A New Control Method of Permanent Magnet Generator for Maximum Power Tracking in Wind Turbine Application

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  • 8/3/2019 A New Control Method of Permanent Magnet Generator for Maximum Power Tracking in Wind Turbine Application

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    Abstract This paper discusses a new and simple control

    method for maximum power tracking in a variable speed wind

    turbine by using a step-up dc-dc converter. The output voltage of

    permanent magnet generator is connected to a fixed dc-link

    through a three-phase rectifier and the dc-dc converter. A

    maximum power-tracking algorithm calculates the speed

    command that corresponds to maximum power output of the

    turbine. The dc-dc converter uses this speed command to control

    the output power of the permanent magnet generator, such thatthe speed of generator tracks the command speed. A current

    regulated PWM voltage source inverter maintains the output

    voltage of dc-dc converter at a fixed value by balancing the input

    and output power to the dc-link. In addition, the inverter can

    improve power factor and inject a current with very low

    harmonic distortion into the utility grid. The generating system

    has potentials of high efficiency, good flexibility, and low cost.

    Index Termsdc-dc converter, Maximum power tracking,

    Permanent magnet generator, PWM inverter, Speed control,

    Variable speed wind turbine.

    I. INTRODUCTIONaximized electricity generation by wind turbines is aninteresting topic in electrical engineering and manytypes of variable speed generating systems have been

    researched to achieve this goal. Use of a variable speedgenerating system in wind power application can increase thecaptured power from wind. In fact, the system based onpermanent magnet generator (PMG) is one of the mostfavorable and reliable methods of power generation.However, electricity generated directly by PMG has variableamplitude and frequency, requiring additional conditioning tomeet the amplitude and frequency requirements of the utilitygrid and/or conventional loads. Many types of power

    electronic converters were introduced to find an appropriateand inexpensive solutions to the problems of electricityconditioning and the results are promising [1][2][5].

    The use of the variable speed PMG in wind turbine

    application can increase the energy capture from wind,

    resolve other problems such as noise, and improve efficiency.

    For example, in a wind turbine system if a gearbox is used,

    noise, power losses, additional cost, and potential of

    mechanical failure can cause problems. The use of a variable

    speed PMG could solve these problems [8].

    In a variable speed PMG system, a vector control approach is

    often employed to achieve nearly decoupled active and

    reactive power control on the supply side power converter,

    which is a current regulated voltage source inverter. In this

    way, the power converter maintains the dc-link voltage and

    improves power factor of the system [4][5][9]. Different

    control methods for maximum power tracking in variable

    speed wind turbine generators have been discussed in

    [5][6][7].

    This study presents a new control approach and the related

    power converter topology to track the maximum power

    without measuring wind or generator speed, which is of great

    importance for small size and low cost wind turbines. Using

    PSIM software simulation, the circuit topology and control

    method of the wind power generating system is investigated

    with a PMG and a back-to-back ac-dc-ac power converter.

    Also included in the investigation is the wind turbines

    dynamics.

    The paper is organized as follows: in section IIaerodynamic characteristics of turbine and principles of

    maximum power tracking method are explained. Systemconfiguration, circuit topology, and power converters arediscussed in section III. In section IV simulation results arepresented to confirm that the control method for speed controland capturing maximum power from wind works properly.Section V summarizes the advantages of the overall systemand gives some final remarks.

    II. WIND TURBINE

    A. Wind Turbine Aerodynamic Characteristics

    The amount of mechanical power captured from wind by awind turbine could be formulated as [3]:

    3

    Pm vAC21P = (1)

    where, : air density (Kg/m3)

    A : swept area (m2)

    CP: power coefficient of the wind turbineV : wind speed (m/s)

    Therefore, if the air density, swept area, and wind speed areconstant the output power of the turbine will be a function ofpower coefficient of the turbine. In addition, the wind turbineis normally characterized by its CP-TSR curve; where, TSR,tip-speed ratio, is given by:

    A New Control Method of Permanent MagnetGenerator for Maximum Power Tracking in

    Wind Turbine ApplicationR. Esmaili, Student Member, IEEE, and L. Xu, Fellow, IEEEand D. K. Nichols, Member, IEEE

    M

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    v

    RTSR = (2)

    In (2), , R, and v are the turbine rotor speed in rad/s,

    radius of the turbine blade in m, and wind speed in m/s,

    respectively. Fig.1 shows a typical CP-TSR curve for a wind

    turbine.

    Fig. 1. Power coefficient versus tip-speed ratio.

    As can be seen from Fig.1, at TSRopt CP has its maximumvalue which results in the optimum efficiency; therefore,maximum power is captured from wind by the wind turbine.

    Fig. 2 illustrates the output power of a wind turbine versusrotor speed while speed of wind is changed from v1 to v3(v3>v2>v1). As can be seen from Fig. 2, for example, if thespeed of wind is v1 the maximum power could be captured

    when the rotor speed is 1; in other words, the operating pointof the system is Point A which corresponds to the maximumoutput power. If wind speed changes from v1 to v2 while the

    rotor speed is fixed at 1, the operating point of system isPoint B which does not correspond to maximum power

    tracking. The rotor speed should be increased from 1 to2which results in the maximum power at operating point C.

    Fig. 2. Output power versus rotor speed for three different wind speeds.

    Based on (2) and Fig.1, the optimum speed of rotor can beestimated as follows:

    opt

    optopt

    optTSRRv

    RTSRv == (3)

    Unfortunately, measuring the wind speed in the rotor ofturbine is very difficult; so, to avoid using wind speed, (1)needs to be revised. By substituting the wind speed equivalentfrom (3) into (1), the output power of the turbine is given asfollows:

    3

    opt

    opt

    PmTSR

    RAC

    2

    1P

    = (4)

    Finally, the target torque can be written as follows:2

    optopttarget kT = (5)

    where:

    3

    opt

    PMaxoptTSR

    RAC

    2

    1k

    =

    B. Maximum Power Tracking Algorithm

    This algorithm includes several steps, which are:

    1. Choose the initial reference rotor speed and measured theoutput power of the generator;

    2. Increase or decrease the reference rotor speed by one stepand measure the output power again;

    3. Calculate Sign(P) and Sign();4.ref(n)= ref(n-1)+ Sign(P) Sign() step ;5. Repeat from step 3 to reach to optimum operating point.

    Fig. 3 is used to make this algorithm clearer. Let us assumethe speed of wind is v1 and operating point of the turbine ispoint A, represented as (A, PA) in P- characteristic curve.Also, let us assume that the turbine speed is increased by step,which results in a new speed B.The new operating point willbe (B, PB) which gives:

    stepBref

    AB

    AB

    sign

    PsignPPP

    +=

    =>=

    =>=

    1)(0

    1)(0

    After the first iteration, the new operating point becomes (C,PC). The iterative process will continue till the operating pointof the system is found at (1, P1), corresponding to themaximum power for the wind speed of v1. If the wind speedchanges to v3, the new operating point will be searchedstarting at (D, PD) which results in:

    steprefD

    D

    sign

    PsignPPP

    +=

    ===

    =>=1

    1

    1

    1)(0

    1)(0

    The next point will be (E, PE) and similarly this process willcontinue in the same manner as explained, till the finaloperating point is found at (3, P3), corresponding to themaximum power capture for the wind speed of v3. Now, if thewind velocity changes to v2, the operating point will move to(F, PF) that result in:

    stepBref

    F

    F

    sign

    PsignPPP

    =

    ===

    =

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    Fig. 3. Adjustment of turbine operating point for maximum power tracking.

    III. POWER ELECTRONICS AND CONTROL STRATEGY

    A. Circuit Topology

    Fig. 4 shows the proposed circuit topology for wind powergeneration system, which is used, to realize the aboveprinciples of maximum winding power capture. This systemincludes a wind turbine (WT), a permanent magnet generator(PMG), a three-phase diode rectifier bridge, a step-up dc-dc

    converter, and a current regulated PWM voltage sourceinverter (CRPWM).

    Fig. 4. Topology of wind power generation system.

    The system has the following features: a). PMG has highperformance, higher efficiency, no exciting current, smaller insize, and less in weight in comparison to other types ofgenerators; b). The generated ac power from PMG is

    converted to dc power through a diode bridge which is simple,robust, cheap and requires no control circuit; and c). Only onepower switching device is used in dc-dc converter, resulting inlow cost and simple control. In the following sections powerconverters and their control methods are discussed.

    B. DC-DC converter and control algorithm

    The basic structure and control topology of the boostconverter is shown in Fig. 5. This converter divides the dc-link into two levels: dc-link voltage at the output terminals ofthe diode rectifier, which is a variable dc voltage, and the dc-link voltage at the input terminals of the voltage sourceinverter, which is fed from a fixed dc voltage. By varying theswitch duty cycle of the DC-DC converter the output voltageof the generator-rectifier system can be controlled. Thepurpose of this circuit is to control the shaft speed of thePMG so that the maximum power can be captured from windby the turbine.

    iL

    idc

    ref

    L

    +

    -

    Sdc+

    -

    -+PI

    -+

    PI

    iC

    C

    m

    Vdc

    Fig. 5. Power circuit and control topology of the dc-dc converter.

    The state equation that describes the DC-DC boostconverter is given by (6), where Sdc is the switch status thattakes the value of 1 or 0.

    +

    =

    dc

    in

    dc

    L

    dc

    dc

    dc

    L

    i

    V

    C

    L

    V

    i

    C

    S

    L

    S

    dt

    dV

    dt

    di

    10

    01

    01

    10

    (6)

    C. Active and Reactive Power in Rotating Reference Frame

    Fig.6 shows the vector representation of a balanced three-phase system and their equivalent vectors in a rotating d-qreference frame.

    Fig. 6. Definition of rotating reference frame.

    The variables in ABC system can be transformed to arotating d-q reference frame by using a time-varyingtransformation given in

    ( )

    ( )

    2

    1

    2

    1

    2

    1

    3

    2sin

    3

    2sinsin

    3

    2cos

    3

    2coscos

    3

    2

    +

    =

    T (7)

    f

    f

    f

    T

    f

    f

    f

    C

    B

    A

    o

    q

    d

    =

    (8)

    =

    =

    o

    q

    d

    C

    B

    A

    T-

    ff

    f

    Tff

    f

    TT

    11

    2

    3(9)

    where the variables f can be define as a set of voltages orcurrents in the system. Also, in a balanced three-phasesystem always fo, called zero sequence component, is equal tozero. The instantaneous power in a three-phase system isgiven by:

    [ ]

    =++=

    C

    B

    A

    CBACCBBAA

    i

    i

    i

    VVViViViVP(t) (10)

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    Using the transformation matrix and substituting the voltageand current vectors from (9) into (10) results in:

    ( )qqdd iViVP +=2

    3 (11)

    From Fig. 6, the rotating reference frame is chosen in sucha way that: Vq=0 and Vd=|V|, so the equation of active powercan be simplified in the rotating reference frame as

    diVP

    2

    3= (12)

    In a similar way, the equation of reactive power in therotating reference frame can be calculated as

    qiVQ2

    3= (13)

    D. Supply Side Converter Control Strategy

    Fig.7 shows a simplified representation of the supply side

    converter which includes a dc-side capacitor, a 3-phase PWM

    inverter, and series impedances which interface the output of

    the inverter to the utility grid.

    Fig. 7. Supply-side converter arrangement.

    The voltage equations in Fig.7 can be written by using

    KVL law as:

    +

    =

    CC

    BB

    AA

    S

    C

    B

    A

    S

    S

    C

    B

    A

    Ve

    Ve

    Ve

    Li

    i

    i

    L

    R

    i

    i

    i

    p1

    100

    010

    001

    (14)

    where: p=d/dt

    Transforming the voltage equations into the synchronous

    reference frame by using the transformation matrix results in:

    +

    =

    q

    d

    q

    d

    S

    S

    S

    S

    q

    d

    e

    Ve

    Li

    i

    L

    R-

    L

    R

    i

    ip

    1 (15)

    To provide decoupled control of active power, or id,and

    reactive power, or iq, base on (15), the output voltage from the

    inverter in the synchronous reference frame should beV)i(xLe qSd += 1 (16)

    )i(xLe dSq += 2 (17)

    By substituting (16) & (17) into (15), the decoupled equations

    of the system can be rewritten as follows:

    +

    =

    2

    1

    0

    0

    x

    x

    i

    i

    L

    R

    L

    R

    i

    ip

    q

    d

    S

    S

    S

    S

    q

    d (18)

    As can be seen from (12) and (13) the active and reactive

    power could be controlled through id and iq, respectively.

    Therefore, the control rules of (16) and (17) can be completed

    through defining the current feedback loops as follows:

    ( )d*d iis

    kkx

    += 211 (19)

    ( )q*q iisk

    kx

    += 212 (20)

    Fig.8 shows the control block diagram of supply side

    inverter based on the vector-control algorithm.

    Fig. 8. Schematic of control strategy for supply side inverter.

    IV. SIMULATION RESULTS

    To check the proposed algorithm in Section III for speed

    control of PMG, a dynamic simulation is implemented using

    PSIM software when the wind speed was changed. There are

    two sets of simulation results which are to be explained in the

    following sections. Table I shows the parameters of the PMG

    used in simulation.

    TABLE I

    PERMANENT MAGNET GENERATOR PARAMETERS

    Rated Power Output 20kW

    Rated Speed 211r/min

    Stator Connection winding Star

    Number of Rotor poles 36

    Stator Phase Resistor 0.1764

    Synchronous Inductance 4.24mH

    Rated Phase Current 35A

    Rated Phase Voltage 205V

    A. Speed Control of PMG

    In this case the reference turbine speed of the generator is

    the command signal to prepare a switching pattern for the

    DC-DC boost converter. Fig.9-d shows speed-tracking

    characteristic of the generator when the reference command

    turbine signal increases linearly from 80 to 120 r/min and

    again from 120 to 200 r/min and finally decreases linearly

    from 200 to 160 r/min, assuming the wind speed has changed.

    As can be seen from Fig. 9-a and b, by controlling the input

    current to the DC/DC boost converter the output voltage of

    generator-rectifier system could be controlled so that

    generators shaft follows the speed command.

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    As shown in Fig.4 a current regulated PWM voltage

    source inverter is used to interface the dc-link bus to utility

    grid. This inverter can maintain the voltage of dc-link at a

    constant voltage. As shown in Fig.9-c the dc-link voltage is

    adjusted at 810 volts in this system. Furthermore, it can

    improve power factor and reduce current harmonic distortion.

    As can be seen from Fig.10, power factor of the system is

    adjusted to almost unity power factor and total harmonic

    distortion of injected current is less than 3%.

    Fig. 9. Turbine speed tracking.

    B. Maximum Power Tracking

    The simulation program uses the typical wind turbine

    characteristics that are shown in Fig. 11. As revealed by the

    graphs, the optimum operating points of the turbine are(175r/min, 10kW), (188r/min, 15kW), and (203r/min, 20kW)

    for three different wind speeds.

    In this simulation the algorithm iteration period and step are

    chosen 1 second and 2 r/min, respectively. As can be seen

    from Fig. 12 the generator speed starts from zero and reaches

    to 1752 r/min, related to the maximum output power of

    10kW for the turbine at the wind speed of v1. In 20 seconds it

    is assumed that the wind speed increases to v3; therefore, the

    control system changes the required turbine speed by using

    the maximum power tracking algorithm to capture the

    maximum power from wind in this speed. As can be seen

    from Fig. 12 the speed of PMG (or turbine shaft) is adjusted

    to 2032 r/min that generates 20kW power. After 42 seconds

    from the beginning the wind speed decreases to v2 from v3.

    Consequently, the reference turbine speed will be decreased

    by the control system. Fig.12 shows speed of the PMG is

    adjusted to 1882 r/min in 10 seconds. As a result, the output

    power of turbine is 15kW.

    Fig. 10. Grid phase voltage and Phase current of PWM inverter

    Fig. 11. Turbine characteristics used for simulation.

    FIG. 12. OUT PUT POWER AND ROTOR SPEED OF PMG.

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    Fig.13 Simulation results showing maximum power

    tracking.

    Fig. 13. Tracking the maximum power by wind turbine.

    V. CONCLUSION

    This paper presents a power electronic converter structureand related simple speed control method that can be used to

    implement maximum power tracking in wind turbine

    application. The proposed system and control algorithm

    reduces the cost of the system, because there is just one

    switching device in the dc-dc converter. Also no copper loss

    in rotor circuit in PMG ensures higher efficiency.

    Additionally, independent control of active and reactive

    power on the power grid side is possible. Simulation results

    confirm that control algorithm works well to track the

    maximum power for different wind speeds.

    At present, a prototype system including a 10kW Bergey

    wind turbine, a three-phase 40kW Powerx inverter, a 10 kWstep-up dc-dc converter and digital controller to be

    implemented on TMS320F2812-DSP platform are planned at

    Dolan Technology Center. The preparation of prototype and

    laboratory testing of PMG based wind turbine is in progress

    and the final testing results are to be reported.

    VI. REFERENCES

    [1] Z. Chen and E. Spooner,Wind turbine power converters: a comparative

    study, in Proc. 1998 IEE Power Electronics and Variable Speed Drives,

    Seventh International Conference, pp. 471 476.

    [2] Z. Chen and E. Spooner, A modular, permanent magnet generator for

    variable speed wind turbines, in Proc. 1995 IEE Electrical Machines

    and Drives, Seventh International Conference, pp. 453 457.

    [3] E. Muljadi, S. Drouilhet, R. Holz, and V. Gevorgian, Analysis of

    permanent magnet generator for wind power battery charging, in Proc.

    1996 IEEE Industry Applications Conference, pp. 541 548.

    [4] Y. Tang and L. Xu, flexible active and reactive power control strategy for

    a variable speed constant frequency generating system, in Proc. 1993

    IEEE Power Electronics Specialists Conference , pp.568 573.

    [5] S. Song, S. Kang, and N. Hahm, Implementation and control of grid

    connected AC-DC-AC power converter for variable speed wind energy

    conversion system, in Proc. 2003 IEEE Applied Power Electronics

    Conference and Exposition, pp.154 - 158 vol.1

    [6] F. Martinez Rodrigo, J. M. Ruiz Gonzalez, J. A. Dominguez Vazquez,

    and L. C. Herrero de Lucas, Sensorless control of a squirrel cage

    induction generator to track the peak power in a wind turbine, in Proc.

    2002 IEEE Industrial Electronics Society Conference, pp.169 - 174 vol.1.

    [7] R. Datta and V. T. Ranganathan, A method of tracking the peak power

    points for a variable speed wind energy conversion system,

    IEEE Trans. Energy Conversion,vol.18, pp.163 168, Mar. 2003.

    [8] Y. Higuchi,N. Yamamura, M. Ishida, and T. Hori, An improvement of

    performance for small-scaled wind power generating system with

    permanent magnet type synchronous generator, in Proc. 2000 IEEE

    Industrial Electronics Society Conference , pp.1037-1043 vol.2.

    [9] C. Schauder and H. Mehta, Vector analysis and control of advanced static

    VAr compensators, in Proc. 1993 IEE Generation, Transmission and

    Distribution Conference, pp.299-306, vol.140.

    VII. BIOGRAPHIES

    Reza Esmaili (S05) received his B.S. and M.S.

    degrees from Isfahan University of Technology,

    Isfahan, Iran, in 1993 and 1996 both are in Electrical

    Engineering. He is currently pursuing the Ph.D.

    degree in the Department of Electrical Engineering at

    the Ohio State University, Columbus, OH. From 1997

    to 2000, he was faculty member of school of

    engineering at Isfahan University, Isfahan, Iran. Since

    2001, he has been an Intern Engineer at Dolan

    Technology Center of American Electric Power. His research interest includes

    design and control of power converters for variable speed generating and drive

    systems, wind turbine, and supercapacitor application. Mr. Esmaili is a student

    member of IEEE.

    Longya Xu (S89-M90-SM93-F04) receivedhis M.S. and Ph.D. degrees from the University of

    Wisconsin, Madison, in 1986 and 1990 both are in

    Electrical Engineering. He joined the Department of

    Electrical Engineering at the Ohio State University in

    1990, where he is presently a Professor. He has served

    as a consultant to many industry companies including

    Raytheon Co., US Wind Power Co., General Motor,

    Ford and Unique Mobility Inc. for various industrial

    concerns.

    Dr. Xu received the 1990 First Prize Paper Award in the Industry Drive

    Committee, IEEE/IAS. In 1991, Dr. Xu won a Research Initiation Award from

    National Science Foundation. Dr. Xu is also a recipient of 1995 and 1999

    Lumley ResearchAward for his understanding research accomplishments fromCollege of Engineering, The Ohio State University.

    Dr. Xus research and teaching interests include dynamic modeling andoptimized design of electrical machines and power converters for variable speed

    generating and drive system, application of advanced control theory and digital

    signal processor for controlling of motion and distributed power systems in

    super-high speed operation.

    Dr. Xu is an IEEE fellow and served as the chairman of Electric Machine

    Committee of IEEE/IAS and an Associate Editor of IEEE Transactions on

    Power Electronics in the past several years.

    David K. Nichols holds a BSEE degree from Akron

    University. He began work at American Electric Power in

    1972. He transferred to the Electrical Laboratory in 1976

    and is currently manager of AEPs Technology Solutions

    Management Section at the Dolan Technology Center in

    Groveport, Ohio. A specialist in high-voltage electrical

    and mechanical equipment, Nichols oversees research anddevelopment projects, including several distributed

    resource and energy storage projects. Nichols is a member

    of IEEE.