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γ r b
F T
r b
Rotor converter
m b
r p
Low-speed shaft
High-speed
shaft
I w
I x
θ
B l
θ
K b
B b
r
l
T l
T r
B h
T g
P,Q
m h
K l
T h
R t
Transformer
θ
θ
K h
g I g
Generator
h
ψ
V
y t
Gearbox
Wind
m n
Nacelle
I r
Rotor
ψ
Grid
β
Wind direction
Pitch
actuator
h
m t
Tower
K t
B t
α
Yaw
actuator
Fig. 14.12 A variable-speed pitch-controlled wind turbine (see [ 2 ])
The Euler-Lagrange method (energy-based approach) is applied to obtain
general mechanical state space model of wind turbine. The main parameters of the
wind turbine model are described in Table 14.1 (see [ 2 ] for more details).
The wind turbine dynamic equations of motion that describe the behavior of the
system, under the influence of external forces (wind), and as a function of time, are
developed as a set of mechanical differential equations. The equations of motion in
Lagrangian mechanics are the Lagrange equations of the second kind, also known
as the Euler-Lagrange equations. Note that E k is used for kinetic energy and E p
for potential energy. D n is the dissipation function to include non-conservative
forces, Q i the conservative generalized forces and q i for the generalized coordi-
nates. Defining L as the Lagrangian function L = E k - E p , the Euler-Lagrange
equation is as follows:
o L
oq i
d
dt
oL
o q i
þ o D n
o q i
¼ Q i
ð 14 : 11 Þ
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