SURFACE WAVE SURVEYS LIMITED

Slides:



Advertisements
Similar presentations
ANALYSIS OF THE LIGHT WEIGHT DEFLECTOMETER IN-SITU STRESS AND STRAIN
Advertisements

Patricia Capistrant & Troy Christensen. Introduction To Refraction -Seismic refraction surveying provides earth scientists and engineers with information.
P-wave S-wave Particles oscillate back and forth Wave travels down rod, not particles Particle motion parallel to direction of wave propagation Particles.
The Asymptotic Ray Theory
Chapter 1- General Properties of Waves Reflection Seismology Geol 4068
Development of an In-Situ Test for Direct Evaluation of the Liquefaction Resistance of Soils K. H. Stokoe, II, E. M. Rathje and B.R. Cox University of.
Upper mantle of the Bohemian Massif (Central Europe) studied by surface waves from Kurile Islands M8.1 and M8.3 earthquakes Petr Kolinsky Jiri Malek Institute.
Multichannel Analysis of Surface Waves (MASW)
SOFT SOIL (PROBLEMS & STABILISATION METHOD) Session 2 - 7
INTRODUCTION Session 1 – 2
Near-surface Imaging at Meteor Crater, Arizona Soumya Roy, Ph. D. Student Advisor: Dr. Robert R. Stewart AGL Annual Meeting University of Houston, 2 nd.
Physical processes within Earth’s interior Topics 1.Seismology and Earth structure 2.Plate kinematics and geodesy 3.Gravity 4.Heat flow 5.Geomagnetism.
GG450 April 22, 2008 Seismic Processing.
Consolidation Theory Examples.
Seismic Wave Propagation
Lab 2 Seismogram Interpretation
Characterization of Glacial Materials Using Seismic Refraction and Multichannel Analysis of Surface Waves Glenn Larsen Ohio Department of Natural Resources.
Seismic Refraction Method for Groundwater Exploration Dr. A K Rastogi Professor, Dept. of Civil Engineering I I T Bombay.
Seismic waves. When an earthquake occurs shockwaves of energy, called seismic waves, are released from the earthquake focus. They shake the Earth and.
A disturbance that propagates Examples Waves on the surface of water
Lecture-15 1 Lecture #15- Seismic Wave Overview. Lecture-15 2 Seismograms F Seismograms are records of Earth’s motion as a function of time.
Reflection Field Methods
CE 486 DEEP COMPACTION Name : Ali Hamood Al-teeb. ID :
Reflection Processing and Analysis Bryce Grimm Mayo Thompson Shallow Subsurface Investigation across many areas of the V-line and Truckee Canal Fallon,
Electromagnetic Wave Theory
Downhole seismic and S-Waves Jacques JENNY Geo 2X Genève.
Analyses of tunnel stability under dynamic loads Behdeen Oraee; Navid Hosseini; Kazem Oraee 1.
Chapter 1- General Properties of Waves Reflection Seismology Geol 4068 Elements of 3D Seismology, 2nd Edition by Christopher Liner.
VII. Earthquakes A.Introduction B.Source of seismic energy C.Propagation of seismic energy D.Recording earthquakes E.Magnitude scales.
GG450 March 20, 2008 Introduction to SEISMIC EXPLORATION.
Body Waves and Ray Theory
Evaluating paleoseismic ground motions using dynamic back analysis of structural failures in archaeological sites Ronnie Kamai (1), Yossef Hatzor (1),
GG 450 March 19, 2008 Stress and Strain Elastic Constants.
University of Missouri - Columbia
Earthquakes (Chapter 13). Lecture Outline What is an earthquake? Seismic waves Epicenter location Earthquake magnitude Tectonic setting Hazards.
GLY 521 Hydrogeophysics. Upland Recharge to a Valley Fill Aquifer.
Session 7 – 8 SETTLEMENT OF SHALLOW FOUNDATION
Earthquake Engineering GE / CEE - 479/679 Topic 13. Wave Propagation 2
Geology 5660/6660 Applied Geophysics Last time: Brief Intro to Seismology & began deriving the Seismic Wave Equation: Four types of seismic waves:  P.
Geophysics/Tectonics
Earthquakes Chapter 16 In Textbook. What Is An Earthquake? What Is An Earthquake? An earthquake is the vibration of Earth produced by the rapid release.
SASW – an in situ method for determining shear modulus
PEER 2G02 – Code Usage Exercise: OpenSees Zhaohui Yang UCSD 2/15/2005.
TOPIC 3: DESIGN AND ANALYSIS OF SHALLOW FOUNDATION WEEK 6
Application of the two-step method for the solution of the inverse gravity problem for the Kolárovo anomaly.
The main instrument used is called the sonde. A basic sonde consists of a source and two receivers one-foot apart. The sonde is lowered down the borehole.
GG450 April 1, 2008 Huygen’s Principle and Snell’s Law.
Feb 26, John Anderson: GE/CEE 479/679: Lecture 11 Earthquake Engineering GE / CEE - 479/679 Topic 11. Wave Propagation 1 John G. Anderson Professor.
Geophysics/Tectonics GLY 325. Elastic Waves, as waves in general, can be described spatially...
1 BROOKHAVEN SCIENCE ASSOCIATES NSLS – II CFAC Review Conventional Facilities Geotechnical Conditions Tom Joos Civil/Structural Engineer BNL Plant Engineering.
Seismology Part V: Surface Waves: Rayleigh John William Strutt (Lord Rayleigh)
The crust and the Earth’s interior
1 Wavefield Calibration Using Regional Network Data R. B. Herrmann Saint Louis University.
Earthquakes.
Tom Wilson, Department of Geology and Geography Environmental and Exploration Geophysics II tom.h.wilson Department of Geology.
Environmental and Exploration Geophysics II tom.h.wilson Department of Geology and Geography West Virginia University Morgantown, WV.
On the investigations of Resilient Modulus of Residual Tropical Gravel Lateritic Soils from Senegal (West Africa) for Road Design Purposes Introduction.
PILE FOUNDATIONS UNIT IV.
Does It Matter What Kind of Vibroseis Deconvolution is Used? Larry Mewhort* Husky Energy Mike Jones Schlumberger Sandor Bezdan Geo-X Systems.
Seismic waves Mathilde B. Sørensen and Jens Havskov.
September 18, 2002Ahmed Elgamal 1 Seismic Waves Ahmed Elgamal.
Microtremor method Saibi. Dec, 18, 2014.
Seismic Waves Large strain energy released during an earthquake
How the ground shakes? Dr. Syed Mohamed Ibrahim M.Tech., Ph.D., by
Measurement of Dynamic Properties of Viscoelastic Materials
Applied Geophysics Fall 2016 Umass Lowell
Hamiltonian formalism, seismic waves, and seismic barriers
Creating a Conference Poster
Seismic Waves and the Earth’s Interior Structure
Presentation transcript:

SURFACE WAVE SURVEYS LIMITED Non-intrusive measurement of ground stiffness Website: www.surfacewavesurveys.co.uk E-mail: info@surfacewavesurveys.co.uk

Idealised stiffness - strain behaviour exhibited by most soils The CSWS measures Gmax. Gop/Gmax is 0.5 to 0.8 for soils and near unity for sands and soft rocks. Stiffness values can be converted to Young’s Modulus (E) using Poisson’s ratio () E = 2(1+ )G

The different types of seismic wave Energy source Geophone detector Ground level Surface waves Shallow reflection Boundary between earth layers Refraction Deep reflection Body waves: reflections and refractions Two types: P-waves (Pressure waves) S-waves (Shear waves) Surface waves Two types: Love waves (A type of S-wave) Rayleigh waves (Neither P- nor S- waves)

Seismic wave particle motion P- Wave Direction of propagation Direction of movement S-Wave Direction of propagation Direction of movement (Or any other direction at right angles to the propagation direction) Rayleigh Wave Direction of propagation Direction of movement

The surface wave method Frequency controlled vibrator 2Hz natural frequency geophones Amplifier unit Controller unit

Site recording 1

Site recording 2

Site recording 3

CSWS principle of operation (1) A range of frequencies is selected and the vibrator, under computer control, automatically shakes the ground at each frequency throughout this range. For each frequency the surface waves are detected by the geophones which send signals representing the ground motion as a function of time back to the controller. This data is Fourier transformed to give the phase of the Rayleigh wave at each geophone position.

CSWS principle of operation (2) The gradient of the phase-distance relationship gives the wavelength of the Rayleigh wave. The wavelength and frequency of the Rayleigh wave give its velocity. Elastic theory is used to convert the Rayleigh wave velocity to the shear wave velocity and the shear wave velocity to the stiffness. The stiffness value is allocated to a depth which is 1/3 of the Rayleigh wave wavelength (/3 inversion).

Calculation of Rayleigh wave velocity d Frequency = f Distance between geophones = d Phase difference  = 2 - 1 =  By proportion  = d 360  Therefore  = 360.d  And Rayleigh wave velocity V = f     R 1 2 By knowing the frequency, f, and the change in phase with distance from the vibrator, d, we can determine the Rayleigh wave velocity, V . R

Calculation of stiffness From the theory of elasticity VS = Shear wave velocity VR = Rayleigh wave velocity P = f(Poisson’s ratio ) for = 0.25, P = 1.09 for = 0.50, P = 1.05 G = Shear modulus  = Bulk density VS = PVR G = VS2 = P2VR2

Chalk under shallow fill Depth (m) 1000 2000 3000 4000 5000 Fill -5 Dense chalk -10 -15 -20 -25 -30 Gmax (MPa)

Stiffness inversion due to buried alluvium 50 100 150 200 250 300 Fill Soft, grey, slightly sandy silty clay [Alluvium] Depth (m) Medium dense, sub-angular to sub-rounded sandy fine to medium flint gravel -5 -10 -15 Gmax (Mpa)

Sequence of clays Weathered, sandy clay Silty clay Depth (m) Clay marl Gmax (Mpa) 200 400 600 800 Weathered, sandy clay -5 Silty clay -10 -15 Clay marl -20 -25 -30 -35

By courtesy of Keller Ground Engineering Example of using CSWS to measure the degree of ground improvement resulting from the insertion of vibro stone columns 20 40 60 80 100 120 140 160 180 -2.00 -4.00 Depth (m) -6.00 -8.00 -10.00 -12.00 -14.00 Gmax (Mpa) Column diameter 500mm Depth 6m Triangular grid spacing 1500mm By courtesy of Keller Ground Engineering

Dynamic compaction with 1.75m stone pillars From Moxhay et al. (2001)

Vibro stone columns with surface tamping – deep ash fill From Moxhay et al. (2008)

Stiffness increase after a temporary loss during ground treatment

Stiffness increase with time elapsed after ground treatment

Settlement prediction from CSW data Required information: CSW stiffness/depth profile, foundation shape, size, depth below ground and load. The sub-surface is divided into layers and average Gmax values are found for each. The initial value of Young’s Modulus E for each layer is taken to be 2.5Gmax (average). The vertical stress at the centre of each layer is found using the appropriate Boussinesq formula. Initial values of strain for each layer are found from the vertical stress and initial E values. These strains will be too high to relate to the CSW Gmax values. The E values are therefore revised using factors from a standard curve of stiffness against strain (see Moxhay at al. (2008) Appendix 2). The calculations are repeated to produce new strains. After repeating several times the new E values converge to the previous ones. The settlement in each layer is calculated by multiplying the final strain by the layer thickness. Addition of the settlements in each layer gives the total settlement.

Vibro stone column site - example data for settlement calculation From Moxhay et al. (2008)

Example settlement calculation Z E Strain Settlement 0.5 27.5889 0.144048 1.440479 1.5 26.85222 0.138098 1.380982 2.5 18.53303 0.168462 1.684624 3.5 22.26731 0.111213 1.112125 4.5 29.84521 0.06478 0.647796   6.266007 Originally calculated settlement: 60mm. Settlements for whole site calculated from CSW data varied between 6mm and 15mm, average: 11mm. Observed settlement after four years: 10mm.

Example of the effect on CSWS results of a very hard raft of material near the surface

Advanced processing of CSW data using WinSASW2 software with PreCSW An experimental dispersion curve for input to WinSASW2 is prepared from the field data using PreCSW. A polynomial, called the representative dispersion curve, is fitted to it. This essentially produces a smoothed version of the field data. An initial estimate of the earth model in terms of layer thicknesses is made. The dispersion curve that would be produced by this model is generated and superimposed on the smoothed experimental one. Adjustments to the model are made to produce a reasonable fit. The best-fit model is used as the starting point for the main matrix inversion. Initially, layer thicknesses are held constant and the optimum velocities found by iteration. Thickness and velocity are then iterated together to produce the final result.

Example WinSASW2 output - a steady increase of stiffness with depth By courtesy of ESG Pelorus Surveys

Example WinSASW2 output – a ‘hard-layer sandwich’

Example WinSASW2 output – a stiffness inversion By courtesy of ESG Pelorus Surveys

Example WinSASW2 quality control (1) Criteria for a satisfactory result: The model is plausible. The dispersion curve for the model and the representative dispersion curve are a good match. The resolution of the shear wave velocity does not fall below 0.1.

Example WinSASW2 quality control (2) Index for the different dispersion curves: Grey - Experimental Blue - Representative Red - Final model By courtesy of ESG Pelorus Surveys

Advantages of the CSWS Non – invasive. Representative. Independent of soil type. Quick. Portable. Low – cost. Provides a direct route to settlement prediction.

Future development Processing software enhancement. The Unbiased Short Array (USA) Beamforming Technique, currently under development by Professor Joh in South Korea, will improve the results produced by WinSASW2.