Rock Mechanics

Learning Objectives

  • Separate intact-material properties from discontinuity-controlled rock-mass behavior.
  • Calculate overburden and effective stresses with consistent signs and units.
  • Interpret a Mohr circle, a selected plane and the limits of strength criteria.
  • Use RQD, RMR and Q without treating an empirical rating as a support design.
  • Distinguish excavation mechanisms and identify the measurements needed to reassess support.

Intact rock and rock mass

Intact rock is the material between discontinuities. A rock mass includes that material, its discontinuities and their spatial arrangement at the engineering scale.

Select the mechanism before the strength model

A laboratory core can measure intact uniaxial compressive strength (UCS), deformation and failure behavior without sampling the joint that controls a tunnel wedge. Joint persistence, orientation, roughness, infill and water pressure can govern sliding or block release. Conversely, massive rock under high stress may fail through intact material. Neither a rock name nor high UCS establishes excavation stability.

Use a mapped discontinuity model for a persistent weak plane; use a suitable equivalent rock-mass model only when its scale and structure assumptions fit. Peak and residual strength, sample disturbance and the tested stress range must match the proposed analysis.

A small intact core samples material between joints while a larger excavation intersects several discontinuities.

Original conceptual sections, not measured site geometry. Dashed sample outline marks the small volume represented by a core; continuous joints can release blocks at excavation scale. Based on FHWA NHI-09-010 chapter 6.

A small intact core samples material between joints while a larger excavation intersects several discontinuities.

Total stress, pressure and effective stress

Compression-positive stress

Normal compression is positive in this lesson. Principal stresses are ordered from major to minor: σ1≥σ2≥σ3\sigma_1 \geq \sigma_2 \geq \sigma_3. Shear stress acts tangentially to a plane.

Overburden estimate

Sum layer weights per unit horizontal area under an approximately level profile.

σv=∑iγihi\sigma_v=\sum_i\gamma_i h_i

Variables

SymbolDescriptionUnit
σv\sigma_vApproximate total vertical stress; divide kPa by 1000 to obtain MPakPa
γi\gamma_iTotal unit weight of layer ikN/m3kN/m^3
hih_iVertical thickness of layer i above the pointm

Horizontal stress needs independent evidence

The estimate does not determine principal directions or horizontal stresses. Tectonic history, erosion, topography, anisotropy and excavation modify the stress field. The ratio k=σh/σvk=\sigma_h/\sigma_v can exceed one in rock; it is not a universal material constant. Measure or justify the stress field rather than infer it from depth alone. Excavation stresses differ from the pre-excavation field.

A two-layer profile gives total vertical stress of 2.4 MPa at 100 m and 5.1 MPa at 200 m.

Analytical synthetic example with 100 m at 24 kN/m³ over 100 m at 27 kN/m³. The graph shows total vertical stress only; horizontal stress and pressure are not inferred.

A two-layer profile gives total vertical stress of 2.4 MPa at 100 m and 5.1 MPa at 200 m.

Effective normal stress on a water-filled joint

For uniform pressure acting across the joint, subtract pressure from total normal compression.

σn′=σn−u,σi′=σi−u\sigma_n'=\sigma_n-u,\qquad \sigma_i'=\sigma_i-u

Variables

SymbolDescriptionUnit
σn,σn′\sigma_n,\sigma_n'Total and effective normal stresses on the same planeMPa
uuJoint water pressure relative to the same pressure datumMPa
σi,σi′\sigma_i,\sigma_i'Total and effective principal stresses for this uniform-pressure model, assuming unit effective-stress coefficientMPa
Total normal compression clamps a joint while water pressure acts outward on both joint faces.

Original traction schematic: opposing total compression and joint-pressure arrows use distinct styles. Their difference is contact compression. A negative difference requires opening or tensile analysis; do not extrapolate compressive friction through it.

Total normal compression clamps a joint while water pressure acts outward on both joint faces.

Linear shear strength and the Mohr circle

Effective Mohr–Coulomb parameters

The cohesion intercept c′c' and friction angle ϕ′\phi' define a fitted linear relationship between compressive effective normal stress and limiting shear stress for the specified material or discontinuity.

Mohr–Coulomb shear envelope

Use the effective-stress parameters and a compressive effective normal stress.

∣τf∣=c′+σn′tan⁡ϕ′|\tau_f|=c'+\sigma_n'\tan\phi'

Variables

SymbolDescriptionUnit
τf\tau_fLimiting shear stress; two signs describe opposite shear sensesMPa
c′c'Fitted effective cohesion intercept; not necessarily intrinsic bondingMPa
ϕ′\phi'Effective friction angle for the applicable stress rangedegrees

Circle and selected plane

Restrict normals to the major–minor principal section. Theta is the angle from the major principal stress direction to the plane normal, not to the plane itself.

C=σ1′+σ3′2,R=σ1′−σ3′2,σn′=C+Rcos⁡2θ,τ=Rsin⁡2θC=\frac{\sigma_1'+\sigma_3'}2,\quad R=\frac{\sigma_1'-\sigma_3'}2,\quad \sigma_n'=C+R\cos2\theta,\quad \tau=R\sin2\theta

Variables

SymbolDescriptionUnit
C,RC,RCircle center and radius, also the maximum shear magnitudeMPa
θ\thetaSelected plane-normal angle; 0° gives major principal normal stress, 90° gives minordegrees

Tangency is a model limit, not a collapse forecast

For an isotropic Mohr–Coulomb material in compression, the circle lies below the shear envelope when R<Csin⁡ϕ′+c′cos⁡ϕ′R\lt C\sin\phi'+c'\cos\phi', touches it at equality, and extends beyond it when the inequality reverses. Equivalent triaxial compression at failure satisfies σ1f′=[σ3′(1+sin⁡ϕ′)+2c′cos⁡ϕ′]/(1−sin⁡ϕ′)\sigma_{1f}'=[\sigma_3'(1+\sin\phi')+2c'\cos\phi']/(1-\sin\phi').

Subtracting uniform pressure translates the circle left by uu and leaves its radius unchanged. Equal principal stresses give a visible point with zero shear. If σ3′<0\sigma_3'\lt0, opening and tensile strength need a separate model. Checking only the maximum-shear point is insufficient: the envelope is inclined. For an existing joint, check the stress at its actual orientation rather than assume the weakest theoretical plane exists.

Interactive Exploration

Change pressure while keeping total stresses fixed, then rotate the plane normal. Compare translation of the circle with movement along the circle. Set the stress difference to zero to inspect the hydrostatic limit.

Mohr circle and effective stress

Concept and model scope

Explore how confinement, stress difference, water pressure and plane orientation affect a rock stress state and its relation to a linear shear envelope.

Model and limits: Compression positive, MPa, uniform pressure with unit effective-stress coefficient and prescribed strength. Plane normals lie in the major–minor principal section. The full circle screens an isotropic Mohr–Coulomb material; one persistent joint requires its own orientation and strength check. No tensile cutoff, rockburst prediction, support design or universal safety factor is included.

Controls
20 MPa

Minor total stress

Compression-positive total minor principal stress σ₃. Major total stress is σ₃ plus the stress difference; their order cannot reverse.

Range: 0–40 MPa. Step: 1 MPa.

60 MPa

Principal stress difference

σ₁ − σ₃. Half this value is the Mohr-circle radius and maximum shear stress. Zero produces a point, not a failed circle.

Range: 0–100 MPa. Step: 1 MPa.

0 MPa

Joint water pressure

Uniform pressure u is subtracted from both total principal stresses. It translates the circle left without changing its radius. Effective tension is outside this compression-only shear assessment.

Range: 0–40 MPa. Step: 1 MPa.

10 MPa

Effective cohesion

The fitted c′ intercept of the effective-stress shear envelope. It is not automatically an intrinsic cementation strength and must match the material and tested stress range.

Range: 0–30 MPa. Step: 1 MPa.

30 °

Effective friction angle

φ′ controls the slope tan φ′ of the straight shear envelope. It is distinct from a geological joint dip or the selected plane-normal angle.

Range: 0–45 °. Step: 1 °.

30 °

Plane-normal angle

The normal lies in the major–minor principal section. θ is measured from the major principal stress direction to this normal. The graph point moves through angle 2θ. At θ = 0° normal stress is σ₁′; at 90° it is σ₃′.

Range: 0–90 °. Step: 1 °.

Effective principal-stress circle with equal stress scalesCompression is positive to the right; positive shear is upward. The solid circle shows the prescribed effective stress state; dashed lines show the two shear envelope branches for compressive normal stress. The outlined point represents the selected plane. A zero-radius circle remains a visible point.-80-4004080-4004080120Shear τ (MPa)Effective normal σₙ′ (MPa)
Solid: stress state. Dashed: |τ| = c′ + σₙ′ tan φ′, for σₙ′ ≥ 0. Outlined point: selected plane. Both axes use the same fixed MPa scale.
Major total stress σ₁
80.00 MPa
Effective principal stresses σ₁′ / σ₃′
80.00 / 20.00 MPa
Circle center C / radius R
50.00 / 30.00 MPa
Selected plane σₙ′ / τ
65.00 / 25.98 MPa
Selected plane shear strength
47.53 MPa
Envelope distance − radius
3.660 MPa

Stress circle below envelope. This compares a prescribed stress state with an idealized shear envelope. Equality is a limiting state, not a prediction of collapse or support performance.

Prescribed-plane resistance ratio

For positive driving shear on a specified plane, use consistent stresses or forces over the same area.

FS=c′+(σn−u)tan⁡ϕ′∣τd∣FS=\frac{c'+(\sigma_n-u)\tan\phi'}{|\tau_d|}

Variables

SymbolDescriptionUnit
τd\tau_dPrescribed driving shear stress; zero demand requires a separate interpretationMPa
FSFSAvailable shear resistance divided by the prescribed positive demanddimensionless

A linear fit has a stress range

Do not extrapolate a fitted line to untested confinement or effective tension. Bias relative to a nonlinear envelope depends on the fit and range; overestimation is not universal. A resistance ratio above one alone does not establish acceptable design, reliability or support needs. Specify the project criterion and evaluate mechanisms, water, geometry and parameter uncertainty.

Generalized Hoek–Brown strength

Geological Strength Index

GSI describes rock-mass structure and discontinuity surface condition for estimating equivalent rock-mass properties within the method's applicability.

Generalized Hoek–Brown criterion, 2002 basis

Nonlinear effective principal-stress strength, using a representative equivalent rock mass.

σ1f′=σ3′+σci(mbσ3′σci+s)a\sigma_{1f}'=\sigma_3'+\sigma_{ci}\left(m_b\frac{\sigma_3'}{\sigma_{ci}}+s\right)^a

Variables

SymbolDescriptionUnit
σci\sigma_{ci}UCS of intact material, distinct from unconfined rock-mass strengthMPa
mb,s,am_b,s,aRock-mass parameters; use supplied values or the stated edition's mappingdimensionless

Hoek–Brown parameter mapping

The 2002 relationships include intact material constant mi, mapped GSI and disturbance D.

mb=miexp⁡(GSI−10028−14D),s=exp⁡(GSI−1009−3D),a=12+e−GSI/15−e−20/36m_b=m_i\exp\left(\frac{GSI-100}{28-14D}\right),\quad s=\exp\left(\frac{GSI-100}{9-3D}\right),\quad a=\frac12+\frac{e^{-GSI/15}-e^{-20/3}}6

Variables

SymbolDescriptionUnit
mim_iIntact-material constantdimensionless
DDDisturbance factor from 0 to 1; estimate from actual excavation disturbancedimensionless

Check applicability before converting parameters

At zero confinement the model gives σcm=σcisa\sigma_{cm}=\sigma_{ci}s^a. This need not equal intact UCS. The intact limit has s=1s=1, a=0.5a=0.5 and mb=mim_b=m_i. A dominant persistent weak plane needs explicit discontinuity analysis; do not hide directional sliding in a single isotropic strength. Equivalent Mohr–Coulomb parameters depend on the selected confinement interval. The square-root teaching curve below uses prescribed constants, not a mapped site.

A nonlinear principal-stress failure curve rises from a rock-mass unconfined strength of 10 MPa.

Analytical synthetic data: intact UCS 100 MPa, mb = 1, s = 0.01, a = 0.5. Horizontal axis is minor effective principal stress; vertical axis is major effective principal stress at failure. This is not the shear-normal Mohr plot.

A nonlinear principal-stress failure curve rises from a rock-mass unconfined strength of 10 MPa.

Core logging and empirical classification

Rock Quality Designation

RQD is the sum of qualifying sound core lengths between natural discontinuities divided by the drill-run length, expressed as a percentage. The logging convention here counts lengths longer than 0.10 m; artificial drilling breaks are fitted back together where justified.

RQD and total core recovery

Use the complete run length as denominator; recovered fragments alone do not define rock quality.

RQD=100∑LqualifyingLrun,TCR=100LrecoveredLrunRQD=100\frac{\sum L_{\mathrm{qualifying}}}{L_{\mathrm{run}}},\qquad TCR=100\frac{L_{\mathrm{recovered}}}{L_{\mathrm{run}}}
A one-metre run has full recovery but two short pieces do not qualify, giving RQD 85 percent.

Synthetic sound pieces 20, 8, 12, 7, 25 and 28 cm, all separated by natural breaks. Total recovery is 100%; qualifying length is 85 cm. Exact-threshold pieces are avoided; log soundness, natural breaks and the applicable convention.

A one-metre run has full recovery but two short pieces do not qualify, giving RQD 85 percent.

RMR: keep the version and adjustment visible

The RMR89 basic rating sums five ratings: intact strength (maximum 15), RQD (20), discontinuity spacing (20), discontinuity condition (30) and groundwater (15). The discontinuity-orientation adjustment depends on the application and can reduce the basic rating. State the version, observations and adjustment; do not mix tables from different versions. UCS is a material input, while the final rating characterizes the investigated rock mass. A rating is not a computed factor of safety.

Q-system

Q is an empirical rock-mass classification used with excavation geometry and an excavation support ratio to inform underground support assessment.

Q and equivalent dimension

Use the applicable NGI handbook tables and record all six selected ratings.

Q=RQDQJnJrJaJwSRF,De=BESRQ=\frac{RQD_Q}{J_n}\frac{J_r}{J_a}\frac{J_w}{SRF},\qquad D_e=\frac{B}{ESR}

Variables

SymbolDescriptionUnit
RQDQRQD_QRQD percentage entered in Q; NGI uses 10 for logged RQD values from 0 to 10percent value
Jn,Jr,JaJ_n,J_r,J_aJoint-set, roughness and alteration ratingsdimensionless
Jw,SRFJ_w,SRFWater reduction and stress reduction ratingsdimensionless
B,De,ESRB,D_e,ESRRelevant excavation span, equivalent dimension and excavation support ratiom, m, dimensionless

Use ratings as evidence, not a recipe

The three Q quotients represent jointing/block size, joint friction, and water/stress conditions. Support assessment needs both Q and equivalent dimension, with weakness-zone geometry and the handbook's limitations. Preserve parameter ranges rather than conceal spatial variability in one average. Q alone cannot specify bolt spacing or shotcrete thickness. Its stress rating can depend on intact strength even though UCS is absent from the displayed product.

Excavation and ground response

Stand-up time

Stand-up time describes the period an unsupported opening of a stated span remains stable under specified ground and stress conditions. An empirical estimate is not permission to leave an excavation unsupported.

Rockburst, squeezing and swelling

A rockburst involves rapid energy release and violent rock failure. Squeezing is time-dependent deformation associated with overstressing weak ground. Swelling is volume increase associated with physicochemical processes, often involving water; it is not synonymous with squeezing.

Match excavation and support to the mechanism

Drill and blast is cyclic and permits changes in profile and excavation sequence. A TBM can achieve sustained mechanical excavation, but performance depends on abrasivity, strength, discontinuities, water, access, machine type and logistics. Not every TBM installs segments; an open hard-rock machine differs from a shielded system.

Deep massive rock warrants stress and brittle-failure investigation, not a guaranteed rockburst prediction. Weak ground warrants convergence and water assessment, not an assumption of inevitable crushing. Support selection considers load, displacement, energy demand, installation timing and system connections. Energy-absorbing support or yielding elements may be appropriate, but no generic bolt or method guarantees containment.

Observational tunneling uses a planned excavation/support sequence, monitoring, trigger criteria and predesigned responses. Control deformation within design limits; do not wait for all movement to cease before every final lining or prescribe NATM from a rock name. Reassess when mapping, pressure or convergence departs from the design assumptions.

Key Takeaways
  • Separate intact tests, discontinuity mechanisms and equivalent rock-mass assumptions.
  • Uniform pressure changes effective normal stress, not the Mohr-circle radius.
  • Plane-normal angle and equal axis scales are essential to correct stress interpretation.
  • Strength-envelope equality, a rating and a design acceptance decision are different results.
  • Record model edition, measured evidence, parameter ranges and excavation-response checks.

References