STRAIN RATE & RHEOLOGY                                  

Strain Rate=Strain per unit time

Time required to accumulate a given strain

Expressed as the elongation per time

Picture (12x12, 869 bytes) e= e/t= L-Lo/(Lot)= 

    =change in length/ (original length)(time)

Geologic strain rates typically ~ 10�12 - 10�15.

Note that 3.15 X 1013 seconds are in 1 my

 

Rheology- study of flow of matter

 

Ideal Materials: Elastic, Viscous, Plastic

 

 

1.Elastic Behavior- linear plot of stress vs strain. When stress is applied, strain is instantaneous; i.e., not time dependent. Furthermore, instantaneous recovery ensues upon removal of stress. Some rocks at shallow depths and for short periods of time, approach ideal elastic behavior during small magnitudes of deformation. Seismic waves are an example of elastic behavior. Recoverable or Reversible strain     Picture (20x40, 980 bytes)= (E)(Picture (14x40, 956 bytes)) Picture (363x288, 4.2Kb)

Picture (20x40, 980 bytes)= Stress    Picture (14x40, 956 bytes)= strain

Picture (14x40, 956 bytes)= Strain= elongation of a line= 

Picture (14x40, 956 bytes)= change in length/ original length of line

 

E= Young�s Modulus of Elasticity= constant of proportionality that describes the slope of the line  

Young's modulus (constant;stress vs strain slope line) is a measure of resistance to elastic distortion.

E~ 10�11 Pa for crustal rocks. As E increases, the slope becomes steeper, i.e. the rock is  �stiffer�.Picture (531x288, 7.8Kb)

Elastic behavior is also known as Hookean behavior in which stress is proportional to strain.


Elastic Behavior may also be described for shear strain and volume change:

Shear Strain        Picture (20x40, 980 bytes)s= GPicture (13x40, 950 bytes)                   

G=rigidity or resistance to change in shape (constant of proportionality)

 Picture (13x40, 950 bytes)= shear strain

Dilation Picture (20x40, 980 bytes)= K (V-Vo)/Vo

 

K= Bulk Modulus= ratio of the pressure change to the resultant dilation

 

K=Picture (20x40, 991 bytes)p/Picture (20x40, 991 bytes)v = change in pressure divided by change in volume

 

Bulk Modulus (K)= incompressibility

incompressibility= measure of resistance to change in shape

Poissons Ratio   v=-Picture (14x40, 956 bytes)1 / Picture (14x40, 956 bytes)3                    

Picture (14x40, 956 bytes)1= elongation normal to compressive stress

Picture (14x40, 956 bytes)3= elongation parallel to compressive stress

 

Check out the following website:

http://silver.neep.wisc.edu/~lakes/Poisson.html

 

Akin to Bulk Modulus (K), Poisson's ratio (v, nu) is another means to describe the relationship between volume change and stress. v may range from 0- 0.5 (compressible (0) to (0.5) incompressible). Incompressible materials maintain constant volume regardless of the stress applied. Most rocks have a Poisson's ratio ~0.25-0.35. Poisson's ratio describes the ability of a material to shorten parallel to Picture (20x40, 980 bytes)1 without corresponding elongation in the Picture (20x40, 980 bytes)3 direction.

 

2.Viscous Strain- Stress is proportional to strain rate (Newtonian behavior; not really observed in rocks); characteristic of some fluids. Low viscosity fluids deform more rapidly than high viscosity fluids, under a given set of conditions. No critical stress value is required to achieve strain. The constant of proportionality is the viscosity of the fluid. Permanent strain

Picture (20x40, 980 bytes)=Picture (13x40, 950 bytes)Picture (20x40, 979 bytes)= Stress= (shear strain rate)(Viscosity)                             

 Picture (363x288, 4.5Kb)    Picture (478x288, 7.6Kb)

                 

3.Plastic Behavior- continuous deformation after some critical stress (Picture (31x63, 1.1Kb)c) value is achieved and maintained. Many rocks exhibit plastic behavior. Permanent Strain             Picture (396x288, 3.9Kb)

 

Three Megascale Types of Deformation-

Visible effects of strain in rocks are usually of plastic or rupture variety as elastic strain produces little long term features.

a.Elastic Deformation

b.Plastic Deformation

c.Rupture Deformation

Elastic Deformation-Occurs when a body is deformed in response to a stress, but returns to its original shape when stress is removed. Stress is totally reversible or recoverable.

 

Viscoelastic (Anelastic) Strain- strain totally recoverable but not instantaneous recovery; time dependent, describe in terms of strain rate. Most rocks have elastic and anelastic properties at small stress magnitudes.

 

Plastic Deformation- Irreversible strain without visible fractures. Stress is applied to a rock body and deformation occurs. When stresses are removed, a portion of the strain remains. That portion of the rock that is deformed has experienced plastic strain. Permanent plastic deformation precludes visible fractures. Material deforms but does not break and produce visible fractures. Microscopic fracturing may occur, however. Plastic strain is not recoverable or reversible.

 

Rupture Deformation- visible fractures form. Irreversible, not recoverabe strain. Material loses cohesion.

 

 

Terms describing Behavior of Materials during Deformation:

Ductile- Rocks experience large amounts of plastic deformation before rupturing.

Plastic-flow without mesoscopic brittle behavior

 

Brittle- Rocks that exhibit elastic behavior followed by rupture.

Rupture- loss of cohesion; occurs prior to significant amounts of plastic deformation.

 

Elastic Limit- ductile rocks deform elastically to a point (stress value of which is the yield strength), beyond this point, plastic deformation ensues with increasing stress.

 

Rupture point- (rupture strength) brittle rocks experience elastic deformation until a rupture point is attained, whereat the rock deforms by brittle rupture.

 

Failure- point when a brittle rock loses all resistance to stress and crumbles.

Failure is difficult to discern in plastic deformation.

 

Ultimate Strength- maximum stress that a rock can support before failure.

 

Competency- relative term that compares the resistance of rocks to flow.

 

Generalized Stress-Strain Curve for Rocks

Picture (489x288, 5.9Kb)

 

Brittle Rocks- exhibit elastic behavior before rupture

 Picture (389x326, 7.2Kb)

Ductile Rocks- exhibit elastic-plastic behavior  before rupture

Picture (413x288, 6Kb)

 

Rock Tests = Stress - Strain Behavior

 

Triaxial Test- used to simulate behavior of rocks at depth. A cylindrical sample is enclosed in a jacket through which a radial confining pressure can be applied using gases or liquids. An axial load is then applied. Repeated tests are conducted to determine failure at different axial (normal) and confining (shear) values. Thus a failure envelope may be constructed on a Mohr's diagram by constructing tangential lines to Mohr's circle representing the failure values for each test result. Note that failure does not occur at the maximum shear level.

 

Effects of Confining Pressure (Pc): The unconfined compression test is applicable to rock engineering where rock masses are exposed at the Earth�s surface. However, in the design of tunnels, mines, or other underground excavations (waste repositories), confining pressures are important. At depth, the minimum principal stress is Picture (20x40, 980 bytes)3 is no longer zero as in unconfined compression tests.

 

Pc= Picture (18x40, 985 bytes) g h          

Picture (18x40, 985 bytes)= density                                                          

Pc= lithostatic pressure

       g= gravity

       h= depth

 

Confining pressure- due to the weight of the surrounding rock. Unlike hydrostatic pressure which is equal in all directions, lithostatic pressure is not always equal in all directions. The principal compressive stress Picture (20x40, 980 bytes)1 may be oriented vertically or laterally.

 

As confining pressure increases:

1.Rock strain proceeds from brittle to ductile behavior. Ductile deformation dominates at Pc > 700 kg/cm2.

2.Higher confining pressures resists opening of fractures

2.Rock strength increases (greater amounts of strain accumulate before failure occurs).

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Rock strength decreases with:

1.Increasing temperatures (reduces rock strength and increases ductility)

2.decreasing strain rate (increasing time); rocks more ductile at lower strain rates.

3.Foliations

4.Increased porosity

5.Presence of water

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Effective Pressure= Pc-Pf                 

     Pc= confining pressure

    Pf= fluid pressure

 

 

Work Hardening- Stress necessary to continue deformation increases as strain increases

Work Softening- Stress necessary to continue deformation decreases as strain increases

Thus, Rock Strength determined by:

  Degree of interlocking of mineral grains

                Presence of discontinuities

                Degree of weathering

                Mineral properties

                Climate

                Grain size and variability

                Rock density

                Cementation and compaction

and          temperature

                confining pressure

                fluid pressure

                porosity

                time (strain rate)

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