Hydro-mechanical behavior of single rock fracture under different confining pressures

Size: px
Start display at page:

Download "Hydro-mechanical behavior of single rock fracture under different confining pressures"

Transcription

1 Hydro-mechanical behavior of single rock fracture under different confining pressures Advisor: Prof. Jia-Jyun DONG Presenter: Xuan-Xinh Nguyen Date: 17/4/

2 Outline Introduction Literature review Methodology Results and discussion Conclusion Future work

3 Introduction Fluid flow through rock mass is highly depended on rock fracture. Fracture aperture is important factor effecting the fluid flow through fractured rock. Correlation between hydraulic (e h ) and mechanical (E) aperture under normal stress Stress closure conductivity coupling e h =E e h < E Bandis et al.,

4 Literature review Validity of cubic law for fluid flow in a deformable rock fracture (Witherspoon et al., 198. ) Modify the cubic law with friction factor (f) is valid for mechanic aperture from 4 5 m and f = (not measure directly mechanical aperture) Fundamentals of rock joint deformation. (Bandis et al., 1983). Hydraulic conductivity of rock fracture under normal and shear stress (normal and shear stiffness) Laboratory studies of gas flow though a single natural fracture. (Schrauft et al., 1986). Independently measuring the mechanical aperture from the fracture volume measurements of single granodiorite fracture. On the role of fracture surface roughness in fluid flow and solute transport through fractured rock. (Zhao et al., 15). Fracture network model based on a number of empirical models proposed to relate the reduced hydraulic aperture to the mechanical aperture duo to surface roughness. 4

5 Hydraulic and mechanical aperture definition Hydraulic aperture, e h : Darcy s law q ka dp dx Mechanical aperture, E: E V A f e h =E Cubic law (Snow et al., 1965) q 3 ewdp h 1 dx A = e h w Where q = flow rate = fluid viscosity w = fracture width dp/dx = pressure gradient V = fracture volume A f = fracture area A = cross section area e < <E Literature review 5

6 Normal stiffness of fractured rock (K n ) V m a b Hyperbolic relationship: n 1 V a bv j j K ni 1 a JCS: Joint Compressive Strength JRC: Joint Roughness Coefficient Bandis et al., 1983 Literature review Normal stiffness, Kn: K n K ni VK 1 n m ni n JCS Vm A B( JRC) C a j JCS Kni. JRC 1 a j D 6

7 Fracture flow regime 4 MPa confining pressure Linear Darcy flow zone: P AQ q ka P JRC = 7.1 Non-Darcy flow zone Forchheimer s law P AQ BQ (Forchheimer, 191) 1 P Q Q we w e 3 h h A, B = equaiton coefficients β = non Darcy coefficient Using dimensional analysis (Schrauf and Evans, 1986) P ad Q b 3 D Q Where: 3 ehw ehw Literature review a D = 1, for straight flow a D = 3, for pipe flow The hydraulic test of single granite rock b D = f D / f D = friction factor (roughness and tortuous flow) Chen et al., 15 7

8 Roughness effect Modified Cubic law: q 3 1 ewdp h f 1 dx (Witherspoon et al., 198) Where: q = flow rate e h = hydraulic aperture = fluid viscosity dp/dx = pressure gradient f = fiction factor (roughness and tortuous flow) Mechanic aperture (E): 4 5 m Friction factor, f = 1.4 to 1.65 Walsh (1981) K K 1 K 1 K Where: K = permeability of rough surface K = permeability of smooth surface Zimmerman et al., = the ratio of contact area to total area fracture (1 b) 4b ; b is the aspect ratio of the ellipse. Literature review 8

9 Mechanical and hydraulic aperture correlation Li et al., 13 Barton et al., 1985 E / e 1 Z h.5 E / e 1 Z (.6.4* Z )(Re1) h.5.5 E/e h e h E JRC.5 JRC log Z Rasouli and Hosseinian, 11 eh / E 1.3d.565 mc JRC a 1/3 E (mm) d mc = constant minimum closure distance Z = RMS of the first derivative of the profile JRC a = average joint roughness coefficient Roughness profile, Barton and Choubey (1977) Literature review For higher flow rates and larger apertures e h E (Iwai, 1976) With higher normal stress, e h << E (Cook et al., 199) 9

10 Methodology Roughness profile measurement. Fracture volume and permeability tests using YOKO system. Using steel sample for the beginning study. Apply study results for rock material 1

11 Steel sample YOKO system V (mm 3 ) A f (mm ) mm Joint wall 6. mm First test: Fracture volume test: 3 8 MPa Fracture permeability test: 3 6 MPa Second test: Fracture volume test: 1 17 MPa Fracture permeability test: 5 3 MPa Methodology 11

12 Fracture volume test Effective stress (MPa) Effective stress (MPa) Pressure gauge Frist test Second test Fracture volume: V P P V V i1 f p s l Pf P i. Mechanic aperture: Mechanic aperture, E (mm) Joint closure (mm) E V A p f Result and discussion 1

13 ) P d L ) P d L Fracture permeability test Linear Darcy zone: 4L By using dimensional analysis (Ward, 1964) 4L LbD P Q Q P Q 3 P Q 3 m eh oew h f m 3 m m oehw f oehw f 3 a bq Hydraulic aperture: 4L Qm W P e h o f m 4LP Q W P P d m f ( u d ) o P P u Pd P u Pd The first test.e+.e-6 4.E-6 6.E-6 Volumetric flow rate, Q (m 3 /s) The second test.e+ 5.E-6 1.E-5 1.5E-5 Volumetric flow rate, Q (m 3 /s) 6 MPa 5 MPa 4 MPa 3 MPa MPa 15 MPa 1 MPa 8 MPa 5 MPa 3 MPa 3 MPa 5 MPa MPa 15 MPa 1 MPa 5 MPa Result and discussion The plot of pressure versus discharge of two tests 13

14 Correlation between hydraulic and mechanic aperture Hydraulic aperture, eh (m) 1.E-3 1.E-4 1.E-5 1.E-6 1.E-6 1.E-5 1.E-4 1.E-3 Mechanical aperture, E (m) Result and discussion Marble fracture (Witherspoon et al., 198) 14

15 E/e JRCn Compare the results with a numerical of critical models e E e JRCn.1.5 1/ JRC Mechanic aperture (E). 1 cm cm 3 cm 4 cm 5 cm 6 cm 1 cm cm 5 cm JRC =.8 JRC =.7 JRC =.6 JRC =.5 JRC =.4 JRC =.3 First test Second test JRC with considering the scale effect L JRC JRC L n n.jrc where JRC n = JRC value at n length JRC = JRC value at length of 1 cm L n = sample length L = 1 cm Result and discussion 15

16 E/e Hydraulic aperture, e (m) Relationship between mechanical and hydraulic aperture Rasouli and Hosseinian (11) Li and Jiang (13) Rasouli and Hosseinian, 11 3 eh 1.3d E.565 mc JRC a Mechanical aperture, E (m) Mechanical, E (m) First test Second test Relation ship between mechanical aperture and the ratio of mechanical aperture to hydraulic aperture Result and discussion Rasouli and Hosseinian (11) Li and Jiang (13) First test Second test Li and Jiang, 13 eh E eh E 1 Z (Re<1).5 1 Z (.6.4* Z )(Re1) (Re>1) Assumed:.5.5 d mc =.3 mm JRC a =.5 Z =.17 for JRC = - 16

17 Conclusion The steel sample used to test is identical sample with the results similar for the first and second test. The gas flow through single steel fracture is in linear Darcy zone. Because the fracture surface is smooth surface. Mechanic aperture is greater than hydraulic aperture due to the small holes on the fracture surface. More test with different roughness surfaces need to be experimented. 17

18 Future work Use cooper sample to do next test with rougher fracture surface. Predict fracture surface profile using 3D scan laser machine. 18

19 Thank you for your attention! 19

Stress-Permeability Relationships in Low Permeability Systems: Application to Shear Fractures

Stress-Permeability Relationships in Low Permeability Systems: Application to Shear Fractures PROCEEDINGS, Thirty-Ninth Workshop on Geothermal Reservoir Engineering Stanford University, Stanford, California, February 24-26, 2014 SGP-TR-202 Stress-Permeability Relationships in Low Permeability Systems:

More information

PLANES OF WEAKNESS IN ROCKS, ROCK FRCTURES AND FRACTURED ROCK. Contents

PLANES OF WEAKNESS IN ROCKS, ROCK FRCTURES AND FRACTURED ROCK. Contents PLANES OF WEAKNESS IN ROCKS, ROCK FRCTURES AND FRACTURED ROCK Contents 7.1 Introduction 7.2 Studies On Jointed Rock Mass 7.2.1 Joint Intensity 7.2.2 Orientation Of Joints 7.2.3 Joint Roughness/Joint Strength

More information

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

Deformability Modulus of Jointed Rocks, Limitation of Empirical Methods and Introducing a New Analytical Approach University of Wollongong Research Online Coal Operators' Conference Faculty of Engineering and Information Sciences 2016 Deformability Modulus of Jointed Rocks, Limitation of Empirical Methods and Introducing

More information

Two-Phase (Air and Water) Flow through Rock Joints: Analytical and Experimental Study

Two-Phase (Air and Water) Flow through Rock Joints: Analytical and Experimental Study University of Wollongong Research Online Faculty of Engineering - Papers (Archive) Faculty of Engineering and Information Sciences 2003 Two-Phase (Air and Water) Flow through Rock Joints: Analytical and

More information

Coupled air-water flow through fractured sandstones

Coupled air-water flow through fractured sandstones University of Wollongong Research Online Faculty of Engineering - Papers (Archive) Faculty of Engineering and Information Sciences 2 Coupled air-water flow through fractured sandstones Buddhima Indraratna

More information

Scaling of fluid flow versus fracture stiffness

Scaling of fluid flow versus fracture stiffness GEOPHYSICAL RESEARCH LETTERS, VOL. 40, 2076 2080, doi:10.1002/grl.50479, 2013 Scaling of fluid flow versus fracture stiffness Christopher L. Petrovitch, 1 David D. Nolte, 1 and Laura J. Pyrak-Nolte 1,2,3

More information

The Open Civil Engineering Journal

The Open Civil Engineering Journal Send Orders for Reprints to reprints@benthamscience.ae The Open Civil Engineering Journal, 6,, 53-53 53 The Open Civil Engineering Journal Content list available at: www.benthamopen.com/tociej/ DOI:.74/874495653

More information

Permeability Evolution in Natural Fractures Subject to Cyclic Loading and Gouge Formation. Daniel Vogler, Florian Amann, Peter Bayer & Derek Elsworth

Permeability Evolution in Natural Fractures Subject to Cyclic Loading and Gouge Formation. Daniel Vogler, Florian Amann, Peter Bayer & Derek Elsworth Permeability Evolution in Natural Fractures Subject to Cyclic Loading and Gouge Formation Daniel Vogler, Florian Amann, Peter Bayer & Derek Elsworth Rock Mechanics and Rock Engineering ISSN 723-2632 Rock

More information

Mechanics and fluid transport in a degradable discontinuity

Mechanics and fluid transport in a degradable discontinuity Engineering Geology 53 (1999) 243 249 Mechanics and fluid transport in a degradable discontinuity A.P.S. Selvadurai *, T.S. Nguyen 1 Department of Civil Engineering and Applied Mechanics, McGill University,

More information

Compressible Duct Flow with Friction

Compressible Duct Flow with Friction Compressible Duct Flow with Friction We treat only the effect of friction, neglecting area change and heat transfer. The basic assumptions are 1. Steady one-dimensional adiabatic flow 2. Perfect gas with

More information

Fracture void structure: implications for flow, transport and deformation

Fracture void structure: implications for flow, transport and deformation Fracture void structure: implications for flow, transport and deformation A. Aydin Abstract This review focuses on studies of flow, transport and deformation processes at a scale of a single discontinuity.

More information

CHAPTER FIVE CLASSIFICATION OF SHEAR STRENGTH OF JOINTS IN ROCK

CHAPTER FIVE CLASSIFICATION OF SHEAR STRENGTH OF JOINTS IN ROCK CHAPTER FIVE CLASSIFICATION OF SHEAR STRENGTH OF JOINTS IN ROCK 5.1 Introduction The shear strength of joint surfaces in a rock mass is a difficult parameter to determine. Several researchers, including

More information

Laboratory Assessment of Fracture Permeability under Normal and Shear Stresses

Laboratory Assessment of Fracture Permeability under Normal and Shear Stresses Laboratory Assessment of Fracture Permeability under Normal and Shear Stresses D. Phueakphum* and K. Fuenkajorn Geomechanics Research Unit, Suranaree University of Technology 111 University Avenue, Nakhon

More information

q v = - K h = kg/ν units of velocity Darcy's Law: K = kρg/µ HYDRAULIC CONDUCTIVITY, K Proportionality constant in Darcy's Law

q v = - K h = kg/ν units of velocity Darcy's Law: K = kρg/µ HYDRAULIC CONDUCTIVITY, K Proportionality constant in Darcy's Law Darcy's Law: q v - K h HYDRAULIC CONDUCTIVITY, K m/s K kρg/µ kg/ν units of velocity Proportionality constant in Darcy's Law Property of both fluid and medium see D&S, p. 62 HYDRAULIC POTENTIAL (Φ): Φ g

More information

Uniform Channel Flow Basic Concepts. Definition of Uniform Flow

Uniform Channel Flow Basic Concepts. Definition of Uniform Flow Uniform Channel Flow Basic Concepts Hydromechanics VVR090 Uniform occurs when: Definition of Uniform Flow 1. The depth, flow area, and velocity at every cross section is constant 2. The energy grade line,

More information

Rock Joint and Rock Mass Shear Strength

Rock Joint and Rock Mass Shear Strength Rock Joint and Rock Mass Shear Strength GEO-SLOPE International Ltd. www.geo-slope.com 1400, 633-6th Ave SW, Calgary, AB, Canada T2P 2Y5 Main: +1 403 269 2002 Fax: +1 403 266 4851 Introduction SLOPE/W

More information

USING FULLY COUPLED HYDRO-GEOMECHANICAL NUMERICAL TEST BED TO STUDY RESERVOIR STIMULATION WITH LOW HYDRAULIC PRESSURE

USING FULLY COUPLED HYDRO-GEOMECHANICAL NUMERICAL TEST BED TO STUDY RESERVOIR STIMULATION WITH LOW HYDRAULIC PRESSURE PROEEDINGS, Thirty-Seventh Workshop on Geothermal Reservoir Engineering Stanford University, Stanford, alifornia, January 30 - February 1, 2012 SGP-TR-194 USING FULLY OUPLED HYDRO-GEOMEHANIAL NUMERIAL

More information

Implications of groundwater behaviour on the geomechanics of rock slope stability

Implications of groundwater behaviour on the geomechanics of rock slope stability APSSIM 2016 PM Dight (ed.) 2016 Australian Centre for Geomechanics, Perth, ISBN 978-0-9924810-5-6 https://papers.acg.uwa.edu.au/p/1604_0.3_price/ Implications of groundwater behaviour on the geomechanics

More information

The Influence of Shear and Deviatoric Stress on the Evolution of Permeability in Fractured Novaculite and Diorite

The Influence of Shear and Deviatoric Stress on the Evolution of Permeability in Fractured Novaculite and Diorite Igor Faoro, Andre Niemeijer, Chris Marone, Derek Elsworth The Influence of Shear and Deviatoric Stress on the Evolution of Permeability in Fractured Novaculite and Diorite Department of Energy and Geo-Environmental

More information

Calculation of Pipe Friction Loss

Calculation of Pipe Friction Loss Doc.No. 6122-F3T071 rev.2 Calculation of Pipe Friction Loss Engineering Management Group Development Planning Department Standard Pump Business Division EBARA corporation October 16th, 2013 1 / 33 2 /

More information

REE 307 Fluid Mechanics II. Lecture 1. Sep 27, Dr./ Ahmed Mohamed Nagib Elmekawy. Zewail City for Science and Technology

REE 307 Fluid Mechanics II. Lecture 1. Sep 27, Dr./ Ahmed Mohamed Nagib Elmekawy. Zewail City for Science and Technology REE 307 Fluid Mechanics II Lecture 1 Sep 27, 2017 Dr./ Ahmed Mohamed Nagib Elmekawy Zewail City for Science and Technology Course Materials drahmednagib.com 2 COURSE OUTLINE Fundamental of Flow in pipes

More information

An-Najah National University Civil Engineering Department. Fluid Mechanics. Chapter 1. General Introduction

An-Najah National University Civil Engineering Department. Fluid Mechanics. Chapter 1. General Introduction 1 An-Najah National University Civil Engineering Department Fluid Mechanics Chapter 1 General Introduction 2 What is Fluid Mechanics? Mechanics deals with the behavior of both stationary and moving bodies

More information

A theoretical model for relative permeabilities in two-phase flow in a fracture

A theoretical model for relative permeabilities in two-phase flow in a fracture A theoretical model for relative permeabilities in two-phase flow in a fracture M. Fourar & C. Moyne Ecole des Mines Laboratoire d'energetique et de Mecanique Theorique et Appliquee Pare de Saurupt - 54042

More information

COUPLED SHEAR-FLOW PROPERTIES OF ROCK FRACTURES

COUPLED SHEAR-FLOW PROPERTIES OF ROCK FRACTURES Thesis summary COUPLED SHEAR-FLOW PROPERTIES OF ROCK FRACTURES Graduate School of Science and Technology Nagasaki University, Japan Bo LI Abstract: In rock engineering, two issues have been considered

More information

Relative Permeability Measurement and Numerical Modeling of Two-Phase Flow Through Variable Aperture Fracture in Granite Under Confining Pressure

Relative Permeability Measurement and Numerical Modeling of Two-Phase Flow Through Variable Aperture Fracture in Granite Under Confining Pressure GRC Transactions, Vol. 36, 2012 Relative Permeability Measurement and Numerical Modeling of Two-Phase Flow Through Variable Aperture Fracture in Granite Under Confining Pressure Noriaki Watanabe, Keisuke

More information

A GEOMETRICAL APPROACH FOR THE ESTIMATION OF SCALE EFFECTS IN ROCK JOINT BEHAVIOUR

A GEOMETRICAL APPROACH FOR THE ESTIMATION OF SCALE EFFECTS IN ROCK JOINT BEHAVIOUR 57ième CONGRÈS CANADIEN DE GÉOTECHNIQUE 5ième CONGRÈS CONJOINT SCG/AIH-CNN 57TH CANADIAN GEOTECHNICAL CONFERENCE 5TH JOINT CGS/IAH-CNC CONFERENCE A GEOMETRICAL APPROACH FOR THE ESTIMATION OF SCALE EFFECTS

More information

Uniform Channel Flow Basic Concepts Hydromechanics VVR090

Uniform Channel Flow Basic Concepts Hydromechanics VVR090 Uniform Channel Flow Basic Concepts Hydromechanics VVR090 ppt by Magnus Larson; revised by Rolf L Feb 2014 SYNOPSIS 1. Definition of Uniform Flow 2. Momentum Equation for Uniform Flow 3. Resistance equations

More information

FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER

FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER FLUID MECHANICS PROF. DR. METİN GÜNER COMPILER ANKARA UNIVERSITY FACULTY OF AGRICULTURE DEPARTMENT OF AGRICULTURAL MACHINERY AND TECHNOLOGIES ENGINEERING 1 5. FLOW IN PIPES 5.1.3. Pressure and Shear Stress

More information

Journal of Petroleum Science and Engineering

Journal of Petroleum Science and Engineering Journal of Petroleum Science and Engineering 78 (2011) 321 327 Contents lists available at ScienceDirect Journal of Petroleum Science and Engineering journal homepage: www.elsevier.com/locate/petrol Applicability

More information

Basic Fluid Mechanics

Basic Fluid Mechanics Basic Fluid Mechanics Chapter 6A: Internal Incompressible Viscous Flow 4/16/2018 C6A: Internal Incompressible Viscous Flow 1 6.1 Introduction For the present chapter we will limit our study to incompressible

More information

Integrating Lab and Numerical Experiments to Investigate Fractured Rock

Integrating Lab and Numerical Experiments to Investigate Fractured Rock Integrating Lab and Numerical Experiments to Investigate Fractured Rock Bradford H. Hager Director, Earth Resources Laboratory and Cecil and Ida Green Professor Department of Earth, Atmospheric and Planetary

More information

Instructional Objectives

Instructional Objectives GE 6477 DISCONTINUOUS ROCK 7. Shear Strength of Discontinuities Dr. Norbert H. Maerz Missouri University of Science and Technology (573) 341-6714 norbert@mst.edu Instructional Objectives 1. Explain the

More information

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

Behaviour of Blast-Induced Damaged Zone Around Underground Excavations in Hard Rock Mass Problem statement Objectives Behaviour of Blast-Induced Damaged Zone Around Underground Excavations in Hard Rock Mass Problem statement Blast-induced damaged zone can affect the affect stability and performance of tunnel. But, we

More information

Hydraulics and hydrology

Hydraulics and hydrology Hydraulics and hydrology - project exercises - Class 4 and 5 Pipe flow Discharge (Q) (called also as the volume flow rate) is the volume of fluid that passes through an area per unit time. The discharge

More information

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.

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. 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. Q.2 Consider the forces of magnitude F acting on the sides of the regular hexagon having

More information

Experimental study and modeling of hydromechanical behavior of concrete fracture

Experimental study and modeling of hydromechanical behavior of concrete fracture Water Science and Engineering 2017, 10(2): 97e106 HOSTED BY Available online at www.sciencedirect.com Water Science and Engineering journal homepage: http://www.waterjournal.cn Experimental study and modeling

More information

Sheared Fracture Conductivity

Sheared Fracture Conductivity PROCEEDINGS, Thirty-Ninth Workshop on Geothermal Reservoir Engineering Stanford University, Stanford, California, February 24-26, 2014 SGP-TR-202 Sheared Fracture Conductivity Ravindra Bhide 1, Tyler Gohring

More information

Lesson 6 Review of fundamentals: Fluid flow

Lesson 6 Review of fundamentals: Fluid flow Lesson 6 Review of fundamentals: Fluid flow The specific objective of this lesson is to conduct a brief review of the fundamentals of fluid flow and present: A general equation for conservation of mass

More information

Brittle Deformation. Earth Structure (2 nd Edition), 2004 W.W. Norton & Co, New York Slide show by Ben van der Pluijm

Brittle Deformation. Earth Structure (2 nd Edition), 2004 W.W. Norton & Co, New York Slide show by Ben van der Pluijm Lecture 6 Brittle Deformation Earth Structure (2 nd Edition), 2004 W.W. Norton & Co, New York Slide show by Ben van der Pluijm WW Norton, unless noted otherwise Brittle deformation EarthStructure (2 nd

More information

A new method to estimate the permeability of rock mass around tunnels Mahdi Zoorabadi

A new method to estimate the permeability of rock mass around tunnels Mahdi Zoorabadi A new method to estimate the permeability of rock mass around tunnels Mahdi Zoorabadi School of Mining Engineering, The University of New South Wales, Sydney, NSW 2052, Australia E-mail: m.zoorabadi@unsw.edu.au

More information

Watershed Sciences 6900 FLUVIAL HYDRAULICS & ECOHYDRAULICS

Watershed Sciences 6900 FLUVIAL HYDRAULICS & ECOHYDRAULICS Watershed Sciences 6900 FLUVIAL HYDRAULICS & ECOHYDRAULICS WEEK Four Lecture 6 VELOCITY DISTRIBUTION Joe Wheaton FOR TODAY, YOU SHOULD HAVE READ 1 LET S GET ON WITH IT TODAY S PLAN VELOCITY DISTRIBUTIONS

More information

PIPE FLOWS: LECTURE /04/2017. Yesterday, for the example problem Δp = f(v, ρ, μ, L, D) We came up with the non dimensional relation

PIPE FLOWS: LECTURE /04/2017. Yesterday, for the example problem Δp = f(v, ρ, μ, L, D) We came up with the non dimensional relation /04/07 ECTURE 4 PIPE FOWS: Yesterday, for the example problem Δp = f(v, ρ, μ,, ) We came up with the non dimensional relation f (, ) 3 V or, p f(, ) You can plot π versus π with π 3 as a parameter. Or,

More information

Fracture-Matrix Flow Partitioning and Cross Flow: Numerical Modeling of Laboratory Fractured Core Flood

Fracture-Matrix Flow Partitioning and Cross Flow: Numerical Modeling of Laboratory Fractured Core Flood Fracture-Matrix Flow Partitioning and Cross Flow: Numerical Modeling of Laboratory Fractured Core Flood R. Sanaee *, G. F. Oluyemi, M. Hossain, and M. B. Oyeneyin Robert Gordon University *Corresponding

More information

A modified model of a single rock joint s shear behavior in

A modified model of a single rock joint s shear behavior in This paper is accepted for publication in the International Journal of Mining Science and Technology A modified model of a single rock joint s shear behavior in limestone specimens Dindarloo Saeid R a*,

More information

SHEAR BEHAVIOUR OF JOINTED ROCK: A STATE OF ART

SHEAR BEHAVIOUR OF JOINTED ROCK: A STATE OF ART IGC 2009, Guntur, INDIA SHEAR BEHAVIOUR OF JOINTED ROCK: A STATE OF ART A.K. Shrivastava Lecturer, Department of Civil Engineering, Delhi College of Engineering, Delhi 110 042, India. E-mail: aksrivastava@dce.ac.in

More information

Fluid Mechanics Prof. T.I. Eldho Department of Civil Engineering Indian Institute of Technology, Bombay. Lecture - 17 Laminar and Turbulent flows

Fluid Mechanics Prof. T.I. Eldho Department of Civil Engineering Indian Institute of Technology, Bombay. Lecture - 17 Laminar and Turbulent flows Fluid Mechanics Prof. T.I. Eldho Department of Civil Engineering Indian Institute of Technology, Bombay Lecture - 17 Laminar and Turbulent flows Welcome back to the video course on fluid mechanics. In

More information

OE4625 Dredge Pumps and Slurry Transport. Vaclav Matousek October 13, 2004

OE4625 Dredge Pumps and Slurry Transport. Vaclav Matousek October 13, 2004 OE465 Vaclav Matousek October 13, 004 1 Dredge Vermelding Pumps onderdeel and Slurry organisatie Transport OE465 Vaclav Matousek October 13, 004 Dredge Vermelding Pumps onderdeel and Slurry organisatie

More information

ROCK MASS PROPERTIES FOR TUNNELLING

ROCK MASS PROPERTIES FOR TUNNELLING ROCK MASS PROPERTIES FOR TUNNELLING Robert Bertuzzi 2 nd November 2017 1 Driver Estimating the strength and deformation characteristics of a rock mass for tunnel design is generally based on empiricism

More information

Chapter 9 Solids and Fluids. Elasticity Archimedes Principle Bernoulli s Equation

Chapter 9 Solids and Fluids. Elasticity Archimedes Principle Bernoulli s Equation Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli s Equation States of Matter Solid Liquid Gas Plasmas Solids: Stress and Strain Stress = Measure of force felt by material Stress= Force

More information

Lab-scale Investigation of a Multi Well Enhanced Geothermal Reservoir

Lab-scale Investigation of a Multi Well Enhanced Geothermal Reservoir PROCEEDINGS, 43rd Workshop on Geothermal Reservoir Engineering Stanford University, Stanford, California, February 12-14, 2018 SGP-TR-213 Lab-scale Investigation of a Multi Well Enhanced Geothermal Reservoir

More information

MODELING FLUID FLOW THROUGH A SINGLE FRACTURE USING EXPERIMENTAL, STOCHASTIC, AND SIMULATION APPROACHES. A Thesis DICMAN ALFRED

MODELING FLUID FLOW THROUGH A SINGLE FRACTURE USING EXPERIMENTAL, STOCHASTIC, AND SIMULATION APPROACHES. A Thesis DICMAN ALFRED MODELING FLUID FLOW THROUGH A SINGLE FRACTURE USING EXPERIMENTAL, STOCHASTIC, AND SIMULATION APPROACHES A Thesis by DICMAN ALFRED Submitted to the Office of Graduate Studies of Texas A&M University in

More information

N = Shear stress / Shear strain

N = Shear stress / Shear strain UNIT - I 1. What is meant by factor of safety? [A/M-15] It is the ratio between ultimate stress to the working stress. Factor of safety = Ultimate stress Permissible stress 2. Define Resilience. [A/M-15]

More information

Chapter 6. Losses due to Fluid Friction

Chapter 6. Losses due to Fluid Friction Chapter 6 Losses due to Fluid Friction 1 Objectives To measure the pressure drop in the straight section of smooth, rough, and packed pipes as a function of flow rate. To correlate this in terms of the

More information

Hydraulics. B.E. (Civil), Year/Part: II/II. Tutorial solutions: Pipe flow. Tutorial 1

Hydraulics. B.E. (Civil), Year/Part: II/II. Tutorial solutions: Pipe flow. Tutorial 1 Hydraulics B.E. (Civil), Year/Part: II/II Tutorial solutions: Pipe flow Tutorial 1 -by Dr. K.N. Dulal Laminar flow 1. A pipe 200mm in diameter and 20km long conveys oil of density 900 kg/m 3 and viscosity

More information

Chapter 10 Flow in Conduits

Chapter 10 Flow in Conduits Chapter 10 Flow in Conduits 10.1 Classifying Flow Laminar Flow and Turbulent Flow Laminar flow Unpredictable Turbulent flow Near entrance: undeveloped developing flow In developing flow, the wall shear

More information

Coupled analysis of two-phase flow in rough rock fractures

Coupled analysis of two-phase flow in rough rock fractures University of Wollongong Thesis Collections University of Wollongong Thesis Collection University of Wollongong Year 2005 Coupled analysis of two-phase flow in rough rock fractures Jeffrey Richard Price

More information

The use of straddle packer testing to hydraulically characterize rock boreholes for contaminant transport studies

The use of straddle packer testing to hydraulically characterize rock boreholes for contaminant transport studies The use of straddle packer testing to hydraulically characterize rock boreholes for contaminant transport studies Patryk Quinn, John Cherry, Beth Parker Presentation for the Solinst Symposium November

More information

3D simulations of an injection test done into an unsaturated porous and fractured limestone

3D simulations of an injection test done into an unsaturated porous and fractured limestone 3D simulations of an injection test done into an unsaturated porous and fractured limestone A. Thoraval *, Y. Guglielmi, F. Cappa INERIS, Ecole des Mines de Nancy, FRANCE *Corresponding author: Ecole des

More information

Friction in Rocks Assigned Reading: {Marone, 1998 #3905; Chapter 8 in \Paterson, 2005 #5865} Resource reading: {Scholz, 1990 #4288; Ruina, 1985 #1586}

Friction in Rocks Assigned Reading: {Marone, 1998 #3905; Chapter 8 in \Paterson, 2005 #5865} Resource reading: {Scholz, 1990 #4288; Ruina, 1985 #1586} 12.524, 2005 09 28 LE04: Friction and Constitutive Laws 1 Friction in Rocks Assigned Reading: {Marone, 1998 #3905; Chapter 8 in \Paterson, 2005 #5865} Resource reading: {Scholz, 1990 #4288; Ruina, 1985

More information

States of Matter. Chapter 9 Solids and Fluids. Solids: Stress and Strain. Solids: Stress and Strain. Stress = Force Area. Strain =!

States of Matter. Chapter 9 Solids and Fluids. Solids: Stress and Strain. Solids: Stress and Strain. Stress = Force Area. Strain =! Elasticity Chapter 9 Solids and Fluids Archimedes Principle Bernoulli s Equation Solid Liquid Gas Plasmas States of Matter 1 2 Solids: Stress and Strain Solids: Stress and Strain Stress = Measure of force

More information

States of Matter. Chapter 9 Solids and Fluids. Solids: Stress and Strain. Solids: Stress and Strain. Stress = Force Area. Strain =!L L. Example 9.

States of Matter. Chapter 9 Solids and Fluids. Solids: Stress and Strain. Solids: Stress and Strain. Stress = Force Area. Strain =!L L. Example 9. Elasticity Chapter 9 Solids and Fluids Archimedes Principle Bernoulli s Equation Solid Liquid Gas Plasmas States of Matter Solids: Stress and Strain Solids: Stress and Strain Stress = Measure of force

More information

P Forsmark site investigation. Borehole: KFM01A Results of tilt testing. Panayiotis Chryssanthakis Norwegian Geotechnical Institute, Oslo

P Forsmark site investigation. Borehole: KFM01A Results of tilt testing. Panayiotis Chryssanthakis Norwegian Geotechnical Institute, Oslo P-03-108 Forsmark site investigation Borehole: KFM01A Results of tilt testing Panayiotis Chryssanthakis Norwegian Geotechnical Institute, Oslo June 2003 Svensk Kärnbränslehantering AB Swedish Nuclear Fuel

More information

2 FLUID FLOW IN JOINTS

2 FLUID FLOW IN JOINTS FLUID FLOW IN JOINTS 2-1 2 FLUID FLOW IN JOINTS 2.1 Introduction UDEC has the capability to perform the analysis of fluid flow through the fractures of a system of impermeable blocks. A fully coupled mechanical-hydraulic

More information

Evaluation of hydrodynamic dispersion parameters in fractured rocks

Evaluation of hydrodynamic dispersion parameters in fractured rocks Journal of Rock Mechanics and Geotechnical Engineering. 2010, 2 (3): 243 254 Evaluation of hydrodynamic dispersion parameters in fractured rocks Zhihong Zhao 1, anru Jing 1, Ivars Neretnieks 2 1 Department

More information

Gas Shale Hydraulic Fracturing, Enhancement. Ahmad Ghassemi

Gas Shale Hydraulic Fracturing, Enhancement. Ahmad Ghassemi Gas Shale Hydraulic Fracturing, Stimulated Volume and Permeability Enhancement Ahmad Ghassemi Tight Gas A reservoir that cannot produce gas in economic quantities without massive fracture stimulation treatments

More information

John E. Gale 1 and Eunjeong Seok 2

John E. Gale 1 and Eunjeong Seok 2 Field and Laboratory Coupled Fracture Deformation-Pore Pressure-Permeability Experiments That Provide Insight for Depressurization of Fractured Rock Slopes John E. Gale 1 and Eunjeong Seok 2 1 Fracflow

More information

Frictional Losses in Straight Pipe

Frictional Losses in Straight Pipe 2/2/206 CM325 Fundamentals of Chemical Engineering Laboratory Prelab Preparation for Frictional Losses in Straight Pipe Professor Faith Morrison Department of Chemical Engineering Michigan Technological

More information

R Long term stability of rock caverns BMA and BLA of SFR, Forsmark. Diego Mas Ivars, María Veiga Ríos Itasca Consultants AB

R Long term stability of rock caverns BMA and BLA of SFR, Forsmark. Diego Mas Ivars, María Veiga Ríos Itasca Consultants AB R-13-53 Long term stability of rock caverns and of SFR, Forsmark Diego Mas Ivars, María Veiga Ríos Itasca Consultants AB Wenjie Shiu, Itasca Consultants SAS Fredrik Johansson, Anders Fredriksson Sweco

More information

External Flow and Boundary Layer Concepts

External Flow and Boundary Layer Concepts 1 2 Lecture (8) on Fayoum University External Flow and Boundary Layer Concepts By Dr. Emad M. Saad Mechanical Engineering Dept. Faculty of Engineering Fayoum University Faculty of Engineering Mechanical

More information

Effect of time and wear on the basic friction angle of rock discontinuities

Effect of time and wear on the basic friction angle of rock discontinuities Effect of time and wear on the basic friction angle of rock discontinuities Ignacio Pérez Rey, Leandro R. Alejano, Noelia González Pastoriza, Javier González, Javier Arzúa John P. Harrison Rock Mechanics

More information

PUBLICATIONS. Geophysical Research Letters. Postinjection Normal Closure of Fractures as a Mechanism for Induced Seismicity

PUBLICATIONS. Geophysical Research Letters. Postinjection Normal Closure of Fractures as a Mechanism for Induced Seismicity PUBLICATIONS Geophysical Research Letters RESEARCH LETTER Key Points: Normal closure of stimulated fractures after the termination of injection enhances postinjection seismicity Processes are strongly

More information

Lecture #2: Split Hopkinson Bar Systems

Lecture #2: Split Hopkinson Bar Systems Lecture #2: Split Hopkinson Bar Systems by Dirk Mohr ETH Zurich, Department of Mechanical and Process Engineering, Chair of Computational Modeling of Materials in Manufacturing 2015 1 1 1 Uniaxial Compression

More information

Outline: Types of Friction Dry Friction Static vs. Kinetic Angles Applications of Friction. ENGR 1205 Appendix B

Outline: Types of Friction Dry Friction Static vs. Kinetic Angles Applications of Friction. ENGR 1205 Appendix B Outline: Types of Friction Dry Friction Static vs. Kinetic Angles Applications of Friction ENGR 1205 Appendix B 1 Contacting surfaces typically support normal and tangential forces Friction is a tangential

More information

The Influence of Rock Mineralogy on Reactive Fracture Evolution in Carbonate-rich Caprocks

The Influence of Rock Mineralogy on Reactive Fracture Evolution in Carbonate-rich Caprocks The Influence of Rock Mineralogy on Reactive Fracture Evolution in Carbonate-rich Caprocks Kasparas Spokas 1, Catherine A. Peters 1 *, Laura Pyrak-Nolte 2,3,4 1 Department of Civil & Environmental Engineering,

More information

Estimating Permeability from Acoustic Velocity and Formation Resistivity Factor

Estimating Permeability from Acoustic Velocity and Formation Resistivity Factor 5th Conference & Exposition on Petroleum Geophysics, Hyderabad-2004, India PP 582-587 and Formation Resistivity Factor Majid Nabi-Bidhendi Institute of Geophysics, University of Tehran, P.O. Box 14155-6466,

More information

A CONSTITUTIVE MODEL TO PREDICT THE HYDROMECHANICAL BEHAVIOUR OF ROCK JOINTS

A CONSTITUTIVE MODEL TO PREDICT THE HYDROMECHANICAL BEHAVIOUR OF ROCK JOINTS OttawaGeo27/OttawaGéo27 A CONSTITUTIVE MODEL TO PREDICT THE HYDROMECHANICAL BEHAVIOUR OF ROCK JOINTS Dominic Tremblay, Richard Simon and Michel Aubertin Department of civil, geological & mining engineering

More information

20. Rheology & Linear Elasticity

20. Rheology & Linear Elasticity I Main Topics A Rheology: Macroscopic deformation behavior B Linear elasticity for homogeneous isotropic materials 10/29/18 GG303 1 Viscous (fluid) Behavior http://manoa.hawaii.edu/graduate/content/slide-lava

More information

The effect of dip of joints on the axial force of rock bolts

The effect of dip of joints on the axial force of rock bolts Journal of Novel Applied Sciences Available online at www.jnasci.org 2015 JNAS Journal-2015-4-4/457-462 ISSN 2322-5149 2015 JNAS The effect of dip of joints on the axial force of rock bolts Farzad bayat

More information

Laminar Flow. Chapter ZERO PRESSURE GRADIENT

Laminar Flow. Chapter ZERO PRESSURE GRADIENT Chapter 2 Laminar Flow 2.1 ZERO PRESSRE GRADIENT Problem 2.1.1 Consider a uniform flow of velocity over a flat plate of length L of a fluid of kinematic viscosity ν. Assume that the fluid is incompressible

More information

2, where dp is the constant, R is the radius of

2, where dp is the constant, R is the radius of Dynamics of Viscous Flows (Lectures 8 to ) Q. Choose the correct answer (i) The average velocity of a one-dimensional incompressible fully developed viscous flow between two fixed parallel plates is m/s.

More information

3D HM-DEM model for Hydro-Fracturing

3D HM-DEM model for Hydro-Fracturing 3D HM-DEM model for Hydro-Fracturing E. Papachristos, F.V. Donzé & B. Chareyre Laboratoire Sols, Solides, Structures, Grenoble, France efthymios.papachristos@3sr-grenoble.fr,, frederic.donze@3srgrenoble.fr,

More information

CHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS

CHAPTER 3 THE EFFECTS OF FORCES ON MATERIALS CHAPTER THE EFFECTS OF FORCES ON MATERIALS EXERCISE 1, Page 50 1. A rectangular bar having a cross-sectional area of 80 mm has a tensile force of 0 kn applied to it. Determine the stress in the bar. Stress

More information

The most common methods to identify velocity of flow are pathlines, streaklines and streamlines.

The most common methods to identify velocity of flow are pathlines, streaklines and streamlines. 4 FLUID FLOW 4.1 Introduction Many civil engineering problems in fluid mechanics are concerned with fluids in motion. The distribution of potable water, the collection of domestic sewage and storm water,

More information

R T-H-M couplings in rock. Overview of results of importance to the SR-Can safety assessment. Harald Hökmark, Billy Fälth, Clay Technology AB

R T-H-M couplings in rock. Overview of results of importance to the SR-Can safety assessment. Harald Hökmark, Billy Fälth, Clay Technology AB R-6-88 T-H-M couplings in rock Overview of results of importance to the SR-Can safety assessment Harald Hökmark, Billy Fälth, Clay Technology AB Thomas Wallroth, BERGAB September 26 Svensk Kärnbränslehantering

More information

Rheology and the Lithosphere

Rheology and the Lithosphere Rheology and the Lithosphere Processes in Structural Geology & Tectonics Ben van der Pluijm WW Norton+Authors, unless noted otherwise 3/8/2017 16:51 We Discuss Rheology and the Lithosphere What is rheology?

More information

PUBLICATIONS. Water Resources Research. Critical Reynolds number for nonlinear flow through rough-walled fractures: The role of shear processes

PUBLICATIONS. Water Resources Research. Critical Reynolds number for nonlinear flow through rough-walled fractures: The role of shear processes PUBLICATIONS Water Resources Research RESEARCH ARTICLE Key Points: A criterion for flow nonlinearity (CFN model) was developed for rock fractures Critical Reynolds number was defined based on the CFN model

More information

Material is perfectly elastic until it undergoes brittle fracture when applied stress reaches σ f

Material is perfectly elastic until it undergoes brittle fracture when applied stress reaches σ f Material is perfectly elastic until it undergoes brittle fracture when applied stress reaches σ f Material undergoes plastic deformation when stress exceeds yield stress σ 0 Permanent strain results from

More information

Effects of shearing direction on shear behaviour of rock joints

Effects of shearing direction on shear behaviour of rock joints University of Wollongong Research Online Coal Operators' Conference Faculty of Engineering and Information Sciences 2014 Effects of shearing direction on shear behaviour of rock joints Ali Mirzaghorbanali

More information

Experiment (4): Flow measurement

Experiment (4): Flow measurement Experiment (4): Flow measurement Introduction: The flow measuring apparatus is used to familiarize the students with typical methods of flow measurement of an incompressible fluid and, at the same time

More information

Analysis of Fracture Network Response to Fluid Injection

Analysis of Fracture Network Response to Fluid Injection PROCEEDINGS, Fourtieth Workshop on Geothermal Reservoir Engineering Stanford University, Stanford, California, January 26-28, 2015 SGP-TR-204 Analysis of Fracture Network Response to Fluid Injection Moien

More information

THE EFFECT OF THERMOELASTIC STRESS CHANGE IN THE NEAR WELLBORE REGION ON HYDRAULIC FRACTURE GROWTH

THE EFFECT OF THERMOELASTIC STRESS CHANGE IN THE NEAR WELLBORE REGION ON HYDRAULIC FRACTURE GROWTH PROCEEDINGS, Thirty-Seventh Workshop on Geothermal Reservoir Engineering Stanford University, Stanford, California, 30 Jan 2011-1 Feb 2012 THE EFFECT OF THERMOELASTIC STRESS CHANGE IN THE NEAR WELLBORE

More information

Production-induced stress change in and above a reservoir pierced by two salt domes: A geomechanical model and its applications

Production-induced stress change in and above a reservoir pierced by two salt domes: A geomechanical model and its applications Production-induced stress change in and above a reservoir pierced by two salt domes: A geomechanical model and its applications Peter Schutjens, Jeroen Snippe, Hassan Mahani, Jane Turner, Joel Ita and

More information

ME 305 Fluid Mechanics I. Part 8 Viscous Flow in Pipes and Ducts. Flow in Pipes and Ducts. Flow in Pipes and Ducts (cont d)

ME 305 Fluid Mechanics I. Part 8 Viscous Flow in Pipes and Ducts. Flow in Pipes and Ducts. Flow in Pipes and Ducts (cont d) ME 305 Fluid Mechanics I Flow in Pipes and Ducts Flow in closed conduits (circular pipes and non-circular ducts) are very common. Part 8 Viscous Flow in Pipes and Ducts These presentations are prepared

More information

Dry Friction Static vs. Kinetic Angles

Dry Friction Static vs. Kinetic Angles Outline: Types of Friction Dry Friction Static vs. Kinetic Angles Applications of Friction 1 Contacting surfaces typically support normal and tangential forces Friction is a tangential force Friction occurs

More information

FE Exam Fluids Review October 23, Important Concepts

FE Exam Fluids Review October 23, Important Concepts FE Exam Fluids Review October 3, 013 mportant Concepts Density, specific volume, specific weight, specific gravity (Water 1000 kg/m^3, Air 1. kg/m^3) Meaning & Symbols? Stress, Pressure, Viscosity; Meaning

More information

Initial and Boundary Conditions

Initial and Boundary Conditions Initial and Boundary Conditions Initial- and boundary conditions are needed For a steady problems correct initial conditions is important to reduce computational time and reach convergence Boundary conditions

More information

FE Fluids Review March 23, 2012 Steve Burian (Civil & Environmental Engineering)

FE Fluids Review March 23, 2012 Steve Burian (Civil & Environmental Engineering) Topic: Fluid Properties 1. If 6 m 3 of oil weighs 47 kn, calculate its specific weight, density, and specific gravity. 2. 10.0 L of an incompressible liquid exert a force of 20 N at the earth s surface.

More information

Piping Systems and Flow Analysis (Chapter 3)

Piping Systems and Flow Analysis (Chapter 3) Piping Systems and Flow Analysis (Chapter 3) 2 Learning Outcomes (Chapter 3) Losses in Piping Systems Major losses Minor losses Pipe Networks Pipes in series Pipes in parallel Manifolds and Distribution

More information

Chapter 3 Permeability

Chapter 3 Permeability 3.2 Darcy s Law In 1856, Darcy investigated the flow of water through sand filters for water purification. His experimental apparatus is shown in Figure 3.11. By empirical observation Figure 3.11 Schematic

More information

Numerical Simulation of Unsaturated Infilled Joints in Shear

Numerical Simulation of Unsaturated Infilled Joints in Shear University of Wollongong Research Online Coal Operators' Conference Faculty of Engineering and Information Sciences 2018 Numerical Simulation of Unsaturated Infilled Joints in Shear Libin Gong University

More information