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Engineering Properties of Rocks

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Title: Engineering Properties of Rocks


1
Engineering Properties of Rocks
  • Associate Professor John Worden DEC
  • University of Southern Qld

2
Engineering Properties of Rocks
  • At this point in your course, you should
    appreciate that rock properties tend to vary
    widely, often over short distances.
  • A corollary of this is that during Engineering
    practice, the penalties for geologic mistakes can
    be severe.
  • We will therefore briefly review factors that
    quantise rocks.
  • The study of the Engineering Properties of Rocks
    is termed Rock Mechanics, which is defined as
    follows
  • The theoretical and applied science of the
    mechanical behaviour of rock and rock masses in
    response to force fields of their physical
    environment.
  • It is really a subdivision of Geomechanics
    which is concerned with the mechanical
    responses of allgeological materials, including
    soils.

3
Engineering Properties of Rocks
  • During Engineering planning, design and
    construction of works, there are many rock
    mechanics issues such as
  • Evaluation of geological hazards
  • Selection and preparation of rock materials
  • Evaluation of cuttability and drillability of
    rock
  • Analysis of rock deformations
  • Analysis of rock stability
  • Control of blasting procedures
  • Design of support systems
  • Hydraulic fracturing, and
  • Selection of types of structures.
  • For this lecture we will confine our study to
    thefactors that influence the deformation and
    failureof rocks.

4
Engineering Properties of Rocks
  • Such factors include
  • Mineralogical composition and texture
  • Planes of weakness
  • Degree of mineral alteration
  • Temperature and Pressure conditions of rock
    formation
  • Pore water content, and
  • Length of time and rate of changing stress that a
    rock experiences.
  • Mineralogical Composition and Texture.
  • Very few rocks are homogeneous, continuous,
    isotropic (non directional) and elastic.
  • Generally, the smaller the grain size, the
    stronger the rock.

5
Engineering Properties of Rocks
  • Texture influences the rock strength directly
    through the degree of interlocking of the
    component grains.
  • Rock defects such as microfractures, grain
    boundaries, mineral cleavages, twinning planes
    and planar discontinuities influence the ultimate
    rock strength and may act as surfaces of
    weakness where failure occurs.
  • When cleavage has high or low angles with the
    principal stress direction, the mode of failure
    is mainly influenced by the cleavage.
  • Anisotropy is common because of preferred
    orientations of minerals and directional stress
    history.
  • Rocks are seldom continuous owing to pores and
    fissures (i.e. Sedimentary rocks).
  • Despite this it is possible to support
    engineering decisions with meaningful tests,
    calculations, and observations.

6
Engineering Properties of Rocks
  • Temperature and Pressure
  • All rock types undergo a decrease in strength
    with increasing temperature, and an increase in
    strength with increasing confining pressure.
  • At high confining pressures, rocks are more
    difficult to fracture as incipient fractures are
    closed.
  • Pore Solutions
  • The presence of moisture in rocks adversely
    affects their engineering strength.
  • Reduction in strength with increasing H2O content
    is dueto lowering of the tensile strength, which
    is a functionof the molecular cohesive strength
    of the material.
  • Time-dependent Behavior
  • Most strong rocks , like granite show little
    time-dependent strain or creep.

7
Engineering Properties of Rocks
  • Since there are vast ranges in the properties of
    rocks, Engineers rely on a number of basic
    measurements to describe rocks quantitatively.
    These are known as Index Properties.
  • Index Properties of Rocks
  • Porosity- Identifies the relative proportions of
    solids voids
  • Density- a mineralogical constituents parameter
  • Sonic Velocity- evaluates the degree of
    fissuring
  • Permeability- the relative interconnection of
    pores
  • Durability- tendency for eventual breakdown of
    components or structures with degradation of
    rockquality, and
  • Strength- existing competency of the rock fabric
    binding components.

8
Engineering Properties of Rocks
  • Porosity Proportion of void space given by- n
    ?p/ ?t , where ?p is the pore volume and ?t is
    the total volume. Typical values for sandstones
    are around 15. In Igneous and Metamorphic
    rocks, a large proportion of the pore space
    (usually lt 1-2) occurs as planar fissures.With
    weathering this increases to gt 20. Porosity is
    therefore an accurate index of rock quality.
  • Density Rocks exhibit a greater range in density
    than soils. Knowledge of the rock density is
    important to engineering practice. A concrete
    aggregate with higher than average density can
    mean a smaller volume of concrete required for a
    gravity retaining wall or dam. Expressed as
    weight per unit volume.
  • Sonic Velocity Use longitudinal velocity Vl
    measured on rock core. Velocity depends on
    elastic properties and density,but in practice a
    network of fissures has an overriding effect.Can
    be used to estimate the degree of fissuring of a
    rock specimen by plotting against porosity ().

9
Engineering Properties of Rocks
  • Permeability As well as the degree of
    interconnection between pores / fissures, its
    variation with change in normal stress assesses
    the degree of fissuring of a rock. Dense rocks
    like granite, basalt, schist and crystalline
    limestone possess very low permeabilities as lab
    specimens, but field tests can show significant
    permeability due to open joints and fractures.
  • Durability Exfoliation, hydration, slaking,
    solution, oxidation abrasion all lower rock
    quality. Measured by Franklin and Chandras
    (1972) slake durability test. Approximately 500
    g of broken rock lumps ( 50 g each) are placed
    inside a rotating drum which is rotated at 20
    revolutions per minute in a waterbath for 10
    minutes. The drum is internally divided by
    asieve mesh (2mm openings) and after the 10
    minutesrotation, the percentage of rock (dry
    weight basis) retainedin the drum yields the
    slake durability index (Id). A sixstep ranking
    of the index is applied (very high-very low).

10
Engineering Properties of Rocks
  • Strength- Use Point Load Test of Broch and
    Franklin (1972). Irregular rock or core samples
    are placed between hardened steel cones and
    loaded until failure by development of tensile
    cracks parallel to the axis of loading.
  • IS P/D2 , where P load at rupture D distance
    between the point loads and I s is the point load
    strength.
  • The test is standardised on rock cores of 50mm
    due to the strength/size effect
  • Relationship between point load index (I s) and
    unconfined compression strength is given by q u
    24I s (50) where q u is the unconfined
    compressive strength, and I s (50) is the point
    load strength for 50 mm core.
  • All of the above are measured on Lab specimens,
    not rock masses/ outcrops, which will differ due
    to discontinuities at different scales.

11
Engineering Properties of Rocks
  • Engineering Classification Systems for Rock
  • Use of classification systems for rock remains
    controversial.
  • Bieniawskis Geomechanics system uses a rock mass
    rating (RMR) which increases with rock quality
    (from 0-100). It is based on five parameters
    namely, rock strength drill core quality
    groundwater conditions joint and fracture
    spacing, and joint characteristics. Increments
    from all five are summed to determine RMR.
  • While point load test values give rock strength,
    drill corequality is rated according to rock
    quality designation(RQD) introduced by Deere
    (1963). The RQD of a rockis calculated by
    determining the percentage of core in lengths
    greater than twice its diameter.
  • Spacing of Joints is determined from available
    drill core.

12
Engineering Properties of Rocks
  • It is assumed that rock masses contain three sets
    of joints, but the spacing of the most critical
    for the application is used.
  • Condition of joints is treated similarly. Covers
    the roughness and nature of coating material on
    joint surfaces, and should be weighted towards
    the smoothest and weakest joint set.
  • Ground water can exert a significant influence on
    rock mass behavior. Water inflows or joint water
    pressures can be used to determine the rating
    increment as either completely dry moist water
    under moderate pressure, or severe water
    problems.
  • Bieniawski recommended that the sum of these
    ratingsbe adjusted to account for favorable or
    unfavorable jointorientations. No points are
    subtracted for very favorablejoint orientations,
    but ? 12 points for unfavorable joint
    orientations in tunnels, and ? 25 points in
    foundations.

13
Engineering Properties of Rocks
  • Deformation and Failure of Rocks
  • Four stages of deformation recognised
  • Elastic
  • Elastico-viscous
  • Plastic, and
  • Rupture.
  • All are dependent on the elasticity, viscosity
    and rigidity of the rock, as well as temperature,
    time, pore water, anisotropy and stress history.
  • Elastic deformation disappears when responsible
    stressceases. Strain is a linear function of
    stress thus obeyingHookes law, and the constant
    relationship between themis referred to as
    Youngs modulus (E).
  • Rocks are non ideal solids and exhibit hysteresis
    during unloading.

14
Engineering Properties of Rocks
  • The elastic limit, where elastic deformation
    changes to plastic deformation is termed the
    Yield Point. Further stress induces plastic flow
    and the rock is permanently strained.
  • The first part of the plastic flow domain
    preserves significant elastic stress and is known
    as the elastico-viscous region. This is the
    field ofcreepdeformation. Solids are termed
    brittleor ductiledepending on the amount of
    plastic deformation they exhibit. Brittle
    materials display no plastic deformation.
  • The point where the applied stress exceeds the
    strength of the material is the ultimate
    strength and rupture results.
  • Youngs modulus (E) is the most important
    elasticconstant derived from the slope of the
    stress-strain curve.Most crystalline rocks have
    S-shaped stress-strain curvesthat display
    hysteresis on unloading. E varies with the
    magnitude of the applied stress and transient
    creep.
  • Deere and Miller (1966) identified six
    stress-strain types.

15
Engineering Properties of Rocks
  • Brittle Failure
  • Sudden loss of cohesion across a plane that is
    not preceded by any appreciable permanent
    deformation.
  • For shear failure, Coulombs Law applies ? c
    ? n tan ? , where ? the shearing stress c
    the apparent cohesion ? n the normal stress
    and ? the angle of internal friction or
    shearing resistance. see diagram.
  • For triaxial conditions ? 0.5 (? 1 ? 3)
    0.5 (? 1 -? 3 ) cos 2? and,? 0.5 (? 1 - ? 3)
    sin 2? , where ? 1 stress at failure , ? 3
    confining pressure .
  • Substitution for ? n and ? in the Coulomb
    equation 2c ? 3 sin 2? tan ? (1-
    cos 2?)?1 -----------------------------------
    ---------- sin 2? - tan ? ( 1
    cos 2?)

16
Engineering Properties of Rocks
  • As ? 1 increases, there will be a critical plane
    on which the available shear strength is first
    reached. For this critical plane, sin 2? cos
    2?, and cos 2 ? sin ? so the above equation
    reduces to 2c cos ? ? 3 (1 sin
    ?)
    ? 1
    ----------------------------------

    1- sin ?
  • As per Coulombs hypothesis, an apparent value
    of the uniaxial tensile stress, ?1 can be
    obtained from ? 1 2 cos ? / 1 sin ? ,
    but measured values of tensile strength are
    generally lower than those predicted by the
    equation.
  • For rocks with linear relationships between
    principalstresses at rupture, there is
    agreement, but most rocksare non linear. Perhaps
    this is due to increasing frictionalgrain
    contact as pressure increases?
  • Theoretical direction of shear failure is not
    always inagreement with experimental
    observations, nor does it occur at peak strength.

17
Engineering Properties of Rocks
  • Mohr (1882) modified Coulombs concept. Mohrs
    hypothesis states that when a rock is subjected
    to compressive stress, shear fracturing occurs
    parallel to those two equivalent planes for which
    shearing stress is as large as possible whilst
    the normal pressure is as small as possible.
  • Griffith (1920) claimed that minute cracks or
    flaws, particularly in surface layers reduced the
    measured tensile strengths of most brittle
    materials to less than those inferred from the
    values of their molecular cohesive forces.
    Although the mean stress throughout the body may
    be relatively low, local stresses in the vicinity
    of flaws were assumed to attain values equal to
    the theoretical strength.
  • Under tensile stress, stress magnification around
    a flaw is concentrated where the radius of
    curvature is smallest, ie at its end.
  • Concentration of stress at the ends of flaws
    causes themto enlarge and presumably develop
    into fractures.

18
Engineering Properties of Rocks
  • Brace (1964) demonstrated that fracture in hard
    rocks was usually initiated in grain boundaries,
    which can be regarded as inherent flaws under
    Griffiths theory.
  • Subsequently Hoek (1968) determined that modified
    Griffith theories while adequate for prediction
    of fracture initiation in rocks, could not
    describe their propagation and subsequent failure
    of rocks.
  • Hoek and Brown (1980) reviewed published data on
    the strength of intact rock and developed an
    empirical equation (subsequently modified in
    1997) that allows preliminary design calculations
    to be made without testing, by using an
    approximate rock typedependent value (m I ), and
    determining a value of unconfined compressive
    strength.
  • Lastly we will briefly examine the Deere and
    Miller (1966) classification of intact rock.

19
Engineering Properties of Rocks
  • Deere and Miller (1966) Classification of intact
    rock
  • Any useful classification scheme should be
    relatively simple and based on readily
    measurable physical properties.
  • Deere and Miller based their classification on
    unconfined (uniaxial) compressive strength (? 1)
    and Youngs Modulus (E) or more specifically, the
    tangent modulus at 50 of the ultimate strength
    ratioed to the unconfined compressive strength
    (E/? 1 ).
  • Rocks are subdivided into five strength
    categories on a geometric progression basis very
    high high medium low -very low.
  • Three ratio intervals are employed for the
    modulus ratiohigh medium low.
  • Rocks are therefore classed as BH (high strength-
    highratio) CM (medium strength medium ratio),
    etc.
  • This data should be included with lithology
    descriptions and RQD values.
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