Dr John J M Powell Geolabs Ltd

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Transcription:

When or should advanced laboratory testing be routine Dr John J M Powell Geolabs Ltd 7/11/2012 - Doha

Routine tests Atterbergs Particle size, density, specific gravity Compaction, CBR Shear box Triaxial UU CU Permeability IL oedometers, Rowe cells Ring shear

Routine tests The profession often have trouble even getting these repeatable and of a consistent quality

Cone Penetration (mm) Proficiency / Interlaboratory Comparison Testing Scheme 12 14 16 18 20 22 24 26 40 45 50 55 60 65 70 Moisture Conent (%) LAB 1 LAB 5 LAB 6 LAB 7 LAB 8 LAB 10 LAB 13 LAB 15 LAB 16 LAB 17 LAB 21 LAB 23 LAB 24 LAB 27 LAB 30 LAB 32 LAB 34 LAB 35 LAB 36

Proficiency / Interlaboratory Comparison Testing Scheme

Proficiency / Interlaboratory Comparison Testing Scheme

Proficiency / Interlaboratory Comparison Testing Scheme

Advanced Tests Advanced triaxial, (a significant enhancement on the standard effective stress capability); including features such as local axial and radial strain, mid height pwp, piezobenders and anisotropic stress control (CAU) Cyclic triaxial Cyclic and static simple shear Resonant column Don t forget the CRS oedometer And more

But first So you want to get reliable parameters for your design using laboratory testing! So you need samples, but not just any old samples, they need to be representative in terms of structure and composition Sample Quality!

Eurocodes (love them hate them) Recognises the need for sample quality

Quality and QA Quality in sampling Quality in transport and storage Quality in preparation and testing Quality in reporting Quality throughout!! All rely on Quality in equipment and personnel!!!

Samples

Varying levels of disturbance!

Tube sampling Sources of disturbance

Stages in sampling and preparing soil specimen for laboratory test

Sources of tube sampling disturbance Open drive and piston

Indent fractur Sources of tube sampling disturbance Plugging Jarring Plugging Jarring Indentation fractures

Measured water content distributions across the diameter of tube samples of soft clay

Measured water content distributions across the diameter of tube samples of heavily overconsolidated plastic clay

Sampling effects in soft clays

Control vertical mopvement Rotation - Water or bentonite mud Canadian Sherbrooke block sampler Annular slot Borehole 400 mm in diameter Water or mud circulated at each cutting tool Cutting tool every 120 degr. No tube sampling strains!! Block sample being carved out

Block sampling with Sherbrooke sampler Block sample cleaned and wrapped in plastic cling film

Effect of structure of natural clays All natural clays have developed some structure Degree of structure can be assessed by comparing behaviour of an undisturbed sample to that of a remoulded clay (eg. in oedometer tests) Soil structure is a result of several processes including, but not limited to: secondary compression, thixotropy, cementation, cold welding between soil particles (ageing--) Effect of sample disturbance is to partly or fully break down the structure of the soil sample parameters measured by lab tests may not be representative for in situ conditions

Results of CRS tests Clearly block sample gives a more stiff behaviour showing less sample disturbance Better definition of preconsolidation stress, p c Lierstranda clay 12,3 m depth Semilogarithmic scale

Comparison of IL and CRS Consolidation Data 0 P c (b) Vertical Strain v (%) 10 20 CRS IL 24 hr. ' vo Boston Blue Clay - Newbury Depth = 7.3 m w = 53%, PI = 21, LI = 1.4 30 10 100 1000 Vertical Effective Stress ' v (kpa) Better definition of preconsolidation stress, p c, from CRS

UU triaxial compression tests on Laval and piston samples. Bothkennar Clay Strength and stiffness!!

Results from shearing phase of CAUC tests Similar failure envelopes? Lierstranda clay from 6.1 m depth Stress path diagram (Lunne et al, 2001)

Sample tube geometries

Unconfined compression tests on Ariake Clay (Tanaka and Tanaka, 1999) Compressive Stress (kpa) 40 30 20 10 Shelby tube ELE100 NGI54 54 Japanese standard Standard piston Piston Sherbrooke sampler Laval sampler 10m 0 0 2 4 6 8 10 12 14 Axial strain (%) What are YOU trying to test??

Disturbance during specimen preparation Bothkennar Clay

Sampling effects in stiff clays

( a - r)/2 Stiff Sandy Clays C = f(w) u Stiff clays: distinction on basis of unconsolidated undrained triaxial compression 0 ( a - r)/2 0 ( + )/2 a ( + )/2 a r Stiff Fissured plastic Clays C = f(p ) u 0 r ( a - r)/2 Stiff Medium plastic Clays C = f(w, p ) u 0 0 ( + )/2 a r

Conventional practice for sampling stiff plastic clays Shell and auger boring, dry hole, cased to cut off ground water entry Open drive tube sampling Unconsolidated undrained triaxial compression tests for stress-strain-strength Invariably large scatter in strength and stiffness parameters variously attributed to: fabric sample disturbance stress relief sample size

Depth below top of London Clay (m) Results of conventional site investigation in London Clay Undrained shear strength, C u (kpa) SPT N (blows/300) 0 100 200 300 400 500 600 0 20 40 60 80 0 0 5 5 10 10 15 15 20 20 25 25 30 30 35 35

Initial effective stresses in rotary cores and thin wall tube samples of London Clay Probably between rotary foam and pushed

Effects of sampling method in UU triaxial compression tests on Upper Mottled Clay, Lambeth Group

Evaluation of sample quality

Evaluation of sample quality Fabric inspection X- ray Comparison of tube sampling strains and yield strains Reconsolidation strains (esp in oed) Measurement of initial effective stress Comparison of in situ and laboratory measurements of shear wave velocity/dynamic shear modulus

How can we then reduce effects of sample disturbance? Use the best sampler possible for the project Careful sample handling and testing recompression technique may to some extent repair the sample Trimming of sample to smaller diameter may help in some cases but can also damage sample if not undertaken with great care (tubing vs hand trimming).

Sample disturbance effects Conclusions: Sample disturbance(sd) can be very significant! Effect of SD is to partly or completely destroy structure SD has significant effects on deformation and strength characteristics as measured in oedometer and triaxial tests e/e o is a consistent measure of SD for soft clays SD effects can best be minimized by carefull choice of drilling and sampling methods Sample handling and consolidation techniques may reduce SD effects In situ tests will also give essential input to choice of soil design parameters, but will not eliminate need for sampling and laboratory testing

So we have good quality sample!

Advanced Tests Advanced triaxial, (a significant enhancement on the standard effective stress capability); including features such as local axial and radial strain, mid height pwp, piezobenders and anisotropic stress control (CAU) Cyclic triaxial Cyclic and static simple shear Resonant column Don t forget the CRS oedometer And more

Advanced Tests Advanced triaxial, (a significant enhancement on the standard effective stress capability); including features such as local axial and radial strain, mid height pwp, piezobenders and anisotropic stress control (CAU) Cyclic triaxial Cyclic and static simple shear Resonant column Don t forget the CRS oedometer And more

Shearing Tests we often have conflicting requirements of our tests: Strength need large strains with minimum restraint while maintaining uniform stresses & strains in sample Stiffness need to apply and measure very small stress/strain changes triaxial apparatus is fairly unique in its ability to perform both functions

Triaxial Test Advantages a drainage can be controlled complete stress state is known ( a, r, and U) and can be controlled r r r a Disadvantages: axi-symmetric loading soil parameters depend on mode of loading

Shear stress, = ( a- r)/2 kpa Triaxial testing CAUC 50 40 30 20 10 0 0 4 8 12 16 20 Axial strain, a, % The most basic and useful geotechnical test

We now have Excellent equipment that allows us to, control: Axial stresses Radial stresses Closed loop measure: Accurate axial displacements Radial displacements Mid ht pore pressures Small strain stiffnesses in varying directions Volume changes

Mid-height pore pressure measurement Flush surface (Hight, 1982) use without lateral filter paper will lengthen tests considerably

Mid-height pore pressure measurement (Hight, 1982) Prebore hole and push in probe

Local Strain Measurement - Axial LVDTs (Cuccovillo & Coop, 1997) most accurate difficult to mount Inclinometers (Jardine et al., 1984) sensitive to rigid body rotation of sample need to take average of two readings on opposite sides of sample Hall Effect (Clayton & Kathrush., 1986) accurate relatively easy to mount cannot be used for r transducers generally only glued to membrane pins no longer used

Resolution 0.0003mm

Local Strain Measurement - Radial single LVDT version or Hall effect Submersible cable Right-angle connection LVDT-body Fixing screw LVDT-core Flexible wire Radial strain belt Mount double LVDT or Hall effect version - allows larger r -difficult to mount Sample -BUT SPACE (Klotz & Coop, 2002)

Resolution 0.0001 0.0002mm

Bender Elements shear plane wave travelling through an elastic isotropic or cross-anisotropic medium measure elastic shear stiffness, G 0 Output D Input v = D/t arr G 0 = rv 2 (r = mass density) Piezoelectric Bender Elements Kramer (1996) (Dyvik & Madhus, 1985)

Lateral benders

Lateral benders

Piezobender trace

Output First Arrival 10 8 6 from 0.000050 sec to 0.000333 sec Shv 4 2 0-2 -4-6 -8-10 -0.0005 0.0000 0.0005 0.0010 0.0015 0.0020 Time (seconds) 72

Control of triaxial tests: feedback loop triaxial transducer output (voltage) data logger (analogue-digital conversion) transducer output (digital) computer simple basic program a command r r change of stress or strain controller automated control of tests much less common than data-logging

Setting it all up not much space

Setting it all up not much space

Larger cells more space, large strains id 220mm (165)

Anisotropy of Elastic Stiffnesses: Cross-Anisotropic Soil behaviour defined by the following parameters: E v = vertical Young s modulus E H = horizontal Young s modulus VH = Poisson s ratio for influence of V on H HV = Poisson s ratio for influence of H on V HH = Poisson s ratio for influence of H1 on H2 or H2 on H1 G VH = shear modulus in vertical plane G HV = shear modulus in vertical plane G HH = shear modulus in horizontal plane 5 independent parameters

Strain (%) Strains during a stage 0.5 0.45 0.4 0.35 0.3 local axial external vol local vol 0.25 0.2 0.15 0.1 0.05 0-10 0 10 20 30 40 50 60 70 80 90 100 Change in mid-plane effective stress (kpa)

Isotropic Consolidation Stress Path

Anisotropic Consolidation Stress Path

2 nd Anisotropic Consolidation Stress Path

Shearing Stress Path

Shear stress t (kpa) Stress path of a test 150 100 finish 50 0-50 -100-150 this stage previous stages aniso3 aniso2 aniso1 start -200 0 50 100 150 200 250 300 350 400 450 Mean effective stress, s' (kpa)

Measurements allow for different orientations

Stiffness G Measurement of Stiffness Typical strain ranges Retaining walls Foundations Tunnels 0.0001 0.001 0.01 0.1 1 10 Shear strain dynamic methods s : % local gauges (Atkinson, 2000) conventional soil testing

G (MPa) q q calculation of tangent stiffnesses E tan = dq/d a critical state E tan = dq/d a E sec = q/ a a a 120 100 80 60 tangent secant - gradient over odd number of points - No. of points in regression depends on No. of number data points recorded (use a fixed strain interval) - plot stiffness against strain at central point 40 20 0 0.0001 0.0010 0.0100 natural London clay (Gasparre, 2005) shear strain (%) tangents always more scattered than secant at small strains (also have more meaning)

Gu (MPa) (Cuccovillo & Coop, 1997) Gu (MPa) Measurement of Stiffness Examples of Tangent Stiffnesses 120 3000 80 local LVDTs external LVDT 2500 2000 1500 local LVDTs external LVDT 40 1000 500 0 0.0001 0.0010 0.0100 0.1000 axial strain (%) reconstituted kaolin low G 0 0.0001 0.0010 0.0100 0.1000 1.0000 axial strain (%) natural Greensand very high G suction cap used & compliance correction made strains prior to shearing small

Local secant Young's modulus (MPa) Stiffness, local and external 700 600 500 400 300 200 100 0-4 -3-2 -1 0 1 2 log(local axial strain (%))

Local secant Young's modulus (MPa) Stiffness, local and external 700 600 500 400 300 200 100 0-4 -3-2 -1 0 1 2 log(local axial strain (%))

Anisotropy in London Clay Gasparre (2005)

Sample quality assessment based on shear wave velocity

Using the equipment for Poisson s ratio and small strain stiffness of rock

Where have we come in 25+yrs?? Is it new or just commercially viable?

Summary there is much that can go wrong in conducting and interpreting tests But it can be done we should conduct and interpret tests within a chosen and appropriate theoretical framework level of complexity of tests should be appropriate to theoretical framework and design method You need to know what you are specifying and what can be realistically achieved, commercial vs research You need to have confidence is those performing the tests

Value for money

I must say - thanks I wish to acknowledge the help from David Hight Tom Lunne Matthew Coop For some of the slides contained in this presentation

Conclusions! Rubbish in Rubbish out! Quality in Quality out (hopefully/possibly)

Conclusions! We now have a new level of testing available to us which I believe should be consider routine (advanced) testing for use when projects warrant it and samples are of the right quality. Particularly relevant for modelling and in serviceability situations

Available for consultancy

And finally Thank you for your attention Contact jpowell@geolabs.co.uk