inappropriatness of the current offshore guidelines …
TRANSCRIPT
INAPPROPRIATNESS OF THE CURRENT OFFSHORE
GUIDELINES FOR THE DESIGN OF LARGE-DIAMETER
MONOPILES IN SANDS – DEMONSTRATION THROUGH
5-MW REFERENCE WIND TURBINE FROM NREL
Djillali Amar BOUZID
Department of Civil Engineering, University of Blida, Route de Soumaa
Blida 9000, Algeria
ABSTRACT
Since the World’s demand on energy is constantly raising, many countries built and are
currently building their offshore wind farms to produce cheap, clean and renewable energy as
a substitute to fossil fuel based energy which is the source of green-house gases leading the
main cause of global heating. Despite the increasing in turbine capacity, the preferred
foundations for these offshore wind turbines (OWTs) are large diameter monopiles due to
their ease of installation in shallow to medium water depth.
For decades the well-known curve method (adopted by API and DNV Offshore Guide
Lines) in which the monopile/soil interaction is considered by non-linear curves
derived from field tests, has been applied to analyze monopiles supporting OWTs. Although
the formulation has been applied successfully in designing piles supporting gas and oil
platforms in offshore industry due to the low failure rate observed in piles, its application to
design large-diameter monopiles supporting offshore wind energy converters has not been
validated for monopiles of diameter up to 6 m as many authors reported inconsistencies in the
use of these design rules. In this paper the weakness points of the Winkler model based on
curves are also given along with the recent propositions to enhance the performance of
the Winkler models which are described. Then a new finite element procedure based on the
combination use of 2D FE analysis and finite differences method suitable for 3D soil/structure
interaction problems is briefly described. By considering a 5-MW reference offshore wind
turbine from NREL embedded in sand, the study focus then, on the examination monopile
head stiffness which is the key element in quantifying the monopile/soil interaction. The
monopile head stiffness is significantly important for the determination of the first OWT
natural frequency which is in turn a crucial parameter for the monopile design.
1. INTRODUCTION
As wind energy is one of the most promising and fastest-growing renewable energy sources
around the world, there has been a rapid development in the installation of wind farms in both
onshore and offshore locations to secure clean electricity as a permanent source of energy.
Because offshore winds tend to have higher speeds and less turbulent than onshore winds,
resulting in an increase in the potential energy produced in offshore locations than in onshore
ones, several offshore wind farms have been already installed all over the planet the last
decade and a vast number is being planned for the near future. Although, there are many
Offshore Wind Turbines (OWTs) support options depending on the water depth (ranging from
gravity foundations for shallow depths of to floating foundations for very deep
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waters of ), the most widely used option for supporting offshore wind-turbines is
the monopile foundations, which consist of welded steel pipe piles driven open-ended into
soil. This type of foundations has proven to be an efficient solution in water depths ranging
between and and consequently it is the most appropriate choice for offshore wind
farms, due to the ease and speed of installation and cost of construction (Achmus et al. 2009;
Adhikari and Bhattacharya (2011, 2012); Carswell et al. 2015; Laszlo et al. (2016, 2017);
Galvin et al. 2016).
The primary objective of this paper is twofold. The first, is to show that a FE analysis based
on a nonlinear soil model is the best choice as a method of analysis for safe design of OWTs.
The second, is to confirm what has been stated about the behavior of laterally loaded
monopiles since the emerging of OWT industry by many researchers who ascertain that the
O’Neill and Murchison’s (1983) formulation which has been adopted first by the API and
then by the DNV, is no longer appropriate for the analysis of large-diameter monopoles under
horizontal loading.
2. P-Y CURVES USED IN THE CURRENT OFFSHORE GUIDELINES
FOR THE DESIGN OF LARGE-DIAMETER MONOPILES
Using this piecewise curve proposed by Reese et al. (1974) and a relatively large
database of laterally loaded pile tests, O’Neill and Murchison (1983) suggested a hyperbolic
formula for curve in order to describe the relationship between soil resistance and
lateral pile deflection in sand:
(1)
In equation (1), is the ultimate soil resistance and represents the initial coefficient of
subgrade reaction depending on the angle of internal friction of the cohesionless soil. The
initial stiffness of the curves , recommended in the design can be obtained by
evaluating the slope of the curve tangent at .
(2)
It is quite clear from the equation (2), that the initial stiffness is independent on pile properties
(diameter and bending stiffness) and it is linearly dependent on the depth .
Standards for designing laterally loaded piles, e.g. the American Petroleum Institute (API,
2011), Det Norske Veritas (DNV, 2013) are based on the Winkler model using curves
whose expressions are given by equation (1).
2.1 Drawbacks of the formulations of curves
Although, they have been employed for designing offshore piled foundations by the offshore
oil and gas industry for decades, these design recommendations (API, and DNV) are not
appropriate for designing foundations for offshore wind turbine structures, for many reasons:
a) They have been developed on the basis on full-scale load tests on long, slender and
flexible piles with a diameter of 0.61 m, whereas monopiles are relatively shorter and
stiffer piles with diameters up to 6.0 m in the offshore wind turbine industry.
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b) The widely used API model is calibrated against response to a small number of cycles
for offshore fixed platform applications. However, an offshore wind turbine may
undergo 107-10
8 cycles of loading over its lifetime of 20-25 years.
c) Under cyclic loading, the API and DNV models always predict degradation of
foundation stiffness in sandy soil. However, it has been showed that the monopile
stiffness in sandy soil will increase as a result of densification of soil in the vicinity of
the monopile.
For further details about the shortcomings inherent to the model formulation the reader
is referred to Amar Bouzid and Medjitna (2017).
2.2 Most recent modifications to improve the performance of the winkler
model The p-y curve given by the equation (1) is composed by to fundamental elements which are
the initial stiffness and the ultimate soil resistance . Most researchers found that the
linear variation with depth of as indicated in equation (2) is inappropriate for monopoles
from the fact that it heavily overestimates the soil stiffness at depth. However, the
overwhelming majority of authors considered appearing in the formulation by Reese et
al.1974, adequate for design of large-diameter monopiles and kept it unaltered in their new
curve formulations. Consequently, the most recent proposed modifications are listed in
Table 1.
Table 1. Proposed formulae for the curve initial stiffness.
Authors Proposed formulae Assigned parameters
O’Neill and Murchison
1983 (API 2014 and DNV
2011)
appearing in equations (1) and (2)
Wiemann et al. (2004)
for a medium dense sand
for a dense sand
Sorensen et al. (2010)
,
Kallehave et al. (2012)
Sorensen et al. (2012)
3. COMPUTER CODES USED IN THIS PAPER
A pseudo 3D finite element model has been performed to analyze soil/structure interaction
problems in non-linear media. This numerical technique, which has been called Nonlinear
Finite Element Vertical Slices Model (NFEVSM), is based on the discretization of the 3D
soil/structure medium into a series of vertical slices, each one represented by a 2D boundary
value problem (Figure 1). The procedure involves the combination of the finite element (FE)
method and the finite difference (FD) method for analyzing the embedded structure and the
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surrounding soil sub-structured. The soil in this approach, was considered to obey the
hyperbolic model proposed by Duncan and Chang (1970). The numerical procedure has been
implement in a computer code called NAMPULAL (Details of this computer code are found
in Otsmane and Amar Bouzid (2017).
Figure1. (a) Offshore Wind Turbine as SSI problem, (b) The Vertical Slices Model showing
the interacting slices subjected to external and body forces.
For the Winkler model computations another computer code called Winkler-ROWKSS has
been written by the author including in addition, to Reese et al. and O’Neill and Murchison
formulations, all the proposed modifications presented in Table 1. Winkler-ROWKSS uses
the concept of a Beam on Nonlinear Winkler foundation (BNWF) to discretize the monopile
in finite differences method and the curves to model the soil lateral response.
4. ASSESSMENT OF HEAD MOVEMENTS OF THE MONOPILE
SUPPORTING 5-MW REFERENCE WIND TURBINE FROM NREL
IN SAND
The monopile head movements (lateral displacements and rotations) are the crucial
parameters required to design a monopile supporting an offshore wind turbine under
horizontal force or an overturning moment. In deed they are the key elements for the
determination of the monopile head stiffness which can be quantified by three springs, two for
controlling horizontal and rocking movements and one for the cross-coupling interaction. The
Monop
ile
Tower
Nacell
e
(a
)
(b
)
Medium to
be
discretised
V M
H
The fisrt three
slices
The
slice
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relationship between lateral stiffness , rocking stiffness and cross-coupling stiffness
may be expressed in a maytrix form as:
(3)
Where, and are respectively the shear force and the overturning moment applied at the
monopile head and and are respectively the lateral displacement and rotation of the
monopile head.
In order to assess the finite element results through the use of NAMPULAL against those of
API and those from the recently developed p-y curves implemented in Winkler-ROWKSS, it
is useful to consider the NREL 5-MW baseline wind turbine from the National renewable
energy laboratory (NREL) which is mounted atop a monopile with a flexible foundation in 20
m water depth (Jonkman et al., 2009 and Jung et al., 2015).
The NREL 5-MW mass and structural details are listed respectively in Tables 2 and 3. In this
study a representative soil profile was assumed, which was adopted from the work of Passon
(2006) as shown in Figure 2.
Figure 2. Soil profile and monopole dimensions for the NREL-5MW reference wind turbine.
Table 2. Reference wind Turbine masses
Table 3. Reference wind Turbine geometrical properties
Tower height (m) Tower diameter (m) Tower wall thickness (m)
At the base At the top At the base At the top
87.6 6.00 3.87 0.027 0.019
Rotor mass (tons) Nacelle mass (tons) Tower mass (tons)
110.0 240.0 347.5
MSL 0.0
- 20.0
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The geometrical characteristics are given in Table 4.
Table 4. Monopile properties
Monopile length (m) Monopile diameter (m) Monopile wall thickness (m)
Embedment length overhang
36.0 30.0 6.0 0.06
The evolution of monopole head movements (displacements and rotations) with the
increasing applied loading at the monopole top constitutes the main purpose of the present
investigation. In order to achieve this target both NAMPULAL and Winkler-ROWKSS
have been applied to examine the different tendencies. Figures 3 shows the monopile head
displacement and rotation with increasing lateral load or overturning moment. It seems from
the first sight that the results are separated in the three global categories. From the first,
relevant to finite element results, it is quite clear that the results of present method are nearly
identical to those of the FEM provided by Jung et al. (2015). The second, results by Reese et
al., O’Neill and Murchison and those of LPILE yield almost the same values and
consequently their curves are nearly above each other. However, the third category, relevant
to the Winkler methods based on the latest curves improvements, are occupying quite
different locations. Some near the FE curves, whereas others are even behind those of API
models.
Figure 3. Evolution of monopole head movements with applied loading: (a)
curves, (b) curves and (c) curves.
(a) (b)
(c)
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5. CONCLUSIONS
In this paper the author presented a numerical investigation of a laterally loaded monopoles
supporting 5-MW reference wind turbine in a sandy subsoil. Two types of numerical codes
have been applied to perform the numerical investigations. The first called NAMPULAL has
been used to discretize the medium into vertical slices, each is analyzed using the 2D
conventional finite element method with soil obeying to Duncan and Chang’s hyperbolic
model. The second computer code called Winkler-ROWKSS has been written on the basis of
finite difference scheme to model the monopole as a Beam on Nonlinear Winkler Foundation
(BNWF).
Through the examination of the monopole head movements, the paper investigated the lateral
behavior of a monopile supporting 5-MW reference wind turbine embedded in sands. From
the close examination of the load-deformation curves three major conclusions were reached:
[1] The results by NAMPULAL have been found to be in a close agreement with those
provided Abaqus reported in Jung et al. 2015. This confirms first, that the NAMPULAL
results are reliable since they are in perfect match with those of well-known FE package.
Secondly, the finite analysis reasonably assesses the monopile head stiffness which is a
crucial criterion of its design, ascertaining thus, that this rigourous method is not restricted to
parametric studies but also should be used in daily routine analysis of large-dialeter
monopiles.
[2] The Winkler methods (Reese et al. 1974 and O’Neill and Murchison 1983) on which
API and DNV have drawn their design guideline for large-diameter monopiles overestimate
the soil stiffness which may lead to inaccurate estimation of some dynamic characteristics of
offshoe wind turbine. This confirms that they are inappropriate for designing large-diameter
monopiles under lateral loading.
[3] From the load-deformation curves relevant to the winkler models based on the last
improvements in curves, different tendencies are noticed. Some are close to finite
element analysis, whereas others are even far from those adopted by both API and DNV. It
seems that sorensen and al. 201 have brought some improvement whereas the proposed curve by Kallehve et al. is not suitable at all to deal with large-diameter monopiles.
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