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Geology 341/342 |
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Fall 2004 |
Old
Sample Test
Outline
Topics
covered since Test #1
1. Joints, veins and styloliths
Joints :
- -Fractures with very small displacements
- -Oriented systematically over large geographic areas (joint
sets)
- -Indicative of the orientation of the stress field during
deformation
- -Often there is a set of joints parallel to the fold axis
(longitudinal joints) and a set perpendicular to the fold axis
(cross joints)
- -Joints form during:
- 1) regional deformation
- 2) uplift and unloading
- 3) shringking of igneous rocks during cooling.
Veins
- -Opening mode fractures
- -Formed under high fluid pressure
- -The fracture is held open by the fluid pressure and filled
with a mineral deposited from the water
- -They are important indicators of local stress conditions
- -Sometimes they form "en echelon" arrays within
a shear zone.
- -Can you tell sense of shear of an en echelon vein array?
Stylolites
- -Irregular surfaces of dissolution induced by high stress
- -They form perpendicular to sigma 1.
- -Usually found in limestone and other easily soluble rocks
types.
2) Introduction to Faults
- -What is a fault?
- A geological discontinuity
- A shear fracture
- -Orientation of faults with respect to sigma 1.
- Ideally at about 30 degrees to sigma 1.
- In reality zones of weakness in the rock affect fault orientation
- -Conjugate fault sets
- -How do you determine sense and magnitude of fault slip?
- Offset marker layers
- Drag folds
- Striations on fault plane
- -Separation vs. true slip (need to think about the 3-D geometry)
- Footwall-hanging wall relationships for thrust and normal
faults
- -Normal fault places younger on older rocks (or shallow level
on deep level rocks).
- -Thrust (or reverse) fault places older on younger rocks
(or deep level on shallow level).
3) Thrust faults
Outline
-Tectonic setting (mainly convergent plate boundaries)
-Components of a fold and thrust belt
- Foreland
- hinterland
- basement
- cover
- thrust sheets
- duplexes
- backthrusts
- -Geometry of thrust faults (flat-ramp geometry)
- -Relationship between ramp-flats and anticlines in the hanging
wall
- -Sequence of faulting (from hinterland to foreland)
- -Map patterns of thrust faults
- -Critical wedge model of fold and thrust belts ( Bulldozer
model)
- -Mechanical paradox of large over thrusts
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- Tectonic setting
o Fundamental characteristic: thrust faults accommodate shortening
of the earth's crust.
o Most big mountain ranges are fold-and-thrust belts
o Consists of a set of folds and thrust faults that extend for
10s to 100s of kilometers along strike
o Usually shortening takes place near the plate boundary in convergent
margins:
- 1. Continent/continent collision (Himalayas, Alps, Appalachians,
Urals)
2. Arc-continent collision (Timor, Brooks Range)
3. Ocean-Continent convergence (Andes)
- o Sometimes stress is transmitted far into the continental
plate and thrust faults develop far from the boundary (Wind River
Range of Wyoming, Tien Shan (China))
o Accretionary prisms are submarine fold-and-thrust belts (Barbados,
Taiwan)
o There may be hundreds of kilometers of shortening (negative
extension) across a fold and thrust belt.
Example: Restoration of a cross section of the Canadian Cordillera.
Components of a Thrust System
o Individual fault blocks are typically broad relative to their
thickness.
- They are called a thrust sheets or a nappes
o Allochthon is a thrust sheet that has moved a long way
with respect the underlying basement (the autochthon).
o Foreland is the area in front of the thrust belt
o Hinterland is the area behind the thrust belt
o Decollement or detachment fault separates the
fold and thrust belt from the basement
- Found in "thin-skinned" thrust belts, where the sedimentary
cover is scraped off of the basement, like a crumpled rug.
-In thick-skinned thrust belts the basement is involved in the
shortening
o Imbricate fan: Individual thrust sheets overlap like
roofing tiles
o Duplex: system of imbricate thrusts that branch off
from a single fault below and merge with a thrust fault above.
The rock body bounded by fauots above and below is called a horse.
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- Shape and displacement of thrust faults
o Ramp-flat geometry
- Faults will generally form along bedding planes in weak layers.
This is the "flat"
* shale
* salt
- Then it may cut upwards through the strong layers in the direction
of displacement to form a ramp
- Ramp will end in another weak layer
- Why do they form? Is it easier to continue deforming along
the same layer
or is it mechanically easier to cut upwards toward the surface?
- The spacing between ramps tends to be fairly uniform . This
is controlled by factors such as basal friction on the detachment,
thickness of the competent layers, dip of the ramp
o Movement on the ramp forms folds in the thrust sheet
- This is are fault-bend folds
- Ramp anticlines
o Eventually it becomes easier to cut a new fault in front =
forward propagation sequence
o Blind thrusts are common (don't breach the surface) may form
"fault-propagation folds"
o The map trace of thrust faults is generally irregular
o Thrust faults are typically low-angle
o Erosion of a thrust sheet can leave an isolated part of the
hanging wall, = Klippe
o If erosion creates a hole in the thrust sheet, we get a window
into the footwall rocks
o Spacing of thrusts depends on thickness of the thrust sheet
(thicker = wider spacing)
Recognition of thrust faults
o Fundamental characteristic: older beds end up above younger
rocks
o Stratigraphic sections are generally duplicated
o Igneous rocks or high-grade metamorphic rocks may overlie lower
grade or unmetamorphosed rocks.
o Highly folded rocks could be thrust over relatively undeformed
rocks.
o May even transport rocks that are still hot over lower grade
rocks, creating an inverted
metamorphic gradient
o Because thursts can transport rocks a great distance, rocks
of the same age but different sedimentary facies may overlie
each other
- o All low-angle faults are not thrusts! Normal faults can
be rotated to lower angle, and in some cases normal faults form
at low angles (see discussion of metamorphic core complexes)
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- Thrust faults in outcrop
o Reverse faults are steeper than 45°
o Thrust faults are shallower than 45° and more common.
o Even the largest thrust faults appear as knife-sharp surfaces
that separate rocks that were
far apart before movement on the fault
o Often you can put your finger on the fault
o Evidence of rigid-body translation or rotation following brittle
fracture
o Ductile deformation also occurs, but the displacements are
much smaller
o Faults have to die out somewhere, and at the end of the fault,
along strike, you can
see continuous, unfaulted rocks. So the displacement decreases
along strike.
o Strain is generally heterogeneous on the scale of a thrust
sheet, and even on outcrop scale.
Mechanical Model for Thrust Fault Systems
o We know that thrust sheets have a large surface area relative
to their thickness
-dimensions on the order of 5-15 km thick, 75-150 km in length
o How did they move?
o If you take a thin sheet of rock with those approximate dimensions,
the stress applied to the rear of the block must exceed the frictional
resistance at the base of the sheet.
o Problem: the stress required exceeds the rock strength by a
factor of 10 !
o The problems is analogous to trying to shove a flat slab of
Jell-O across the kitchen table without it crumpling.
o This has been called "The mechanical paradox
of large overthrusts"
Possible solutions
- Thrust sheets are actually sliding downhill, by gravity (doesn't
work: faults dip the wrong way)
- Rocks are deforming ductilely, rather than sliding over a surface
(not usually the case)
- Fluid pressure offsets the normal stress at the detachment,
thus reducing friction
- The assumption in this paradox is that the entire thrust sheet
moves at the same time. This assumption is wrong.
o Actually only a small part of the fault surface is moving at
any one time like a wrinkle in a rug being pushed forward or
a dislocation moving through a crystal.
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- Bulldozer model
o Think of a thrust system as a WEDGE, such as would form in
front of a bulldozer that is pushing snow
- When the wedge reaches a "critical taper" (angle
alpha) it begins to slide
- The wedge will grow with time, but the taper will stay the
same.
- If the material is weak, or if there is less friction, the
taper will be low
- This model matches the shape of most thrust belts
- Probably oversimplified, but it's a good way to think about
the process
o Faults usually get younger toward the foreland
o The whole system grows in the direction the thrusts are moving
o Erosion tends to decrease the slope of the wedge. That can
lead to fault reactivation in the hinterland to build the taper
back up. There is a feedback between surface processes and tectonics.
Active Thrust faults and Earthquakes
o Large thrust faults associated with subduction produce some
of the most powerful earthquakes
o One of the best studied earthquake is the 1964 Alaska Earthquake
- Displacement was at least 20 m
- Thrust was shallowly dipping, only 5 to 10°, dipping to
the north
- Hypocenter was between 20 and 50 km depth
- Uplifts were locally as much as 10 m, and other areas dropped
1-2 m
- The entire sheet didn't move all at once, but it propagated
during the course
of the earthquake, which lasted almost a minute
References:
Price, R. A., The mechanical paradox of large overthrusts, GSA
Bull. v. 100, p. 1898-1908, 1988.
4) Normal Faults
- -Tectonic setting
- Divergent plate boundaries
- zones of gravity-driven extension
- passive margins
- orogenic collapse
- -Types of normal fault systems to accommodate extension
- -Horst and graben
- -Conjugate normal faults
- -Listric faults and hanging wall roll-over anticlines
- -Growth faults
5) Strike-Slip fault systems
-Tectonic setting
- Transform plate boundaries
- Escape structures in the hinterland of plate collision zones
- Transfer zones in thrust belts or normal fault systems
- -Development of a strike slip fault
- -Strain within a strike slip shear zone en echelon
structures
- -Releasing bends and restraining bends
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- 6) Quakes
- · Faults and Earthquakes
· Strength profile of the crust
· Elastic Rebound theory
· P and S waves
· Quadrants of compressional and dilatational first arrivals
· Focal mechanisms (beach ball diagrams)