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Fig. 2.22 Seismic
refraction profile SIS-04,
offshore Morocco
(Contrucci et al. 2004 ),
projected onto the direction
of Triassic-Jurassic rifting
( top ). The green line
represents the bathymetric
surface. The bottom panel
shows a plot of the crustal
thickness (excluding
sediments),
H ( x )
b ( x ), along
the margin. The stretched
continental margin as
width L
D
a ( x )
193 km. If we
restore the thickness to
H 0 D
Š
35 km, the width of
the margin is reduced to
L 0
110 km (pre-rift
width). Therefore, the
stretching factor “ is given
by: “ D L / L 0 Š1.75
Š
say a D a ( x )and b D b ( x ), of seaward increas-
ing offsets x along the profile. The example il-
lustrated in Fig. 2.22 shows the seismic pro-
file SIS-04, located offshore Morocco (Contrucci
et al. 2004 ), after projection onto the direction
of Triassic-Jurassic rifting (Schettino and Turco
2009 ). If L is the size of the stretched margin
(for example determined by the COB) and H 0 is
the normal unstretched crustal thickness, then the
pre-rift restored size, L 0 , and the stretching factor,
“, will be given by (Fig. 2.22 ):
LH 0
D L=L 0 D
(2.38)
Z
L
H.x/dx
0
As soon as the stretching factor “ has been
estimated, there are three possibilities for taking
into account thinning of passive margins during
the syn-rift stage in pre-rift reconstructions. In
a first method, the tectonic elements are defined
through their present day stretched boundaries,
but a pre-rift reconstruction will require an over-
lap of the stretched margins, as illustrated in
Fig. 2.23 . This method works well both in the
case of passive margins of oceans and for failed
Z
Z
L
L
1
H 0
1
H 0
L 0 D
Œa.x/ b.x/dx
H.x/dx
0
0
(2.37)
 
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