Y. Geraud et al., CRACK LOCATION IN GRANITIC SAMPLES SUBMITTED TO HEATING, LOW CONFINING PRESSURE AND AXIAL LOADING, Geophysical journal international, 133(3), 1998, pp. 553-567
Until now, observations of mechanically and thermally induced microcra
cks in rocks could only be carried out by indirect measurements or des
tructive observations on samples brought back to atmospheric pressure
conditions. A special triaxial test cell was designed in order to perf
orm direct observations during loading. The use of a cell in tomograph
y apparatus involves new devices: (1) a movable horizontal load frame
around a scanner; and (2) a test cell transparent to X-rays, able to w
ithstand up to 28 MPa maximum confining pressure and temperatures of u
p to 180 degrees C. Volumetric strains are compared with radiological
density measurements. The first processed X-ray images locating microc
racks during propagation are also presented. Mineralogical effects on
the crack location can be demonstrated. Strain inferred from CT densit
y measurement is clearly correlated with the strain usually measured b
y a strain gauge. Different phases of mechanical behaviour are describ
ed: contracted phase and failure by macrocrack formation. The principa
l results obtained with this tool are the description of the porosity
formation and macrocracking. Results show two principal factors locali
zing the porosity. First, the diffused porosity volume is controlled b
y mineralogical parameters, quartz and plagioclase grains, and boundar
ies of biotite grains during the thermal and mechanical loading. Secon
d, macrocracking begins at the perimeter of the central section of cor
e and grows towards the sample/piston interface. It seems that the fir
st macrocracking is not located in the high-porosity zone formed durin
g the loading phase, but in a relatively low-porosity zone.