2-trench effect on the fatigue life of a scr_y.t.kim.pptx
TRANSCRIPT
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Trench effect on the Fatigue life of a SCR
Prepared by Y.T.Kim
Offshore Engineering Lab. Seminar No. 2
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Current developments of SCR technology focus on improving fatigue life
in the touchdown region and better understanding the interaction between
the SCR and the seabed.
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1. Review
The pipe is initially in contact with a virgin soil
The pipe penetrates into the soil, plastically deforming
it. The pipe and soil interaction curve tracks on the
backbone curve.
The pipe moves upward and the soil responds
elastically. The pipe/soil interaction curve breaks away
from the backbone curve ,the force reduces over a
small displacement.
The pipe again penetrates the soil, deforming it
elastically. The pipe/soil interaction curve follows an
elastic lading curve similar to the previous elastic
unloading curve of step 3.
The pipe again penetrates into the soil, plastically
deforming it. The pipe/soil interaction curve rejoins and
follows the backbone curve.
(Steel catenary riser touchdown point vertical interaction models-Bridge, C., Laver, K.,
Clukey, Ed., and Evans, T.)
igure 1-Illustration of Pipe/Soil Interaction
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1. Review
1. Penetration-the pipe penetrates into th
soil to a depth where the soil force equal
the penetration force following backbon
curve. The soil deforms plastically.
2. Unloading-the penetration force reduce
to 0 N allowing the soil to swell as the pip
moves upwards.
3. Soil suction-as the pipe continues to mov
upwards the adhesion btw the soil and th
pipe causes a tensile force that resists th
pipes motion. The adhesion force quickl
increases to a maximum then reduces to
N as the pipe moves vertically upwards and
out of trench.
Backbone Curve
Penetration
Unloading
Soil Suction
Re-penetration after breakout
Figure 2. Re-penetration pipe/soil interaction curves
4. Re-penetration-the pipe penetrates into the existing trench that was created during the initial penetration. The re-penetration force/displacement curve has zero force when the pipe re-enters the trench, only increasing the interaction
force when the pipe re-contacts the soil. The pipe/soil interaction force then increases until it rejoins the backbone curve
at a lower depth than the previous penetration. Any further penetration follows the backbone curve.
(Steel catenary riser touchdown point vertical interaction models-Bridge, C., Laver, K., Clukey, Ed., and Evans, T.)
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2. Soil Stiffness
In order to analyze any kind of structure, or any kind of solid or fluid continuum, it is
necessary to have relation ships btw stresses and strains.
A
Figure 3. A typical stress-strain curve for soil Figure 4. Tangent and secant stiffness moduli
Siffness- the gradient of the stress-strain line. If this is linear the gradient is easy to
determine but, if it is curved, the stiffness at a point such as A in fig. 4 may be quoted as atangent or as a secant.
(The mechanics of soils and foundations, John Atkinson)
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2. Soil Stiffness
The two tests commonly used in soil mechanics are the triaxial test and the shear test
illustrated in Fig.5
A
Figure 5. Common soil tests
(The mechanics of soils and foundations, John Atkinson)
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2. Strength, Stiffness and Rigidity
The strength of a material is the maximum shear stress which it can sustain and its
stiffness is the ratio of changes of stress to the resulting strain.
A material ay be relatively strong or relatively weak: it may be relatively stiff or relatively
soft. Concrete and rubber have similar strengths but concrete is much stiffer than rubber.
(The mechanics of soils and foundations, John Atkinson)
Rigidity R-the ratio of stiffness to strength, commonly defined as
=
-Youngs modulus (stiffness)
-strength expressed as the diameter of the Mohr circle at failure
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2. Strength, Stiffness and Rigidity
Table 1. Typical values of stiffness, strength and
rigidity of some common materials
(The mechanics of soils and foundations, John Atkinson)
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2. Trench effect on the Fatigue life of a SCR
Non-Degradating and Degradating Models
Non-Degradating-neglecting degradation effect of cyclic loading, that is, it states
that a riser follows the same P-y curve repeatedly if cyclic loading remains the
same.
Degradating-In reality, cyclic loading degrades the soil condition. After many
cycles of pounding the pipe into the soil, a plastic deformation is formed, which
explains why the observed penetration is much greater than computed
penetration governed by the backbone curve using a non-degradation P-y curve.
Ali Nakhaee & Jun Zhang Effects of the interaction with the seafloor on the fatigue life of a SCR. ISOPE 2008
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2. Trench effect on the Fatigue life of a SCR
The degradation mechanism involves soil remolding in each downward and upward
motion that may reduce the stiffness and strength of the soil
Figure 6. Stiffness degradation due to
cyclic loading
Degradation of the soil or plastic deformation of
the seafloor can significantly affect the curvature
of a riser near its TDZ, thus the bending moment
and the variation in bending moment.
Cluckey et al. (2005) concluded that as the pipe
moves back toward the soil , the water
underneath the pipe is pushed downward. The
jetting action by the water can lead to soil-water
mixing and trench erosion which can also reduce
the strength and stiffness of the soil.
Ali Nakhaee & Jun Zhang Effects of the interaction with the seafloor on the fatigue life of a SCR. ISOPE 2008
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2. Trench effect on the Fatigue life of a SCR
Figure 7. Typical Degradading P-y Curves
Yaguang Jiao Non-linear load-deflection models for seafloor interaction with steel catenary risers A thesis for master of science
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2. Trench effect on the Fatigue life of a SCR
Ali Nakhaee & Jun Zhang Effects of the interaction with the seafloor on the fatigue life of a SCR. ISOPE 2008
After hundreds of loading cycles thetrench development on the seafloor
make the riser penetrate into the soil.Figure 8. Trench development
(heave amp=1m, heave period=12s, medium soil)
ff f f SC
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2. Trench effect on the Fatigue life of a SCR
Ali Nakhaee & Jun Zhang Effects of the interaction with the seafloor on the fatigue life of a SCR. ISOPE 2008
Figure 9. Maximum movement variation along the riser
Maximum moment variation near the TDZ afunction of time after they started
experiencing continuous cyclic loading.
It shows maximum variation of bending
moment near the TDZ gradually reduces due
to the development of trenching.
The reduction in the maximum variation in
bending moment reduction of dynamicstress of a riser prolongs the fatigue life ofthe riser
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Ali Nakhaee & Jun Zhang Effects of the interaction with the seafloor on the fatigue life of a SCR. ISOPE 2008
Figure 10. Maximum moment variation in Riser
for different types of soils
A deeper trenching is developed on the
seafloor of soft soil greater reduction in themaximum variation of bending momentgreater increase in fatigue life of the riser
2. Trench effect on the Fatigue life of a SCR
3 F t Pl
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How to derive the fatigue life from the TDP result?
Fatigue analysis based on DNV
3. Future Plan