Ar. Zang et al., Source analysis of acoustic emissions in Aue granite cores under symmetricand asymmetric compressive loads, GEOPHYS J I, 135(3), 1998, pp. 1113-1130
The effect of stress anisotropy on the brittle failure of granite is invest
igated under uniaxial compression. Non-standard asymmetric compression test
s are performed on cores of Aue granite (diameter 52 mm, length 100 mm), in
which 20 per cent of the core top surface remains unloaded. The edge of th
e asymmetric steel loading plate acts as a stress concentrator, from where
a shear rupture is initiated. The propagation of the fracture-related proce
ss zone from top to bottom of the core is mapped by microcrack-induced acou
stic emissions. Compared to standard uniaxial tests with symmetric loading,
in the asymmetric tests both a greater quantity and more localized distrib
utions of emission event hypocentres are observed. The maximum event densit
y doubles for asymmetric (20 events per 10(-6) m(3)) compared to symmetric
tests. The cluster correlation coefficient, a measure of strain localizatio
n in the faulting process, reaches 0.15 for symmetric and 0.30 for asymmetr
ic tests. The clustering of events, however, is found post-failure only. Th
ree different amplitudes are used to determine b-values discussed as a poss
ible failure precursor. Focal amplitudes determined at a 10 mm source dista
nce and maximum amplitudes measured at eight piezoceramic sensors lead to b
-values that drop before rock failure. First-pulse amplitudes automatically
picked from emission wavelets show no anomaly. First-motion polarity stati
stics of amplitudes indicate that a shear-crack-type radiation pattern is r
esponsible for 70 per cent of the failure of granite, irrespective of stres
s boundary conditions. For type-S events with an equal percentage of dilata
tional and compressional first motions, focal mechanisms are determined by
fitting measured first-pulse amplitudes to an assumed double-couple radiati
on pattern. While hypocentres of large type-S events align parallel to the
later fracture plane, their fault plane solutions show no coherent pattern.
Spatial views of fracture planes reconstructed from X-ray computed tomogra
ms reveal local small-scale changes in fracture plane orientation. Nodal pl
anes from average fault plane solutions of the microscopic acoustic emissio
n events coincide with the overall orientation of the macroscopic fracture
plane azimuth (strike angle) determined from thin sections and tomograms.