Lithospheric strength and its relationship to the elastic and seismogenic layer thickness

Plate flexure is a phenomenon that describes how the lithosphere responds to long-term (> 10(5) yr) geological loads. By comparing the flexure in the vicinity of ice, volcano, and sediment loads to predictions based on simple plate models it has been possible to estimate the effective elastic thickness of the lithosphere, T-e. In the oceans, T-e is the range 2-50 km and is determined mainly by plate and load age. The continents, in contrast, are characterised by T-e values of up to 80 km and greater. Rheological considerations based on data from experimental rock mechanics suggest that T-e reflects the integrated brittle, elastic and ductile strength of the lithosphere. T-e differs, therefore, from the seismogenic layer thickness, T-s, which is indicative of the depth to which anelastic deformation occurs as unstable frictional sliding. Despite differences in their time scales, T-e and T-s are similar in the oceans where loading reduces the initial mechanical thickness to values that generally coincide with the thickness of the brittle layer. They differ, however, in continents, which, unlike oceans, are characterised by a multi-layer rheology. As a result, T-e much greater than T-r in cratons, many convergent zones, and some rifts. Most rifts, however, are characterised by a low T-e that has been variously attributed to a young thermal age of the rifted lithosphere, thinning and heating at the time of rifting, and yielding due to post-rift sediment loading. Irrespective of their origin, the Wilson cycle makes it possible for low values to be inherited by foreland basins which, in turn, helps explain why similarities between T-e and T-s extend beyond rifts into other tectonic regions such as orogenic belts and, occasionally, the cratons themselves. (C) 2003 Elsevier Science B.V. All rights reserved.