We present a model for the nucleation and growth of faults in intact b
rittle rocks. The model is based on recent experiments that utilize ac
oustic emission events to monitor faulting processes in Westerly grani
te. In these experiments a fault initiated at one site without signifi
cant preceding damage. The fault propagated in its own plane with a le
ading zone of intense microcracking. We propose here that faults ire g
ranites nucleate and propagate by the interaction of tensile microcrac
ks in the following style. During early loading, tensile microcracking
occurs randomly, with no significant crack interaction and with no re
lation to the location or inclination of the future fault. As the load
reaches the ultimate strength, nucleation initiates when a few tensil
e microcracks interact and enhance the dilation of one another. They c
reate a process zone that is a region with closely spaced microcracks.
In highly loaded rock, the stress field associated with microcrack di
lation forces crack interaction to spread in an unstable manner and re
cursive geometry. Thus the process zone propagates unstably into the i
ntact rock. As the process zone lengthens, its central part yields by
shear and a fault nucleus forms. The fault nucleus grows in the wake o
f the propagating process zone. The stress fields associated with shea
r along the fault further enhance the microcrack dilation in the proce
ss zone. The analysis shows that faults should propagate in their own
plane, making an angle of 20 degrees-30 degrees with the maximum compr
ession axis. This model provides a physical basis for ''internal frict
ion,'' the empirical parameter of the Coulomb criterion.