TY - JOUR
T1 - Numerical models of the evolution of accretionary wedges and fold-and-thrust belts using the distinct-element method
AU - Burbidge, D. R.
AU - Braun, J.
PY - 2002
Y1 - 2002
N2 - A 2-D numerical model is used to investigate the evolution of accretionary wedges and fold-and-thrust belts. The numerical method is based on the distinct-element method (DEM). Unlike many continuum numerical models, DEM allows localization to occur even after substantial amounts of deformation. The method is used to study the evolution of simple accretionary wedges and thrust belts with a rigid backstop and base. Experiments are done with a large range of coefficients of interelement friction (μe) and element-wall friction (μb). Two modes of deformation, which depend mainly on μb, are observed. For the weak base case (low μb), the dominant mode is frontal accretion by 'pop-up' structures at or near the toe of the wedge. For the strong base case (high μb), uplift is concentrated near the back of the wedge, and is accompanied by underthrusting along a flat-ramp-flat (or 'staircase') thrust fault structure. At intermediate values of μb, the wedge oscillates between the two modes of deformation. During periods of frontal accretion, normal faulting sometimes occurs in regions where the material has thickened considerably. The transition between the two modes of deformation is found to be a strong function of μb but a weak function of μe. A simple explanation of the experimental results is made using the principle of work minimization. Comparisons between the results and some accretionary wedges/fold-and-thrust belts are also made.
AB - A 2-D numerical model is used to investigate the evolution of accretionary wedges and fold-and-thrust belts. The numerical method is based on the distinct-element method (DEM). Unlike many continuum numerical models, DEM allows localization to occur even after substantial amounts of deformation. The method is used to study the evolution of simple accretionary wedges and thrust belts with a rigid backstop and base. Experiments are done with a large range of coefficients of interelement friction (μe) and element-wall friction (μb). Two modes of deformation, which depend mainly on μb, are observed. For the weak base case (low μb), the dominant mode is frontal accretion by 'pop-up' structures at or near the toe of the wedge. For the strong base case (high μb), uplift is concentrated near the back of the wedge, and is accompanied by underthrusting along a flat-ramp-flat (or 'staircase') thrust fault structure. At intermediate values of μb, the wedge oscillates between the two modes of deformation. During periods of frontal accretion, normal faulting sometimes occurs in regions where the material has thickened considerably. The transition between the two modes of deformation is found to be a strong function of μb but a weak function of μe. A simple explanation of the experimental results is made using the principle of work minimization. Comparisons between the results and some accretionary wedges/fold-and-thrust belts are also made.
KW - Collision belts
KW - Crustal deformation
KW - Faulting
KW - Lateral heterogeneity
KW - Normal faulting
KW - Numerical techniques
UR - http://www.scopus.com/inward/record.url?scp=0036127319&partnerID=8YFLogxK
U2 - 10.1046/j.1365-246x.2002.01579.x
DO - 10.1046/j.1365-246x.2002.01579.x
M3 - Article
SN - 0956-540X
VL - 148
SP - 542
EP - 561
JO - Geophysical Journal International
JF - Geophysical Journal International
IS - 3
ER -