Upload
kapola
View
215
Download
0
Embed Size (px)
Citation preview
8/8/2019 ASCEsem1txt (1)
1/38
Rock Engineering Basics
Rock: compact, indurated natural material (composed of oneor more minerals) that requires drilling, blasting, wedging, orother brute force to excavate.
Rock Substance: solid rock material which does not containobvious structural features (discontinuities) and which usuallycan be sampled and tested in the lab; known as intact rock.
Rock Mass: a complex system of natural rock materialcomprised of blocks of intact rock and structural features(discontinuities) that allow for interactions among the blocks;too large and complex to sample and test in the lab
8/8/2019 ASCEsem1txt (1)
2/38
8/8/2019 ASCEsem1txt (1)
3/38
Geologic Info for Rock Slope Engineering
1. Geologic mapping of formations and units needed togenerate surface-geology maps and cross-sections
2. Site topography and proposed cut-slope geometries (best to
display cross-sections 1:1 with no vertical exaggeration)
8/8/2019 ASCEsem1txt (1)
4/38
8/8/2019 ASCEsem1txt (1)
5/38
Geologic Info for Rock Slope Engineering
1. Geologic mapping of formations and units needed togenerate surface-geology maps and cross-sections
2. Site topography and proposed cut-slope geometries (best to
display cross-sections 1:1 with no vertical exaggeration)
3. Relevant rock-strength data for the rock substance
4. Engineering properties of rock discontinuities, includingorientation, geometry, shear strength
5. Groundwater regime (water table, piez. head distributions)
8/8/2019 ASCEsem1txt (1)
6/38
8/8/2019 ASCEsem1txt (1)
7/38
8/8/2019 ASCEsem1txt (1)
8/38
8/8/2019 ASCEsem1txt (1)
9/38
Uniaxial Compressive Strength
A cylinder of rock taken from drill-core is cut square on theends, then the ends are ground smooth, and the specimenloaded to failure in a testing machine. The length-to-diameterratio (L/d) typically ranges between 2 and 3.
UCS = Pf / A (stress units of psi, psf, MPa, tsm)
where: Pf = ultimate failure load (at rupture);
A= cross-sectional area of the cylindrical specimen
= Td2/4
8/8/2019 ASCEsem1txt (1)
10/38
Reporting of UCS Standardized Results
Empirical corrections of the tested value of UCS tostandardized L:d values are given below:
For L:d of 2:1
UCS2:1 = UCS / [0.88 + 0.24(d/L)]
For L:d of 1:1
UCS1:1 = UCS / [0.778 + 0.222(d/L)]
8/8/2019 ASCEsem1txt (1)
11/38
Point Load Index
The point load test is conducted on a piece of drill core (withragged ends) with L/d > 1.5 whereby the core piece is loadedperpendicular to the core axis between cone-shaped platensuntil failure occurs and the core is split. The core diameterand instrument gage pressure at failure are recorded. The
Point Load Index then is given by:
PtL = Pg(Ar) / d2
where: d= core diameter, Pg = instrument gage pressure atspecimen failure, and Ar = cross-sectional area of instrument
loading ram.
8/8/2019 ASCEsem1txt (1)
12/38
8/8/2019 ASCEsem1txt (1)
13/38
8/8/2019 ASCEsem1txt (1)
14/38
Using PtLto Estimate UCS
UCS $ PtL(14 + 0.175d)
for d measured in units of mm
For typical core diameters (47 61 mm), use the
approximation:
UCS $ 23(PtL)
8/8/2019 ASCEsem1txt (1)
15/38
Estimating UCS Using a SchmidtHammer
A Schmidt Type-L rebound hammer can be used toapproximate the UCS. A reas onable estimate of therock unitweightalso is needed.
Rebound measurements often are qui te variable, s othe field investigation should include at least 10measurements at a given sampling site (for averagingpurposes).
8/8/2019 ASCEsem1txt (1)
16/38
Brazilian Disk Tension Testing
A small disk of rock core with known diameter (d) andthickness (h) is loaded along its diameterto induce anapparent tensile stress field and cause the disk torupture. T he tensile strength then is given by:
T = 2(Pf) / (Tdh)
where Pf = failure load atwhich the disk ruptured
A general rule-of-thumb: (10 x T) $ UCS
8/8/2019 ASCEsem1txt (1)
17/38
Mapping & Display of Discontinuity Data
Field mapping methods to obtain information on discontinuityorientations, spacing, length, roughness, etc.:
Scanline mapping detailed mapping of individual discontin-
uities that intersect a designated mapping line or linearwindow
8/8/2019 ASCEsem1txt (1)
18/38
8/8/2019 ASCEsem1txt (1)
19/38
8/8/2019 ASCEsem1txt (1)
20/38
Mapping & Display of Discontinuity Data
Field mapping methods to obtain information on discontinuityorientations, spacing, length, roughness, etc.:
Scanline mapping detailed mapping of individual discontin-
uities that intersect a designated mapping line or linearwindow
Fracture-Set mapping (Cell mapping) mapping of fracture-set properties observed within user-defined cells on the rockexposure
8/8/2019 ASCEsem1txt (1)
21/38
Mapping & Display of Discontinuity Data
Field mapping methods to obtain information on discontinuityorientations, spacing, length, roughness, etc.:
Scanline mapping detailed mapping of individual discontin-
uities that intersect a designated mapping line or linearwindow
Fracture-Set mapping (Cell mapping) mapping of fracture-set properties observed within user-defined cells on the rockexposure
Oriented core logging mapping of oriented drill core toobtain orientations, fracture spacings, roughness
8/8/2019 ASCEsem1txt (1)
22/38
8/8/2019 ASCEsem1txt (1)
23/38
8/8/2019 ASCEsem1txt (1)
24/38
8/8/2019 ASCEsem1txt (1)
25/38
8/8/2019 ASCEsem1txt (1)
26/38
8/8/2019 ASCEsem1txt (1)
27/38
Display of Discontinuity Orientations
The orientations of planar discontinuities are best displayedand evaluated by plotting their poles (normals) on lower-hemisphere stereographic projections (known as stereonetplots). A cluster of such poles then represents a fracture sethaving planes in similar orientations.
W
N
E
S
+ + + +
+ + + + + ++ + +
+ +
+
+ + +
+ +++ +
+ +
+ + +
++
Example of lower-hemis. stereonet plot of fracture poles.
8/8/2019 ASCEsem1txt (1)
28/38
Display of Discontinuity Orientations
Poles near the center of the stereonet are for shallow-dipping(fairly flat) fractures, and poles near the outer edge of thestereonet are for steeply dipping fractures.
Thus, a cluster of fracture poles in the upper-right portion ofthe lower-hemisphere stereonet plot indicates a fracture setwith planes dipping toward the southwest.
8/8/2019 ASCEsem1txt (1)
29/38
ShearStrength Modeling for Discontinuities
1. Linear Mohr-Coulomb failure envelope with y-intercept(known as cohesion) and slope (known as the coefficientof friction, tanJ):
X = c + Wn tanJ
where: X = shear strength along the discontinuity;
Wn = effective normal stress acting on the discontinuity;c = cohesion (generally equal to zero or a very small
value for clean rock fractures);
J = friction angle.
8/8/2019 ASCEsem1txt (1)
30/38
ShearStrength Modeling for Discontinuities
2. General nonlinear, power-curve model:
X = c + a(Wn )b
where: X = shear strength along the discontinuity;
Wn = effective normal stress acting on the discontinuity;
a, b, c = power-curve parameters.
Note that when b = 1.0, this model reduces to a linear modelwith the parameter a = tanJ. Therefore, this general
model also covers the special case of the linear model.
8/8/2019 ASCEsem1txt (1)
31/38
ShearStrength Modeling for Discontinuities
3. JRC model of shear strength (nonlinear model):
X = Wn tan[(JRC)log10(JCS/Wn) + Jb]
where: X = shear strength along the discontinuity;
Wn = effective normal stress acting on the discontinuity;
JRC = joint roughness coefficient (typ. values: 2 to 6);
JCS = joint-wall compressive strength (UCS of intact rock);
Jb = base friction angle (i.e., for saw-cut, smooth surfaces).
8/8/2019 ASCEsem1txt (1)
32/38
ShearStrength Modeling for Discontinuities
4. Back-analysis of a rock-slope failure with well-defined geometry and groundwater conditions:
We set the FOS equal to 1.0, and back-calculate thecorresponding combinations of J and waviness that seemappropriate (linear shear-strength model with zerocohesion). We can follow the same approach with the JRC
model of shear strength (select appropriate values of Jb,JCS, and JRC that give FOS = 1.0).
8/8/2019 ASCEsem1txt (1)
33/38
Shear Strength
Analysis ofLaboratory Direct-Shear Data
During the laboratory direct-shear test of a natural
rock joint, data are collected to record the shear load
as a function of the applied normal load and the shear
displacement. The graph of shear load vs. shear
displacement for each applied normal load provides
the basis for describing the shear strength of the
specimen.
8/8/2019 ASCEsem1txt (1)
34/38
Shear
L ad
Shear Dis lacement
1
2
3
4
Residuals
rmal
L ads
8/8/2019 ASCEsem1txt (1)
35/38
Laboratory Direct-Shear Data
The contact area in shear when the specimen attains either the
peak shear load or the residual shear load is needed to
calculate the corresponding normal stress and shear stress
(strength) for any particular graph trace (trial).
For circular or rectangular specimens, this contact area can be
calculated directly, once the pertinent shear displacement is
identified. For irregularly shaped specimens, a reference tablemust be constructed that displays the contact area as a
function of shear displacement.
8/8/2019 ASCEsem1txt (1)
36/38
Laboratory Direct-Shear Data
A least-squares regression program (such as Taussm
or the Mathcad sheet entitled TauRegr) then
provides the linear and power models for shear
strength, as shown in the typical plots of shear
strength on the overheads
8/8/2019 ASCEsem1txt (1)
37/38
OverallShearStrength for Highly FracturedRockMasses
1. Exponential RQD Method
Required input:Average RQD (Rock Quality Designation) of the
rock mass (%)Estimated c (psi) and J for intact rockEstimated c (psi) and J for natural fractures
Intermediate factors (weights):A= .475exp(.007 x RQD) B = .188exp(.013 x RQD)
Then:cm = cr (B
2) + cf (1-B2) in psi
Jm = Jr (A2) + Jf(1-A2) in deg.
8/8/2019 ASCEsem1txt (1)
38/38
2. Hoek-Brown Rock Mass Strength Model
Required input:mi - Hoek-Brown constant (a material constant
ranging from about 4 to 33)GSI - Geological Strength Index (see handout)
Ci - uniaxial compressive strength of intact rockD - estimated rock-mass disturbance factor (0 for
insitu rock or for carefully designed blastingprograms; 1 for poor blasting practices with
considerable overbreak)
See Mathcad calculation sheet for examples.