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Accepted Manuscript
Title: Comparison of maximum peak power trackingalgorithms for a small wind turbine
Author: R. Kot M. Rolak M. Malinowski
PII: S0378-4754(13)00065-7DOI: http://dx.doi.org/doi:10.1016/j.matcom.2013.03.010Reference: MATCOM 3922
To appear in: Mathematics and Computers in Simulation
Received date: 1-11-2011Revised date: 30-1-2013Accepted date: 7-3-2013
Please cite this article as: R. Kot, M. Rolak, Comparison of maximum peak powertracking algorithms for a small wind turbine, Mathematics and Computers in Simulation(2013), http://dx.doi.org/10.1016/j.matcom.2013.03.010
This is a PDF file of an unedited manuscript that has been accepted for publication.As a service to our customers we are providing this early version of the manuscript.The manuscript will undergo copyediting, typesetting, and review of the resulting proofbefore it is published in its final form. Please note that during the production processerrors may be discovered which could affect the content, and all legal disclaimers thatapply to the journal pertain.
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Comparison of maximum peak power tracking algorithms for a small wind turbine
R. Kot, M. Rolak, M. Malinowski
Warsaw University of Technology, ul. Koszykowa 75, 00-662 Warsaw, Poland.
e-mail: [email protected], [email protected], [email protected]
Abstract – This paper reviews Maximum Power Point Tracking (MPPT) algorithms dedicated for
Small Wind Turbines (SWT). Many control strategies with different features are available and it is
very important to select proper one in order to achieve best performance and low cost. Three most
widely used algorithms are discussed. Two are based on turbine static parameters such as power
versus rotational speed characteristic Pm(ω) and optimum tip-speed ratio λopt. Third one, which
seems to be most promising, iteratively searches for optimum operating point and it doesn’t
require prior knowledge of the turbine. This work attempts to summarize and compare these
algorithms. Detailed description of each one is made with most significant qualities emphasized.
Discussion is supported by the simulation studies using Synopsys Saber software. Results for
5 kW SWT with diode rectifier and DC/DC boost converter are shown and commented.
Keywords – Maximum Power Point Tracking (MPPT), Small Wind Turbine (SWT), PMSG.
1. Introduction
Wind turbines are one of the most important and promising Renewable Energy Sources (RES), largely
contributing in world’s energy production. European wind power industry has formulated generation targets of
180GW, and 300GW in 2020 and 2030 respectively [10,16]. Due to huge improvement in power converter
control and technology wind energy, especially in the form of Small Wind Turbines (SWT), becomes more and
more available for individual customers. SWT is defined as a wind turbine with a rotor swept area less than
200m2 and rated power range of 1-15kW (residential) and 15-100kW (light commercial) [1]. Such turbines are
able to supply households or small companies as well as to support electrical grids on the low voltage side.
Poland with its 1 GW capacity and current 53% growth rate predicts 8,6 GW to be installed by 2020 [17].
However, considering SWTs, only 6 MW capacity is installed and 550 MW is expected to be deployed by the
same time. Hence, a significant development is assumed in the next few years. This work paper covers the 5 kW
wind energy system currently being developed (Fig. 1), [14]. It consist of three blade horizontal axis wind
turbine (HAWT), low-speed permanent magnet synchronous generator (PMSG), AC/DC/AC converter and the
energy storage module with Dual Active Bridge (DAB) DC/DC converter. AC/DC converter is controlled by
Maximum Power Point Tracking (MPPT) algorithm in order to ensure efficient energy conversion for various
atmospheric conditions. Paper focuses on different MPPT methods implemented for a particular AC/DC
converter configuration (diode bridge rectifier with DC/DC boost converter).
Fig. 1.Considered wind energy system
Manuscript
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2. Wind power basics
Power generated by the wind turbine is proportional to the area swept by its blades and the third power of the
wind velocity,
pm CVRP 32
2
1 (1)
where:
R: turbine rotor radius (m)
ρ: air density (kg/m3)
Cp: turbine power coefficient (-)
V: wind speed (m/s)
Power coefficient Cp is defined as the ratio between mechanical power Pm and power available from the wind Pw
:
w
m
P
PpC
(2)
Theoretically, value of Cp cannot exceed the limit expressed by Betz’ Law as follows[2,11]:
593.027
16max pC (3)
Power coefficient itself is not constant and strongly depends on the linear speed of the turbine blade tip and wind
speed. Ratio between these two quantities is called the tip-speed ratio and used as the important parameter in
wind turbine design:
V
R (4)
where:
ω: turbine rotational speed
Power coefficient changes also with turbine rotor blade pitch angle. Thus, it can be written that:
),( pp CC (5)
However, small wind turbines usually have fixed pitch mainly due to reduced cost and simplified maintenance.
Therefore:
.0 const (6)
Typical CP(λ) curve is presented in Fig. 2. For certain tip-speed ratio value, Cp is maximized. Based on this
curve, the actual turbine output power can be calculated as a function of its rotational speed for different wind
speeds. As a result the power versus rotational speed characteristic Pm(ω) is created as shown in Fig. 3. It can be
noticed that for every wind speed exist single point for which the amount of generated power is the highest. The
red curve connecting these points sets the range of desirable operating points. It is convenient to control the
turbine rotational speed to maintain the operation point as close as possible to the peak power curve. At very
high wind speeds, when the generated power exceeds the nominal power of the plant, the surplus of captured
energy has to be either stored or dissipated. Above the critical wind speed the turbine has to be stopped to avoid
damaging the system. On the other hand, for very light breeze turbine operation is not justified economically.
Referring to Fig. 2 and Fig. 3 it is worth mentioning that the efficiency of the wind turbine system has to be
taken into account. The product of wind turbine power coefficient, generator efficiency and power converter
efficiency gives the total efficiency of the system. Note that usually value of Cp contains also the aerodynamic
efficiency of the rotor.
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0 2 4 6 8 10 12 140
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45
0.5
Cp
Fig. 2. Power coefficient versus tip-speed ratio
Power delivered to the load Pe is then equal to:
cgpe CVRP 32
2
1 (7)
where:
ηg: generator efficiency
ηc: converter efficiency
In general, efficiency of the gearbox interconnecting the turbine and the generator should be included in (7).
However, discussed system consist of 5 kW multi-pole, low speed generator. Thus, gearbox is not required.
During the design process one of the most important factor is the energy yield in long time scale, that is, how
much energy can potentially be captured for a given turbine design and location. Fig. 4 presents the predicted
energy yield for 5 kW SWT as a function of wind speed. System efficiency, i.e. effective energy capture, is also
presented. The plot is based on the Rayleigh distribution of wind speed. It shows that for lighter and more
frequent winds, energy capture is smaller but the efficiency of the system is much higher than in the case of
stronger but very rare winds. It means that designing the turbine for lower wind speed is actually much more
reasonable in terms of energy gain. Long-term average wind speed in Poland varies from 5.5 to 7 m/s at 50 m
height and 3.5÷4.5 m/s at 30 m. The blue field in Fig. 4 represents the region of interest being the trade off
between the amount of captured energy per year and efficiency.
0 5 10 15 20 25 30 35 400
2000
4000
6000
8000
10000
12000
14000
16000
[rad/s]
Pm
[W
]
v = 5 m/s
v = 10 m/s
v = 9 m/s
v = 11 m/s
v = 4 m/s
v = 6 m/s
v = 7 m/s
v = 8 m/s
Typical Designed
Fig. 3. Mechanical power versus turbine rotational speed characteristic (typical: red dashed line, especially
designed for low wind speeds: red solid line)
2.5 3.0 3.5 4.0 4.5 5.0 5.5 6.0
ŚREDNIA DŁUGOTERMINOWA PRĘDKOŚĆ WIATRU V[m/s]
0
2000
4000
6000
8000
10000
12000
14000
16000
18000
20000
WY
DA
JN
OŚ
Ć E
NE
RG
ET
YC
ZN
A [
kW
h/r
ok]
20
30
40
SP
RA
WN
OŚ
Ć E
NE
RG
ET
YC
ZN
A [%
]
region of interest
en
erg
y y
ield
[kW
h/y
ea
r]
eff
icie
ncy [%
]
high powerfrequent winds
long-term mean wind speed [m/s] Fig. 4. SWT energy yield and system efficiency versus long-term average wind speed
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3. MPPT algorithms
Power produced by a wind turbine strongly depends on wind speed and rotor rotational speed, as was shown
in Section 2. In order to extract maximum energy, the generator rotational speed has to be controlled accordingly
by means of AC/DC converter with MPPT algorithm. There are many different MPPT types, but two basic
groups are most common. First of them requires prior knowledge of turbine parameters to calculate the operating
point. Algorithms from second group iteratively search the optimum with the use of power and rotational speed
increments. Fig. 5 presents more detailed subdivision of these methods, which differ in implementation and type
of required sensors. However, principle of operation remains the same.
In this paper a DC/DC boost converter supplied by three phase diode rectifier is used to control the
turbine/generator rotational speed. Converter plays the role of an apparent load for the generator. It can be shown
that the equivalent resistance Req seen from the input terminal of a boost converter with load resistance R is given
as:
2)1( DRReq (8)
It means that changing duty cycle of the boost converter results in change of generator load and therefore its
rotational speed.
3.1. MPPT algorithms based on Pm(ω)
Algorithms based on knowledge of Pm(ω) characteristics are well known and widely used [3,9,15]. Block
diagram of this method is presented in Fig. 6. Peak power curve for desired power range (Fig. 3) is stored in a
microcontroller memory or approximated by a polynomial function. To calculate the optimum operation point
measurement of either the power or rotational speed is required.
MPPT
algorithms
· knowledge of
Pm(ω)
characteristic
· power and
rotational speed
measurement
with rotational
speed control
with power
control
· knowldge of λopt
· wind speed and
generator
rotational speed
measurement
based on
iterative search
With outer generator
rotaional speed
control loop:
· power and
rotational speed
measurement
With duty cycle as
direct refernce:
· power
measurement
based on
knowledge of
turbine
parameters
data required
[8-9]
[11-12][10]
[13-16] [10]
Fig. 5. Classification of MPPT algorithms
PMSG
iL
UdcUd
io
PI
pd = ud∙iL
-
udiL
iL*ω* D*ωPI
-
++
-
+
Fig. 6 Control scheme for Pm(ω) characteristic based MPPT.
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Based on the measurement and stored data the reference value (power or rotational speed) is determined. Main
advantage of this method is its simplicity and fast response. Assuming precise data, algorithm immediately finds
optimum operation point. Unfortunately, accurate determination of optimum Pm(ω) curve is unavoidably
connected with aerodynamic tests using wind tunnel, which in practice is omitted due to the high cost. Moreover,
it may vary significantly with time and atmospheric conditions. Factors like icing, dirt and aging are the cause of
decrease in turbine rotor efficiency and cannot be compensated by the control algorithm.
In this paper PMSG rotational speed has been chosen as a control variable. The optimum power curve was
generated by taking a vector of maximum power points existing in assumed wind speed range. It was then
approximated by the third order polynomial with the help of Matlab/Simulnik curve fitting functions. Actual
values of the polynomial result only from particular wind turbine model parameters.
01
2
2
3
3
* aPaPaPa eee (9)
where:
a0 - a3: polynomial coefficients
ω*: reference speed of the generator
Based on the power measurement the reference speed is calculated and compared to actual generator speed.
Resulting error is then used to calculate the reference value for inductor current iL*. Hence, current controller
determines the adequate duty cycle D* for boost converter.
3.2. MPPT algorithms based on λopt
Similar method, based on wind speed measurement, is shown in Fig. 7, [5,12]. In this case, according to
Fig.2, knowledge of optimum tip-speed ratio λopt is required in order to calculate the reference generator
rotational speed:
R
Vopt *
(10)
PMSG
V
ω
iL
UdcUd
io
PI
-iL*ω* D*
PI-
++-
+
iL
Fig. 7 Control scheme for λopt based MPPT
Despite the determination of ω*, algorithm remains unchanged comparing to one described in Section 3.1.
Nevertheless, there are some important features, which need to be addressed. First, using wind speed as input
variable allows for fast operating point determination and dynamic response. On the other hand, data acquisition
from anemometer has to be insensitive to rapid wind gusts to eliminate unwanted changes in operating point. It
should be pointed that inertia of the turbine is generally one order of magnitude higher that the one of the
generator. Thus, even with strong gust of wind turbine power variation is slow . Sudden change in operating
point, set by control algorithm, may cause high torque difference resulting in mechanical stress on the turbine
rotor blades. Moreover, the use of anemometer increases overall cost and complexity of the system. As in the
case of previous MPPT algorithm λopt cannot be determined with high degree of accuracy and varies with time
and atmospheric conditions . However, λopt is a single parameter and it can be adjusted much more easily than
polynomial coefficients in optimum power curve approximation.
3.3. Incremental MPPT algorithms
Output power can be maximized without any information of turbine parameters by iteratively changing the
control variable which results in generator rotational speed adjustment [4,6-7,9,13]. Although the steepest ascent
method is generally used for this purpose, all algorithms of this type are based on the assumption that for a given
wind velocity maximum power is produced when:
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0
eP
(11)
It can be proven that for a boost converter condition (11) is also satisfied by [9]:
0
D
Pe (12)
Thus, this particular method requires only power measurement. Flowchart the algorithm is presented in Fig. 8.
Power is continuously sampled and increment ΔP is calculated after each cycle. In order to reach condition (12),
the actual derivative sign has to be evaluated. Therefore individual signs of the power SP and duty cycle SD
increments are determined to get information about power change and the last search direction, respectively
(Table I, Fig. 9). Step size K is often constant, although variable step size can be used for tracking performance
improvement. It should be mentioned that algorithm operates constantly and as a result, oscillations around the
optimum are unavoidable. To minimize the unwanted changes due to small power variations, hysteresis was
introduced.
This class of algorithms allows to minimize the number of sensors. There is no dependency on specific type
of turbine or its rated power. A key role in implementation plays proper selection of the step size K. Higher value
of K accelerates the tracking process but results also in larger oscillations about the optimum operating point.
.
PMSG
iL
UdcUd
io
pd = ud∙iLiL
D*
-
+
ud
ΔP(k)=P(k)-P(k-1)
Sd = Sign(ΔD(k-1))
D*(k) = D*(k-1)
D*(k) = D*(k-1) + ΔD(k)
D*(k-1) = D*(k)
ΔD(k-1) = ΔD(k)
P(k-1) = P(k)
Yes
ΔD(k) = K∙Sd∙Sp
Sp = Sign(ΔP(k))
ΔP(k)≤ Hist
No
fT
Fig. 8. Control scheme for incremental MPPT algorithm
Table I. Operation principle of the incremental MPPT algorithm
calculated condition result from previous change required action
SD SP eq. (11) eq. (12) D ω
-1 1 0
eP
0
D
Pe ↑ ↓
1 -1
-1 -1 0
eP
0
D
Pe ↓ ↑
1 1
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0
P0
P
0
D
P0
D
P
Fig. 9. Possible conditions for incremental MPPT algorithm
Another important issue is the proper selection of sampling frequency fT. Too high may effect in false selection
of tracking direction. Wind turbine with its rotor inertia represents the dominant time constant of the system and
creates a low-pass filtering action for rapid wind speed changes. This results in relatively low MPPT sampling
frequency fT required for stable power tracking. Obviously, with too low frequency algorithm will not be able to
track the wind changes with adequate precision, decreasing the efficiency of the system. For the purpose of this
study fT of 10 Hz was chosen.
4. Model description
In order to verify and compare presented algorithms the simulation studies were provided using Synopsys
Saber software. Full model configuration is presented in Fig. 10. MPPT algorithms were implemented using
MAST language with its syntax and instruction set very similar to C.
4.1. Wind turbine
Wind turbine model was based on the real three-blade, HAWT design. It converts the wind speed to a
mechanical torque as follows:
32 )(2
1VCR
PT
pm
m (13)
here: ρ = 1.225 kg/m3, R = 3.75 m
The power coefficient as a function of tip-speed ratio can be generally represented by the exponential function
with coefficients selected to fit given turbine parameters. For the purpose of this scope, Matlab wind turbine
model was selected and adjusted accordingly. It was assumed that λopt= 8
4.2. Generator
The 5 kW axial flux PMSG model was created. With 20 pole pairs the nominal rotational speed is 150 rpm.
Detailed parameters are shown in Table II.
Table II. PMSG simulation model parameters
Parameter Value
Rated power 5 kW
Moment of inertia 6 kgm2
d-axis inductance 10 mH
q-axis inductance 10 mH
Damping constant 0.002 kgm2/ s
Rated speed 150 rpm (15.7 rad/s)
Number of pole pairs 20
PM flux linkage 1.07 Wb
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4.3. Converter
The AC/DC converter consists of six-pulse diode bridge rectifier and DC/DC boost converter Considering
maximum ripple in inductor current and capacitor voltages the inductance and capacitances for the converter
were selected using eq. (15-17) accordingly [8]:
Fig. 10. Simulation model (Synopsys Saber)
s
IonIL
Lf
DV
L
tVI (14)
1
16 Cf
IV
g
LC
(15)
s
OonOC
fC
DI
C
tIV
22
2 (16)
where:
C1: boost converter input capacitor value
C2: boost converter output capacitor value
fg: frequency of the generator phase voltage
IL: inductor current
IO: output current
L: boost converter inductor value
VI: boost converter input voltage
Converter parameters are summarized in Table III. The value of inductor, which is the most expensive part of the
converter, can be easily adjusted with respect to nominal generator voltage and switching frequency as shown in
Fig. 11.
5. Simulation results and comparative study
All three MPPT algorithms have been implemented in Saber software and tested for the same wind speed and
load conditions. Results are presented in Fig. 12. It can be seen that every MPPT algorithm works properly, i.e.
successfully tracks the optimum power point. Dynamic response for algorithms based on Pm(ω) and λopt is
similar. In comparison, the incremental algorithm is slower but it is not too important due to high inertia of the
turbine.
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VI [V] fs [Hz]
Δi
[%]
L=10 mH
L=5 mH
Fig. 11. Inductor current ripples ΔiL as a function of switching frequency fs and input voltage VI for different
values of inductance: 5 mH, 10 mH.
Table III. Boost converter simulation model parameters
Parameter Value
L 12 mH
C1 400 uF
C2 400 uF
fs 10 kHz
Fig. 12. Comparison of discussed MPPT algorithms: based on Pm(ω) (orange), based on λopt (black), incremental
(blue); from the top: reference wind speed, turbine rotational speed, turbine power
6. Conclusion
In this paper a description and comparison of Maximum Power Point Tracking (MPPT) algorithms has been
presented. All most important features are summarized in Table IV. Control schemes requiring turbine
parameters are fast and simple in implementation, but their application is limited to specific turbine designs.
Algorithm based on incremental search of optimum operating point seems to be most promising due to
elimination of wind and rotational speed measurements which ensures low cost and flexibility. Computational
effort is comparable for all methods. There are, however, slight differences in signal filtering and algorithm
tuning requirements.
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Table IV. Summary and comparison of described MPPT algorithms
Feature based on Pm(ω)
characteristic
based on λopt and wind
speed measurement incremental
Efficiency depends on accurate
approximation of Pm(ω)
depends on accurate
determination of λopt
depends on proper
adjustment of K and fT
Flexibility
very low: unique for a single
turbine / periodic adjustments
required
low: unique for a single
turbine / periodic
adjustments required
high: self-adjusting /
continuous oscillations
around operating point
Complexity very high: approximation of
Pm(ω) required
high: knowledge of λopt
required
low: no prior knowledge of
turbine parameters required
Dynamics very fast very fast slow
Price
high: PMSG rotational speed
and power measurement
required
very high: wind speed and
PMSG rotational speed
measurement required
low: only power
measurement required
Computation
complexity
low: PMSG rotational speed
and ud filtering required (for
power calculation)
low: PMSG rotational speed
and wind speed filtering
required
very low: only ud filtering
required (for power
calculation); no PI controllers
Acknowledgment
Described problems are part of the research project No. N R01 0015 06/2009 “Complex solution for low speed
small wind turbine with energy storage module for distributed generation systems”, sponsored by The National
Centre for Research and Development.
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