scour holes/scour protection: effect on wave loads ewec 2007 milano erik asp hansen erik damgaard...
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Scour holes/Scour protection: Effect on wave loads
EWEC 2007 MILANO
Erik Asp Hansen
Erik Damgaard Christensen
Outline of the presentation
Added mass for a vibrating cylinder(Related to dynamical analyses of the entire wind turbine)• Description of inertia and added mass• Three deflections of the cylinder• Effect on damping
Scour hole: effect on loadsscour protection: effect on loads(Better estimation of wave loads)• Method based on CFD
Two different tools used: WAMIT
WAMIT (“Wave analyses MIT”, it was developed at MIT)• A first order panel method• It solves diffraction and radiation problems for offshore structures• It can be used to analyse floating body motions• In this study the added mass is determined by WAMIT
Two different tools used: NS3
Navier-Stokes solver in 2D and 3D Finite volume approach Multi-block domain Structured grid in each block Free surface, Volume of Fluid (VOF) Forces on hydraulic structures
Two different tools used: NS3
Animation:
A comparison: A non-cylindrical structure
Regular waves:Wave period = 9.4 sWater depth = 25 mLarge diameter = 15 mSmall diameter = 5 m
Panels for WAMIT calculations
Inertia and added mass
Definition of inertia coefficeintCan be said to be a combination of Froude-Krylow force and added
mass.The Inertia coefficient for a large vertical cylinder:
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10
0.5
1
1.5
2
2.5
3
D/L
CM
MacCamy Fuchs
dt
UdACf x
Mx
dt
Ud x
MC
Phase difference
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
-1.5
-1
-0.5
0
0.5
1
1.5
D/L
rad
MacCamy Fuchs
Why do we get a phase difference?
structure
dundisturbex dApinstead
dt
UdVol
The phase difference is partly due to:
effect of diffraction
phase difference and size of added mass
Added mass
td
Xd2
2
dt
dXACf aadd
1 Ma CC
2D cylinder in aninfinite large volume of waterCa is equal to oneand:
Three types of deflections
tT
sinXt,zX odef
2
tT
sinXh
zzt,zX o
beddef
2
tT
sinXh
zzt,zX o
beddef
22
2
Inertia and added mass
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10
1
2
3
D/L
CM
D/h=0.4 Inertia Coefficient VS. AddedMass Coefficient
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10
0.5
1
1.5
2
Added m
ass c
a
Inertia Coefficent for uniform oscillation
AddedMass Coefficient
uniform
linear
parabolic
The horizontal force
damping_wave
dt
XdDC
dt
UdDC
dt
XdU
dt
XdUDC½f
ax
M
xxD
2
222
damping_wave
dt
XdD
dt
Xd
dt
UdDC
dt
XdU
dt
XdUDC½f
xM
xxD
2
22
2
22
1 Ma CCOften: is used though not in general correct =>
CFD calculations
Effect of scour protection on wave load: TEST A
Calculated horizontal forces and overturning moment for water depth h=10m, wave period T=8s wave height H=5.0m,
Effect of scour protection on wave load: TEST B
Calculated horizontal forces and overturning moment for water depth h=10m wave period T=8s wave height H=6.0m
Effect of scour protection on wave load: TEST C
Calculated horizontal forces and overturning moment for water depth h=10m wave period T=8s wave height H=5.0m current velocity V=1m/s
Conclusions
• Based on the calculation presented, it can be concluded that for offshore wind turbines the added mass is not related to by the equation.
• This will influence the dynamics of the structure and might give wrong estimates of the frequencies
• The wave damping could have a major influence as well• The horizontal forces are affected by the presence of a scour
hole or a scour protection. • scour protection will reduce the horizontal forces • scour protection will reduce the horizontal forces • but reduce the overturning moment compared to the plane bed
situation• A scour hole will increase the horizontal forces • but reduce the overturning moment compared to the plane bed
situation