Risk assessment of collapse in shallow caverns using numerical modeling of block interactions with DDA: Suggested approach and case studies

Similar documents
THE VOUSSOIR BEAM REACTION CURVE

ARTICLE IN PRESS. International Journal of Rock Mechanics & Mining Sciences

Site Response Analysis with 2D-DDA

The Stability of a Laminated Voussoir Beam: Back Analysis of a Historic Roof Collapse Using DDA

Behaviour of Blast-Induced Damaged Zone Around Underground Excavations in Hard Rock Mass Problem statement Objectives

Tunnelling and Underground Space Technology 21 (2006) 29 45

Introduction and Background

Module 9 : Foundation on rocks. Content

CHAPTER 8 SUMMARY, CONCLUSIONS AND RECOMMENDATIONS

Wave Propagation through Discontinuous Media in Rock Engineering

In situ fracturing mechanics stress measurements to improve underground quarry stability analyses

Hatzor, Y.H. and Glaser, S., Environmentally controlled, multi scale, dynamic behavior of rock masse SUMMARY... 3

MEMORANDUM SUBJECT: CERTIFICATE IN ROCK MECHANICS PAPER 1 : THEORY SUBJECT CODE: COMRMC MODERATOR: H YILMAZ EXAMINATION DATE: OCTOBER 2017 TIME:

Entrance exam Master Course

Further Research into Methods of Analysing the October 2000 Stability of Deep Open Pit Mines EXECUTIVE SUMMARY

Stress arch bunch and its formation mechanism in blocky stratified rock masses

Borehole Camera And Extensometers To Study Hanging Wall Stability Case Study Using Voussoir beam - Cuiabá Mine

**********************************************************************

Seismic analysis of horseshoe tunnels under dynamic loads due to earthquakes

Numerical modelling for estimation of first weighting distance in longwall coal mining - A case study

Geotechnical & Mining Engineering Services

Rock slope failure along non persistent joints insights from fracture mechanics approach

B. Table of Contents

ENG1001 Engineering Design 1

Application of a transversely isotropic brittle rock mass model in roof support design

The effect of discontinuities on stability of rock blocks in tunnel

An introduction to the Rock Mass index (RMi) and its applications

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each. Q.1 Find the force (in kn) in the member BH of the truss shown.

GEOSYNTHETICS ENGINEERING: IN THEORY AND PRACTICE

Session 3: Geology and Rock Mechanics Fundamentals

Critical Borehole Orientations Rock Mechanics Aspects

Engineering Science OUTCOME 1 - TUTORIAL 4 COLUMNS

ON THE FACE STABILITY OF TUNNELS IN WEAK ROCKS

A new design approach for highway rock slope cuts based on ecological environment protection

Engineering Geophysical Application to Mine Subsidence Risk Assessment

Numerical modelling of mining subsidence, upsidence and valley closure using UDEC

Ground Support in Mining and Underground Construction

SYLLABUS AND REFERENCES FOR THE STRATA CONTROL CERTIFICATE. METALLIFEROUS MINING OPTION Updated November 1998

CHAPTER 5 Statically Determinate Plane Trusses

Structurally controlled instability in tunnels

CHAPTER 5 Statically Determinate Plane Trusses TYPES OF ROOF TRUSS

Estimation of rock cavability in jointed roof in longwall mining

THE INFLUENCE OF ROOF BOLTS LOCATION ON ITS INTERACTION WITH THE ROCK MASS.

2 Open Stoping Using Vertical Retreat

1 of 46 Erik Eberhardt UBC Geological Engineering ISRM Edition

ROCK MASS PROPERTIES FOR TUNNELLING

Analysis of Blocky Rock Slopes with Finite Element Shear Strength Reduction Analysis

Theory of structure I 2006/2013. Chapter one DETERMINACY & INDETERMINACY OF STRUCTURES

NNN99. Rock Engineering for the Next Very Large Underground Detector. D. Lee Petersen CNA Consulting Engineers

Flin Flon Mining Belt

Haulage Drift Stability Analysis- A Sensitivity Approach

Calculation of periodic roof weighting interval in longwall mining using finite element method

Building on Past Experiences Worker Safety

Research on Coal Pillar Width in Roadway Driving Along Goaf Based on The Stability of Key Block

Earthquake response analysis of rock-fall models by discontinuous deformation analysis

SIMULATION AND MECHANISM ANALYSIS OF WATER INRUSH FROM KARSTIC COLLAPSE COLUMNS IN COAL FLOOR

Mechanics of Solids. Mechanics Of Solids. Suraj kr. Ray Department of Civil Engineering

Rock slope rock wedge stability

EDEM DISCRETIZATION (Phase II) Normal Direction Structure Idealization Tangential Direction Pore spring Contact spring SPRING TYPES Inner edge Inner d

STABILITY PLANNING USING RELIABILTY TECHNIQUES. ASEAN Moving Forward. November 11, 2013, Chiang Mai, THAILAND

16. Mining-induced surface subsidence

Effect of lateral load on the pile s buckling instability in liquefied soil

The University of Melbourne Engineering Mechanics

Experimental Research on Ground Deformation of Double Close-spaced Tunnel Construction

CHAPTER 4: BENDING OF BEAMS

Module 5: Failure Criteria of Rock and Rock masses. Contents Hydrostatic compression Deviatoric compression

Kinematics of Overhanging Slopes in Discontinuous Rock

Sabah Shawkat Cabinet of Structural Engineering Walls carrying vertical loads should be designed as columns. Basically walls are designed in

Pillar strength estimates for foliated and inclined pillars in schistose material

3D ANALYSIS OF STRESSES AROUND AN UNLINED TUNNEL IN ROCK SUBJECTED TO HIGH HORIZONTAL STRESSES

Numerical Approach to Predict the Strength of St. Peter Sandstone Pillars acted upon by Vertical Loads A case study at Clayton, IA, USA.

Influence of the undercut height on the behaviour of pillars at the extraction level in block and panel caving operations

The effect of stope inclination and wall rock roughness on backfill free face stability

FLEXIBILITY METHOD FOR INDETERMINATE FRAMES

Lecture 15 Strain and stress in beams

Mechanical Behaviors of Cylindrical Retaining Structures in Ultra-deep Excavation

Finite difference modelling in underground coal mine roadway

1. Rock Mechanics and mining engineering

SYLLABUS AND REFERENCES FOR THE STRATA CONTROL CERTIFICATE COAL MINING OPTION

MAE 322 Machine Design. Dr. Hodge Jenkins Mercer University

Rock Material. Chapter 3 ROCK MATERIAL HOMOGENEITY AND INHOMOGENEITY CLASSIFICATION OF ROCK MATERIAL

PURE BENDING. If a simply supported beam carries two point loads of 10 kn as shown in the following figure, pure bending occurs at segment BC.

Large scale three-dimensional pit slope stability analysis of the structurally controlled mechanism in Mae Moh coal mine

Structural control on the stability of overhanging, discontinuous rock slopes

Deformability Modulus of Jointed Rocks, Limitation of Empirical Methods and Introducing a New Analytical Approach

Design of Beams (Unit - 8)

UNIVERSITY PHYSICS I. Professor Meade Brooks, Collin College. Chapter 12: STATIC EQUILIBRIUM AND ELASTICITY

Optimum Size of Coal Pillar Dimensions Serving Mechanised Caving Longwall Face in a Thick Seam

Open Pit Rockslide Runout

Limit analysis of brick masonry shear walls with openings under later loads by rigid block modeling

13 Step-Path Failure of Rock Slopes

Jeff Brown Hope College, Department of Engineering, 27 Graves Pl., Holland, Michigan, USA UNESCO EOLSS

If the number of unknown reaction components are equal to the number of equations, the structure is known as statically determinate.

UNIVERSITY OF SASKATCHEWAN ME MECHANICS OF MATERIALS I FINAL EXAM DECEMBER 13, 2008 Professor A. Dolovich

Dynamic Stability Analysis and Forecast of Surface Mine Dump

Received 9 February 2015; accepted 6 March 2015; published 12 March 2015

Support Idealizations

UNIT IV FLEXIBILTY AND STIFFNESS METHOD

Evaluation of the behaviour of an arch-gravity dam. featuring a pre-existing crack

EQUIVALENT FRACTURE ENERGY CONCEPT FOR DYNAMIC RESPONSE ANALYSIS OF PROTOTYPE RC GIRDERS

Transcription:

Risk assessment of collapse in shallow caverns using numerical modeling of block interactions with DDA: Suggested approach and case studies Yossef H. Hatzor Professor and Chair in Rock Mechanics, BGU, Israel Visiting Professor, CAS, Wuhan, China International Top-level Forum on Engineering Science and Technology Development Strategy Safe Construction and Risk Management of Major Underground Engineering May 17 19, Wuhan, China.

Shallow caverns, typically of Karstic origin, may pose great risk to surface civil engineering structures, but are quite difficult to detect, therefore exploration drilling is often employed: Research Question: What is the limiting relationship between cavern span (B) and cover height (h) that will ensure stability? The answer will constrain the required drilling length (D) and distance (d) in the exploration effort. Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 2

One way to answer this question is to study it numerically with discrete element methods, by generating, synthetically, Blocky rock masses and then running forward modeling. Here we keep the rock mass structure constant and change in each simulation the span width (B) and cover height (h) to obtain the structural response with DDA: h B An example of a blocky rock mass structure with a synthetic jointing pattern as generated with DDA Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 3

The modeled rock mass in our simulations is a typical blocky rock mass as found in central Israel, with a horizontal bedding planes set and two sub-vertical and sub-orthogonal joint sets: Joint Set Dip/Direction Trace Length Mean Spacing Degree of Randomness Rock Bridge Length 1 /.7 m 1. m 2 88/182 5 m.96 m.5 2.5 m 3 88/12 5 m.78 m.5 2.5 m These structural parameters represent mean values obtained from a number of joint surveys in central Israel where the problem of karstic cavern collapse exists The large value of assigned rock bridge length (2.5m) is used to simulate the phenomena of mechanical layering, where the extent of joint trace length is conditioned by bed thickness The same effect is obtained by using a relatively small value of trace length (5m) with respect to bed thickness (.7m). Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 4

To estimate the mechanical stability of each structural configuration, we measure the vertical displacement (v) and the horizontal stress (s x ) components as obtained with forward DDA at four measurement points evenly distributed at the roof of the modeled excavation: The lateral boundaries are set at a distance of b = 3B to ensure the decay of stress concentrations near the boundaries of the modeled domain. Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 5

The results of forward modeling with DDA are classified into three categories of structural response, depending on the vertical displacement (v) and horizontal stress (s x ) component outputs at the measurement point locations: Stable Configuration: the 3 upper measurement points exhibit static stability Marginally Stable: the 2 upper measurement points exhibit static stability Unstable: Only the upper measurement point or no measurement point exhibit static stability Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 6

h/b =.78 Example of Stable configuration 1 m. -.1 2 4 6 8 1 12 Time, sec. Measurement Point 1-5 -1 2 4 6 8 1 12 Time, sec. Measurement Point 1 Measurement Point 2 -.2 -.3 Measurement Point 2 Measurement Point 3 Measurement Point 4-15 -2-25 Measurement Point 3 Measurement Point 4 -.4-3 -.5-35 -4 -.6 v,m -45 s x,kn/m 2 Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 7

h/b = 1. Extension of Stable definition 1 m. 5 1 15 2 5 1 15 2 Time, sec. Time, sec. -1-2 -2-4 -6-3 -8-4 -1-5 -6 v,m -12 Measurement Point 1 Measurement Point 2 Measurement Point 3 Measurement Point 4-14 s x,kn/m 2 Measurement Point 1 Measurement Point 2 Measurement Point 3 Measurement Point 4 Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 8

h/b =.76 Marginally stable configuration 1 m -1 5 1 15 Time, sec. -2-4 5 1 15 Time, sec. -2-6 -8-3 -1-4 -12-5 -6 v,m -14-16 Measurement Point 1 Measurement Point 2-18 Measurement Point 3 Measurement Point 4 s x,kn/m 2 Measurement Point 1 Measurement Point 2 Measurement Point 3 Measurement Point 4 B Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 9

h/b =.5 Unstable configuration 1 m. 5 1 15 2 5 1 15 2 Time, sec. Time, sec. -1-2 -2-4 -6-3 -8-4 -1-5 -6 v,m -12 Measurement Point 1 Measurement Point 2 Measurement Point 3 Measurement Point 4-14 s x,kn/m 2 Measurement Point 1 Measurement Point 2 Measurement Point 3 Measurement Point 4 Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 1

As we know, per a given cover height (here h ~ 2 m) the span width adversely affects stability: h/b =.76 B = 25 m 1 m. h/b =.73 1 m. B = 3 m h/b =.5 1 m. Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China B = 4 m 11

Similarly, per given cavern span ( here B = 25 m) the cover height positively affects stability: h = 3 m h/b = 1.2 1 m. h/b = 1. h = 25 m 1 m. h/b =.5 h = 12.5 m 1 m. Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 12

The final resulting relationship between B and h required for stability however proves to be not linear: h, m h/b = 1 35 Ayalon Cave h 17(3) 13(3) 3 B Zedekiah Cave h/b =.5 15(25) 25 Safe 1(25) 19(22) 12(22) 2 16(19) 9(2) 15 7(14) Marginal 11(15) 8(15) 3(11) 6(1) 14(12.5) 1 18(11) 1(6) 2(6) 4(6) Unsafe 5(6) 5 Tel Beer Sheva B, m 1 2 3 4 5 Legend: Safe Marginal Unsafe Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 13

The above was shown for the same, synthetically generated, rock mass structure. Results from three different case studies in different rock masses support our concluding chart: 1. The Ayalon cave underneath Ramle open pit mine central Israel 2. The 2 year old Zedekiah quarry - underneath the old city of Jerusalem 3. The Tel Beer Sheva 3 year old underground water storage system southern Israel. Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 14

Case 1: Ayalon Cave a present day 4 meter span karstic cavern underneath an active open pit mine with 3 meters of rock cover: Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 15

Statistical joint survey results: J1 J 3 J 2 J 2 J 3 Frequency 45 4 35 3 25 2 15 1 5.3.6.9 1.2 1.5 1.8 2.1 2.4 2.7 3 3.3 Thickness (m) J2 J3 Frequency 35 3 25 2 15 1 5..3.6.9 1.3 1.6 1.9 2.2 2.5 2.8 3.1 3.4 3.8 4.1 4.4 4.7 Spacing (m) Frequency 35 3 25 2 15 1 5..3.6.9 1.3 1.6 1.9 2.2 2.5 2.8 3.1 3.4 3.8 4.1 4.4 4.7 Spacing (m) Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 16

Current configuration of explored cavern underneath the mine: No. of Blocks A mean 15,11 1.7 m 2 Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 17

Results of forward analysis with DDA: Marginally stable configuration No. time steps Real Time 9, 35.4 s -1-2 -3 1 2 3 4 t, sec -1-2 1 2 3 4 t, sec Mean no. it. pts. CPU time 5.26 361 hr. -4-5 -6 Point 1 Point 2 Point 3 Point 4-3 -4-5 Point 1 Point 2 Point 3 Point 4-7 v, m -6 s x, kpa Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 18

Case 2: Zedekiah cave a 2 years old 3 meter span cavern with 25 meter cover under the old city of Jerusalem: Maximum Length 23 m Maximum Width 1 m Average Height 15m Estimated Area - 9 m 2 Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 19

Cross section through main chamber A A 5m 1m 15m Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 2

Rock Mass Structures Bedding planes Vertical Joints Set Type Dip Spacing 1 Bedding 8/91.85 2 Shears 71/61.79 3 Shears 67/231 1.48 4 Joints 75/155 1.39 Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 21

Roof stability assuming bedding planes only Free span (L) 3 m Beam thickness (t).85 m Unit weight (g ) 19.8 kn/m 3 Elastic modulus (E') 8*1 3 MPa Uniaxial compressive strength (s c ) 16.4 MPa (bedding parallel) Tensile strength (s t ) 2.8 MPa Maximum deflection at centerline (η) Maximum shear stress at abutments (t max ) Maximum axial stress (s) 8.67 cm.445 MPa 1.5 MPa The roof should have failed in tension Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 22

Roof stability assuming the Voussoir analogue Since the tensile strength of the material is exceeded in at the lowermost layers of the roof a vertical crack may propagate and decompose the continuous roof slab into two blocks, thus forming the so called Voussoir Bean (See Ray Sterling PhD thesis and Brady and Brown, 24): S f c n T Z T t f c Mid-Span Crack With the given dimensions the roof should undergo buckling culminating in a snap through mechanics (Z < ). So, what is keeping the roof stable?... Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 23

Results of forward modeling with DDA: 1m 1MPa 4 3 2 1 Vertical Displacement (m) Horizontal Compressive Stress ( kpa) -.5 -.1 -.15 -.2 -.25 -.3 -.35-1 -2-3 -4-5 -6-7 -8 a m point 4 m point 3 m point 2 b m point 1 -.25.5.5 1 1.5 2 2.5 3 3.5 4 4.5 5 Time (sec) Stable Configuration Surprisingly, the jointing patterns keeps the roof stable Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 24

Case 3: Tel Beer-Sheva a 3 years old underground water storage system Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 25

Underground System Layout: a a b b The collapse which occurred during time of construction was supported by the ancient engineers with a massive stone pillar. Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 26

Joint spacing, orientation, and friction angle: 5 4 (deg.) 3 2 1 2 4 6 8 Normal Stress (kpa) For the estimated level of normal stress the friction angle is assumed to be 35 o Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 27

Kinematics of a Jointed Beam (Voussoir) S = 8m, t =.5m, S j =.25m Initial Geometry = 45 = 3 = 8 = 75 o Deformed state Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 28

Forward DDA modeling results proves to be a function of vertical joint spacing and friction angle: 1 9 Friction angle required for stability 8 7 6 5 4 3 2 1 For the attempted opening span the existing spacing between vertical joints dictates an Unstable configuration 1 2 3 4 5 6 7 8 Vertical joint spacing (cm) Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 29

Required friction angle for stability [Degree] DDA vs. UDEC Beam span = 7m Beam thickness = 2.5m Layer thickness =.5m 9 8 7 6 5 4 3 2 1 1 2 3 4 5 6 7 Mean joint spacing [cm] DDA Element size.1 m Element size 1 m Barla, Monacis, Perino, and Hatzor (21), Rock Mechanics & Rock Engineering. Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 3

The numerically obtained relationship between B and h with the case studies shown: h, m Hatzor, Wainshtein, and Bakun-Mazor (21), IJRMMS. 35 Ayalon Cave h 17(3) 13(3) 3 B Zedekiah Cave 15(25) 25 Safe 1(25) 19(22) 12(22) 2 16(19) 9(2) 15 7(14) Marginal 11(15) 8(15) 3(11) 6(1) 14(12.5) 1 18(11) 1(6) 2(6) 4(6) Unsafe 5(6) 5 Hatzor and Benari (1998), IJRMMS. Tel Beer Sheva B, m 1 2 3 4 5 Legend: Safe Marginal Unsafe Bakun-Mazor, Hatzor and Dershowitz (29), IJRMMS. Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 31

Summary Sinkhole collapse can pose a significant risk for people and surface civil engineering operations. We develop here, using the numerical DDA method, a function that marks the boundary between Stable and Unstable shallow cavern geometries, for blocky rock masses consisting of horizontal bedding planes and vertical joints. Our results are confirmed by three independent stability analyses of underground openings in blocky rock masses possessing different mechanical properties for intact rock elements as well as different joint friction and spacing. Y. Hatzor: Risk assessment of collapse in shallow caverns. CAE Top Level Forum. May 18 212 Wuhan China 32