Structural geology Flashcards

1
Q

The study of the origin, geometry, and kinematics of the formation of structures.

A

STRUCTURAL GEOLOGY

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2
Q

A continuous deformation that produces specific kinds of folds, ductile faults, cleavages, and foliation.

A

Ductile Deformation

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3
Q

A discontinuous deformation that produces specific kinds of folds, brittle faults, and joints.

A

Brittle Deformation

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4
Q

A rock mass in which the original position is questionable with respect to the adjacent terrane or continent to which it is presently attached.

A

Suspect Terrane

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5
Q

Bears no resemblance to the mass to which it is attached, where the source may be the opposite side of a major
ocean.

A

Exotic Terrane

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6
Q

A distinct crustal block transported by tectonic processes.

A

Terrane

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7
Q

The shape of the surface topography.

A

Terrain

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8
Q

The opening and closing cycle of an ocean.

A

Wilson Cycle

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9
Q

A rule that states that micro- or small structures are keys to mimic the styles and orientations of macro- or larger structures of the same generation within a particular area.

A

Pumpelly’s Rule

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10
Q

Structures that occur pervasively throughout the rock mass (e.g., cleavage, foliation, and certain folds).

A

Penetrative Structures

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11
Q

Structures that occur as single features (e.g., a single fault or an isolated fold)

A

Non-penetrative Structures

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12
Q

The state of gravitational equilibrium between Earth’s crust and mantle, such that the crust “floats” at a certain elevation that depends on factors such as thickness and density.

A

ISOSTASY

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13
Q

A hypothesis, developed by John Henry Pratt, that states that the Earth’s crust has a uniform thickness below sea level with its base everywhere supporting a density at a depth of compensation.

A

Pratt’s Hypothesis

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14
Q

Megascopic rock masses of the Earth’s crust with lesser density, such as mountain ranges, project higher elevations above sea level compared to those with greater density.

A

Pratt’s Hypothesis

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15
Q

A hypothesis, developed by Sir George Biddell Airy, which proposes that the Earth’s crust is a more rigid shell floating on a more liquid substratum of greater density.

A

Airy’s Hypothesis

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16
Q

The theory assumes that the crust has a uniform density throughout, but do not have a uniform thickness of crustal layer.

A

Airy’s Hypothesis

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17
Q

The hypothesis is said to be supported by the notion that mountains resulted from the upward expansion of locally heated crustal material, which had a larger volume but a lower density after it had cooled.

A

Pratt’s Hypothesis

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18
Q

Force applied to a material that tends to change the material’s dimension.

A

STRESS

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19
Q

The type of stress that tends to pull a body mass apart.

A

Tensional Stress

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20
Q

The type of stress that squeezes a body mass.

A

Compressional Stress

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21
Q

Stress that acts perpendicular to a reference surface.

A

Normal Stress

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22
Q

Stress that acts parallel to a reference surface.

A

Shear Stress

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23
Q

Stress vectors oriented along the principal stress directions, defined as sigma1 > sigma2 > sigma3.

A

Principal Stress

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24
Q

the non-hydrostatic stress or difference between the maximum and minimum principal stress (sigma1 > sigma2), being the diameter of the Mohr Circle.

A

Differential Stress

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25
also known as Deviatoric stress
Differential Stress
26
The force applied perpendicular to a surface of an object per unit area where the force is distributed.
Pressure
27
The pressure that is exerted by a fluid at equilibrium at a given point within the fluid, due to the force of gravity. This is a state of isotropic state of stress, where pressure is equal throughout, defined as 01 = 02 = 03.
Hydrostatic Pressure
28
The pressure applied by the weight of an overlying material and burial depth.
Lithostatic pressure
29
A component of deformation where every particle of a rock is moved in the same direction and distance, with its displacement field consisting of parallel M vectors of equal length.
Translation
30
A component of deformation where it is taken le as a rigid rotation that involves physical rotation of a rock bvolume relative to an external coordinate system.
Rotation
31
Any change in shape of the deformed rock volume
STRAIN
32
The difference between the position, shape and orientation of an object before and after the deformation.
Deformation
33
The ratio of the length of a rock mass before its deformation from its deformed state
Elongation
34
Stretching of a rock mass in one-dimension due to strain
Stretch
35
An equation associated with the Mohr Circle for strain
Quadratic Elongation
36
ONE-DIMENSIONAL STRAIN
Elongation , Stretch, Quadratic Elongation
37
TWO-DIMENSIONAL STRAIN
Angular Shear, Shear Strain
38
The change in angle between two originally perpendicular lines in a deformed medium.
Angular Shear
39
A dimensionless parameter that develops when differential movement occurs along a set of parallel lines
Shear Strain
40
a type of strain with three-dimensional change, where it is a ratio of values with the same units, hence, a dimensionless. Positive A represent volume gain, whereas negative A represent volume loss.
Volume Change
41
THREE-DIMENSIONAL STRAIN
Volume Change
42
A type of strain, that is a perfect coaxial deformation, that involves no internal rotation.
Pure SHear
43
A combination of Pure and Simple Shear.
Subsimple Shear
44
A combination of Simple Shear and Rigid rotation
Supersimple Shear
45
Deformed features in rock mass, where the original shape can be qualitatively compared to its presently deformed shape.
STRAIN MARKERS
46
Small, mostly sphorical features in fine grained sediments, where the red to brownish oxidized sediment has been chemically reduced to a greenish color.
Reduction spots
47
Among the most frequently used strain markers to indicate directions of the strain.
Pebbles
48
Preserved ancient lifeforms used in determining finite strain.
Fossils
49
Gas bubbles in volcanic rocks used in determining finite strain.
Vesicles
50
A graphical diagram that describes the shape of the strain ellipsoid by plotting the axial ratios X/Y and Y/Z as coordinates.
Flinn Diagram
51
A geometric construction for finding strain in two dimensions, typically demonstrated on fossils with orthogonal lines of symmetry in the undeformed state.
Wellman's Method
52
A method to determine the deformation of a rock mass that utilizes the systematic shape changes that occur in deformed ellipsoidal objects.
Rf/θ method
53
Uses the analysis of the distances between the centers of objects that are systematically related to the orientation of the finite strain ellipsoid.
Center-to-center Method
54
A simpler version of the center-to-center method, where it is done by manually tracing an overlay of coordinate origin per ellipsoid and a pair of reference axes on top of the sketch or photo of the section.
Fry Method
55
The study of the ability of stressed solid materials, as well as fluids and gases, to flow or deform due to strain rate, elasticity, and viscosity.
RHEOLOGY
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Materials that have properties that are the same throughout any sample size.
Homogenous Materials
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Materials that have properties that varies with location for either within a hand specimen, or on a regional scale, which leads to a scale- dependent rock behavior.
Heterogenous Material
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Materials that have the same properties in all directions.
Isotropic Materials
59
Materials that have properties that vary with direction.
Anisotropic materials -
60
___________ are strongly anisotropic to stress, but the degree of expression of the anisotropy depends on the direction in which the stress is oriented.
Layered materials
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Non-permanent or recoverable, instantaneous strain.
Elastic
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Permanent or non-recoverable strain, where deformation involves breaking of atomic bonds without losing material coherency.
Plastic
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Permanent strain that accumulates with time, where the strain rate-stress relationship is linear.
Viscous
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The reciprocal or opposite of viscosity.
Fluidity
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Elastic modulus, is an equation that measures the stiffness, or stretchability, of a material, defined as the ratio of stress (a) over strain (ε)
Young's Modulus
66
Rigidity modulus, is closely related to Young's modulus, is the elasticity coefficient for shearing or torsion force, being the equation that measures that rigidity of a material. Defined as the ratio of shear stress (0s) and shear strain (A):
Shear Modulus
67
The equation that relates the pressure change, AP, to volume change when pressure changes cause elastic deformation rather than directed force, calculating its compressibility
Bulk Modulus
68
An equation that expresses the relationship between volume change and stress, where the ratio of the proportional decrease in lateral measurement to the proportional increase in length in a sample material that is elastically stretched.
Poisson's Ratio
69
A type of rock material behavior describing the fluid-like behavior of rocks, hence, creates irreversible and permanent strain, and shows the relationship as the viscosity (1) between stress (a) and strain rate (7"), defined
VISCOUS BEHAVIOR
70
Stationary fluids that does not transmit shear stress.
Perfect Fluids
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The ideal type of viscous behavior, described as a linear viscous behavior, where "linear" is used to emphasize a distinction from nonlinear viscous behavior, having a linearly proportional relationship between differential stress and shear strain rate.
Newtonian Fluids
72
BEHAVIOR A type of rock material behavior describing permanent change in shape or size of a body without fracture, accumulated over time by a sustained stress beyond the elastic limit, or yield point, of the material.
PLASTIC (SAINT-VENANT) BEHAVIOR
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A perfect plastic material is one where the stress cannot rise above the yield stress and strain can continue to be accumulated forever without any change in the stress level.
PLASTIC (SAINT-VENANT) BEHAVIOR
74
Occurs when the rock becomes stronger or harder to deform when the stress necessary to deform the rock increases as the strain increases.
Strain hardening
75
Occurs when less stress is required to keep the deformation going.
Strain softening
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A combination of elastic and viscous behavior where elastoviscous materials accumulate strain from the moment a stress is applied, initially behaving elastically before gradually behaving in a viscous manner. 
ELASTOVISCOUS (MAXWELL) BEHAVIOR
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A combination of viscous and plastic behavior where viscoplastic materials flow as perfectly viscous materials, but only above a certain yield stress, a characteristic of plastic behavior.
VISCOPLASTIC (BINGHAM) BEHAVIOR
78
A combination of elastic and plastic behavior where stress and elastic strain acting on a material increase until the yield point is reached, beyond which the deformation is plastic.
ELASTIC-PLASTIC (PRANDTL) BEHAVIOR