Aerodynamics of Wind Turbines, 1 by Sven Schmitz

Aerodynamics of Wind Turbines

A Physical Basis for Analysis and Design

Sven Schmitz

Department of Aerospace Engineering
The Pennsylvania State University
PA, USA

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To my son Andreas.

Never lose your spirit of invention. You can change the world.

About the Author

Sven Schmitz is an Associate Professor in the Department of Aerospace Engineering and The Institutes of Energy and the Environment (IEE) at The Pennsylvania State University. He is an expert in rotary wing aerodynamics, with particular emphasis on wind turbines and rotorcraft. He has authored 30 peer‐reviewed journal publications and more than 60 conference papers and presentations. His research program embraces the areas of wind turbine aerodynamics and rotorcraft aeromechanics. Current activities include improvements to wind turbine blade‐element momentum theory, wind farm wake modeling, icing on wind turbines, rotor hub flows, rotor active control, ship airwake modeling, and future concepts for transonic commercial aircraft. At Penn State, he developed and maintains the XTurb code, a wind turbine design and analysis software that he integrates in his teaching and research.

Sven Schmitz grew up in Effeld (Germany), a small and beautiful village on the German‐Dutch border in the lower Rhineland, approximately 60 km west of Düsseldorf and north of Aachen. In the Fall of 1996, he enrolled in the Engineering program at the Rheinisch‐Westfälische Technische Hochschule (RWTH) Aachen where he graduated in 2002 with a Diploma degree. From 2002 to 2006, he was a Ph.D. student at the University of California (UC) Davis under the guidance of Professor Jean‐Jacques Chattot. From 2006 to 2010, he was a postdoctoral researcher and project scientist at the U.S. Army Aero Flight Dynamics Directorate (AFDD) at the NASA Ames Research Center in Moffett Field, CA and at UC Davis. During this time, he also worked as a Computational Fluid Dynamics (CFD) consultant for wind energy applications with General Electric (GE) Global Research. In 2010, he joined the faculty of Aerospace Engineering at The Pennsylvania State University. He continues to publish and teach in the areas of wind turbine aerodynamics and rotorcraft aeromechanics.

Preface

The vision for the book was to develop a self‐contained and affordable unique text with focus on the aerodynamics, scaled design and analysis, and aerodynamic optimization of horizontal‐axis wind turbines. It is not a systems‐engineering text on wind energy, which distinguishes the book from other available texts. On the contrary, the author was encouraged by many colleagues over the past several years to develop a well‐integrated and focused account on the blade aerodynamics of horizontal‐axis wind turbines. The technical content is based on lecture notes developed by the author at the senior‐level undergraduate and graduate level. A further unique aspect of the book is the close integration of the text with the wind turbine design and analysis software, XTurb, developed and maintained by the author at The Pennsylvania State University. The XTurb code is essentially a teaching and research tool used since 2011 by the author in his graduate course and by Penn State students participating in the U.S. DOE Collegiate Wind Competition. The XTurb examples in the book add a “hands‐on” component, thus enhancing the learning experience to readers and resulting in a deeper and more complete understanding of the subject matter. This gives readers from interdisciplinary backgrounds in the area of wind energy the opportunity to fully absorb and understand the design principles and governing concepts in blade aerodynamics through the text and independent analyses using XTurb.

Chapter 1 concerns a brief description of horizontal‐axis wind turbine development, with particular considerations for the history of aerodynamics and its impact on the design evolution of wind turbines. In addition, the reader is introduced to the atmospheric boundary layer and the wind resource. Chapter 2 is a classical account on momentum theory for horizontal‐axis wind turbines, with some differences and additions compared to most texts. Chapter 3 covers classical Blade Element Momentum (BEM) theory. A special section includes a detailed description of root and tip loss factors used in today's BEM‐type methods and a discussion of their respective limitations. As far as BEM solution techniques are concerned, the presentation of classical work is accompanied by a description of various numerical techniques of solving the BEM equations (new in this book), followed by a complete description of models for the turbulent wake state (also not in any other text). A simplified BEM theory is described as a classical means to introduce simplified dependencies of the effect of design parameters on power coefficient, with the later subsection containing multiple examples of XTurb analyses and associated input decks. Chapter 4 begins with an introduction to thin‐airfoil theory and the foundations of viscous airfoil flow. This is followed by a brief historical review on wind turbine airfoil design and airfoil design criteria along the blade radius. The chapter concludes with a catalog of wind turbine airfoils. Chapter 5 focuses on introducing unsteady aerodynamics occurring on horizontal‐axis wind turbines, with subsections describing yaw effects, tower interaction, and dynamic stall. A big portion of this chapter is devoted to a comprehensive review on rotational augmentation and available stall‐delay models (also new in this text). Chapter 6 concerns vortex‐wake methods and starts off by a comprehensive introduction to lifting‐line theory and describes the basics of computing induced velocities from planar and vortical wake sheets. A unique subsection on prescribed wake methods (not in any other text) includes additional XTurb examples. A subsection on free‐wake methods includes classical descriptions and introduces the reader to the numerical problem of vortex cores to avoid wake singularities, including recent advances on singularity‐free‐wake methods. Chapter 7 gives an introduction to advanced computational methods including Computational Fluid Dynamics (CFD), hybrid CFD methods, and an introduction to recent advances in actuator‐type methods for wake modeling (i.e. actuator disk, actuator line, actuator surface). Chapter 8 introduces the reader to principles of (scaled) wind turbine design and optimization. The technical content draws from the author's experience in designing scaled experiments in both wind‐/water tunnels for wind turbine and rotorcraft applications. This is a very unique chapter of the book and one that is vitally important to the wind energy community at large. The XTurb software is used extensively in this chapter and brings the material of previous chapters into an overarching context to the reader, thus allowing a deeper understanding of the book material by considering the difficult and non‐unique aspects of scaled blade design and optimization. Supplementary files including XTurb input decks are available on a respective Wiley website.

The primary intended audience consists of senior undergraduate students and graduate students in MSc. and Ph.D. programs at universities, focusing on coursework and research in wind energy in engineering, atmospheric science, and meteorology. Further audiences are instructors and university professors, as well as practicing engineers and scientists in industry and national laboratories. Readers are expected to have basic knowledge of incompressible flows through coursework or work experience. The book is written at an intermediate level using college‐level algebra and analysis. The book can be used as a primary text for courses on wind turbine aerodynamics and/or as an affordable instructional aid for a multitude of courses on wind energy systems and power engineering in the international wind energy community.

In essence, this is a book “for Students, written by a student,” as the author sees himself as a continuous learner. I hope that you will find the book helpful to your careers. Wind energy has the potential to playing a major role in battling climate change by powering the world with a clean and renewable source of energy. Never give up, not as long as you have strength left.

January 2019

Sven Schmitz
State College, PA

Acknowledgments

A number of individuals have assisted the author and contributed to the book in different ways. I want to start by thanking my beloved wife Cristina for her patience and encouragement while writing the manuscript. I am especially grateful to my parents Helmut and Irmgard Schmitz who have always supported me in the path I have taken far away from home. I am also thankful to my Ph.D. advisor Professor Jean‐Jacques Chattot at the University of California Davis who educated me in wind turbine aerodynamics and numerical methods.

Many thanks are directed at The Pennsylvania State University for allowing me to spend my sabbatical leave at home. Furthermore, I am grateful to Professor Carlo L. Bottasso of the Technical University of Munich (TUM) and Professor Jens. N. Sørensen of the Technical University of Denmark (DTU) for hosting me a week each and their many valuable suggestions. The discussions with many colleagues at TUM and DTU were inspiring and helpful in organizing some of the book content.

I also acknowledge very much the help of my dear colleague Professor Mark D. Maughmer for numerous discussions on aerodynamics during my time at Penn State and for checking many subtle details thoroughly in the book. Furthermore, I am thankful to the former Aerospace Department Head Professor George A. Lesieutre for his encouragement in developing a graduate course focused on wind turbine aerodynamics, as well as colleagues Dr. Susan W. Stewart and Professor Dennis K. McLaughlin without whose dedication there would not be a continuing graduate certificate in wind energy in the department.

Special thanks to Dr. Scott Larwood of the University of the Pacific and Dr. Mike P. Kinzel of the University of Central Florida for reading the entire manuscript. Scott and Mike represent a portion of a diverse readership with different background and experience; their many questions and comments helped clarifying derivations, figures, and the narrative. I would also like to thank Mr. Dan Somers of Airfoils Inc. in Port Matilda, PA for his review and suggestions on the history of airfoil design for wind turbines over the past 30 years. In addition, comments and suggestions by Dr. Niels Troldborg of Risø National Laboratories on advanced computational methods and actuator line modeling are very much appreciated.

Last but not least, I want to thank my students in wind energy for their commitment to hard work, inspiration, and passion for wind energy as a viable source of renewable energy. The future lies with our students who will advance wind energy to the next generation. I would like to close by thanking the U.S. Department of Energy (DOE), the National Science Foundation (NSF), the University Corporation for Atmospheric Research (UCAR), and industry for their generously supporting my students at Penn State.

Abbreviations

1P
One Per revolution
2‐D
Two‐Dimensional
3‐D
Three‐Dimensional
ABL
Atmospheric Boundary Layer
ACE
Actuator Curve Embedding
AEP
Annual Energy Production
ALM
Actuator Line Model
AoA
Angle of Attack
AR
Aspect Ratio
BEM
Blade‐Element Momentum
BEMT
Blade‐Element Momentum Theory
CF
Capacity Factor
CFD
Computational Fluid Dynamics
COE
Cost of Energy
DTU
Technical University of Denmark
DUT
Delft University of Technology
ECN
Energy Research Center of the Netherlands
FS
Full Scale
HAWT
Horizontal‐Axis Wind Turbine
HVM
Helicoidal Vortex Model
IEC
International Electrotechnical Commission
KJ
Kutta–Joukowski
LCOE
Levelized Cost of Energy
LIR
Low Induction Rotor
MEXICO
Model rotor EXperiments In COntrolled conditions
MS
Model Scale
NACA
National Advisory Committee for Aeronautics
NASA
National Aeronautics and Space Administration
NREL
National Renewable Energy Laboratory
PIV
Particle Image Velocimetry
PSU
Penn State University
rpm
Revolutions Per Minute
RWT
Research Wind Turbine
SST
Shear Stress Transport
TKE
Turbulent Kinetic Energy
TS
Tollmien–Schlichting; Technical Specifications (Chapter 8)
TUM
Technical University of Munich
UIUC
University of Illinois Urbana‐Champaign
VWM
Vortex Wake Method

List of Symbols

Note: This list includes the most relevant symbols used in the book, and omits some symbols that are unique to particular subchapters.

English

a
axial (flow) induction factor
a
angular (flow) induction factor
adv i
(vortex) sheet advance ratio (Chapter 6)
A
actuator/rotor disk area
A 0
entrance area of streamtube (Chapter 2); Fourier coefficient in airfoil theory (Chapter 4)
A 1
exit area of streamtube
A n
Fourier coefficients in airfoil/wing theory (Chapters 4, 6)
A t
airfoil cross‐sectional area (Chapter 4)
b
wing span
B
blade number
c
blade chord; Weibull scale parameter (Chapter 1)
images
mean aerodynamic chord
c 0
wing mid‐span chord
c d
section (profile) drag coefficient
c d,min
minimum section (profile) drag coefficient
c l
section lift coefficient
c l,max
maximum section (airfoil) lift coefficient
c l,α
airfoil lift‐curve slope
c m
section moment coefficient about quarter‐chord location
c m,0
section moment coefficient about leading edge
c p
pressure coefficient; specific heat constant (at constant pressure)
C(k)
complex Theodorsen function
c D
wing drag coefficient
images
wing induced drag coefficient
c L
wing lift coefficient
C P
power coefficient
C P,max
maximum power coefficient
C Q
torque coefficient
C T
thrust coefficient
d
spacing between semi‐infinite planar vortex sheets; airfoil camber
dr
incremental width of blade element (or rotor annulus)
dA
incremental disk‐annulus area (2πr · dr )
dA c
wetted area of infinitesimal blade element ( c · dr )
dD
incremental/sectional profile drag force
dF N
incremental/sectional (or blade‐element) normal force – i.e. force normal to local airfoil/section chord line towards upper airfoil/section surface
dF T
incremental/sectional (or blade‐element) tangential force – i.e. force parallel to local airfoil/section chord line towards leading edge of airfoil/section
dL
incremental/sectional lift force
images
incremental mass‐flow rate
dQ
incremental torque
dQ B
blade‐element torque, incremental torque (one blade)
dP
incremental power
dT B
blade‐element thrust, incremental thrust (one blade)
D
rotor diameter; (profile) drag force
D i
induced drag
e
Oswald efficiency factor
f( )
functional relationship
f N,m
elemental rotor/blade force vector (Chapter 7)
F
total loss factor – i.e. product of local root‐ and tip‐loss factor ( F R  · F T )
F( )
objective function (Chapter 8)
F(k)
real part of Theodorsen function
images
airfoil force vector images
Fr
Froude number images
F C
centrifugal force ( mΩ2 R )
F Co
Coriolis force (−2mΩv rel )
F 1
tip correction factor applied to section normal‐/tangential force coefficients (Section 3.4)
F B
Prandtl's approximate loss factor to account for a finite number of blades (Section 3.4)
F P
volumetric body‐force vector (Chapter 7)
F R
root‐loss factor
F T
tip‐loss factor
g
gravitational acceleration; coefficient or function used in tip corrections (Section 3.4)
G(k)
imaginary part of Theodorsen function
H
shape factor of airfoil boundary layer ( δ *)
images
unit vector in the x‐direction
I
turbulence intensity; mass moment of inertia
images
unit vector in the y‐direction
k
integer; shape parameter for Weibull distribution (Chapter 1); reduced frequency (Chapter 5); specific turbulent kinetic energy (Chapter 7)
images
unit vector in the normal/vertical z‐direction
l
turbulent mixing length
L
lift force; Monin–Obukhov length scale (Chapter 1)
Lo
Lock number ( c l,α ρcR 4/I )
m
mass
images
mass flow rate
M 0
pitching moment about leading edge
Ma
(tip) Mach number ( λV 0/a 0 )
n
integer; coordinate normal to surface (element)
images
outer unit normal vector (along contour or control‐volume surface)
p
fluid static pressure
p 0
ambient static pressure
p
freestream static pressure
p(U)
probability density function
P
actuator/rotor/turbine power
images
average wind/turbine power
P Rated
rated wind/turbine power
q s
surface heat flux
Q
rotor torque
r
radial blade coordinate (radial location)
images
marker position vector (Chapter 6)
r
normalized radial blade coordinate ( r/R )
r c
viscous core radius (Chapter 6)
r j
radius of vortex filament j emanating from blade trailing edge in HVM (Chapter 6)
images
initial position vector (or vector to starting point) of vortical trailer in HVM (Chapter 6)
r Root
(blade) root cut‐out radial location
R
blade radius; specific gas constant (air)
Re
Reynolds number
Re c
chord‐based (blade section) Reynolds number ( ρV rel c/μ )
Re D
Reynolds number based on rotor diameter (2ρV 0 R/μ )
s
coordinate tangential to surface (element)
S
wing area
t
time; airfoil thickness (Chapter 4); blade thickness distribution (Chapter 8)
t*
eddy turnover time
T, T(z)
actuator/rotor thrust force; absolute temperature
u
uniform axial (x‐direction) velocity across actuator/rotor disk
u 1
uniform axial (x‐direction) velocity across streamtube exit plane
u i
axial induced velocity (Chapter 6)
u, u(t)
instantaneous wind speed along the x‐direction
u′, u′(t)
fluctuating wind speed along the x‐direction; perturbation velocity in the x‐direction
u*
horizontal velocity scale (friction velocity) in boundary layer
U, U(z)
mean wind speed in the x‐direction (mean value of u(t))
images
average wind speed in the x‐direction (typically taken over a period of 10 minutes or 1 hour)
U e
edge velocity of airfoil boundary layer
U
freestream speed (referring to airfoil flows)
images
fluid‐parcel velocity vector relative to rotating system
images
wind speed (average) at hub height
V In
cut‐in wind speed
V Out
cut‐out wind speed
V Rated
rated wind speed
V rel
(local) inflow/relative velocity
images
marker advection velocity (Chapter 6)
w
fluctuating wind speed along the z‐direction; perturbation velocity in the z‐direction
w*
vertical velocity scale in boundary layer
w i
angular induced velocity (Chapter 6)
w T
downwash in Trefftz plane
w W
downwash at lifting line (or wing)
x
downwind/streamwise coordinate (fixed and rotating axis systems)
x a.c.
chordwise location of airfoil aerodynamic center (measured from leading edge)
x c.p.
chordwise location of airfoil center of pressure (measured from leading edge)
y
lateral (across‐wind) coordinate with respect to vertical axis in fixed axis system; wing‐span coordinate; radial (along blade length) coordinate in rotating axis system
z
vertical coordinate (upwards positive) in fixed axis system
z 0
surface roughness
z i
height of capping inversion; boundary‐layer height/depth

Greek

α
angle of attack – i.e. angle between (local) flow incident on the airfoil/blade and the blade chord line; (wind‐shear) power‐law exponent
images
mean angle of attack
images
time rate‐of‐change of angle of attack
α 0
airfoil zero‐lift angle of attack
α g
wing setting angle (or geometric angle of attack)
α e
effective angle of attack ( α g  + α i )
α i
induced angle of attack
α Stall
deep‐stall angle (of attack)
α W
wing setting angle at mid‐span
β
blade pitch angle – i.e. angle between local chord line and rotor plane ( β Twist  + β 0 )
β 0
collective blade pitch angle ( β Tip  − β Twist (R)) – i.e. the collective blade pitch angle is chosen such that when applied to a built‐in twist, results in the desired blade tip pitch angle.
β Tip
blade tip pitch angle, β(R) – i.e. angle used to describe “pitch setting” of blade
β Twist
built‐in (manufactured) twist
γ
vorticity distribution along airfoil camber line (Chapters 4, 5); rotor/turbine yaw angle (Chapter 5)
γ w
wake vorticity (Chapter 5)
Γ
(bound) circulation on airfoil (and along wing or blade)
Γ B
circulation of rotor with B blades
Γ max
maximum circulation
Γ
circulation of rotor with infinite number of blades
Γ( )
gamma function (Chapter 1)
Γ d
adiabatic lapse rate
δ
boundary‐layer thickness (Chapter 4); relative drag increase (Chapter 6)
δ *
displacement thickness
Δc l
viscous lift‐coefficient correction (Chapter 4)
Δc p
local change/difference in pressure coefficient from upper to lower airfoil surface
Δ grid
grid spacing
Δp
pressure discontinuity/jump at actuator disk
Δt
time step
Δα
amplitude of angle‐of‐attack oscillation; range of angle of attack
δΓ
trailing vorticity
Δδ TE
difference between upper and lower boundary‐layer thickness at airfoil trailing edge ( δ u  − δ l )
ΔΓ
viscous circulation correction (Chapter 4)
ε
specific turbulent energy dissipation rate; Gaussian projection radius (Chapter 7)
η N,m
Gaussian projection function (Chapter 7)
Θ
transformed chordwise coordinate in airfoil frame (Chapter 4); momentum thickness (Chapter 4)
Θ0
potential temperature on the ground (z = 0)
φ
local blade flow angle ( α + β ) – i.e. angle between local flow incident and rotor plane
κ
von Kármán constant; thrust constraint parameter (Chapter 8)
λ
tip speed ratio
λ r
local speed ratio ( r/R · λ )
Λ
Lagrange multiplier (Chapter 8)
μ
air (or fluid) dynamic viscosity
μ t
turbulent eddy viscosity
ν
air (or fluid) kinematic viscosity
Ξ
blade geometry parameter ( λσrc l )
ρ
air (or fluid) density
ρ
freestream air (or fluid) density
σ
rotor solidity (integral of local solidity along blade radius)
σ
local solidity ( Bc/2πr )
σ u
standard deviation of wind speed in the x‐direction
σ v
standard deviation of wind speed in the (across‐wind) y‐direction
σ z
standard deviation of wind speed in the (vertical) z‐direction
τ
shear stress; time constant; characteristic time
τ 0
wall shear stress (on boundary‐layer surface)
images
skin friction (or wall shear stress) on airfoil
images
turbulent shear stress in the x‐direction (normal vector in the z‐direction)
ϕ(k)
phase angle of Theodorsen function
ϕ j
phase angle of initial position vector images (Chapter 6)
ψ
azimuthal (or circumferential) angle – i.e. blade angle in rotor plane with respect to tower axis
ω
wake angular speed (or wake swirl, added wake rotation, Chapter 2); vorticity (Chapter 4); angular frequency (Chapter 5); turbulent energy frequency (Chapter 7)
ω N
natural frequency
images
vorticity vector (images)
Ω
disk/rotor angular speed (or rotor speed); simply‐connected domain (Chapter 4)
images
angular velocity vector
∂Ω
boundary of simply connected domain
images
nabla operator (images)

Subscripts

0
reference condition (upstream or wall/surface); reference angle; reference to airfoil leading edge
1
reference condition (downstream); reference in tip loss correction
farfield/freestream condition; reference to infinite number of blades
normalized quantity in airfoil boundary layer
A
aerodynamic
a. c.
aerodynamic center
B
blade; reference to finite number of blades
Bo
bound
c
chord; core (Chapter 6)
crit
critical
c. p.
center of pressure
C
reference to arbitrary point/location; centrifugal
CO
Coriolis
d
drag; adiabatic
e
effective
D
reference to rotor diameter; drag
fs
fully separated
hub
hub height
He
helix
i
integer; inversion; induced
inv
inviscid
iter
iteration
j
integer
k
integer
l
lift; lower
m
integer; moment
n
integer index used for fourier coefficients
N
integer; normal; natural
opt
optimum
p
pressure; pitching
P
power; reference to arbitrary point/location
r
radial coordinate along blade; reference quantity
rel
relative (at blade section)
rot
rotor entrainment
s
surface
S
small scale
t
turbulent; thickness
T
thrust; tangential; Trefftz
TE
trailing edge
u
reference to wind speed in the (streamwise) x‐direction; upper
U
utility scale
v
reference to wind speed in the (lateral) y‐direction
w
reference to wind speed in the (vertical) z‐direction; wake
W
wing; wake
x
vector component in the x‐direction; streamwise variable
Xtr
chordwise location of laminar‐turbulent transition (measured from leading edge)
y
vector component in the y‐direction
z
vector component in the z‐direction

Superscripts

*
reference to velocity scale in boundary layer
normalized/dimensionless; fluctuating component; per unit length/width; slope (first derivative) of function; perturbation
images
time average
images
normalized
rem
remainder
st
static

About the Companion Website

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www.wiley.com/go/schmitz/wind‐turbines flastg002

The website includes:

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flastg002

XTurb executable & User's manual can be downloaded from:

https://www.rotoraero.psu.edu/xturb‐psu/