There are currently contrasting views
on the way strain is distributed within the lithosphere during rifting and the
formation of passive continental margins, with direct implications for the subsidence
and heat flow histories of the overlying sedimentary basins, and potentially
also for the timing and degree of source rock maturity in these systems.
According to some authors, the
asymmetry observed between most conjugate margin pairs (e.g. West
Iberia-Newfoundland, East Coast USA-NW Africa, NE Brazil-West Africa and the
Southern Australia-Antarctica) results from the activity of low-angle normal
faults (detachments), which shift the region of pervasive upper crustal
thinning and normal faulting (lower plate) from that of intense lower crust and
mantle lithosphere thinning (upper plate; see Rosenbaum et al., 2008 and
references therein). A paradoxical
observation, nevertheless, is that in most margins the extension measured from
normal fault throws appears to be much smaller than that inferred from
subsidence and gravity modelling, thus implying
ubiquitous upper-plate rift margin settings (the “Upper Plate Paradox”;
Driscoll & Karner, 1998; Davis & Kusznir, 2004).
Pervasive depth-dependent
stretching (DDS) is also implied in dynamic models of rifting to explain
features such as the deposition of salt over extremely thinned crust (e.g. off
western Angola) and the exhumation of continental mantle prior to breakup in
magma-poor margins (e.g. the West Iberia Margin; Lavier & Manatschal, 2006;
Huismans & Beaumont, 2011). In contrast, results from a recently published
kinematic rift model suggest that the crustal structure and subsidence along most passive continental margins
can be explained assuming an essentially depth-uniform strain distribution
through time (Crosby et al., 2011). Alternative models have also been put
forward to explain the apparent deficit of extension in the brittle upper
crust, namely by Reston (2005) and Ranero & Perez-Gussinyé (2010), who argue that the amount of extension accommodated
in normal faults may have been largely underestimated in earlier
studies.
The figures below illustrate the
results from two simple experiments in actively explored rift settings: (Figure
1) the North Sea; and (Figure 2) the Angola passive continental margin. The
pseudo wells were built from published seismic data and assume a simplified
stratigraphy, where the thin black layers correspond to the location of two
hypothetical source rocks in each setting. For simplicity all models assume a
constant temperature at the base lithosphere of 13300C, and the
source rocks use a Type II, marine shale kerogen facies, with an initial TOC of
5% wt and HI of 500 mg/g TOC. The impact of varying the rift model assumptions
is then evaluated in terms of the SR’s maturity.
The North Sea comprises a series of rift basins that formed over a
sequence of extensional pulses between the Permian-Triassic and Early
Cretaceous, interspersed with periods of thermal quiescence, volcanic activity
and doming (Ziegler and Cloetingh, 2003). The Pseudo-well in this experiment
was built from a NW-SE seismic constrained transect redrawn from Bell et al.
(2014), at a location where the inferred total stretching factor (β) is 2; i.e.
the crust, or the whole lithosphere, have been stretched to half their initial
thickness during rifting (if the rift is assumed instantaneous; McKenzie, 1978).
For the purposes of the experiment it is assumed that all extensional
deformation took place during the Late Jurassic (160-150 Ma), except in the
last scenario, where most thinning occurs during an earlier rift stage, in the
Permian (260-250 Ma), in agreement with the published profile (see Bell et al.,
2014 and references therein).
The models show that changing the
amount of lithosphere thinning within a reasonable range (black lines),
imposing significant differential stretching between crust and mantle, has some
impact on the timing/degree of maturity of the deeper, pre-rift SR. This
results from differences in the post-rift thermal structure of the basin combined
with rapid sediment burial. However, a similar effect is obtained by varying
the steady state thickness of the lithosphere by only ±10 km, often beyond realistic
model constraints, and a greater impact is even predicted when distributing the
extensional deformation over several rift events (or varying the duration of
rifting). The maturity of the shallower SR is independent of the rift model, although
some differences are noticed for variations in the thickness of the steady
state lithosphere.
The Angola (deep) passive continental margin formed due to intense stretching
during the Early Cretaceous (mostly Berriasian-Aptian) followed by a transition
period of thick salt deposition (Aptian) and continental break-up (e.g. Teisserenc
& Villemin 1990). The transect shown above is redrawn from Lentini et al.
(2010), based on deep seismic reflection and refraction data. At the location
of the Pseudo-well the present day thickness of the crust is 8 km, measured
between the base of the sediments and the Moho. For the experiment it is
assumed that all extensional deformation took place during the Early Cretaceous
(145-135 Ma) and that the initial crustal thickness is 32 km (i.e. βcrust
= 4).
In the margins, where the lithosphere
stretches to infinity prior to break-up, depth dependent stretching (DDS) may
have a greater impact on the distribution of heat during and following rifting,
and thus in the maturity of SR’s. In the experiment above this is observed when
varying the amount of stretching in the mantle (βmantle) between a
factor of 3 and 4. For higher stretching factors, in this particular setting,
the increase in heat flow converges asymptotically. The models also show,
however, that similar magnitude effects, or even more pronounced, are produced when
varying the thickness of the lithosphere and/or the duration of the rifting
events. As in the case of the North Sea experiment the maturity of the
shallower SR is independent of the rift model.
In summary, the experiments discussed
here show that the implications of assuming conceptually different rift models
for the timing and degree of source rock maturity in these settings may be of
the same order of magnitude, and thus indistinguishable, from those inherent to
the uncertainty in the parameterization of the rift model, such as the
thickness of the underlying lithosphere and the age and duration of the rift
events. Moreover, it is likely that the maturity of most syn- and post-rift
source rocks does not depend significantly on the rift model, but mostly on the
rate of post-rift burial. As good practice, these effects should be tested in
order to identify the key sensitivities of the basin model, at least within a
first order approximation.
References:
Bell, R. E., C.
A.-L. Jackson, P. S. Whipp, and B. Clements (2014), Strain migration during multiphase extension:
Observations from the northern North Sea, Tectonics,
33, doi:10.1002/2014TC003551.
Crosby, A. G., N. J. White, G. R. H. Edwards, M. Thompson, R.
Corfield, and
L. Mackay (2011). Evolution of deep‐water rifted margins: Testing depth‐dependent
extensional models, Tectonics, 30, doi:10.1029/2010TC002687.
Davis, M., and N. Kusznir (2004), Depth-dependent
lithospheric stretching at rifted margins, in
Karner, G. D., Taylor, B., Driscol, N. W., & Kohlstedt, D. L (eds), Rheology
and Deformation of the Lithosphere at Continental Margins, pp 92-137 Columbia University Press.
Driscoll,
N. W., and G.D. Karner (1998), Lower crustal extension across the Northern
Carnarvon Basin, Autralia: Evidence for an eastward dipping detachment, Journal of Geophysical Research, 103,
4975-4992.
Huismans,
R., and C. Beaumont (2011), Depth-dependent extension, two-stage breakup and
cratonic underplating at rifted margins, Nature,
doi:10.1038/nature09988.
Lavier,
L.L., and Manatschal, G. (2006) A
mechanism to thin the continental lithosphere at magma-poor margins, Nature, 440, doi:10.1038/nature04608.
Lentini, M.R., S. I. Fraser, H. S. Sumner and R. J. Davies (2010), Geodynamics of the
central South Atlantic conjugate margins: implications for hydrocarbon
potential, Petroleum Geoscience, 16, 217-229, DOI 10.1144/1354-079309-909.
McKenzie, D (1978), Some remarks on the development of
sedimentary basins. Earth and Planetary
Science Letters, 40, 25-32.
Ranero, C.R. and M. Perez-Gussinyé (2010), Sequential
faulting explains the asymmetry and extension discrepancy of conjugate margins, Nature, doi:10.1038/nature09520.
Reston,
T.J. (2005), Polyphase faulting during the development of the west Galicia
rifted margin, Earth Planetary Science
Letters, 237, 561-576, doi:10.1016/j.epsl.2005.06.019.
Rosenbaum, G., R. F. Weinberg and K. Regenauer-Lieb (2008),
The geodynamics of lithospheric extension, Tectonophysics,
458, 1-8.
Teisserenc, P. and J. Villemin (1990), Sedimentary basin
of Gabon; geology and oil systems, in Divergent/passive Margin Basins, AAPG
Memoir 48, 117–199.
Ziegler P. A. and S. Cloetingh (2003), Dynamic processes
controlling evolution of rifted basins, Earth-Science Reviews , 1-50, doi:10.1016/S0012-8252(03)00041-2.
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