location
along the wall where initial rupture occurs, has been the subject of a great deal of previous research. Most
published work (e.g., Parfitt et al., J. Volc. Geotherm. Res., 55, 1993) indicates that the balance of stresses
normal to the reservoir wall, largely determined by depth-dependent variations in magma and host rock density
structure, is the predominant factor controlling the rupture process and location. Recent work, however, points out
that the relative change in the wall-parallel component of the lithostatic stress, measured from the crest to the
base of the reservoir, is far greater in magnitude than the change in normal stress across the wall for the same
depth range (Grosfils, J. Volc. Geotherm. Res., in press). We thus predict that, while magma NB likely dictates
where a reservoir will form, the relative density structures in the reservoir and host rock with depth will have little
effect on either the conditions required to induce failure or the failure location. Using FEM techniques, we test this
hypothesis by examining the failure of magma reservoirs under NB and non-NB conditions. The reservoirs range
in size from 0.2-4 km, in depth from 0.3-20 km, and in magma density from 175(gas)-3500 kg/m3; the host rock is
defined by uniform, two-layer and smoothly varying density structure with depth. Our results demonstrate that the
relative density structure of the magma and host rock contributes only negligibly to the overpressure required to
induce failure and the initial rupture location, i.e. that magma NB is not an important consideration when
evaluating reservoir failure.
DE: 0560 Numerical solutions (4255)
DE: 5480 Volcanism (6063, 8148, 8450)
DE: 6225 Mars
DE: 6295 Venus
DE: 8439 Physics and chemistry of magma bodies
SC: Planetary Sciences [P]
MN: 2007 Fall Meeting