Course CEE9577Rock Mechanics I Course CEE9577 Properties of Rocks Rock as an Engineering Material...
Transcript of Course CEE9577Rock Mechanics I Course CEE9577 Properties of Rocks Rock as an Engineering Material...
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Rock Mechanics ICourse CEE9577
Properties of Rocks
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Rock as an Engineering Material
Rock as an Engineering Material
• It differs from other engineering materials in that it containsdiscontinuities such as joints, bedding planes, folds, shear zones andfaults which render its structure discontinuous
• It could be broadly classified into two categories according to thel d it i fl th ll b h i f th kscale and its influence on the overall behaviour of the rock mass
Intact Rock• Continuum of polycrystalline solid between continuities consisting ofp y y g
an aggregate of minerals or grains. Its properties are governed bythe physical properties of the materials of which it is composed ofand the manner in which they are bonded to each other
Rock Mass• The in-situ medium which comprises intact rock blocks separated by
discontinuities. Rock masses are generally discontinuous and oftenhave heterogeneous and anisotropic properties.
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Simplified Representation of Transition fromIntact Rock to Heavily Jointed Rock Mass
Simplified representation of transition from intact rockto heavily jointed rock mass due to scale effect (after Hoek, 1995)
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Geological Classification of Intact Rock
Geological Classification of Intact Rock
( ) I t t R k R k f i i l(a) Intact Rock - Rock-forming minerals
Rock are composed of minerals. The common rock forming minerals are:
O th l f l Orthoclase felspar Plagioclase felspar Quartz Muscovite Bi tit Biotite Hornblende Augite Olivine C l it Calcite Dolomite Kaolinite Hematite
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Common Rock Forming Minerals
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Intact Rock – Elementary Rock Classification
(b) Intact Rock – Elementary Rock Classification
Intact rocks are classified into three (3) main groups according to processes by which they are formed:
• Igneous Rocks – formed by crystallization of molten magma Mode• Igneous Rocks – formed by crystallization of molten magma. Mode of crystallization at depth or by extrusion (rising from depth) and the rate of cooling affect the rock structure and crystal size
• Metamorphic Rocks formed as a result of metamorphism which is• Metamorphic Rocks – formed as a result of metamorphism which is the solid state conversion of pre-existing rocks by temperature, pressure or chemical changes
• Sedimentary Rocks sedimentary rocks are formed from the• Sedimentary Rocks – sedimentary rocks are formed from the consolidation of sediments. As a result of this process, sedimentary rocks almost invariably possess a distinct stratified, or bedded structure
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Geological Classification of Igneous Rocks
Geological Classification of Igneous Rocks
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Igneous Rocks in Thin Sections
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Mafic Igneous Rocks
Mafic minerals are usually dark in colour with high s..g (>3)
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Felsic Igneous Rocks
Felsic minerals are lighter in colourin colour with lower s.g. (<3)
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Geological Classification of Metamorphic Rocks
• Geological Classification of Metamorphic Rocks
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Metamorphic Rocks in Thin Sections
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Geological Classification of Sedimentary Rocks
Geological Classification of Sedimentary Rocks
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Sedimentary Rocks in Thin Sections
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Engineering Classification of Intact Rocks
Engineering Classification of Intact Rocks
• The engineering classification of intact rocks is based ofstrength and/or deformation properties of the rock.g p p
• According to the classification system recommended by theInternational Society of Rock Mechanics (ISRM 1978c)International Society of Rock Mechanics (ISRM 1978c),rock may range from extremely weak to extremely strongdepending on the unconfined compressive strength (orPoint Load Strength Index) or approximate fieldg ) ppidentification.
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Engineering Classification of Rocks by Strengthy g
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Engineering Classification of Intact Rocks by Strength and Deformation Properties
Engineering Classification of Intact Rocks by Strength and Deformation Properties (AfterDeformation Properties (After Deere and Miller, 1966)
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Index Properties of Intact Rocks
I d P ti f I t t R kIndex Properties of Intact Rocks
Index properties of rocks are generally determined in the laboratory or in the field to provide an initial quantitative description of the rocks. They can be used to estimate the mechanical and hydraulic properties of the rocks. However, determination of the index properties could not replace detailed characterization of the rocks.
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Common Laboratory Index Tests for Rock
• Unconfined (uniaxial) compression Primary index test for strength and deformability of intact rock; required input to rock mass classification systems.
• Point load test Indirect method to determine unconfined compressive (UC) strength; can be performed in the field on core pieces unsuitable for UC tests
• Water content Indirect indication of porosity of intact rock or clay p y ycontent of sedimentary rock.
• Unit weight and total porosity Indirect indication of weathering and soundness.
• Splitting strength of rock Indirect method to determine the tensile strength of (Brazilian tensile strength method) intact rock(Brazilian tensile strength method) intact rock.
• Durability (Slake durability) Index of weatherability of rock exposed in excavations.
• Specific gravity of solids Indirect indication of soundness of rock intended for use as riprap.
• Rebound number Index of relative hardness of intact rock cores.
• Permeability Intact rock (no joints or major defects).
• Petrographic examination Performed on representative cores of each significant• Petrographic examination Performed on representative cores of each significant lithologic unit.
• Specific gravity and absorption Indirect indication of soundness and deformability
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Typical Porosity Values of Intact Rocks
Porosity (n) – ratio of void or pore volume , Vv to the total volume, V of the rock. It is dimensionless and varies significantly forvaries significantly for different rock types or even for the same rock type due to different factors such as grain i di t ib ti isize distribution, grain
shape, depth and pressure
n = Vv/V
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Point Load Strength Index
The Point Load Strength Index is often used to provide a quick assessment of the uniaxial tensile and compressive strength of the rock and can easily be determined in the field or laboratory on rock lumps or cored samples.
Fig. 4.1
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Determination of Point Load Strength Index
Note: N-size core is 50mm dia.
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Determination of Uniaxial Tensile Strength from Point Load Strength Indexg
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Correlation Between Point Load Strength Index and Uniaxial Compressive Strengthp g
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Typical Values of Schmidt Hammer Rebound Numbers and Variation of Point Load Index
Typical Values of L-type Schmidt Hammer Rebound Numbers andHammer Rebound Numbers and Variation of Point Load Index with Schmidt Hammer Rebound Number
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Dynamic Elastic Constants
• The dynamic elastic constants of a solid material can be determined by measuring the propagation velocities of the material.
• For an isotropic solid, there are two types of body or free‐medium waves:
‐ a longitudinal or compression wave which travels with velocity Vp
‐ a shear or trasverse wave which travels with velocity Vs
• These velocities are related to the elastic constants by
E = Modulus of elasticity, G = Modulus of rigidity (or Shear modulus)ν= Poisson’s ratio , g = gravitational acceleration, γ= Unit weight of the material
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Dynamic Elastic Constants
G can be determined from the shear wave velocity, Vs ,without the knowledge of the Poisson’s ratio, ν. However the determination of the Elastic modulus E requires the value of ν. B d th l ti hiBased on the relationship:
Both the E and νcan be determined by the following equation:
Also from the relationshipAlso from the relationship
The bulk modulus K can be determinedThe bulk modulus K can be determined
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Range of P wave velocity and S Wave Velocity of Intact Rocks
Range of P wave velocity and S Wavevelocity and S Wave velocity of Intact Rocks
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Variation of P Wave Velocity with Porosity and Densitywith Porosity and Density
V i ti f P WVariation of P Wave Velocity with Porosity and Density
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Variation of Point Loand Index withP Wave Velocity and PorosityP Wave Velocity and Porosity
Variation of Point Load Index with P Wave Velocity and Porosityand Porosity
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Weathering Grade of Rock Mass
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Weathering State of Rock Shown in Rock Cores
Completely weatheredCompletely weatheredCompletely weatheredCompletely weathered
Highly weatheredHighly weathered
Moderately weatheredModerately weathered
Slightly weatheredSlightly weathered
FreshFresh
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Schematic Profile and Descriptions ofWeathering in RockWeathering in Rock
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Weathering Indices for Granite andRelationship between Weathering and RQDp g Q
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Total Porosity and Dry Density of Granitic Rocks at Different Weathering Stagesg g
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Jointing and Hydraulic Conductivity of Rock Formations in the Niagara Escarpment –Niagara Area
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Average Physical and Mechanical Properties of Rock Formations in the Niagara Escarpment –Niagara Area