Title: Engineering Properties of Rocks
1Engineering Properties of Rocks
- Associate Professor John Worden DEC
- University of Southern Qld
2Engineering 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.
3Engineering 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.
4Engineering 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.
5Engineering 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.
6Engineering 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.
7Engineering 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.
8Engineering 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 ().
9Engineering 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).
10Engineering 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.
11Engineering 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.
12Engineering 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.
13Engineering 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.
14Engineering 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.
15Engineering 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?)
16Engineering 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.
17Engineering 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.
18Engineering 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.
19Engineering 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.