HR: 0800h
AN: V21D-0630 [Abstracts]
TI: Evaluation of Microcracks orientation at Stromboli volcano using a Magnetic Ferrofluid and the Method
of Anisotropy of Magnetic Susceptibility
AU: Lewis, O
EM: olivia.lewis@ucl.ac.uk
AF: University College London, Gower Street, London, ON WC1E 6BT
United Kingdom
AU: * Benson, P M
EM: p.benson@ucl.ac.uk
AF: University College London, Gower Street, London, ON WC1E 6BT
United Kingdom
AU: Vinciguerra, S
EM: vinciguerra@ov.ingv.it
AF: Istituto Nazionale di Geofisica e Vulcanologia, Via Diocleziano 328, Naples, ON 80124
Italy
AU: Meredith, P G
EM: p.meredith@ucl.ac.uk
AF: University College London, Gower Street, London, ON WC1E 6BT
United Kingdom
AB:
Most crustal rocks are anisotropic. In volcanic areas, anisotropy primarily results due to preferred directions of
microcracks as magma cools. This effect is, in turn, enhanced due to local stress fields during deposition. The combined
effects of these processes may thus give rise to a complex anisotropic fabric. Such fabrics can play crucial roles when
enhancing the formation of slip surfaces which can lead to sector collapses of volcanic edifices, as is the case of Stromboli
volcano (Italy) which experienced 4 sector collapses in the past 13ka. However, the rapid analysis of anisotropic microcrack
fabrics (in terms of magnitude and principal direction) remains non-trivial. Current methods range from time consuming
microcrack analysis of thin sections to the preparation of oriented cores for elastic-wave velocity measurement.
To further our understanding of how microcrack fabrics influence the bulk properties of volcanic basalt, we employ a novel
method which rapidly evaluates the 3-D microcrack orientation using technique of Anisotropy of Magnetic Susceptibility (AMS).
First, we determine the rock matrix AMS (mAMS) using standard methods (via a Agico KLY-4 Kappabridge). Samples are then
saturated with a magnetic ferrofluid, filling the microcrack network with a magnetically susceptible suspension of
microscopic (10nm) magnetite particles. The AMS is then re-measured, with the matrix susceptibility values subtracted from
these readings to yield the average 3-D pore space shape, size and orientation (pAMS).
We describe the use of this method using basalt from Stromboli and comparing to a granite (Takidani) from the Japanese Alps
in order to verify the technique and to investigate the relationship between the basalt microcrack geometry and field scale
observation. For Takidani granite we find the structural anisotropy formed by the void space, as measured by pAMS, is well
described by elastic wave velocity measurement; exhibiting anisotropy values of 19.1% and 7.6% for P-waves and S-waves
respectively. Stromboli basalt possesses a weaker anisotropy of 4.7% and 3.0% (P-wave and S-wave velocity). We relate our
pore space AMS measurements to the layering observed in Stromboli basalt on the flanks of the volcanic edifice; and infer
that the microcrack network is both formed by this deposition and active tectonics as well as providing a key control on its
physical properties. Such data has crucial significance upon the accurate assessment of flank stability, with consequences to
hazard assessment for the surrounding area.
DE: 5109 Magnetic and electrical properties (0925)
DE: 5112 Microstructure
DE: 5194 Instruments and techniques
DE: 8494 Instruments and techniques
SC: Volcanology, Geochemistry, Petrology [V]
MN: Fall Meeting 2005