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142 Cards in this Set
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- Back
annealing
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recovery/recrystallization after deformation
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Coble (grain-boundary) diffusion
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diffusion of material along grain boundaries from areas of high compressive stress to areas of lower stress. Relatively fast, occurring at low temps.
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chemical concentration gradients
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change in chemical concentration of certain materials along surface due to dissolution creep
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dislocation climb
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propagation of a dislocation through a crystal lattice
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dissolution creep
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Same as pressure solution. Minerals dissolve into pore fluid at areas of high stress and are transported to areas of low stress and reprecipitated.
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high-angle boundary
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grain boundary with dislocation greater then 11% from grain to grain
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brittle-ductile transition
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Depth Where deformation of material begins to behave ductile instead of brittle due to increased temperature and pressure. (i.e. for quartz this is about 12 km)
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crustal strength envelope
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composite of Byerlee's law for upper crust and quartz flow law for lower crust
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deformation map
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show the active deformation mechanisms as function of temperature and differential stress (and strain rate) for a specific mineral or mineral. Maps broken in dominant deformation mechanisms.
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dislocation creep
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shearing of the crystal lattice along crystallographic planes
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dynamic recrystallization
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recovery/recrystallization during deformation counteracts hardening and determines rate of dislocation creep
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intergranular microcrack
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microcrack around grains or along grain boundaries
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cataclasis
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brittle granulation of rock, angular fragments, progressive decrease in grain size with deformation, occurs at low temperatures and pressures.
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diffusion creep
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distortion and dilation of crystals by dissolution under stress and precipitation of material in the presence of water
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dilatency
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increase of volume. For us it is the reference to cataclasis that causes a increase in rock volume.
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vacancies
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unoccupied sites within a given crystal
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edge dislocation
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Occurs when stress causes an edge of a crystal lattice to move laterally relative to the lattice below. This edge then moves across the mineral until it is terminated at the grain boundary.
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interstitial atoms
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ions in between normal sites in the crystal lattice.
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cataclastic flow
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slip on discrete surfaces that separate undeformed areas
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deformation mechanisms
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brittle mechanisms, diffustion creep, dislocation creep, dissolution creep, and mechanical twinning.
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dislocation
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line that bound a planar defect in the crystal lattice
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transgranular microcrack
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microcrack that cuts across adjacent grains
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grain boundary sliding
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grain-scale sliding between grains in a rock
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intragranular
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sliding around grains and or along grain boundaries,
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ionic bonds
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when one atom loses/borrows an electron from another atom
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mechanical twinning
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shearing parallel to a crystallographic plane e.g. calcite, plagioclase feldspar
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planar defects
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grain boundaries, or crystallographic twin planes, or extra planes of atoms within a lattice.
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recovery
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"heals" lattice by rearranging or destroying dislocations
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strain hardening
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hardening of a rock as a result of strain
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Theoretical strength
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Based on calculations. Basically what the strength of a rock should be.
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microcracks
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small cracks within a rock. That can be intergranular, intragranular, or transgranular
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point defects
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The crystal lattice has an equilibrium distribution of point defects created during lattice formation, ductile deformation, or rapid cooling from high temperatures.
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recrystallization
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converts old grains with defects into "new" grains. Favored by high temperature.
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stylolites
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Planar occurrences of pressure solution where minerals are dissolved out and usually replaced by less soluble minerals such as mica or clay.
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kinks
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non-uniform bends within a structure
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Nabarro-Herring creep
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volume-diffusion creep. diffusion within grains, effective at high temperatures & low-moderate differential stress. vacancies migrate to max stress. crystals grow parallel to minimum
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pressure shadows
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precipitation on other minerals of low stress
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grain boundary slip
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coble-creep. diffusion of material along grain boundaries from areas of high compressive stress to areas of lower stress
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line defects
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A line defect is made up of a line of atoms that moves through the crystal lattice as a single unit
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overgrowths
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precipitation on the same mineral in area of low stress
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pressure solution
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solution caused by pressure conditions in which minerals are reconfigured to create rock structure
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solid state diffusion
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point defects migrate through the crystal lattice from areas of high stress to areas of low stress.
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abnormal fluid pressure
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abnormal fluid pressure based on fluid pressure ratio = fluid pressure/lithostatic (normal) pressure fpr = Pf/PL
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asperities
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irregularities on the sliding surface.
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Coulomb law of failure
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critical shear stress = cohesive strength + coefficient of internal friction (normal stress) find ratio of shear stress to normal for failure.
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effective stress
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the difference between normal stress and fluid pressure. On-Pf
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hydraulic fracture
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fracture due to fluid
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joint fringe
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joint termination
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ribs
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curved steps in joint face, oriented perpendicular to hackles, old joint terminations
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tensile strength
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the strength a rock has available relative to tensile motion
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slickenlines
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Occur at fault boundaries when protuberances scratch the surface opposite block and or when minerals are reprecipitated along a straight line parallel to fault movement.
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angle of internal friction
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slope of the failure envelope φ
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Byerlee's law
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Failure criterion for pre-fractured rocks. critical shear stress = a (normal stress)
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crack-seal vein
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preserve inclusions indicating repeated fracturing
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fluid pressure ratio
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fluid pressure ratio = fluid pressure/lithostatic (normal) pressure fpr = Pf/PL
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hydrostatic pressure
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pressure within a rock due to fluid inclusion
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joint intersections
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intersections of different types of joints. X-int due to cooling, Y-int systematic joints, T-int younger joint terminate at older ones.
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plume axis
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axis relative to volcanic plume
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ridge-in-groove lineations
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lineations produced by sinistral movement along a fault
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angle of sliding friction
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the angle in which fracture occurs due to sliding
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cohesive strength
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cohesive strength of rock = point where failure envelope intersects τ-axis
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crystal fibers
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They fill openings in joints, preserve record of the opening.
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Griffith Cracks
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cracks due to failure of a brittle material
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joint
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cracks along the axis of a rock/mineral
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Systematic Joints
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Most obvious joint sets along a rock. Non Systematic joints are usually perpendicular and less apparent.
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plumose structure
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hackles. linear or curved markings on joint face
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scissor fractures
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shear parallel to the fracture surface and parallel to the fracture front (faults)
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opening fractures
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fractures that cause a opening due to joints and can be refilled
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Mode I
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(opening, dilation) fractures: extension perpendicular to fracture surface (joints)
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Coulumb envelope
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envelope is parabolic in tensile field of Mohr diagram and linear in compressive field. In particular the failure envelope.
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en echelon joints
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Three or more faults oriented laterally and slightly offset forming a stair-like pattern
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hackles
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feather-like striations on a rock face due to tensile fracturing. They begin at an origin and radiate outward.
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Mode III
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scissor fractures
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shear fractures
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AKA mode II. shear parallel to the fracture surface and perpendicular to the fracture front (faults)
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process zone
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zone of processing
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vein
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a area that can be filled with secondary minerals or precipitation. Crystals grow here.
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syntaxial vein
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add material along the center of the vein
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aspirates
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unevenness of a surface
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thrust-slip
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shorten and thicken layering
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fault-line scarp
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steps in earth formed by active faults that represent accurate faulting planes
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fault zone
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Countless sub parallel connections of fault surfaces
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slip-fiber lineations
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crystals grow in pressure shadow of small steps on fault surface
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microfaults
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faults on a microscopic scale with rocks
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Offset
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the distance between two faulted bodies
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stratigraphic throw
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The distance separating one bedding layer from another one on the fault.
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slickensided surfaces
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striations or lineations on fault surfaces that record the direction of slip
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Breccia
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angular rock fragments in finer matrix, fragments more abundant than matrix, various sizes, from microbreccia (>0.1 mm - <1 mm) to megabreccia (>0.5 m fragments)
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dip-slip fault
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defined by relative movement of hanging wall (above fault surface, or block that fault dips towards) and footwall (below fault surface). slip parallel to dip
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footwall
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rock face below faulting surface
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strike-slip fault
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(horizontal) slip parallel to strike of fault
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Normal fault
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hanging wall moves down relative to footwall but we only know the offset and no slip
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Overlap
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overlapping areas of fault movement
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repetition/omission of strata
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allow us to observe faults that are typically not observable
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right-lateral fault
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strike fault in which the main block uses right hand rule
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slickensides
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striations or lineations on fault surfaces that record the direction of slip
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cataclasite
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very fine grained, strongly indurated rock made up of rock fragments and matrix, typically formed under higher temperatures and pressures than breccias
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drag
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when a rock body drags and causes local folding
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fault scarp
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steps in earth surface formed by recent active faults
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gouge
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fine clay like powder generated at fault boundaries. It is composed of finely, grounded pieces of fault blocks.
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normal-slip fault
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same as normal fault but we know the slip
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paleoseismic
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study of timing, location, and size of prehistoric earthquakes using the rock record
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reverse fault
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hanging wall moves up relative to footwall
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rollover anticline
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anticline that has rolled over
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conjugate set fault
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intersection that cross cuts a fault plane that is parallel to principal stress
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fault surface
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a surface along which fault slip occurred
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hanging wall
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rock face above faulted surface
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listric fault
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a normal fault where the fault plane is curved
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oblique-slip fault
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slip fault that occurs at an oblique angle
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pseudotachylite
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Glass like formation found along fault boundaries. They are formed from frictional heating of fault edges, typically characteristic in deep faults.
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reverse-slip fault
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slip fault where the motion is towards us using the right hang rule
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separation slip
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strike slip fault where separation of the body occurs
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decollement
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gliding surface between two masses in a thrust fault system
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ramp
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angled body due to faulting
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allocthonous
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place other then its origin
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balanced cross section
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cross-section that is balanced in terms of displaying equal bodies separated by a fault
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fault reactivation
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reactivation of a fault due to change in stress
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hanging wall ramp
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ramp due to relative hanging wall
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tectonic transport direction
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direction of transport based on tectonic activity
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coefficient of sliding friction
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static friction that is overcame between two bodies to allow sliding
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blind thrust
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fault-propagation folds - flat-ramp fault geometry
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lateral ramp
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ramp that is lateral to fault movement
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autochthanous
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placed at the point of the bodies origin
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bed-length balancing
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balancing beds using length
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footwall flat
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geometrically flat of footwall
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Hubbert & Rubey
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thrust sheets are too big to be moved by simply pushing from the back of the sheet. normal stress must be offset by elevated pore pressure Otherwise there would just be fracturing.
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Anderson's theory of faulting
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shear stress must be zero at the surface
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foreland-dipping duplex
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largely displaced dipping anticlinal structures
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thin-skinned
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thin-skinned does not involve basement rocks, thick skinned does involve basement
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transfer zones
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zones of displacement due to fault transfer of displacement
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duplex
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multiple faults controlled by presence of an upper detachment horizon
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tear fault
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A very steep to vertical fault associated with and perpendicular to the strike of an overthrust.
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klippe
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an erosional remnant of thrust sheet (hanging wall) surrounded by footwall rocks
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window(fenester)
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an exposure of the footwall of a thrust viewed through the hanging wall
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footwall ramp
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ramp geometry of footwall
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horse
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fault block surrounded by fault surfaces
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syntectonic basin
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basin that was deposited at the same time as formation
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overthrusting
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low angle and large displacement of fault characterized as overthrusting
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Why are actual yield strengths of minerals much lower than theoretical yield strengths?
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This is due to griffiths theory. There are small fractures and discontinuities within a rock. Nothing is perfect unless it is synthetically made, and therefor the strength is always less then what the calculation says.
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Contrast deformation features resulting from pressure solution(dissolution creep) and cataclasis?
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Pressure disolution involved fluid moving through a material. Stylolites are observed in pressure disolution. Dislocation occurs due to defects in crystal structure of a rock. Cataclasis are due to mechanical discontinuities and subsequent fracture movement. Pressure disolution occurs at lower pressures and temperatures.
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Describe the ornamentation associated with the surfaces of tensile fractures in rocks and outline their genetic meaning:
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Tensile fractures show three ornamentations: ribs,origins, and hackles. Ribs are circular and radiate out from origin of fracture. They give us a history of deformation. Origins are simply the point of origin. Hackles are feather like features that radiate out from origin. Most common ornamentatins in faults are slicklines. They are caused by recystallization of minerals and or scratches made by proturbences. They show direction of fault movement.
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What is the physical basis for griffith theory and what does the theory predict?
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Theoretical strength = actual strength. Griffith suggested that the low fracture strength observed in experiments, as well as the size-dependence of strength, was due to the presence of microscopic flaws in the bulk material. We can see this in the way synthetics tend to not break as easy.
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Describe how faults can be recognized in the field?
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Faults are recognized by displacement of rock bodies and related strike and dip. Faults can then be categorized by the direction of movement and the displacement of the surrounding rock bodies.
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