structural geology and tectonic analysis
TRANSCRIPT
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Principles of structural
geology and tectonic
analysis
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Strain
In response to stress, rocks undergotransformations that are decomposed in 3
operations: Rotation Translation
Deformation which corresponds to a change inform
Strain is a change in shape or internal
configuration of a body
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Strain Strain is marked by
Transformation of an initial circle/sphere intoan ellipse/ellipsoid
The axis of deformation
Movement of particules defined by aninstantaneous velocity vector, defining flowlines and finally trajectories
The kinematic notion, a function of time
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Stress and strain Rheology is the study of the relationships between
stress imposed on a body and resulting strains or
strain rates Competence is a general term to describe the ease
with which a material can deform
In response to a stress, strain may be Reversible, elastic deformation
Brittle, failure of a stressed body, at a certainstate, the solid rocks lose their internalcohesion
Permanent, ductile flow without brittledeformation
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3 axis of deformation, a finite strain ellipsoid
Principal
strain directions, X, Y, Z
planes XY, YZ, ZX
changes in length e1, e2, e3
ratios Rxy, Ryz, Rzx
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The Flinn graph for representing the
shape of any ellipsoid
X/Y
Y/Z Ramsay & Huber, Academic Press Lim., 1983
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Strain regimes
Deformation in rocks occurs under 2 strainregimes: Pure shear
Simple shear Under combination of pure and simple
shear
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Simple shear
A displacement which transforms an initialsquare in a parallelogram where thedisplacement vectors are all oriented
parallel to one set of the opposite sides ofthe square and parallelogram. The vectordirection is know as the shear direction.
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Transformation of a sphere in an
ellispoid, 2 strain regimes
Pure shear
Simple shear
/X
/Z
Choukroune, Masson, 1995
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2 end-members
Deformation >
Displacement
Flow lines are parallel to
the shear direction during
the deformation
Flow lines tends to
become perpendicular to
the Z shortening axis
Axis of deformation
rotate (non coaxial and
rotational)
Axis of deformation
remains parallel (coaxial
and non rotational)
Simple shearPure shear
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Finite strain ellipsoid and strain regimes
Choukroune, Masson, 1995
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The Flinn graph for representing the
shape of any ellipsoid
X/Y
Y/Z Ramsay & Huber, Academic Press Lim., 1983
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Change in geometry from coaxial to noncoaxial regimes
Coaxial Non coaxial
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Markers of the finite strain ellipsoid
Fold and boudinage structures Boudinage is a structure produced during heextension of competent layers enclosed in anincompetent matrix
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Deflection of cleavage around a competentfragment of quartzite in an argilite
Ramsay & Huber, Academic Press Lim., 1983
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Folding and boudinage in a Flinn graph
FLATTENING
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Markers of the finite strain ellipsoid
Deformation of pre-tectonic objects pebble, phenocryst, oolithe, redox spot,
fossil.. Mineral fabric and pressure shadows
Fabric is the geometric and spatialrelationships between the crystalcomponents making a rock, i.e. preferredorientation of grain shapes and
crystallographic axis, the grain size Pressure shadow is a region of low strainprotected from deformation by a rigid orcompetent object in a rock of lower
competence
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Pressure shadows in a Flinn graphL>>S
S >> L
L=S
A li t f b i L S f th
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A linear type fabric: L>>S from theHakos mountains
A granitic orthogneiss
A li t f b i : L>>S f th
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A linear type fabric: L>>S from theHakos mountains
A metaconglomerate
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Sheared
Gamsberggranite
XZ plane
YZ plane
1 single rock!
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Shearedrhyolite
XZ plane
YZ plane
1 single rock !
P i i i d i
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Partitioning and time
Homogeneous vs non homogeneous deformation The definition of zones of homogeneous
deformation
The notion of bulk strain, an average strain in aheterogeneously deformed material
Finite strain vs incremental deformation, notion
of progressive deformation Increment from one stage to the next Rate of change along the main strain axis and of
rotation defines the principal strain rates and thevorticity
Definition of the strain regime by identification
and analysis of the markers of incrementaldeformation
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Pure shear and development ofstructural elements
Crenulation and mechanical rotation Pressure-solution, a deformation process
whereby material under stress goes intosolution at a localized point in a material,this material is transported by flow ordiffusion
Recrystallisation Transposition
P h d d l f f ld
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Pure shear and development of folds ,
axial plane cleavage...
P h d d l t f f ld
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Pure shear and development of folds,
axial plane cleavage...
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Progressive stages in fabric
development of a shale
Initial compacted
Ealiest deformation Pencil structure
Embryonnic deformation
plane
deformation plane
deformation plane withstretching lineation
Type of linear fabric
C D E F
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Simple shear and development of shearzone
A shear zone is a zone with sub-parallel
walls in which high deformations arelocalized Effects of non coaxial deformation
Plane strain ellipsoid Markers of rotational deformation
Coexistence of deformation and displacement
planes, S/C/C structures Assymetric pressure shadows and mineral
fabric
Folding
S C C structures
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S C C structures
The S plane: the deformation plane, with no displacementThe C and C
planes: the displacement planes with highdeformation (mylonitisation)
S
C
C//S
C
SC
C
C
S C C structures: a
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C
C
S
C
S C
C
C//S
C
S C C structures: a
progressive phenomenon
t1
t2
t3
S C C structures
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S C C structures
C
C
S
CS
Assymetric pressure shadow
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Assymetric pressure shadow
C
C
Assymetric pressure shadow
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y p
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Cleavage bendingand helicitic
inclusions
A t i f ld
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Assymetric folds
and pressureshadows
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Fabric in a ductile simple shear zone
A reverse shear zone within the basement
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A reverse shear zone within the basementinlier of the Damara foreland
Sheared porphyric granite
L downdip tectonite
C
S
C
S//C
Development of non cylindrical folds
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Development of non cylindrical folds
during non coaxial deformation
Development of non cylindrical foldsd l d f
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during non coaxial deformation
Development of non cylindrical foldsd i i l d f i
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during non coaxial deformation
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Progressive developement of sheath
folds
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Sheath folds fromthe Ile de Groix
Sheath folds from the base of a thrust
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f f m fnappe from the Variscan belt of France
Sheath folds from the base of a thrust
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nappe from the Hakos mountains
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h f l
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Change in geometry from coaxial to non
coaxial regimes
Coaxial Non coaxial
Conjugate shear zones: a coaxial regime
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C
S
CC
S
NNW SSE
vs a non coaxial regime
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vs a non coaxial regime...
C
S
C
S//C