all that factors
tribution and
e elements of the
at a prime factor
ae resulting fi-
rsecting groups
3 discontinuities
astants of the
a higher or lower
plate's interior.
;ak discontinui-
triangular plate
a two perpendi-
ating a possible
3. The lineaments
were filled with
Lty of which is
in the interior
sis was seconded
(fig. 7).
ae on the trian-
conditions. It
:ed field which
le homogeneous
:he blocks se-
of influence
:h the expected
apression (pri-
rallelism with
relatively stiff
riff blocks have
The degree to
are deflected
:en the block
i in a triangle
Is of influence
:s in homogeneous
: axes of maximum
i lineaments =
l; reflected tra-
ompression,
ks / 2.
ie weak linea-
. The axes of
nside the zones
:nd of the line-
.on correspon-
with the res-
dence of the
Figure 7. Elastic stress fields in a discontinuous body.
A. Photoelastic analysis, only the axes of maximum
compression are shown.
trajectories entering the lineaments is determinative
with respect to the consequences of the refraction :
the axis of minimum compression of normally indicent
trajectories is always parallel to the weak zone, in
side as well as outside of it, and the trajectory may
cross the weak zone freely.
Diminishing the thickness of the lineaments as com
pared to the fixed thickness of the blocks, greatly
enhances the deviatoric field in the former (fig. 6d).
Finally do isotropic points of zero deviatoric
stress which are loci of sudden changes in the direc
tions of the trajectories, appear in two out of the
four corners of the blocks surrounded by weak discon
tinuities. The exact location of the isotropic points
within their corners depends on the boundary condi-'
tions of the loaded plate (fig. 8).
4 DISCUSSION
Accepting the possibility that lineaments are somehow
related to crossing discontinuities within the elastic
crust which are weaker than the more homogeneous crus
tal solids and which strongly influence the trajecto-
rues of the primary stress field, provides possible,
though not unique, clues in understanding the fixed
spatial relationship to lineaments in which many geo
logical structures appear.
The deviatoric field in the weak zones is always
higher than the field in the block interior. The
latter, with high mean stress, is often close to litho
static.
Small increments of stress may bring the interior of
the blocks to dilatation and vertical splitting in the
direction of maximum horizontal compression. These
directions are visualised by stress trajectories which
appear to systematically contour the blocks. The
direction of spreading of the trajectories over the
block depends on the position of the isotropic points
within the block. Figure 8 shows that, depending on
the loading conditions, trajectories and resultant
brittle tensional failure may be deviated from a dia
gonal position in the centre, towards a less inclined
Figure 7. Elastic stress fields in a discontinuous body.
B. FEM-analysis, axes of maximum and minimum compres
sion.
position with respect to the weak zones in the vicini
ty of the latter. This result of the investigation may
explain the systematicity in the directions of geolo
gical structures and their relation to confining line
aments as weak zones which was discussed in 2.1. It is
quite clear that the above discussion is limited in
time to the first phases of rift formation. True ex-
tensional rifting will be accomodated by only l.Out of
all possible sets of transverse structures which even
tually evolved into a transform fault.
The weak zones proper, here modelled as an elastic
medium, might in fact conform better with true elastic-
plastic bodies or contain a visco-elastic element. A
strong deviatoric field in thege zones, which is ab
sent from the interior of the blocks, may eventually
lead to permanent strain, shortening and uplift. The
compression from within the lineaments onto the rhom
bic blocks finally thickens the edges of the blocks.
Stresses resulting from the consequential bending of
the homogeneous rhombic block will then substitute the
stresses emanating from the boundary forces. The block
.interior fails by vertical rupturing or is bent into