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    Lecture 4 Index properties

    Longitudinal Velocity and Degree of Fissuring

    Uniaxial Compression

    Point Load Strength

    Shore Hardness

    Schmidt Hardness

    Brazilian Test

    4-point Beam Test

    Uniaxial Tension Test

    Rock Quality Designation

    Testing Mechanical Properties

    1 Uniaxial Compression Tests

    Direct test

    Load P

    Rock cylinder

    X-sectionarea = A

    Endcap

    Strain

    Gages E

    1Stress

    Axial

    Strain (1)Lateral

    Strain (2)

    12=2/1

    1

    C0 (failure)

    C0 : Uniaxial Compressive Strength

    E: Modulus of Elasticity

    : Poissons RatioAP

    Cpeak

    o =

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    Indirect test (Point LoadTest)

    Steel

    cones rock

    Hydraulic

    ram

    Testing Mechanical Properties1. Uniaxial Compressive Strength Tests

    Measurement of the Point LoadStrength Is and of the indirect C0

    A rock core is loaded diametrically between the tips oftwo hardened steel cones, causing failure through thedevelopment of tensile cracks parallel to the loadingdirection.

    2

    peak

    sD

    PI =

    The load at failure Ppeak is recorded and the pointload strength is calculated from:

    where D is the distance between the two cone tips.

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    Measurement of the point loadstrength Is and of the indirect C0

    The uniaxial compressive strength C0 is then indirectlyobtained by using the empirical relationship:

    where Is(50) is the point load strength of 50 mm (2 in.)diameter cores

    )50(soI24C =

    Testing Mechanical Properties (contd.)

    2. Hardness (also used as Indirect Uniaxial CompressiveStrength Tests)

    (a) Shore Scleroscope (b) Schmidt Hammer

    Rock

    specimen

    Graduated window showing the rebound of

    pellet or spring

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    Measurement of the Shore hardness HShore

    and the Indirect Determination of C0

    Shore hardness (HShore) is measured as the extent ofrebound of a steel bullet dropped from a specificheight onto the surface of a rock specimen.

    The harder the rock, the higher the bounce.

    An empirical correlation between rock hardness and

    its uniaxial compressive strength has been obtainedbased on a large number of tests on different rocks,and is given by:

    62.3H)ft/lb(000066.0)psi(ClogShore

    3

    dryo+=

    Measurement of the Schmidt hardnessHSmdt, and the Indirect Determination of C0

    The Schmidt Hammer is a portable tool, similar inprinciple to the Shore Scleroscope. It is usedexclusively for rock and rock-like materials and iseasy of use in the field. It measures the rebound offthe surface of rock of a spring-driven steel pellet.

    An empirical correlation between the Schmidt rockhardness and uniaxial compressive strength hasbeen obtained based on a large number of tests ondifferent rocks:

    16.3H)ft/lb(00014.0)psi(ClogSmdt

    3

    dry0+=

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    Testing Mechanical Properties (contd.)3. Tensile Strength Tests

    (a) Brazilian (indirect) Test

    Flat

    platens

    Rock

    disk

    (a) Measurement of the Brazilian

    tensile strength TB

    This is an indirect measurement of the tensilestrength of rock.

    A rock disk of uniform thickness is cut from a rockcore, and is loaded diametrically between upper andlower flat (or rounded) platens in a compressiontesting machine. Thus, a compressive line-load is

    applied to the disk.

    When the peak load Ppeak is reached the disk willtypically split along the loaded diameter.

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    Theoretical Stresses in Rock during

    Brazilian Test

    Stress Parallel to load is compressive at the edges and tensile in the middle.

    Stress perpendicular to the load is greater but rocks are stronger in compression than

    tension so the rock splits in tension.

    Measurement of the Braziliantensile strength TB (contd.)

    Theoretical analysis shows that uniform tensilestress develops along this diameter. The tensilestrength TB can be obtained from the elasticsolution:

    tD

    P2T peak

    B

    =

    where Ppeak is the load at failure, t and D are thethickness and diameter of the disk respectively.The ratio of t/D is 1/4 to 1/2.

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    L / 3 L / 3 L / 3

    P

    P / 2 P / 2

    D Rock Core

    3

    peak

    MRD3

    LP1T

    =

    (b) Four-point-beam modulus ofrupture (tensile strength) TMR.

    In this test a long rock core is flexured to failure. There are

    four contacting points dividing the core into three sections ofequal length. The middle section is under pure bending. Themaximum tensile stress occurs in the bottom layer of the

    middle section of the core, and this is where failure typicallyoccurs as P reaches Ppeak. This test determines the modulus of

    rupture (TMR) (beam flexural tensile strength). From the theoryof beams:

    Direct Uniaxial Tension Test Setup

    steam/water

    actuator

    Woods metal

    pull

    load cell

    specimen threaded bolts

    Difficult to attach

    sample ends and not

    bend the sample

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    Rock Mass Classifications

    Rock Mass Rating (see tables inIntroduction to Rock Mechanics)

    Strength of the rock

    Drill core quality (RQD)

    Groundwater conditions

    Joint and fracture spacing

    Joint characteristics

    Add values from the 5 tables to get total score

    Rock Strength

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    Rock Quality Designation

    Applies to NX core (2.125 diameter)

    Hi RQD few fractures in core

    Low RQD many fractures in core

    MidWest Geosciences

    Joint Spacing

    Can use drill core, if available

    Should consider joint set most

    likely to influence work

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    Joint Condition

    Groundwater Conditions

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    Geomechanics Classification of

    Rock Masses

    0-20Very Poor RockV

    21-40Poor RockIV

    41-60Fair RockIII

    61-80Good RockII

    81-100Very Good

    Rock

    I

    RMR Sum of

    Ratings from 5

    categories

    Description of

    Rock Mass

    Class