A flexural-cantilever simple-shear/pure-shear model of continental lithosphere extension: applications to the Jeanne d’Arc Basin, Grand Banks and Viking Graben, North Sea

Abstract Mathematical models have been constructed of the geometric, thermal and flexural-isostatic response of the lithosphere to extension by faulting (simple-shear) in the upper crust and plastic, distributed deformation (pure-shear) in the lower crust and mantle. Models involving upper-crustal extension by both listric and planar faults have been developed. These coupled simple-shear/pure-shear models have been used to calculate extensional sedimentary basin geometry, subsidence history and crustal structure. Basin geometry and subsidence history are controlled by fault geometry (planar or listric), the amount of fault extension, fault dip, the depth of the transition from simple-shear to pure-shear, and the flexural rigidity of the lithosphere during both syn-rift and post-rift stages of basin formation. For the planar fault model, footwall and hangingwall blocks are considered to behave as two interacting flexural cantilevers; the response of these cantilevers to the isostatic forces produced by extension generating footwall uplift and hangingwall collapse. For a set of adjacent planar faults the lateral superposition of flexural footwall uplift and hangingwall collapse generates the familiar ‘domino’-style block-rotation of such multiple fault systems. The listric fault model assumes that the hangingwall collapses onto a rigid footwall by vertical shear, and that the tectonic denudation of the upper crust by faulting generates isostatic uplift producing limited footwall uplift. Deep seismic reflection data and earth-quake seismology suggest that the fundamental basement faults controlling lithosphere extension are planar. It is argued that the vertical shear construction of hangingwall collapse onto a rigid footwall is inappropriate for basement response. The coupled simple-shear/pure-shear models of extensional basin formation, using both listric and planar fault geometries, have been applied to the formation of the Jeanne d’Arc basin, Grand Banks, and the Viking Graben of the northern North Sea. The numerical modelling shows that the crustal thinning, thermal and sediment-fill loads generated during and after lithosphere extension need to be distributed flexurally in order to generate the observed basin depth and geometry. The flexural-cantilever, planar-fault model provides closer agreement to observed basin depth and subsidence than the listric-fault model. The planar fault model also produces more footwall uplift than a listric fault model. Erosion of this footwall uplift generates substantial isostatic uplift through unloading, leading to a large underestimate of the horizontal displacement on basin-bounding faults. The low values of effective elastic thickness obtained by extensional basin modelling are substantially less than the thickness of the cool, brittle upper crust. It is suggested that flexural bending stresses associated with lithosphere extension on planar faults are sufficiently large to generate brittle failure within the upper crust, so producing the low values of effective elastic thickness. This is consistent with the predictions of the flexural-cantilever model.

[1]  N. Kusznir,et al.  Intraplate lithosphere deformation and the strength of the lithosphere , 1984 .

[2]  B. Wernicke,et al.  Uniform-sense normal simple shear of the continental lithosphere , 1985 .

[3]  J. Jackson,et al.  The geometrical evolution of normal fault systems , 1983 .

[4]  W. R. Buck,et al.  Flexural rotation of normal faults , 1988 .

[5]  N. Kusznir,et al.  The extensional strength of the continental lithosphere: its dependence on geothermal gradient, and crustal composition and thickness , 1987, Geological Society, London, Special Publications.

[6]  G. Yielding,et al.  Deformation around basin-margin faults in the North Sea/mid-Norway rift , 1991, Geological Society, London, Special Publications.

[7]  J. Rundle,et al.  The growth of geological structures by repeated earthquakes, 1, conceptual framework , 1988 .

[8]  J. Weissel,et al.  Flexural uplift of rift flanks due to mechanical unloading of the lithosphere during extension , 1989 .

[9]  D. McKenzie,et al.  Some remarks on the development of sedimentary basins , 1978 .

[10]  N. Kusznir,et al.  Deep Seismic Reflections and the Deformational Mechanics of the Continental Lithosphere , 1988 .

[11]  R. Stein,et al.  Planar high-angle faulting in the basin and range: Geodetic analysis of the 1983 Borah Peak, Idaho, earthquake , 1985 .

[12]  B. Voogd,et al.  Crustal Geometry and Extensional Models for the Grand Banks, Eastern Canada: Constraints from Deep Seismic Reflection Data , 1987 .

[13]  J. Rundle,et al.  The Growth of Geological Structures by Repeated Earthquakes 2. Field Examples of Continental Dip‐Slip Faults , 1988 .

[14]  A. Gibbs Structural evolution of extensional basin margins , 1984, Journal of the Geological Society.

[15]  N. Kusznir,et al.  Simple-Shear and Pure-Shear Models of Extensional Sedimentary Basin Formation: Application to the Jeanne d'Arc Basin, Grand Banks of Newfoundland: Chapter 20: North American Margins , 1989 .

[16]  R. J. Hubbard Age and Significance of Sequence Boundaries on Jurassic and Early Cretaceous Rifted Continental Margins , 1988 .

[17]  N. Kusznir,et al.  Dependence of the flexural rigidity of the continental lithosphere on rheology and temperature , 1985, Nature.

[18]  W. Heiskanen,et al.  The Earth And Its Gravity Field , 1959 .

[19]  D. Barr Lithospheric stretching, detached normal faulting and footwall uplift , 1987, Geological Society, London, Special Publications.

[20]  J. J. Walsh,et al.  Distributions of cumulative displacement and seismic slip on a single normal fault surface , 1987 .