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2nd McClelland Lecture
Analytical contributions to offshore geotechnical engineering
Mark Randolph
Centre for Offshore Foundation Systems (COFS)The University of Western Australia
18th ICSMGE, Paris Tuesday 3rd September 2013
The University of Western Australia
Bramlette McClelland (1921-2010)
• A giant of a man – pioneer of offshore foundation engineering
• Founder and President of McClelland Engineers
– Headquartered in Houston
– 14 offices around the world
• Awards included– 9th Terzaghi Lecturer (1972)
– OTC Distinguished Achievement Award (1986)
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 2
The University of Western Australia
What passes for “analytical” ?
• True analytical solution (algebraic expression)
• Computable analytical formulation (design chart)
• Synthesis of numerical parametric study
– Appropriate non-dimensional parameter groups
– Algebraic or chart outcome
“When I am working on a problem, I never think about beauty but when I have finished, if the solution is not beautiful, I know it is wrong.”Buckminster Fuller
Idea
lisat
ion
Realism
?
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 3
The University of Western Australia
Overview
• Piled foundations– Consolidation after driving
– Axial stiffness and cyclic loading
• Shallow foundations– Rectangular foundations for subsea systems
• Full-flow penetrometers– Resistance factors
– Degree of consolidation during penetration
• Subsea pipelines– Embedment and axial resistance of deep water pipelines
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 4
The University of Western Australia
Piled foundations - consolidation
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 5
• Radial consolidation solution
– Refined through strain path method
• Non-dimensional time: T = cvt/Deq2
– cv as for piezocone dissipation
(horizontal flow; soil stiffness partly swelling)
– Deq reflecting outward flow of soil
Soil flow:Piles: 0:100 D/ ~ 40Suction caissons ~ 50:50 D/ > 300
t
u
r 'r(t)
D
The University of Western Australia
Development of axial pile resistance
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 6
T10 ~ T50/20 : t10 ~ 2 to 5 hours
T50 ~ 0.6 : t50 ~ 2 to 5 days
T90 ~ 20T50 : t90 ~ 1 to 3 months
Consolidation index
75.050T/T1
11~CI
The University of Western Australia
Consolidation around suction caissons
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 7
T10 ~ T50/20 : t10 ~ 2 to 5 hours
T50 ~ 0.6 : t50 ~ 2 to 5 days
T90 ~ 20T50 : t90 ~ 1 to 3 months
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0.1 1 10 100
Rel
ativ
e in
crea
se in
shaf
t res
ista
nce
Time (days) - scaled for Deq = 0.3 m
Radial consolidation solution(cv = 10 m2/yr; Deq = 0.3 m)
Data from suction anchors(Colliat & Colliard 2011)
Colliat & Colliard (2011):
Diameters: 3.8 m to 8 m
Deq ~ 0.28 to 0.45 m (extremely thin-walled)
Consolidation index
75.050T/T1
11~CI
The University of Western Australia
Consolidation - commentary
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 8
• Radial consolidation solution
– Adequate fit to sparse data
– Analytical framework: piles to caissons and different soil types
– Consolidation coefficient: relevant cv difficult to estimate
field data (piezocone dissipation) a vital aid
Do we need the black magic of thixotropy for this problem?
The University of Western Australia
Axial stiffness of piles
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 9
Pt
wt
Pb
wb
Kb
ka ~ 1.5G D
w
LtanhKS
LtanhSKS
wP
Kb
b
t
taxial
S (for L > 2)
app
p
a kEALL
EAS and L
EAk
L
Pile shaftcompliance
Mobilisation of shaft friction initiated near pile head:
- Consequences for progressive failure and cyclic stability
a
p
shaft
slip
kEA
L1
L1~
QP
L
(EA)p
The University of Western Australia
Cyclic stability diagram for axial loading of piles
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 10
0
0.2
0.4
0.6
0.8
1
0 0.2 0.4 0.6 0.8 1
Nor
mal
ised
cyc
lic lo
ad, Q
cycl
ic/Q
shaf
t
Mean load, Qmean/Qshaft
Increasing cycles (N) to failure
Metastable
Unstable N < 10
Stable N > 10,000
N ~ 300
Common form of ‘global’ stability diagram:
Diagram applies at element level -not globally
– Cyclic degradation progresses down
pile from soil surface
– Pile shaft compliance important
– Model tests (low compliance) not
directly applicable for design of more
compliant piles used offshore
The University of Western Australia
Shallow mat foundations
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 11
• Widespread use for subsea systems and pipeline terminations
• Generally rectangular: 50 to 200 m2 in plan area
• Complex 6 degree of freedom loading
Pipeline end termination (PLET) Production sled during lay(photos courtesy Subsea 7)
The University of Western Australia
Design considerations for small mat foundations
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 12
• Industry design guidelines limited
– Strip or circular geometries only
– Oriented towards bearing capacity, with allowance for H, M
• Operational loads for subsea foundation systems
– Vertical load (V) constant; low proportion of bearing capacity
– Thermally induced variations of horizontal (Hx, Hy), moment (Mx,
My) and torsion (T) from eccentric pipeline and spool connections
– Critical failure mode: combined sliding and torsion
Holy grail: analytical failure envelope for general 3-D loading
The University of Western Australia
Numerical analysis: parameterised solutions
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 13
y
V
Hx
Hy
Mx
My
LRP
B
T
z
xL
mudline
z
susum
su0d
k
Simplified soilprofile
• Identify non-dimensional groups:
B/L, d/B, kB/su0, Hx/Hy, My/Mx, V/Asu0, Hres/Asu0 etc
• Evaluate ‘uniaxial’ ultimate capacities for each loading component
• Adjust ultimate horizontal and moment capacities for V/Vult, T/Tult
• ‘Collapse’ 6-dimensional failure envelope into 2 dimensions!
The University of Western Australia
Design approach for small mat foundations
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 14
Parameter Value Units Design loads Value Units RatiosWidth, B 8 m Vert. load, V 1200 kN 0.17Length, L 16 m Load, Hx 200 kN 0.21Skirt, d 0.6 m Load, Hy 300 kN 0.34Strength, sum 5 kPa Moment, Mx 1500 kNm 0.07su gradient, k 2 kPa/m Moment, My -2400 kNm 0.30Skirt friction 0 Torsion, T 2100 kNm 0.45
Mobilisation
Failure envelopes
1hhh1m 22qd
fd M
HdMm
fHHh
0100020003000400050006000700080009000
10000
-1000-750 -500 -250 0 250 500 750 1000
Res
ulta
nt m
omen
t, M
(kN
m)
Resultant horizontal load, H (kN)
V = 1200 kN
Failure envelopesUnfactored
su
Zero torsion
T = 2100 kNm
Design point
The University of Western Australia
0100020003000400050006000700080009000
10000
-1000-750 -500 -250 0 250 500 750 1000
Res
ulta
nt m
omen
t, M
(kN
m)
Resultant horizontal load, H (kN)
Design approach for small mat foundations
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 15
Parameter Value Units Design loads Value Units RatiosWidth, B 8 m Vert. load, V 1200 kN 0.17Length, L 16 m Load, Hx 200 kN 0.21Skirt, d 0.6 m Load, Hy 300 kN 0.34Strength, sum 5 kPa Moment, Mx 1500 kNm 0.07su gradient, k 2 kPa/m Moment, My -2400 kNm 0.30Skirt friction 0 Torsion, T 2100 kNm 0.45
Mobilisation
0.270.330.540.110.480.72
Factored su(by 0.63)
Failure envelopes
1hhh1m 22qd
fd M
HdMm
fHHh
V = 1200 kN
Unfactored su
Zerotorsion
T = 2100 kNm
Factored su
Design point
The University of Western Australia
Full flow penetrometers
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 16
• Penetrometer shapes amenable to analysis– Resistance independent of soil stiffness or in situ stresses
• Sufficient projected area ratio for minimal correction for overburden stress
– Shaft area < 15 % of projected area
• Soil sensitivity measured directly: cyclic testing
• Reduced reliance on ad hoc correlations for shear strength from penetration resistance
– Variations in resistance factors arise from differences in sensitivity (and brittleness), and strain rate dependence
Motivations for introduction, targeting soft soils
T-bar: 100 cm2
ball: 30 to 50 cm2
Pore water pressure filter
Push rod and anti-friction sleeve
Spherical ball
Pore water pressure filter
Push rod and anti-friction sleeve
Spherical ball
The University of Western Australia
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
0.80
0.90
1.00
0 1 2 3 4 5 6 7 8 9 10
Deg
rada
tion
Fact
or
Cycle Number
2.30
2.40
2.50
2.60
2.70
2.80
2.90
3.00
-0.20 -0.10 0.00 0.10 0.20 0.30
Dep
th (m
)
Net ball resistance qball,net (MPa)
Cyclic degradation of soil strength
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 17
Penetro-meter
0
0.5
1
0.25
0.75
penetration
extraction
Cycle No.
0
Nk or q
Cycle number0.25 0.75
Undisturbed
Fullyremoulded
In
Out
The University of Western Australia
Theoretical resistance factors – rate dependence & softening
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 18
Typical parameters:NTbar ~ 10 to 13Nball ~ 12 to 175
10
15
20
25
0 0.05 0.1 0.15 0.2 0.25Rate parameter
NTbar
95 = 5095 = 2595 = 15
Parameters = rem = 0.2Tbar = 3.7
95 = 10
No strain softeninggradient = 4.8
5
10
15
20
25
0 0.05 0.1 0.15 0.2 0.25Rate parameter
Nball 95 = 5095 = 2595 = 15
Parameters = rem = 0.2ball = 3.3
95 = 10
No strain softeninggradient = 4.8
Strain to 95 % remoulded
FE results
Gradient of 4.8 implies 'operative' shear strain
rate of 20 %/s or approximately 0.5v/D
u
netk s
qN T-bar
Ball
The University of Western Australia
Consolidation around penetrometers
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 19
• In situ assessment of consolidation coefficient– Typically 3 to 10 times greater than from laboratory oedometer testing
– Essential for estimating set-up times around piles, caissons etc
– Pipeline-soil interaction (e.g. buckling, walking) sensitive to degree of consolidation during movement
• Penetrometer testing in intermediate soils (silt-sized)– Partial consolidation during penetration – how best to quantify?
– Requires independent measurements – multiple pore pressure sensors?
– Or varying penetration rate
Ideal: continuous sensing during penetration to detect both degree of consolidation and cv
The University of Western Australia
Partial consolidation effects – backbone curves
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 20
Effect on resistance, q, and excess
pore pressure, u
• Function of relative velocity, vD/cv
• Probe by changing penetration rate
• Ideally need prior knowledge of cv -
but at least measure it
Catch 22:
• What is effect of partial
consolidation on subsequent
dissipation test?
0.5
1
1.5
2
2.5
3
0.1 1 10 100 1000
Nor
mal
ised
res
ista
nce,
q/q
un
Normalised velocity, vD/cv
Response to velocitychange (factor of 3)
0
0.2
0.4
0.6
0.8
1
1.2
0.1 1 10 100 1000
Nor
mal
ised
exc
ess p
ore
pres
sure
, Δu/Δu
ref
Normalised velocity, vD/cv
Response to velocitychange (factor of 3)
Penetrationresistance
Excess porepressure
The University of Western Australia
Partial consolidation effects – experimental study
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 21
One soil type; varying velocity
• Dissipation testing after penetration
phase at normalised velocity, vD/cv
• Reduced initial excess pore pressure
• Gradual increase in t50 times
Simple analytical assumption
• Reduced excess pore pressure
corresponds to initial phase of
dissipation test
• Post-penetration dissipation leads to
increased T50
• Consequent under estimation of cv 0102030405060708090
100
0.001 0.01 0.1 1 10 100
Nor
mal
ised
exc
ess p
ore
pres
sure
(Δ
u/Δu
initi
al)
Normalised time factor, T (cvt/D2)
Teh & Houlsby (1991)
Typical data
Hypothetical dissipationduring penetration phase
Subsequentdissipation test
ApparentT50
0
0.2
0.4
0.6
0.8
1
1.2
0.1 1 10 100 1000
Nor
mal
ised
exc
ess p
ore
pres
sure
, Δu/Δu
ref
Normalised velocity, vD/cv
Dissipation
tests
The University of Western Australia
1
10
100
1000
1 10 100 1000 10000cv
(mm2/s)
t50 (s)
Assuming undrained penetration
Allowing for partial consolidation
during penetration
Partial consolidation effects – theory & experiment
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 22
Theoretical approach
• Ignoring partial consolidation effects
gives cv inversely proportional to t50
• Assuming all dissipation part of same
theoretical curve gives apparent lower
limit to t50
Experimental data
• Observed (up to) 3-fold increase in t50
• Experimental data fall between above
two assumptions
• Need revised theory!
0
20
40
60
80
100
120
140
160
0.1 1 10 100 1000 10000
Exc
ess p
ore
pres
sure
(kPa
)
Time (sec)
280 s
600 s400 s
200 s
t50 times
1
10
100
1000
1 10 100 1000 10000cv
(mm2/s)
t50 (s)
Assuming undrained penetration
Allowing for partial consolidation
during penetration
Experimental data
The University of Western Australia
Pipeline geotechnical engineering
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 23
The University of Western Australia
Deep water pipeline geotechnical design issues
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 24
Infrastructure• Pipeline: laid directly on seabed, possibly with concrete weight coating
• Pipeline initiation, anchoring and manifold systems
Embedment in seabed• Pivotal for lateral stability, lateral buckling analysis, axial sliding
• Pipe lay dynamics has major impact on embedment
• Need combination of analytical solutions and empirical adjustments
Lateral stability• Breakout resistance, post-breakout residual resistance
Axial friction• Large range depending on drainage conditions, hence velocity and time
scale of movement
The University of Western Australia
Pipeline geometry and key parameters
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 25
t
zw
Pipeline:Diameter, D Bending rigidity, EISubmerged weight, W'
Tension, T0Seabed (stiff)
Sea surface
Touch down point (TDP)
z
x
s (arc length)
T0
T W'.s
From equilibrium:
Tx constant (T0)
Tz = W'.s
(cumulative pipe weight)
Characteristic length
The University of Western Australia
Pipeline embedment – quick estimate
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 26
• Linear seabed strength gradient (upper 0.5 m): su = z kPa
– Seabed plastic ‘stiffness’ (V/w): k ~ 4D
– Dynamic lay motions remould soil: need rem = /St
– Allowance for buoyancy effects as pipe embeds in soil (consider '/rem)
w/D ranges from 0.065 to 0.9
Force concentrationin touchdown zone:V/W' ~ 1.4 to 2.7
The University of Western Australia
Pipeline embedment – refined approach (Westgate et al.)
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 27
• Detailed assessment of lay-induced vertical and horizontal motions
– Estimated lay rate, metocean conditions – hence number of exposure cycles
– Pipeline configuration in touchdown zone (maximum dynamic vertical loads)
– Cyclic soil degradation model from cumulative pipeline motions
Non-deterministic estimates
consistent with modern
pipeline design approaches
The University of Western Australia
Pipeline axial friction
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 28
• Axial friction controlled by normal effective stress and pipe-soil roughness
– Low effective stress level (< 5 kPa), so enhanced roughness coefficient
– Rapid shearing results in excess pore pressures, reducing normal effective stress
– Consolidation leads to hardening, and local reduction in soil water content
Pipediameter D
w
m
p
n' cos
W'
Average normal stress, n, enhancedby wedging factor, ≤ 1.3
ln 'n
e
emax
q
e0umax
u
e
critical state line
n
The University of Western Australia
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.0001 0.001 0.01 0.1 1 10
Nor
mal
ised
fric
tion,
/
n
Normalised time, T = cvt/D2
0.31
10 330
vD/cv = 0.1Backbone curve
Drained Undrained
Time scale for consolidation during axial sliding
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 29
Critical state framework
• Rapid shearing leads to ‘undrained’ friction values
• Sustained sliding results in consolidation towards ‘drained’ friction
00.10.20.30.40.50.60.70.80.9
1
0.01 0.1 1 10
Nor
mal
ised
fric
tion,
/ n
Normalised axial displacement, /D
31 10
vD/cv = 30
vD/cv ≤ 0.3
T50 = 0.05 Design range
Initial excess pore pressure & friction• Mobilisation time:
slip/v cv /vD × slip/D
• Consolidation time: T10 ~ 0.001; T50 ~ 0.05; T90 ~ 1
The University of Western Australia
Additional effects during axial sliding
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 30
• High strain rates (v/D) enhance shearing resistance
• Sustained volumetric collapse of soil (‘damage’) – source of further u
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.001 0.01 0.1 1 10 100
Normalise
d frictio
n, /
n
Normalised displacement, /D
vd/cv ≤ 0.3
1
10
3
vd/cv = 30
ndamagev Dv
The University of Western Australia
Consolidation properties at shallow depth
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 31
• Near surface measurement of consolidation coefficient– Piezocone no longer practical (shallow penetration; long dissipation times)
– Introducing the ‘parkable piezoprobe’ (PPP) – offline dissipation data
The University of Western Australia
LDFE analyses as basis for interpretation
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 32
• Couple Modified Cam clay large deformation FE analyses– Assessment of excess pore pressure field
– Backbone consolidation curves
0
0.2
0.4
0.6
0.8
1
1.2
0.0001 0.001 0.01 0.1 1 10 100
u/
u i
T = cvt/D2
CPT (using DCPT)CPT (using DPPP)
Pipeline
PPP, w/D = 0.5
CPT (using DCPT)CPT (using DPPP)
Pipeline (w/D = 0.5)
PPP, w/D = 1
The University of Western Australia
Concluding remarks
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 33
• Analysis underpins day to day design
– Direct application of solutions
– Planning of studies based on physical or numerical modelling
– Empirical correlations: a challenge to capture analytically
• Simplicity a guiding light
– Dimensional analysis
– Idealisation of analytical models and input
– Synthesis of outcomes – especially from numerical studies
– Field and laboratory data vital: validation and adjustment of models
All is worthless without understanding!
The University of Western Australia
Acknowledgements
Mark Randolph: 2nd McClelland Lecture: Paris, September 2013 34
• Colleagues and collaborators throughout the world, but particularly at
– Centre for Offshore Foundation Systems at UWA
– Advanced Geomechanics
– ISSMGE Technical Committee 209 on Offshore Geotechnics
• Generous funding support from
– Australian Research Council
– Lloyds Register Foundation
– Industry
• Mentors throughout my career