Opening-mode fractures (joints and veins) in layered sedimentary rocks ofte
n are periodically distributed with spacings linearly related to the thickn
ess of the fractured layer. To better understand this linear relation, we h
ave investigated the stress distribution between two adjacent opening-mode
fractures as a function of the fracture spacing to layer thickness ratio us
ing a three-layer elastic model with a fractured central layer. The results
show that when the fracture spacing to layer thickness ratio changes from
greater than to less than a critical value (approximately 1.0) the normal s
tress acting perpendicular to the fractures changes from tensile to compres
sive. This stress state transition precludes further infilling of fractures
unless there are existing flaws and/or the fractures are driven by an inte
rnal fluid pressure or other mechanisms. Hence, for fractures driven by tec
tonic extension, the critical fracture spacing to layer thickness ratio def
ines a lower limit, which also defines the condition of fracture saturation
. The critical value of the fracture spacing to layer thickness ratio is in
dependent of the average strain of the fractured layer, and it increases wi
th increasing ratio of Young's modulus of the fractured layer to that of th
e neighboring layers. The critical value increases with increasing Poisson'
s ratio of the fractured layer, and with increasing overburden stress (dept
h), but it decreases with increasing Poisson's ratio of the neighboring lay
ers. For representative variation of the elastic constants of the fractured
layer and the neighboring layers, and overburden stress, the critical frac
ture spacing to layer thickness ratio varies between 0.8 and 1.2. This rang
e encompasses the often cited spacing to layer thickness ratios in the lite
rature for well-developed fractures sets. (C) 1999 Elsevier Science Ltd. Al
l rights reserved.