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Universitetet i Stavanger uis.no Ingrid K. Feyling, Siri M. Kalvig & Knut Erik Giljarhus The Fifth Symposium on OpenFOAM in Wind Energy (SOWE 2017) Research Network for Sustainable Energy at UiS & IRIS 26-28 April 2017 Pamplona, Spain

The Fifth Symposium on OpenFOAM in Wind Energy …windbench.net/system/files/ingrid_feyling_-_presentation.pdf · Universitetet i Stavanger uis.no Ingrid K. Feyling, Siri M. Kalvig

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Universitetet i Stavanger

uis.no

Ingrid K. Feyling, Siri M. Kalvig & Knut Erik Giljarhus

The Fifth Symposium on OpenFOAM in

Wind Energy (SOWE 2017)

Research Network for Sustainable Energy at UiS & IRIS

26-28 April 2017

Pamplona, Spain

Overview

Ingrid K. Feyling 2

Introduction

Motivation

Wave-wind interactions

Previous work

Methods

Preliminary comparison

Conclusions and future work

Ingrid K. Feyling 3

Research Network for Sustainable Energy UiS & IRIS

Introduction

5

• The wave’s effect on the wind profiles usually ignored in offshore wind turbine engineering

• Recent research has shown that the MABL is influenced by waves in much higher levels than

previously thought (e.g. S. Kalvig, 2014)

• Waves will influence the power production as well as turbulence levels and wave decay

Challenge:

How can we model the effect the waves have on the wind profile? And

will the wave effect be significant for the performance of a wind

turbine?

Wind wave interaction investigated with two different CFD methods for

wave representation - Solid surface and moving mesh vs. VOF

Ingrid K. Feyling

6

Motivation

Need a better link between

wave models and atmospheric

models

Offshore wind energy – great

potential! Høg-jæren vindpark, photo:

Norsk Vindenergi

0

20

40

60

80

100

0 5 10 15

Heig

ht

(m)

Mean wind speed (m/s)

Photo: Lene Eliassen

Atmospheric stratification and wave

effects are two major factors affecting

wind conditions over sea versus land

Wind and wave

misalignment is quite

common

S.A Hassan (2017)Earth Nullschool

Ingrid K. Feyling

Wave-wind interactions

Wind sea and swell influences the atmosphere different

Wind sea - waves generated by local wind

Swell - long period waves generated by distant storms

Ingrid K. Feyling 8

The marine atmospheric boundary layer (MABL): part of the atmosphere that

is directly influenced by the ocean

One of the major problems in understanding the dynamics of the wind in the

surface layer is the difficulty to get experimental data at spatial scales from

few meters to few kilometers

Parameterization of the wind-waves interaction: complex challenge due

to time-evolving wave fields CFD simulations and comparison to

experimental measurements to evaluate the wave effect on the MABL

Marine Atmospheric Boundary Layer (MABL)

9

Previous work

Grand Valley State University

Need a new boundary condition that take into account the

sinusoidal movement of the “ground”

Kalvig & Manger (2014)

Waves + Actuator Line (SOWFA) FAST

WIWiTS

R.Kverneland (2012)

VOF method:

volume fraction of a

fluid occupying each

element in the

computational domain

is defined by F where

(0 ≤ F ≤ 1)

10

OpenFOAM case set-up:

Boundary Layer test case: pimpleFoam

Volume of Fluid:

interFoam:air/water

waves2foam toolbox

(developed by N.G Jacobsen et al. 2012)

Solid surface and moving mesh:PimpleDyWFoam solver

(developed by Kalvig & Manger 2014)

Methods

Ingrid K. Feyling

Ingrid K. Feyling 11

Based on OpenFOAM solver: pimpleDyMFoam

Wind: ABL inflow

Waves: Stoke’s 1st order (Airy)

PimpleDyWFoam solver (1)

Approximations used:

Newtonian fluid and incompressible flow

Coriolis force and buoyancy not included

Turbulent closure: k-ε (Reynold’s stresses proportional to the mean rates of deformation)

Water depth: set to ‘infinite’ to exclude the effects from the sea bottom

Waves seen as a solid – no deformation due to the wind (!)

“moving mesh”

PimpleDyWFoam solver (2)

𝝽 𝑥, 𝑡 = 𝑎 𝒂𝒏 𝑠𝑖𝑛 2𝜋(𝑥−𝑐𝑡

𝜆) + 𝒘𝒏 𝑐𝑜𝑠 2𝜋(

𝑥−𝑐𝑡

𝜆)

𝝽 is the total wave surface displacement, 𝒂𝒏 and 𝒘𝒏 are unit vectors, x is the horizontal position at a

given time t, a is the wave amplitude, λ is the wavelength and c is the wave speed

Ingrid K. Feyling 12

Ingrid K. Feyling

Results applying this showed that the wind field is influenced by the wave high above the wave boundary layer (WBL)

PimpleDyWFoam solver (3)

The horizontal component

of the wind speed (upper),

the vertical component of

the wind speed, (middle)

and the turbulent kinetic

energy (lower) over a wave

with:

A=4 m, λ =70 m, c=10.5 m/s

Domain size: 450 m x 400 (close up)

R. Kverneland (2012)

Expanded to pimpleDyWTurbineFoam for

inclusion of a wind turbine in 3D

domain

13

14

Developed by Jacobsen et al. (2012)

Uniform wind inflow

Wave theory library included

Relaxation zone technique

Pre- and post-processing utilities tailored for use for free surface flows

Waves2foam

waveFoam: modified waveFlume case

waveProperties input file: wind and wave definition

Ingrid K. Feyling

Ingrid K. Feyling 15

Volume of Fluid: waves2foam Airy wave, no wind applied, c = 10.5 m/s, λ = 70 m, and a = 2 m

Preliminary Comparison (1)

Ingrid K. Feyling 16

Volume of Fluid: waves2foam Airy wave, uniform wind 1 m/s at inlet, c = 10.5 m/s, λ =70 m and a = 2 m

Preliminary Comparison (2)

Ingrid K. Feyling 17

Volume of Fluid: waves2foam Airy wave, uniform wind 10 m/s at inlet, c = 10.5 m/s, λ = 70 m and a = 2 m

Preliminary Comparison (3)

Ingrid K. Feyling 18

Solid surface & moving mesh: pimpleDyWFoam Airy wave, uniform wind 10m/s at inlet, c = 10.5 m/s, λ = 70 m and a = 2 m

Preliminary Comparison (4)

200 m

t=100 s

Fading wave zonePreliminary wind profiles

Preliminary Comparison (5)

Solid surface & moving mesh: pimpleDyWFoam Airy wave

Logarithmic wind at inlet: U400m = 8 m/s and z0=0.0002 m

Domain: 1200m x 25 m x 400 m

Profiles are sampled from the middle of the domain (x=600 m) for every second between 251-300 seconds of simulations

Wave with a = 4 m, λ = 50 m, c = 8.8 m/s Wave with a = 4 m, λ = 100 m, c = 12.5 m/s

Wind velocity profile sampled from

different cases:

(black) wind without waves

(blue) wind aligned with the waves

(red) wind opposed to the waves

(S.Kalvig, 2014)

Ingrid K. Feyling 20

The flow response over the waves is very different compared with flow

over a flat sea surface

Wave direction relative to wind direction important

The wind speed profile and the turbulent kinetic energy pattern far

above the waves will be different depending on the wave state and wave

direction

Both solid wall/moving mesh and VOF method for wave induced wind

simulations works well when dealing with swell conditions

….However, more testing and validation required

Conclusions

Ingrid K. Feyling 21

Implement atmospheric stability

More wind and wave conditions

Opposing and misaligned wind/wave cases

Investigate parametric relationship between wind and waves (!)

Future Work

Overall:

Improve the understanding of the marine atmospheric boundary layer (MABL) and its turbulence

level in the presence of waves of different orientation and magnitude

Improve the understanding of the influence of wave affected MABL on power production and

dynamic loads

Improve the understanding of the influence of wave affected MABL on wind turbine wake

Definition of wave and wind relative orientation

E-mail: [email protected] 22

[1] https://www.fastcompany.com/3059959/scotland-will-be-home-to-the-worlds-largest-wind-floating-wind-farm

[2] www.uis.no/miljoenergi

[3] S. Kalvig, “On wave-wind interactions and implications for offshore wind turbines” (2014)

4] S. Kalvig, E. Manger, B. Hjertager and J. Jakobsen, "Wave influenced wind and the effect on offshore wind turbine performance, Energy Procedia,

vol. 53, pp. 202-213, 2014

[5] S. Kalvig, E. Manger & R.Kverneland “A method for wave driven wind simulations with CFD” (2013)

[6] P. P. Sullivan, J. C. McWilliams and E. G. Patton, "Large-eddy simulation of marine atmospheric boundary layers above a spectrum of moving waves" (2014)

[7] N.G. Jacobsen, D.R. Fuhrman, J. Fredsøe, “ A wave generation toolbox for the open-source CFD library, OpenFOAM” (2012)

[8] R. Kverneland , “CFD – Simulations of wave-wind interaction” (2012)

[9] S.A. Hassan, UiS MSc .Thesis, unpublished (2017)

[10] K.Okamori, «Fluid Simulation Analysis of Multi-phase Flows by Oka-san 3, VOF method” (MSc. Course)

References

Acknowledgement: Statoil Academia & Research Network for Sustainable Energy at UiS & IRIS