sgm bern 11/25/2006 marcel frehner 1 numerical simulations of parasitic folding in multilayers sgm...
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1SGM Bern 11/25/2006 Marcel Frehner
Numerical simulations ofparasitic folding in multilayers
SGM Bern, November 25, 2006
Marcel FrehnerStefan M. Schmalholz
2SGM Bern 11/25/2006 Marcel Frehner
Outline
Motivation
Method
Two-layer folds 3 regions of deformation 3 deformation phases
Multilayer folds 3 deformation phases reformulated Similarity to two-layer folds
Conclusions
3SGM Bern 11/25/2006 Marcel Frehner
Motivation: Asymmetric parasitic folds on all scales
Mount RubinWestern Antarctica
Picture courtesyof Chris Wilson
~1200m
Foliated MetagabbroVal Malenco; Swiss Alps
Picture courtesy of Jean-Pierre Burg
4SGM Bern 11/25/2006 Marcel Frehner
Motivation: The work by Hans Ramberg
Ramberg, H.Geological Magazine1963:
Evolution of drag folds
5SGM Bern 11/25/2006 Marcel Frehner
Motivation
Asymmetric parasitic folds are used in field studies
Problem: Conditions for their development are not thoroughly studied
Why become parasitic folds asymetric?
Goal: Understanding of the strain history and the development of
multilayer folds
Quantify necesary conditions for the development of asymetric parasitic folds
6SGM Bern 11/25/2006 Marcel Frehner
Method
Self-developed finite element (FEM) program Incompressible Newtonian rheology
2D
Dimensionless formulation
Pure shear boundary conditions
Modelled area: Half wavelength of fold
Viscosity contrast: 100
Sinusoidal initial perturbation
7SGM Bern 11/25/2006 Marcel Frehner
Two-layer folds→ Example of numerical simulation
Resolution 11’250
elements
100’576 nodes
8SGM Bern 11/25/2006 Marcel Frehner
Two-layer folds→ After 40% shortening
Strain ellipses
coloured with:
Bulkstrain
Strain ellipses coloured with:
Rotation angle
9SGM Bern 11/25/2006 Marcel Frehner
Two-layer folds→ Three regions of deformation
Fold limb S Transition zone JFold hinge I
10SGM Bern 11/25/2006 Marcel Frehner
Two-layer folds→ Three deformation phases at fold limb
Increasing shortening
1 = Original distance
Co
mp
ress
ion
Sh
eari
ng
Fla
tten
ing
Ab
solu
te
flatte
nin
g
11SGM Bern 11/25/2006 Marcel Frehner
Two-layer folds→ Observations
Three regions of deformation Fold hinge, layer-parallel compression only
Fold limb
Transition zone, complicated deformation mechanism
Three deformation phases at fold limb Layer-parallel compression
Shearing without flattening
Flattening normal to the layers
SI J
12SGM Bern 11/25/2006 Marcel Frehner
Multilayer folds→ Example of numerical simulation
Viscositycontrast: 100
Thickness ratioHthin:Hthick = 1:50
Random initial perturbation onthin layers
Truly multiscale model
Number of thin layers in this example: 20
Resolution: 24‘500 elements
220‘500 nodes
14SGM Bern 11/25/2006 Marcel Frehner
Multilayer folds→ Three deformation phases reformulated
Amplitude
of thin layers of thick layers
15SGM Bern 11/25/2006 Marcel Frehner
Multilayer folds→ Three deformation phases reformulated
Layer-parallel compression No buckling of thick layers
Thin layers start to buckle anddevelop symmetric fold stacks
Shearing without flattening Buckling of thick layers causes shearing between them
Folds of multilayer stack become asymmetric
Flattening normal to layers Increased amplification of thick layers
leads to flattening normal to layers
Amplitudes of thin layers are decreased
17SGM Bern 11/25/2006 Marcel Frehner
Multilayer folds→ Similarity to two-layer folding
Deformation of double layersystem is nearly independentof presence of multilayerstack in between
50% shortening:
Black: Multilayer systemGreen: Two-layer system
18SGM Bern 11/25/2006 Marcel Frehner
Conclusions
Deformation history between a two-layer system at the fold limb can be divided into three phases Layer parallel compression Shearing without flattening Flattening normal to layers
Thin layers develop vertical symmetric fold-stacks during first phase;They deform passively afterwards (like in the double layer case)
Whether fold-stacks survive the flattening phase is due to their amplitude at the point of buckling initiation of the thick layers A bigger number of thin layers amplifies faster
Deformation of a two-layer system is nearly independent of the presence or absence of a multilayer stack in between