CVEEN Table of Contents

Size: px
Start display at page:

Download "CVEEN Table of Contents"

Transcription

1 CVEEN 7330 Table of Contents Table of Contents... 1 Objectives... 2 ackground... 2 Model Setup and Analysis Input... 2 Data for Interfaces... 5 Required Outputs from FLAC Required Calculations and Discussion FLAC Solution: Discussion FISH Code for model... 15

2 Objectives In this exercise, the student develops a FLAC model to replicate the dynamic behavior of geofoam embankment for the case of a rectangular geofoam mass resting on a soil foundation with sliding allowed in the geofoam under horizontal sinusoidal input motion only. The lump mass (load distribution slab, untreated base course and concrete pavement) is placed atop the geofoam and bonded to the top layer, so slippage is not allowed at this interface. ackground Dynamic sliding is one mode of failure and can be explored using interface elements in FLAC and the appropriate friction angle for the interfaces. Model Setup and Analysis Input 1. Model Type: Elastic 2. Elastic material properties ρ (kg/m 3 ) γ (lb/ft 3 ) E (MPa) v K (MPa) G (MPa) Soil Goafoam UTC LDS & PCCP Foundation soil properties (Vs = 1000 ft/s and = 0.35) prop bulk 500e6 shear 185e6 den 2000 Geofoam properties prop bulk 4.198e6 shear 4.53e6 den 20 Concrete mass above geofoam properties prop bulk 15625e6 shear den 2305

3 3. Geometry (Figure 1 below) 4. oundary Conditions a. Static conditions with gravity on see Figure 2. b. Dynamic conditions with horizontal velocity wave - see Figure 3. JO TITLE :. FLAC (Version 5.00) LEGEND Apr-08 7:54 step E+00 <x< 2.111E E+00 <y< 1.661E Grid plot 4 0 5E 0 interface id#'s Fixed Gridpoints -direction oth directions Steven artlett University of Utah Figure 1. Geofoam/Soil model and boundary conditions for static loading under gravity.

4 JO TITLE :. FLAC (Version 5.00) LEGEND Apr-08 7:57 step E+00 <x< 2.111E E+00 <y< 1.661E shear_mod 4.530E E E+10 Fixed Gridpoints -direction oth directions Grid plot 0 5E 0 interface id#'s Steven artlett University of Utah Figure 2. Plot of shear modulus for model. JO TITLE :. FLAC (Version 5.00) LEGEND Apr-08 8:11 step Dynamic Time E E+00 <x< 2.116E E+00 <y< 1.664E+01 shear_mod 4.530E E E+10 Fixed Gridpoints -direction oth directions Grid plot 0 5E 0 interface id#'s Steven artlett University of Utah Figure 3. oundary conditions for dynamic sliding case.

5 5. Fish code for sliding interfaces within geofoam (Fig. 1) a. Generate grid b. Declare model type (note: gaps in model type are left for interfaces) c. Assign elastic properties d. Assign grid to coordinate space (with generate command) e. Create interfaces for sliding planes f. Assign interface properties sand-geofoam interface friction = 31 degrees geofoam-geofoam interface friction = 32 degress normal and shear spring constants 1. Normal Stiffness = 10(K+4/3G)/Δzmin, normal 2. Shear Stiffness = 10(K+4/3G)/Δzmin, normal Data for Interfaces int Normal Stiffness = kn = ks (MPa) Friction Cohesion Dilation z Geofoam-soil Geof-Geof Geofoam-lds glued lds-utbc glued utbc-pccp glued **Use least stiff of two adjacent layers for kn and ks FLAC code for Step 5 generation of grid grid declare model type model elastic j 1 5 model elastic i 6 15 j 7 model elastic i 6 15 j 9 model elastic i 6 15 j 11 model elastic i 6 15 j 13 model elastic i 6 15 j 15 model elastic i 6 15 j 17

6 assign elastic properties prop bulk 500e6 shear 185e6 den 2000 i 1 20 j 1 5 foundation properties vs = 1000 ft/s prop bulk 4.20e6 shear 4.53e6 den 20 i 6 15 j 7 geofoam properties prop bulk 4.20e6 shear 4.53e6 den 20 i 6 15 j 9 geofoam properties prop bulk 4.20e6 shear 4.53e6 den 20 i 6 15 j 11 geofoam properties prop bulk 4.20e6 shear 4.53e6 den 20 i 6 15 j 13 geofoam properties prop bulk 4.20e6 shear 4.53e6 den 20 i 6 15 j 15 geofoam properties prop bulk 15625e6 shear 12712e6den 2305 i 6 15 j 17 mass above geofoam Assign grid to coordinate space gen i 1 21 j 1 6 gen i 6 16 j 7 8 gen i 6 16 j 9 10 gen i 6 16 j gen i 6 16 j gen i 6 16 j gen i 6 16 j create interfaces int 1 Aside from 6,6 to 16,6 side from 6,7 to 16,7 int 2 Aside from 6,8 to 16,8 side from 6,9 to 16,9 int 3 Aside from 6,10 to 16,10 side from 6,11 to 16,11 int 4 Aside from 6,12 to 16,12 side from 6,13 to 16,13 int 5 Aside from 6,14 to 16,14 side from 6,15 to 16,15 int 6 Aside from 6,16 to 16,16 side from 6,17 to 16,17 assign inteface properties int 1 kn 102e6 ks 102e6 friction = 35 coh = 0 dilation = 6 tbond=0 bslip on int 2 kn 102e6 ks 102e6 friction = 32 coh = 0 dilation = 0 tbond=0 bslip on int 3 kn 102e6 ks 102e6 friction = 32 coh = 0 dilation = 0 tbond=0 bslip on int 4 kn 102e6 ks 102e6 friction = 32 coh = 0 dilation = 0 tbond=0 bslip on int 5 kn 102e6 ks 102e6 friction = 32 coh = 0 dilation = 0 tbond=0 bslip on int 6 glue kn 102e6 ks 102e6 6. Perform static analysis a. Turn gravity on b. Establish boundary conditions c. Turn off dynamic module d. Make history of unbalanced forces (his 20) e. Solve for static case by stepping 9000 steps FLAC code for Step 6 GRAVIT ON FOR STATIC FORCES set grav 9.81

7 OUNDAR CONDITIONS FOR STATIC CASE fix right side of soil box fix x i 1 fix left side of soil box fix x i 21 fix x i 6 j 7 18 (don't fix x in geofoam for static case) fix x i 16 j 7 18 (don't fix x in geofoam for static case) fix base fix y j 1 fix x j 1 STATIC LOADING set dyn off his 20 unbal solve 7. Turn on dynamic mode and establish large strain conditions and damping properties. (Note that no damping other than Rayleigh damping has been used for the soil.) (Note hysteretic damping has been used for geofoam using sigmoidal model.) set dyn on set large set dy_damp rayl j 1 5 damping in geofoam ini dy_damp=hyst sig j 7 ini dy_damp=hyst sig j 9 ini dy_damp=hyst sig j 11 ini dy_damp=hyst sig j 13 ini dy_damp=hyst sig j 15 Calculations of hysteretic damping using sigmoidal model a = 1 b = x o = 0.3 Geofoam (lab) Geofoam (sig3 model) L Ms g L Ms

8 G/Gmax L = log 10 Ms = G/Gmax Clay (Seed and Sun) Geofoam (Lab) Geofoam (sig3 model) Shear strain (percent) Figure 4. Sigmodial 3 model fit to geofoam data

9 8. Establish boundary conditions for dynamic case ESTALISH OUNDARIES FOR DNAMIC CASE free x free y OUNDAR CONDITIONS FOR DNAMIC CASE for horizontal wave only fix y j 1 6 fix x j 1 9. Create horizontal wave (1 g amplitude wave at fundamental frequency of geofoam) a. Horizontal velocity wave amplitude = 0.65 m/s for 1 g acceleration. b. Horizontal wave period = 0.41 s (fundamental period of geofoam) CREATE WAVES wave 1 is horizontal wave def wave1 for free vibration wave1=amp1*cos(2*pi/period1*dytime)/(dytime+1)^10 for forced vibration wave1=amp1*cos(2*pi/period1*dytime) end set amp1 = 0.65 for 10 m/s2 accel at base set period1 = 0.41 period1 of 0.41 s is resonant frequency 10. Input waves into bottom of model FOR HOR. WAVE apply xvel 1 hist=wave1 j=1 11. Establish locations for dynamic histories (See Fig. 3) HISTORIES his 1 dytime his 2 wave1 his 3 xvel j 1 i 11 his 4 xdisp j 1 i 11 his 5 xvel j 6 i 11 his 6 xdisp j 6 i 11 his 7 xvel j 18 i 11 his 8 xdisp j 18 i 11 his 10 yvel j 1 i 11

10 his 11 ydisp j 1 i 11 his 12 yvel j 6 i 11 his 13 ydisp j 6 i 11 his 14 yvel j 18 i 11 his 15 ydisp j 18 i 11 his 16 xacc j 1 i 11 his 17 xacc j 6 i 11 his 18 xacc j 18 i Reset displacements to start dynamic case ini xdisp = 0 ydisp = Solve for dynamic case for 4 seconds solve dytime 4.0 Required Outputs from FLAC 1. Plot of the following at the resonant period for a duration t = 5 s. Make all plots at the middle (centerline) of the model: a. Unbalanced forces from static and dynamic loading b. displacement at bottom of soil c. displacement at top of soil d. displacement top of pavement e. acceleration at bottom of soil f. acceleration at top of soil g. acceleration at top of pavement h. Final vector displacement pattern at time = 4 seconds 2. Animation of displacement vectors using an increment of 500 steps for t = 4 s. Required Calculations and Discussion 1. Discuss how the change in the amplitude of the horizontal wave affects the displacement at the top of the geofoam and the sliding within the geofoam. Use graphs or figures to do this. FLAC Solution:

2D Embankment and Slope Analysis (Numerical)

2D Embankment and Slope Analysis (Numerical) 2D Embankment and Slope Analysis (Numerical) Page 1 2D Embankment and Slope Analysis (Numerical) Sunday, August 14, 2011 Reading Assignment Lecture Notes Other Materials FLAC Manual 1. 2. Homework Assignment

More information

CVEEN 7330 Modeling Exercise 2c

CVEEN 7330 Modeling Exercise 2c CVEEN 7330 Modeling Exercise 2c Table of Contents Table of Contents... 1 Objectives:... 2 FLAC Input:... 2 DEEPSOIL INPUTS:... 5 Required Outputs from FLAC:... 6 Required Output from DEEPSOIL:... 6 Additional

More information

CVEEN Table of Contents

CVEEN Table of Contents CVEEN 7330 Table of Contents Table of Contents... 1 Objectives:... 2 FLAC Input:... 3 Model Inputs... 3 Create Grid and Assign Properties... 4 Create Foundation... 4 Create Forcing Function... 4 Create

More information

Numerical Modeling in Geotechnical Engineering October 17,

Numerical Modeling in Geotechnical Engineering October 17, 1 Numerical Modeling in Geotechnical Engineering October 17, 18 2014 PRESENTED BY: Siavash Zamiran Ph.D. Student, Research and Teaching Assistant, Department of Civil Engineering, Southern Illinois University

More information

Earth Pressure Theory

Earth Pressure Theory Lateral Earth Pressure Page 1 Earth Pressure Theory Examples of Retaining Walls Lateral Earth Pressure Page 2 At-Rest, Active and Passive Earth Pressure Wednesday, August 17, 2011 12:45 PM At-rest condition

More information

Dynamic Analysis Contents - 1

Dynamic Analysis Contents - 1 Dynamic Analysis Contents - 1 TABLE OF CONTENTS 1 DYNAMIC ANALYSIS 1.1 Overview... 1-1 1.2 Relation to Equivalent-Linear Methods... 1-2 1.2.1 Characteristics of the Equivalent-Linear Method... 1-2 1.2.2

More information

1D Nonlinear Numerical Methods

1D Nonlinear Numerical Methods 1D Nonlinear Numerical Methods Page 1 1D Nonlinear Numerical Methods Reading Assignment Lecture Notes Pp. 275-280 Kramer DEEPSOIL.pdf 2001 Darendeli, Ch. 10 Other Materials DeepSoil User's Manual 2001

More information

Recent Research on EPS Geofoam Seismic Buffers. Richard J. Bathurst and Saman Zarnani GeoEngineering Centre at Queen s-rmc Canada

Recent Research on EPS Geofoam Seismic Buffers. Richard J. Bathurst and Saman Zarnani GeoEngineering Centre at Queen s-rmc Canada Recent Research on EPS Geofoam Seismic Buffers Richard J. Bathurst and Saman Zarnani GeoEngineering Centre at Queen s-rmc Canada What is a wall (SEISMIC) buffer? A compressible inclusion placed between

More information

1 Slope Stability for a Cohesive and Frictional Soil

1 Slope Stability for a Cohesive and Frictional Soil Slope Stability for a Cohesive and Frictional Soil 1-1 1 Slope Stability for a Cohesive and Frictional Soil 1.1 Problem Statement A common problem encountered in engineering soil mechanics is the stability

More information

7 Uniaxial Compressive Strength of a Jointed Rock Sample

7 Uniaxial Compressive Strength of a Jointed Rock Sample Uniaxial Compressive Strength of a Jointed Rock Sample 7-1 7 Uniaxial Compressive Strength of a Jointed Rock Sample 7.1 Problem Statement The uniaxial compressive strength of a jointed rock sample is a

More information

13 Plastic Flow in a Punch Problem

13 Plastic Flow in a Punch Problem Plastic Flow in a Punch Problem 13-1 13 Plastic Flow in a Punch Problem 13.1 Problem Statement Difficulties are sometimes reported in the modeling of plastic flow where large velocity gradients exist.

More information

DYNAMIC ANALYSIS OF PILES IN SAND BASED ON SOIL-PILE INTERACTION

DYNAMIC ANALYSIS OF PILES IN SAND BASED ON SOIL-PILE INTERACTION October 1-17,, Beijing, China DYNAMIC ANALYSIS OF PILES IN SAND BASED ON SOIL-PILE INTERACTION Mohammad M. Ahmadi 1 and Mahdi Ehsani 1 Assistant Professor, Dept. of Civil Engineering, Geotechnical Group,

More information

1 Slope Stability for a Cohesive and Frictional Soil

1 Slope Stability for a Cohesive and Frictional Soil Slope Stability for a Cohesive and Frictional Soil 1-1 1 Slope Stability for a Cohesive and Frictional Soil 1.1 Problem Statement A common problem encountered in engineering soil mechanics is the stability

More information

8 Displacements near the Face of an Advancing Shaft

8 Displacements near the Face of an Advancing Shaft Displacements near the Face of an Advancing Shaft 8-1 8 Displacements near the Face of an Advancing Shaft 8.1 Problem Statement A circular shaft is excavated in chalk and lined with monolithic precast

More information

Design Procedures For Dynamically Loaded Foundations

Design Procedures For Dynamically Loaded Foundations Design Procedures For Dynamically Loaded Foundations 1/11 Choice of parameters for equivalent lumped systems Lumped mass : the mass of the foundation and supported machinery Damping : 1 Geometrical(or

More information

10 Slope Stability Analysis of a Rock Slope

10 Slope Stability Analysis of a Rock Slope Slope Stability Analysis of a Rock Slope 10-1 10 Slope Stability Analysis of a Rock Slope 10.1 Problem Statement Limit equilibrium methods are commonly used to evaluate the stability of slopes in rock

More information

13 Dewatered Construction of a Braced Excavation

13 Dewatered Construction of a Braced Excavation Dewatered Construction of a Braced Excavation 13-1 13 Dewatered Construction of a Braced Excavation 13.1 Problem Statement A braced excavation is constructed in saturated ground. The excavation is dewatered

More information

13 Step-Path Failure of Rock Slopes

13 Step-Path Failure of Rock Slopes Step-Path Failure of Rock Slopes 13-1 13 Step-Path Failure of Rock Slopes 13.1 Problem Statement While UDEC represents a jointed rock structure as a system of discrete blocks by default, it is also a straightforward

More information

Effect of structural design on fundamental frequency of reinforced-soil retaining walls

Effect of structural design on fundamental frequency of reinforced-soil retaining walls Soil Dynamics and Earthquake Engineering 19 (2000) 137 157 www.elsevier.com/locate/soildyn Effect of structural design on fundamental frequency of reinforced-soil retaining walls K. Hatami*, R.J. Bathurst

More information

Dynamics Manual. Version 7

Dynamics Manual. Version 7 Dynamics Manual Version 7 DYNAMICS MANUAL TABLE OF CONTENTS 1 Introduction...1-1 1.1 About this manual...1-1 2 Tutorial...2-1 2.1 Dynamic analysis of a generator on an elastic foundation...2-1 2.1.1 Input...2-1

More information

Figure A7 22: Micrograph of PX (a) before and (b) after heat treatment to 50ºC

Figure A7 22: Micrograph of PX (a) before and (b) after heat treatment to 50ºC Figure A7 22: Micrograph of PX (a) before and (b) after heat treatment to 50ºC 293 Figure A7 23: Micrograph of PX after heat treatment to 100ºC and 140ºC 294 Figure A7 24: Micrograph of VTA (a) before

More information

ON THE PREDICTION OF EXPERIMENTAL RESULTS FROM TWO PILE TESTS UNDER FORCED VIBRATIONS

ON THE PREDICTION OF EXPERIMENTAL RESULTS FROM TWO PILE TESTS UNDER FORCED VIBRATIONS Transactions, SMiRT-24 ON THE PREDICTION OF EXPERIMENTAL RESULTS FROM TWO PILE TESTS UNDER FORCED VIBRATIONS 1 Principal Engineer, MTR & Associates, USA INTRODUCTION Mansour Tabatabaie 1 Dynamic response

More information

4 Undrained Cylindrical Cavity Expansion in a Cam-Clay Medium

4 Undrained Cylindrical Cavity Expansion in a Cam-Clay Medium Undrained Cylindrical Cavity Expansion in a Cam-Clay Medium 4-1 4 Undrained Cylindrical Cavity Expansion in a Cam-Clay Medium 4.1 Problem Statement The stress and pore pressure changes due to the expansion

More information

NONLINEAR CHARACTERISTICS OF THE PILE-SOIL SYSTEM UNDER VERTICAL VIBRATION

NONLINEAR CHARACTERISTICS OF THE PILE-SOIL SYSTEM UNDER VERTICAL VIBRATION IGC 2009, Guntur, INDIA NONLINEAR CHARACTERISTICS OF THE PILE-SOIL SYSTEM UNDER VERTICAL VIBRATION B. Manna Lecturer, Civil Engineering Department, National Institute of Technology, Rourkela 769008, India.

More information

Introduction to structural dynamics

Introduction to structural dynamics Introduction to structural dynamics p n m n u n p n-1 p 3... m n-1 m 3... u n-1 u 3 k 1 c 1 u 1 u 2 k 2 m p 1 1 c 2 m2 p 2 k n c n m n u n p n m 2 p 2 u 2 m 1 p 1 u 1 Static vs dynamic analysis Static

More information

Lab Practical - Discontinuum Analysis & Distinct Element Method

Lab Practical - Discontinuum Analysis & Distinct Element Method Lab Practical - Discontinuum Analysis & Distinct Element Method Part A The Basics The Universal Distinct Element Code (UDEC) is a two-dimensional numerical program based on the distinct element method

More information

15 Drained and Undrained Triaxial Compression Test on a Cam-Clay Sample

15 Drained and Undrained Triaxial Compression Test on a Cam-Clay Sample Drained and Undrained Triaxial Compression Test on a Cam-Clay Sample 15-1 15 Drained and Undrained Triaxial Compression Test on a Cam-Clay Sample 15.1 Problem Statement Conventional drained and undrained

More information

Dynamic modelling in slopes using finite difference program

Dynamic modelling in slopes using finite difference program Bulletin of the Department of Geology Bulletin of the Department of Geology, Tribhuvan University, Kathmandu, Nepal, Vol. 12, 2009, pp. 89 94 Dynamic modelling in slopes using finite difference program

More information

10 Steady-State Fluid Flow with a Free Surface

10 Steady-State Fluid Flow with a Free Surface Steady-State Fluid Flow with a Free Surface 10-1 10 Steady-State Fluid Flow with a Free Surface 10.1 roblem Statement This numerical simulation analyzes the steady-state seepage flow through a homogeneous

More information

Lab Practical - Discontinuum Analysis & Distinct Element Method

Lab Practical - Discontinuum Analysis & Distinct Element Method Lab Practical - Discontinuum Analysis & Distinct Element Method Part A The Basics The Universal Distinct Element Code (UDEC) is a twodimensional numerical program based on the distinct element method for

More information

3 Cylindrical Hole in an Infinite Mohr-Coulomb Medium

3 Cylindrical Hole in an Infinite Mohr-Coulomb Medium Cylindrical Hole in an Infinite Mohr-Coulomb Medium 3-1 3 Cylindrical Hole in an Infinite Mohr-Coulomb Medium 3.1 Problem Statement The problem concerns the determination of stresses and displacements

More information

1 STRUCTURAL ELEMENTS

1 STRUCTURAL ELEMENTS STRUCTURAL ELEMENTS 1-1 1 STRUCTURAL ELEMENTS 1.1 Overview An important aspect of geomechanical analysis and design is the use of structural support to stabilize a rock or soil mass. Structures of arbitrary

More information

Codal Provisions IS 1893 (Part 1) 2002

Codal Provisions IS 1893 (Part 1) 2002 Abstract Codal Provisions IS 1893 (Part 1) 00 Paresh V. Patel Assistant Professor, Civil Engineering Department, Nirma Institute of Technology, Ahmedabad 38481 In this article codal provisions of IS 1893

More information

2D Liquefaction Analysis for Bridge Abutment

2D Liquefaction Analysis for Bridge Abutment D Liquefaction Analysis for Bridge Abutment Tutorial by Angel Francisco Martinez Integrated Solver Optimized for the next generation 64-bit platform Finite Element Solutions for Geotechnical Engineering

More information

Preliminary Examination - Dynamics

Preliminary Examination - Dynamics Name: University of California, Berkeley Fall Semester, 2018 Problem 1 (30% weight) Preliminary Examination - Dynamics An undamped SDOF system with mass m and stiffness k is initially at rest and is then

More information

Geotechnical Modeling Issues

Geotechnical Modeling Issues Nonlinear Analysis of Viaducts and Overpasses Geotechnical Modeling Issues Steve Kramer Pedro Arduino Hyung-Suk Shin University of Washington The Problem Approach Soil Soil Soil Soil Soil Soil Soil Soil

More information

1-160 Dynamic Analysis

1-160 Dynamic Analysis 1-160 Dynamic Analysis 1.6 Example Application of a Seismic Analysis An example application of a nonlinear seismic analysis is presented in this section. The example illustrates several of the topics discussed

More information

T1 T e c h n i c a l S e c t i o n

T1 T e c h n i c a l S e c t i o n 1.5 Principles of Noise Reduction A good vibration isolation system is reducing vibration transmission through structures and thus, radiation of these vibration into air, thereby reducing noise. There

More information

Dynamics of structures

Dynamics of structures Dynamics of structures 2.Vibrations: single degree of freedom system Arnaud Deraemaeker (aderaema@ulb.ac.be) 1 Outline of the chapter *One degree of freedom systems in real life Hypothesis Examples *Response

More information

Site Response Analysis with 2D-DDA

Site Response Analysis with 2D-DDA Site Response Analysis with 2D-DDA Yossef H. Hatzor Sam and Edna Lemkin Professor of Rock Mechanics Dept. of Geological and Environmental Sciences Ben-Gurion University of the Negev, Beer-Sheva, Israel

More information

INTI COLLEGE MALAYSIA

INTI COLLEGE MALAYSIA EGC373 (F) / Page 1 of 5 INTI COLLEGE MALAYSIA UK DEGREE TRANSFER PROGRAMME INTI ADELAIDE TRANSFER PROGRAMME EGC 373: FOUNDATION ENGINEERING FINAL EXAMINATION : AUGUST 00 SESSION This paper consists of

More information

Dynamic Analysis of a Reinforced Concrete Structure Using Plasticity and Interface Damage Models

Dynamic Analysis of a Reinforced Concrete Structure Using Plasticity and Interface Damage Models Dynamic Analysis of a Reinforced Concrete Structure Using Plasticity and Interface Damage Models I. Rhee, K.J. Willam, B.P. Shing, University of Colorado at Boulder ABSTRACT: This paper examines the global

More information

Dynamic Response of EPS Blocks /soil Sandwiched Wall/embankment

Dynamic Response of EPS Blocks /soil Sandwiched Wall/embankment Proc. of Second China-Japan Joint Symposium on Recent Development of Theory and Practice in Geotechnology, Hong Kong, China Dynamic Response of EPS Blocks /soil Sandwiched Wall/embankment J. C. Chai 1

More information

USER S MANUAL 1D Seismic Site Response Analysis Example University of California: San Diego August 30, 2017

USER S MANUAL 1D Seismic Site Response Analysis Example   University of California: San Diego August 30, 2017 USER S MANUAL 1D Seismic Site Response Analysis Example http://www.soilquake.net/ucsdsoilmodels/ University of California: San Diego August 30, 2017 Table of Contents USER'S MANUAL TABLE OF CONTENTS Page

More information

Numerical Modelling of Dynamic Earth Force Transmission to Underground Structures

Numerical Modelling of Dynamic Earth Force Transmission to Underground Structures Numerical Modelling of Dynamic Earth Force Transmission to Underground Structures N. Kodama Waseda Institute for Advanced Study, Waseda University, Japan K. Komiya Chiba Institute of Technology, Japan

More information

USER S MANUAL 1D Seismic Site Response Analysis Example University of California: San Diego August 30, 2017

USER S MANUAL 1D Seismic Site Response Analysis Example   University of California: San Diego August 30, 2017 USER S MANUAL 1D Seismic Site Response Analysis Example http://www.soilquake.net/ucsdsoilmodels/ University of California: San Diego August 30, 2017 Table of Contents USER'S MANUAL TABLE OF CONTENTS Page

More information

Example-3. Title. Description. Cylindrical Hole in an Infinite Mohr-Coulomb Medium

Example-3. Title. Description. Cylindrical Hole in an Infinite Mohr-Coulomb Medium Example-3 Title Cylindrical Hole in an Infinite Mohr-Coulomb Medium Description The problem concerns the determination of stresses and displacements for the case of a cylindrical hole in an infinite elasto-plastic

More information

1 DYNAMIC ANALYSIS DYNAMIC ANALYSIS Overview

1 DYNAMIC ANALYSIS DYNAMIC ANALYSIS Overview DYNAMIC ANALYSIS 1-1 1 DYNAMIC ANALYSIS 1.1 Overview The dynamic analysis option permits two-dimensional, plane-strain, plane-stress or axisymmetric, fully dynamic analysis with FLAC. The calculation is

More information

Lateral Earth Pressure

Lateral Earth Pressure 1 of 11 6/2/2012 4:28 AM Lateral Earth Pressure The magnitude of lateral earth pressure depends on: 1. Shear strength characteristics of soil 2. Lateral strain condition 3. Pore water pressure 4. State

More information

Static Pile Head Impedance using 3D Nonlinear FEM Analysis

Static Pile Head Impedance using 3D Nonlinear FEM Analysis Static Pile Head Impedance using 3D Nonlinear FEM Analysis Ichiro NAGASHIMA Technology Center, Taisei Corporation, 344-1 Nasecho, Totsuka-ku, Yokohama 245-51, Japan, ichiro.nagashima@sakura.taisei.co.jp

More information

Prob. 1 SDOF Structure subjected to Ground Shaking

Prob. 1 SDOF Structure subjected to Ground Shaking Prob. 1 SDOF Structure subjected to Ground Shaking What is the maximum relative displacement and the amplitude of the total displacement of a SDOF structure subjected to ground shaking? magnitude of ground

More information

DYNAMIC RESPONSE APPROACH AND METHODOLOGY

DYNAMIC RESPONSE APPROACH AND METHODOLOGY DYNAMIC RESPONSE APPROACH AND METHODOLOGY Traditional seismic stability procedures vs coupled effective-stress approach. Traditional seismic stability procedures: Empirical and laboratory corrections and

More information

USER S MANUAL. 1D Seismic Site Response Analysis Example. University of California: San Diego.

USER S MANUAL. 1D Seismic Site Response Analysis Example.  University of California: San Diego. USER S MANUAL 1D Seismic Site Response Analysis Example http://www.soilquake.net/ucsdsoilmodels/ University of California: San Diego August 2, 2017 Table of Contents USER'S MANUAL TABLE OF CONTENTS Page

More information

Lecture 9: Harmonic Loads (Con t)

Lecture 9: Harmonic Loads (Con t) Lecture 9: Harmonic Loads (Con t) Reading materials: Sections 3.4, 3.5, 3.6 and 3.7 1. Resonance The dynamic load magnification factor (DLF) The peak dynamic magnification occurs near r=1 for small damping

More information

Dynamic Soil Pressures on Embedded Retaining Walls: Predictive Capacity Under Varying Loading Frequencies

Dynamic Soil Pressures on Embedded Retaining Walls: Predictive Capacity Under Varying Loading Frequencies 6 th International Conference on Earthquake Geotechnical Engineering 1-4 November 2015 Christchurch, New Zealand Dynamic Soil Pressures on Embedded Retaining Walls: Predictive Capacity Under Varying Loading

More information

University of California at Berkeley Structural Engineering Mechanics & Materials Department of Civil & Environmental Engineering Spring 2012 Student name : Doctoral Preliminary Examination in Dynamics

More information

Example Application 12. Embankment Loading on a Cam-Clay Foundation

Example Application 12. Embankment Loading on a Cam-Clay Foundation Example Application 12 Embankment Loading on a Cam-Clay Foundation 1 Foundation Soil Properties 2 Modeling Procedure Step 1 Create the foundation model grid, set boundary conditions, assign material model

More information

Model tests and FE-modelling of dynamic soil-structure interaction

Model tests and FE-modelling of dynamic soil-structure interaction Shock and Vibration 19 (2012) 1061 1069 1061 DOI 10.3233/SAV-2012-0712 IOS Press Model tests and FE-modelling of dynamic soil-structure interaction N. Kodama a, * and K. Komiya b a Waseda Institute for

More information

Appendix G: UDEC Code. ;UDEC V6 Code to generate 15m tall by 10 m wide pillar with steel platen.

Appendix G: UDEC Code. ;UDEC V6 Code to generate 15m tall by 10 m wide pillar with steel platen. Appendix G: UDEC Code UDEC V6 Code to generate 15m tall by 10 m wide pillar with steel platen. DFN realization is adjusted by changing random seed in set random new set random 1003 round 0.3e-2 set edge

More information

Reciprocal of the initial shear stiffness of the interface K si under initial loading; reciprocal of the initial tangent modulus E i of the soil

Reciprocal of the initial shear stiffness of the interface K si under initial loading; reciprocal of the initial tangent modulus E i of the soil Appendix F Notation a b B C c C k C N C s C u C wt C θ D r D 1 D 2 D 10 D 30 Reciprocal of the initial shear stiffness of the interface K si under initial loading; reciprocal of the initial tangent modulus

More information

Dynamic behavior of turbine foundation considering full interaction among facility, structure and soil

Dynamic behavior of turbine foundation considering full interaction among facility, structure and soil Dynamic behavior of turbine foundation considering full interaction among facility, structure and soil Fang Ming Scholl of Civil Engineering, Harbin Institute of Technology, China Wang Tao Institute of

More information

The... of a particle is defined as its change in position in some time interval.

The... of a particle is defined as its change in position in some time interval. Distance is the. of a path followed by a particle. Distance is a quantity. The... of a particle is defined as its change in position in some time interval. Displacement is a.. quantity. The... of a particle

More information

INFLUENCE OF SOIL NONLINEARITY AND LIQUEFACTION ON DYNAMIC RESPONSE OF PILE GROUPS

INFLUENCE OF SOIL NONLINEARITY AND LIQUEFACTION ON DYNAMIC RESPONSE OF PILE GROUPS INFLUENCE OF SOIL NONLINEARITY AND LIQUEFACTION ON DYNAMIC RESPONSE OF PILE GROUPS Rajib Sarkar 1 and B.K. Maheshwari 2 1 Research Scholar, Dept. of Earthquake Engineering, IIT Roorkee, India, e-mail:

More information

Role of hysteretic damping in the earthquake response of ground

Role of hysteretic damping in the earthquake response of ground Earthquake Resistant Engineering Structures VIII 123 Role of hysteretic damping in the earthquake response of ground N. Yoshida Tohoku Gakuin University, Japan Abstract Parametric studies are carried out

More information

CHAPTER 6: ASSESSMENT OF A COMPREHENSIVE METHOD FOR PREDICTING PERFORMANCE

CHAPTER 6: ASSESSMENT OF A COMPREHENSIVE METHOD FOR PREDICTING PERFORMANCE CHAPTER 6: ASSESSMENT OF A COMPREHENSIVE METHOD FOR PREDICTING PERFORMANCE 6.1 Overview The analytical results presented in Chapter 5 demonstrate the difficulty of predicting the performance of an improved

More information

Computational Simulation of Dynamic Response of Vehicle Tatra T815 and the Ground

Computational Simulation of Dynamic Response of Vehicle Tatra T815 and the Ground IOP Conference Series: Earth and Environmental Science PAPER OPEN ACCESS Computational Simulation of Dynamic Response of Vehicle Tatra T815 and the Ground To cite this article: Jozef Vlek and Veronika

More information

Analysis of Planar Truss

Analysis of Planar Truss Analysis of Planar Truss Although the APES computer program is not a specific matrix structural code, it can none the less be used to analyze simple structures. In this example, the following statically

More information

GEOSYNTHETICS ENGINEERING: IN THEORY AND PRACTICE

GEOSYNTHETICS ENGINEERING: IN THEORY AND PRACTICE GEOSYNTHETICS ENGINEERING: IN THEORY AND PRACTICE Prof. J. N. Mandal Department of Civil Engineering, IIT Bombay, Powai, Mumbai 400076, India. Tel.022-25767328 email: cejnm@civil.iitb.ac.in Module-13 LECTURE-

More information

4 Cylindrical Hole in an Infinite Hoek-Brown Medium

4 Cylindrical Hole in an Infinite Hoek-Brown Medium Cylindrical Hole in an Infinite Hoek-Brown Medium 4-1 4 Cylindrical Hole in an Infinite Hoek-Brown Medium 4.1 Problem Statement Stresses and displacements are calculated for the case of a cylindrical hole

More information

QUAKE/W ProShake Comparison

QUAKE/W ProShake Comparison 1 Introduction QUAKE/W Comparison is a commercially available software product for doing one-dimensional ground response analyses. It was developed and is being maintained under the guidance of Professor

More information

Chapter 13. Simple Harmonic Motion

Chapter 13. Simple Harmonic Motion Chapter 13 Simple Harmonic Motion Hooke s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring A large k indicates a stiff spring and a small

More information

Using the Timoshenko Beam Bond Model: Example Problem

Using the Timoshenko Beam Bond Model: Example Problem Using the Timoshenko Beam Bond Model: Example Problem Authors: Nick J. BROWN John P. MORRISSEY Jin Y. OOI School of Engineering, University of Edinburgh Jian-Fei CHEN School of Planning, Architecture and

More information

4.4 1) 단순지지된깊은보 선형동적해석검증예제 ANALYSIS REFERENCE. REFERENCE NAFEMS 1 Beam elements, solid elements

4.4 1) 단순지지된깊은보 선형동적해석검증예제 ANALYSIS REFERENCE. REFERENCE NAFEMS 1 Beam elements, solid elements 그림 5.4.3 가진방향에따른응답변화예시 Reaction Sum. Total Strain Energy 0 30 60 90 120 150 180 Excitation ngle 4.4 선형동적해석검증예제 1) 단순지지된깊은보 REFERENCE NFEMS 1 ELEMENTS Beam elements, solid elements MODEL FILENME LinearDynamic01.mpb

More information

Soil Dynamics Prof. Deepankar Choudhury Department of Civil Engineering Indian Institute of Technology, Bombay

Soil Dynamics Prof. Deepankar Choudhury Department of Civil Engineering Indian Institute of Technology, Bombay Soil Dynamics Prof. Deepankar Choudhury Department of Civil Engineering Indian Institute of Technology, Bombay Module - 5 Machine Foundations Lecture - 31 EHS Theory, Vibrational Control Let us start our

More information

202 Index. failure, 26 field equation, 122 force, 1

202 Index. failure, 26 field equation, 122 force, 1 Index acceleration, 12, 161 admissible function, 155 admissible stress, 32 Airy's stress function, 122, 124 d'alembert's principle, 165, 167, 177 amplitude, 171 analogy, 76 anisotropic material, 20 aperiodic

More information

Protection of Pipelines and Buried Structures Using EPS Geofoam. Campus Dr., Salt Lake City, UT 84112;

Protection of Pipelines and Buried Structures Using EPS Geofoam. Campus Dr., Salt Lake City, UT 84112; Protection of Pipelines and Buried Structures Using EPS Geofoam Steven F. Bartlett 1, M. ASCE, P.E., Bret N. Lingwall 2 1, Dept. of Civil and Environmental Engineering, University of Utah, 110 Central

More information

Ch 4a Stress, Strain and Shearing

Ch 4a Stress, Strain and Shearing Ch. 4a - Stress, Strain, Shearing Page 1 Ch 4a Stress, Strain and Shearing Reading Assignment Ch. 4a Lecture Notes Sections 4.1-4.3 (Salgado) Other Materials Handout 4 Homework Assignment 3 Problems 4-13,

More information

Engineering Science OUTCOME 2 - TUTORIAL 3 FREE VIBRATIONS

Engineering Science OUTCOME 2 - TUTORIAL 3 FREE VIBRATIONS Unit 2: Unit code: QCF Level: 4 Credit value: 5 Engineering Science L/60/404 OUTCOME 2 - TUTORIAL 3 FREE VIBRATIONS UNIT CONTENT OUTCOME 2 Be able to determine the behavioural characteristics of elements

More information

Numerical Modeling of Interface Between Soil and Pile to Account for Loss of Contact during Seismic Excitation

Numerical Modeling of Interface Between Soil and Pile to Account for Loss of Contact during Seismic Excitation Numerical Modeling of Interface Between Soil and Pile to Account for Loss of Contact during Seismic Excitation P. Sushma Ph D Scholar, Earthquake Engineering Research Center, IIIT Hyderabad, Gachbowli,

More information

16 Rainfall on a Slope

16 Rainfall on a Slope Rainfall on a Slope 16-1 16 Rainfall on a Slope 16.1 Problem Statement In this example, the stability of a generic slope is analyzed for two successive rainfall events of increasing intensity and decreasing

More information

1D Analysis - Simplified Methods

1D Analysis - Simplified Methods 1D Equivalent Linear Method Page 1 1D Analysis - Simplified Methods Monday, February 13, 2017 2:32 PM Reading Assignment Lecture Notes Pp. 255-275 Kramer (EQL method) p. 562 Kramer (Trigonometric Notation

More information

Dr.Vinod Hosur, Professor, Civil Engg.Dept., Gogte Institute of Technology, Belgaum

Dr.Vinod Hosur, Professor, Civil Engg.Dept., Gogte Institute of Technology, Belgaum STRUCTURAL DYNAMICS Dr.Vinod Hosur, Professor, Civil Engg.Dept., Gogte Institute of Technology, Belgaum Overview of Structural Dynamics Structure Members, joints, strength, stiffness, ductility Structure

More information

TABLE OF CONTENTS SECTION TITLE PAGE 2 PRINCIPLES OF SEISMIC ISOLATION OF BRIDGES 3

TABLE OF CONTENTS SECTION TITLE PAGE 2 PRINCIPLES OF SEISMIC ISOLATION OF BRIDGES 3 TABLE OF CONTENTS SECTION TITLE PAGE 1 INTRODUCTION 1 2 PRINCIPLES OF SEISMIC ISOLATION OF BRIDGES 3 3 ANALYSIS METHODS OF SEISMICALLY ISOLATED BRIDGES 5 3.1 Introduction 5 3.2 Loadings for the Analysis

More information

Elasticity: Term Paper. Danielle Harper. University of Central Florida

Elasticity: Term Paper. Danielle Harper. University of Central Florida Elasticity: Term Paper Danielle Harper University of Central Florida I. Abstract This research was conducted in order to experimentally test certain components of the theory of elasticity. The theory was

More information

Preliminary Examination in Dynamics

Preliminary Examination in Dynamics Fall Semester 2017 Problem 1 The simple structure shown below weighs 1,000 kips and has a period of 1.25 sec. It has no viscous damping. It is subjected to the impulsive load shown in the figure. If the

More information

Numerical simulation of inclined piles in liquefiable soils

Numerical simulation of inclined piles in liquefiable soils Proc. 20 th NZGS Geotechnical Symposium. Eds. GJ Alexander & CY Chin, Napier Y Wang & R P Orense Department of Civil and Environmental Engineering, University of Auckland, NZ. ywan833@aucklanduni.ac.nz

More information

Application of pseudo-symmetric technique in dynamic analysis of concrete gravity dams

Application of pseudo-symmetric technique in dynamic analysis of concrete gravity dams Application of pseudo-symmetric technique in dynamic analysis of concrete gravity dams V. Lotfi Department of Civil and Environmental Engineering, Amirkabir University, Iran Abstract A new approach is

More information

8 Lined Circular Tunnel in an Elastic Medium with Anisotropic Stresses

8 Lined Circular Tunnel in an Elastic Medium with Anisotropic Stresses Lined Circular Tunnel in an Elastic Medium with Anisotropic Stresses 8-1 8 Lined Circular Tunnel in an Elastic Medium with Anisotropic Stresses 8.1 Problem Statement This problem concerns the analysis

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

Behavior of Concrete Dam under Seismic Load

Behavior of Concrete Dam under Seismic Load Behavior of Concrete Dam under Seismic Load A. Hebbouche Ecole Nationale Supérieure d Hydraulique, Blida-Algérie Departement of civil engineering, Saad dahlab university, Blida, Algeria M. Bensaibi Departement

More information

Bending Load & Calibration Module

Bending Load & Calibration Module Bending Load & Calibration Module Objectives After completing this module, students shall be able to: 1) Conduct laboratory work to validate beam bending stress equations. 2) Develop an understanding of

More information

Effect of Dynamic Interaction between Train Vehicle and Structure on Seismic Response of Structure

Effect of Dynamic Interaction between Train Vehicle and Structure on Seismic Response of Structure Effect of Dynamic Interaction between Train Vehicle and Structure on Seismic Response of Structure Munemasa TOKUNAGA & Masamichi SOGABE Railway Technical Research Institute, Japan SUMMARY: The conventional

More information

Foundation Engineering Dr. Priti Maheshwari Department Of Civil Engineering Indian Institute Of Technology, Roorkee

Foundation Engineering Dr. Priti Maheshwari Department Of Civil Engineering Indian Institute Of Technology, Roorkee Foundation Engineering Dr. Priti Maheshwari Department Of Civil Engineering Indian Institute Of Technology, Roorkee Module - 02 Lecture - 15 Machine Foundations - 3 Hello viewers, In the last class we

More information

6. NON-LINEAR PSEUDO-STATIC ANALYSIS OF ADOBE WALLS

6. NON-LINEAR PSEUDO-STATIC ANALYSIS OF ADOBE WALLS 6. NON-LINEAR PSEUDO-STATIC ANALYSIS OF ADOBE WALLS Blondet et al. [25] carried out a cyclic test on an adobe wall to reproduce its seismic response and damage pattern under in-plane loads. The displacement

More information

Numerical model comparison on deformation behavior of a TSF embankment subjected to earthquake loading

Numerical model comparison on deformation behavior of a TSF embankment subjected to earthquake loading Numerical model comparison on deformation behavior of a TSF embankment subjected to earthquake loading Jorge Castillo, Yong-Beom Lee Ausenco, USA Aurelian C. Trandafir Fugro GeoConsulting Inc., USA ABSTRACT

More information

1.8 Unconfined Compression Test

1.8 Unconfined Compression Test 1-49 1.8 Unconfined Compression Test - It gives a quick and simple measurement of the undrained strength of cohesive, undisturbed soil specimens. 1) Testing method i) Trimming a sample. Length-diameter

More information

1D Ground Response Analysis

1D Ground Response Analysis Lecture 8 - Ground Response Analyses Page 1 1D Ground Response Analysis 1. 2. 3. Dynamic behavior of soils is quite complex and requires models which characterize the important aspects of cyclic behavior,

More information

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

The effect of stope inclination and wall rock roughness on backfill free face stability The effect of stope inclination and wall rock roughness on backfill free face stability Dirige, A. P. E., McNearny, R. L., and Thompson, D. S. Montana Tech of the University of Montana, Butte, Montana,

More information

Chapter 14: Periodic motion

Chapter 14: Periodic motion Chapter 14: Periodic motion Describing oscillations Simple harmonic motion Energy of simple harmonic motion Applications of simple harmonic motion Simple pendulum & physical pendulum Damped oscillations

More information

Influences of material dilatancy and pore water pressure on stability factor of shallow tunnels

Influences of material dilatancy and pore water pressure on stability factor of shallow tunnels Influences of material dilatancy and pore water pressure on stability factor of shallow tunnels YANG Xiao-li( ), HUANG Fu( ) School of Civil and Architectural Engineering, Central South University, Changsha

More information