Authors: R.H.C. Wong, Y.S.H. Guo, K.T. Chau, Wei Shen Zhu, Shu Cai Li
Abstract: This paper presents the crack growth mechanism from a 3-D surface flaw on gabbro
specimens using strain measurement and acoustic emission (AE) technique. Based on the results of
strain and AE measurement, microcracks initiated inside the rock and extend to the surface of the
specimen. With the observation from the measurements, four types of crack patterns initiate wing
crack, anti-wing crack (opposite direction of wing crack), petal crack and compressive crack. The
strain values of anti-wing cracks are larger 1 to 2 times than that of wing crack. The AE energy
release from anti-wing crack is higher 2.5 times than that of wing crack, while the energy release
form wing crack is the least but the compressive crack is the highest. Thus, the appearance of
initiation and propagation of the anti-wing crack and compressive crack are very actively than that
of the wing crack. The strain and AE measurement is not only to provide a clear concept on the
mechanisms of crack growth form a 3-D surface flaw but also to provide useful knowledge on the
AE property of the crack patterns.
2357
Authors: Y.S.H. Guo, R.H.C. Wong, K.T. Chau, Wei Shen Zhu, Shu Cai Li
Abstract: A number of instability problems in rock engineering projects are caused by crack
propagation. However, crack growth mechanisms from 3-dimentional flaw are not fully understood,
in particular for 3-D flaw case with varied dipping angle. This study focuses on 3-D surface flaw
using real rock specimens containing a flaw with varied inclination angle α from axial loading and
dipping angle γ from specimen surface under uniaxial compression. Acoustic emission technique
was used for tracing the initiation and growth of micro-cracks inside of specimen. It was found that
crack growth process is affected by the dipping angle γ of the 3-D flaw. When dipping angle γ ≠ 90º,
the thickness of rock above the flaw plane is thinner than that of below the flaw plane. As a result,
compressive crack and wing crack initiated easily from the thinner flaw tips. And, the normalized
stress for crack initiation σi /σc, AE events and the AE energy for crack growth decreases with the
dipping angle γ. However, for γ = 90º, the thickness of rock above and below of the flaw tips is the
same, it was observed that anti-wing crack (crack growth direction opposite to wing crack) initiated
first at a certain place away from the flaw tips, then wing crack and compressive crack emerged at
the late stage. For this case, the stress σi /σc, AE events and the AE energy for crack initiation and
propagation are at a high value. Thus, for rock mass contains flaws geometry with small dipping
angle, some problems of crack propagation may be induced easily during excavation.
2353
Authors: Y.S.H. Guo, Wei Shen Zhu, Shu Cai Li, R.H.C. Wong, B. Sin
Abstract: Under extra compressive stress, some phenomena of rock spallings and fractures often
exist on rock mass located in sidewalls of underground house and tunnels. It is the reason that the
crack growth and coalescence initiation from original flaws (or faults) in rock mass. In the previous
studies, many researchers took a flaw as a through flaw (2-dimentional model), but the flaws are not
always through the whole rock mass in fact, most of them are only near the surface of rock mass,
These are so named as surface flaws. They belong to three dimensional (2-D) flaws. Now, the
reports on initiation and growth of 3-D surface flaw are few. So, for the investigation on growth
patterns of 3-D surface flaw, a series of samples containing a surface flaw were carried out using
frozen casting resin material at about -30°C temperatures. The surface flaw was made of a polyester
film was used to model a single closed flaw on rock mass. The experimental results show that the
wrapping wing crack (Mode I) initiated at the ends (or tips) of surface flaw first, and then formed a
kinking zone (mixed crack zone) at a certain place at the middle of surface flaw region. Some petal
cracks (Mode III) and shell-shaped cracks (Mode III) would grow at the middle place of flaw. A big
fin crack (Mixed Mode) also emerged in middle of flaw and grown along loading direction. Finally,
a team of large cracking curved faces deformed inside the resin specimen; the whole specimen
would be splitted off by the initiation and growth of the cracks. The reasons lead to the fracture
patterns of 3-D closed surface flaw were provided with brittle fracture mechanics theory in the
article, preliminarily.
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