C. Beaumont et al., THE CONTINENTAL COLLISION ZONE, SOUTH-ISLAND, NEW-ZEALAND - COMPARISON OF GEODYNAMICAL MODELS AND OBSERVATIONS, J GEO R-SOL, 101(B2), 1996, pp. 3333-3359
The South Island zone of oblique continent-continent convergence occur
s along a 400 km-long section of the modern Australia-Pacific plate bo
undary zone, across which about 50 km of shortening has been accommoda
ted since about 10 Ma. The orogen comprises a central mountain range (
Southern Alps) flanked on both sides by what are interpreted to be for
eland basins, Two essential features that characterize the orogen are
(1) the degree of denudation that accompanied deformation, and (2) a f
undamental structural asymmetry. The architectural asymmetry of the or
ogen can be explained by plane strain, finite element models of contin
ental convergence incorporating mantle subduction. Comparison of model
and orogen polarity implies that Pacific plate mantle subducts. The m
odels predict two crustal-scale dipping shear zones that form above th
e point where the Pacific mantle subducts. The localized one more dist
ant from the incoming plate (retro-step-up shear zone) corresponds to
the Alpine fault, whereas its conjugate (pro-step-up shear zone) corre
sponds to the distributed strain and thrusting along the eastern margi
n of the mountain belt. Parameters that modify the model boundary cond
itions (top surface, degree of denudation; basal zone, subduction load
, crust-mantle velocity discontinuity, subduction of lower crust, mant
le retreat, and distributed decrease in mantle velocity) and the inter
nal strength of the crust (two-layer crust with moderate coupling, tem
perature distribution, strain weakening) are varied in a series of num
erical model calculations that establish the combination of material p
roperties and boundary conditions that lead to different cross section
al architectures of the modeled collision zone. In turn, these are com
pared with observations about the South Island orogen. The calculation
s show how the style and extent of deformation across the whole orogen
depend on the rheological properties of the crustal layer and on the
balance between its internal strength and the combined effects of the
boundary and gravitational stresses. North to south along-strike diffe
rences in the width and two-dimensional architecture of the orogen, si
mulated in the experiments by varying the model parameters, can be exp
lained by a combination of southward increases in preconvergent crusta
l thickness, geothermal gradient, convergence, and potentially subduct
ion retreat, with the added possibility of a southward decrease in the
component of lower crustal subduction.