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sealing properties. In reservoir modelling studies
there are two main activities:
1. Representing fault geometry as accurately
as possible based on the best available seismic
data.
2. Representing the fault flow properties, using
various methods for fault seal analysis.
s 1
a
60°
s 3
s 2
6.7.1.3 Geometry
Estimating fault throw is a key uncertainty, as
seismic image quality tends to deteriorate close
to faults. Fault connections in the 3D network
are a particular issue as fault intersections are
rarely resolved accurately from seismic. It is
therefore typically necessary to edit raw fault
interpretations from seismic to produce a net-
work which is structurally plausible (Fig. 6.46 ).
Judging whether the fault network interpreted
from seismic is indeed plausible and reasonable is
assisted by the knowledge that fault systems - unlike
joint systems - are fractal in nature (Scholz and
Aviles 1986 ; Walsh et al. 1991 ) so fault networks
show size and property distributions which usually
follow a power law. Walsh and Watterson ( 1988 )
showed that for many real fault datasets the length of
a fault, L, is correlated with the maximum displace-
ment on the fault, D, such that D
s 3
b
30°
s 1
s 2
s 2
c
30°
s 3
s 1
Fig. 6.44 Anderson theory of faulting relating faults to
the principal stress directions: ( a ) normal faults, ( b ) thrust
faults, and ( c ) strike-slip faults
L 2 /P (where P is
a rock property factor). A 10 km-long fault would
typically have a maximum displacement of around
100 m. Similar relationships between fault thickness
and displacement have also been established by
Hull ( 1988 )andEvans( 1990 ).
¼
We therefore need to translate structural geolog-
ical features into their flow properties, and this is
not an easy task. Faults often give rise to 'tales of
the unexpected' in reservoir modelling studies
because:
￿ They are relatively narrow features, hard to
sample in well and core data and usually pres-
ent on a sub-seismic scale;
￿ They generally have very low permeability
and high capillary entry pressure;
￿ They are very heterogeneous, both in the
plane of the fault zone and perpendicular to
that plane;
￿ They introduce new layer connections due
to fault offsets.
To have any chance of anticipating the
potential effects of faults on flow behaviour in
a reservoir, we need some appreciation of the
mechanics of faults and the nature of their
6.7.1.4 Sealing Properties
Figure 6.47 shows an example fault where a few
metres of displacement have created a fault with
a thickness of a few centimetres. Also clearly
seen in this example is the drag of a shale layer
along the fault surface creating a baffle or seal
between juxtaposed sandstone layers - the for-
mation of a 'fault gouge' (Yielding et al. 1997 ;
Fisher and Knipe 1998 ).
Empirical data from fault systems has led to a
set of quantitative methods for predicting the
sealing properties of faults. The most widely
used method is the shale gouge ratio, SGR, pro-
posed by Yielding et al. ( 1997 ) who showed that
the cumulative shale bed thickness in a faulted
siliciclastic reservoir sequence could be used to
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