coulomb stress - web.itu.edu.trcakirz/teaching/neotectonics/neotectonics_ch11.pdf · mohr circle a...

25
1/25 COULOMB STRESS COULOMB STRESS

Upload: vophuc

Post on 29-Jul-2019

265 views

Category:

Documents


0 download

TRANSCRIPT

  • 1/25

    COULOMB STRESSCOULOMB STRESS

  • 2/25

    cracks form cracks coalesce

  • 3/25

    3

    P

    1

    (1 + 3 )

    (1 - 3 )

    (1 - 3 )2 2

    2

    n

    s

    point P represents a plane that is degrees from 3plots 2 counterclockwise from 1 (note original diagram in upper right)

    s

    n

    1

    3

    D

    Mohr circle

    A

    BC

    sP

    nP

    normal and shear stresses on point P are nP and sP, respectivelynP = 1/2(1 - 3 ) + 1/2(1 - 3 )cos 2sP = 1/2(1 - 3 ) sin 2

    13

    P: plane to left

  • 4/25

    conduct triaxial loading experiments to determine applied stress at which sample breaks

    c

    a a= axial stress, 1c= confining stress, 3

    first experiment set confining pressure low and increaseaxial load (stress) until sample breaks

    second experiment set confining pressure higher and increaseaxial load (stress) until new sample breaks

    keep repeating experiments

  • 5/25

    you will generate a series of pairs of confining stresses andassociated axial stresses at which samples break

    40 540 500 MPa150 800 650 MPa400 1400 1000 MPa

    ac

    we use these as 1 and 3 and plot Mohr circles

    get a sequence of circlesoffset from one another

    a- c s

    500

    500

    1000n

    1500

    diameters are stress difference;centers are stress sum/2

  • 6/25

    s

    n500

    500

    1000 1500

    Mohr circles that definestress states wheresamples fracture

    (critical stress states) together define the

    failure envelopefor a particular rock

    failure envelope

    failure envelope is tangent to circles of all critical stress statesand is a straight line

  • 7/25

    what does this straight line mean?

    corresponds to Coulomb fracture criterion

    Charles Coulomb in 18th century proposed that formation ofshear stress parallel to failure relates to normal stress by

    s = C + tan (n) (empirical)

    s = shear stress parallel to fracture at failureC = cohesion of rock (constant)n = normal stress across shear zone at instant of failuretan = = coefficient of internal friction (constant of proportionality)

    this has form of y = mx + b (equation of a line)

    y = s x = n b = intercept on s axis m = slope = tan =

    so Coulomb criterion plots as straight line on n , s plot

  • 8/25

    suppose 1 is oriented east-west, horizontal, and equal to 40 MPa

    3 is vertical and equal to 20 MPa

    determine normal and shear stresses on a fault plane thatstrikes north-south and dips 55 west

    5540 MPa

    20 MPaangle, , between 3 and fault plane is 35;

    2 = 70

    1

    3

    but which direction on Mohr circle?

    55

    35

    3

  • 9/25

    convention for shear stresses for Mohr circle diagram: sinistral is considered positive (+) dextral considered negative (-)

    positive (sinistral) negative (dextral)

    1

    3

    our example is dextral andthus, negative

  • 10/25

    to construct Mohr circle, we know

    1 is equal to 40 MPa3 is equal to 20 MPa

    2 = 70 and is negative

    10

    20 4070

    10 n= 33.4 s = -9.4

    P

    n

    s

    1 + 32

    distance from origin of center of circle(40+20)/2=30

    1 - 3 diameter of circle: 40-20=20

  • 11/25

  • 12/25

    stress acts on every surface that passes through the pointwe can use three mutually perpendicular planes to describe

    the stress state at the point, which we approximate as a cube

    each of the three planeshas one normal component

    & two shear components

    therefore, 9 components necessaryto define stress at a point

    3 normal6 shear

    convention for describing: iji= plane on which component acts (defined by perpendicular)j = axis to which component is parallel

    i = 1, 2, 3 j=1, 2, 3

  • 13/25

    the nine components (six of which are independent) can be writtenin matrix form:

    11 12 13

    21 22 23

    31 32 33

    ij =

    this is the stress tensor

    describing stress as tensor allows relative ease of manipulation;can change reference frame (rotation; translation)

    components on diagonal are normal stresses; off are shear stresses

  • 14/25

  • 15/25

  • 16/25

  • 17/25

  • 18/25

  • 19/25

    Earthquake ruptures before the Izmit earthquakeEarthquake ruptures before the Izmit earthquake

  • 20/25

    Coulomb stress field prior to the Izmit earthquakeCoulomb stress field prior to the Izmit earthquake

  • 21/25

    Resolved stresses on the Izmit and Dzce faults before August 99Resolved stresses on the Izmit and Dzce faults before August 99

  • 22/25

    Coulomb stress with varying coefficient of friction valuesCoulomb stress with varying coefficient of friction values

  • 23/25

    Coulomb stress changes due to the Izmit earthquakeCoulomb stress changes due to the Izmit earthquake

  • 24/25

    Stress changes on the Dzce fault due to the previous earthquakeStress changes on the Dzce fault due to the previous earthquakess

  • 25/25

    Present day Coulomb stress changes due to the past earthquakesPresent day Coulomb stress changes due to the past earthquakes

    2