5_IJPAST-192-V7N1.57224426

Embed Size (px)

Citation preview

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    1/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), pp. 48-58

    InternationalJournal ofPure andAppliedSciences andTechnology

    ISSN 2229 - 6107

    Available online atwww.ijopaasat.in

    Research Paper

    Comparison of DFIG and Synchronous Machine for

    Storage Hydro-Power Generation

    Mahdi Johar1,*

    , Ahmad Radan2, Mohammad Reza Miveh

    3and Sohrab Mirsaeidi

    4

    1, 2 Electrical Engineering Department of K.N. Toosi University of Technology3, 4

    Department of Electrical Engineering, Komijan Branch, Islamic Azad University, Komijan, Iran* Corresponding author, e-mail: ([email protected])

    (Received: 28-7-11; Accepted: 3-10-11)

    Abstract: Among the alternative methods for energy storage , using the potentialenergy of water stored in different heights has been considered by human for ages.

    Storage pumping plants have been invented for this purpose and are considered as

    one of the most reliable and effective methods of storing the electrical energy.

    Factors such as having appropriate static and dynamic stability, high efficiency,

    suitable steady state and transient performance, the least cost of manufacturing,

    utilities and etc. can play a major role in choosing the type of machines for energy-

    making. Therefore, advantages and capabilities of variable speed storage -pumping

    plants, compared with conventional synchronous ones, have drawn into

    consideration in this paper. Different viewpoints such as structure and steady state

    behavior are focused for comparing the application of Doubly Fed Induction

    Generators (DFIG) and synchronous ones in storage hydro plants. Dynamic

    stimulations are also used to evaluate the performance of variable-speed versus

    synchronous fixed-speed generation units.

    Keywords: DFIG, Synchronous Machine, Power Generation, Simulation

    1. Introduction:

    Main Developing quick responded energy storing systems is indispensable according tothe expansion of power network and the problems of its stability control consecutively.One of the well-known energy storage systems in networks is Pumped storage powerplants. Producing energy in pumped storage power plant is possible in two ways of fixedand adjustable speed. The usage of optimum operating points of system in recent times

    has made the production of electrical energy by adjustable speed systems more important.DFIG is one of the adjustable speed systems which has many advantages compared to

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    2/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 49

    other systems and became more considerable than synchronous generator in pumpedstorage power plant in late 1980s. Many works have been done on variable speedpumped storage generators and numerous papers have been published on modeling [1,2],dynamic response[1,3,4,5] , control methods [6,7,8], electronic converters [9,10,11], andspeed drive [2,12] of DFIG in pumped storage power plants but comparison between

    synchronous machine and DFIG in pumped storage power plants has never beenperformed up to now. Using DFIG systems comparing synchronous ones increases theusage efficiency and flexibility significantly. Nowadays using DFIG generators instead ofsynchronous ones is an efficient way to solve the problem of efficiency drop from pumpedmode to generator mode due to significant reduction of frequency converter capacity.After this section, a history of variable speed pumped storage power plants, an evaluationof DFIG modeling, and finally a structural and steady state behavior comparison betweenthe two machines are given respectively and the results are presented.

    2. History of variable speed pump-storage power plants

    Unlike conventional pump-storage units, variable speed pump-storage units do not have along history which is because of their dependency on high power transformers. Design ofsuch systems was evaluated theoretically in 1970 for the first time. The first variablespeed storage hydro-power generator was installed at Narude power plant, Japan with acapacity of 22 MVA in 1987 The motor-generator had a cylindrical rotor with a 3-phasedwounded rotor. The 11 KV windings of its rotor had to tolerate a large amount ofcentrifugal force which was a lot more than what small motors had to use for pump-storage motor-generators. Today usage of rotating machines is conventional usingadvanced technology in rotor turns especially in materials and manufacturing. Table 1shows installed samples of variable speed pump-storage generators around the world.

    3. Principles and Modeling of DFIG:

    DFIG is the generator which is fed by both stator and rotor terminals. In other words dualfeed induction generators are called DFIG. The DFIG configuration is shown in Figure 1and consists of the stator directly connected to the grid while the rotor circuit with itsvariable voltage and frequency requires a back-to-back converter for the grid connection.The converter allows the active power flow in two directions: from the grid to the rotor insub-synchronous operation and from the rotor to the grid in over-synchronous mode.

    Table 1: variable speed pump-storage generators around the world [3]

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    3/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 50

    Fig. 1: DFIG electric configuration [2]

    DFIG is recommended in variable speed systems with a limited range of speed to 0 030 ofsynchronous speed. Depending on the poles of the machine the rotor speed is defined asfollows:

    1 2

    1

    ,

    .m

    m R

    p

    =

    =

    (1)Where, p1 and R are the number of pole pairs and the mechanical rotor speed,

    respectively.In comparison with fixed speed synchronous machines which are used in pumped storageunits, DFIG has below advantages: Possibility of operation in high efficiency especially in partial load (about 2%) Capability of control and separation of active and reactive power Capability of power factor control Quicker system response Reduction of the number of starts4. DFIG Models:

    4.1. DFIG Electrical Model:

    The model of the machine, in transient and steady states, is established in a general d-qrotating reference Frame Equivalent circuit and main equations describing a DFIGbehavior are illustrated as follow:

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    4/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 51

    Voltage equations:

    ' ' ' ' '

    ' ' ' ' '

    ' ' ' '

    ,

    ,

    ,

    ( ) ,

    ( ) ,

    qs s qs ds q s

    ds s ds qs d s

    os s os o s

    qr r qr r dr qr

    q r r dr r qr dr

    or r or or

    dv r i

    d t

    d

    v r i d t

    dv r i

    d t

    dv r i

    d t

    dv r i

    d t

    d

    v r i d t

    = + +

    = + +

    = +

    = + +

    = +

    = +

    (2)

    Where, is defined as follows:

    ' ''

    '' '

    '' '

    0 000 0

    0000

    0 000

    0 00 00

    000 0

    0 0 0 0

    os osls

    ds dsmls m

    qs qsmls m

    or or l r

    m lr mdr dr

    m lr mqr qr

    iL

    iLL L

    iLL L

    iL

    L L L i

    L L L i

    + + = + +

    (3)Active and reactive equations:

    3( ),

    23 3

    ( ) ( )2 2

    s ds qs qs ds

    qs ds ds qs ds ds q s q s

    P i i

    Q s V i v i i i

    =

    = = +

    (4)

    4.2. DFIG Mechanical Model:

    The equation of Rotor rotation is obtained from equalizing inertial torque and acceleratingtorque.

    ( )( )

    ,

    / 1

    2

    m

    em m ech dam p

    r b

    em m ech dam p

    dJ T T T

    d t

    dT T T

    d t H

    =

    = (5)

    Where emT , mechT , dampT are electromagnetic torque, external mechanical torque and

    damping torque respectively and H is defined as follows:

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    5/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 52

    2

    2bm

    b

    JH

    S

    = (6)

    5. Structural Comparison of DFIG with conventional synchronous ones:

    Respect to dimensions and structures, a general comparison between mentioned machines arepresented here (Figure 2).

    Fig. 2: a general comparison between mentioned machines [13]

    Fixed speed synchronous machine has equal stator and rotor rotational speed offields and a DC excitation system which is located on the rotor. Power electronicequipment is located on the rotor side. The speed is a function of the number of polesand the frequency of the electrical system. The synchronous machine has a salient pole

    rotor as shown in Figure 3.

    Fig. 3: salient pole rotor in synchronous machine[13]

    The design of DFIG is identical to wound rotor induction machine with the difference thatoutput power from DFIG can be increased from about 30MVA up to 50MVA by somemodifications. DFIG has a cylindrical pole and a wounded rotor as shown in Figure 4. Thespeed is a function of the number of poles and the frequency of the electrical system.Power electronic equipment is located on the rotor side.

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    6/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 53

    Fig. 4: round pole rotor in DFIG [13]

    Stator of synchronous machine and DFIG are the same. The main difference between

    synchronous machine and DFIG is the structure of their rotor as shown in figure 5.

    Fig. 5:Comparison between rotors in synchronous machine and DFIG [13]

    Excitation system of DFIG possesses high-voltage and large current AC field whileexcitation system of SG possesses low voltage and low current DC field.The rotor design of two mentioned machines are quite different and consists of some partssuch as winding design, slip ring, retaining system, winding overhang, rotor rim, coolingsystem and retaining end winding.Between DFIG and salient pole machines with the same power and speed, DFIGpossesses larger dimensions and inertia and smaller air gap. Since the flux must spreaduniformly on rotor surface of DFIG its structure is uniform, cylindrical and laminated.A comparison of diameter, length, number of conductors and turns and volume of copperused in rotor winding with the same specification is done here. This specification is givenas below:

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    7/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 54

    Table 2: Machine specification

    Type AW710L8X8RB

    Rated output(KW ) 500

    Frequency(cps) 50 cps

    Rated voltage(V) 6600 V

    Rated speed(rpm) 744 rpm

    Power factor 0.8

    Stator circuitry Star

    Rotor circuitry delta

    6. DFIG and synchronous machine common specifications:

    Designing values are 34000=ac , 67.0=av

    B , 955.0=w

    K and 8=P , D and L are as

    follows:

    Table 3: Length and diameter in SM and DFIG

    type Synchronous DFIG

    D(m) 1.25 1.4

    L(m) 0.73 0.63

    As a result the volume of DFIG is 307.0 m more than the volume of synchronous machinewhich is true because this machine has a 3-phase rotor.

    Table 4: Volume in SM and DFIG

    type Synchronous DFIG

    Volume(m3) 0.89 0

    The differences in the number of conductors, the number of rotor turns and the volume ofcopper used in rotor windings are shown below:

    Table 5: Number of conductors, Number of turns per phase and Volume of copper in SM and

    DFIGType Synchronous DFIG

    Number of conductors 232 480

    Number of turns per phase 116 80

    Volume of copper(cm3) 8346 15347

    The number of rotor turns of a single phased synchronous machine is equal to 116 and thenumber of conductors is equal to 232 since each turn consists of two conductors. But in aDFIG machine the number of turns considering its 3-phased rotor is equal to 240 and the

    number of conductors is equal to 480. In addition, the surface area of rotor turns of aDFIG machine is 6 mm2 more than a synchronous one due to having a higher voltage

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    8/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 55

    (because of using AC and DC) and working in 3-phased condition. This results show thatthe volume of used copper in rotor turns of a DFIG machine is 2101 cm3 more andconsecutively its volume is 0.07 m2 more than a synchronous machine. Therefore in anequal specification a DFIG machine is slightly bigger than a synchronous one.

    7. Comparison of DFIG and synchronous machine steady stateoperations:

    For evaluating steady state behavior of a DFIG and a synchronous machine differentworking points in usage area are chosen in our simulation which delivers one belowconditions:

    Equal stator output power and power ratioIt should be mentioned that transmitted power of a DFIG to network is equal to

    sum of the stator output power and rotor input power, while transmitted power of asynchronous machine to network is equal to the stator output power.

    7.1. Equal stator output power and power ratio:

    In this paragraph at first the stator output power and the power ratio of DFIG machine areassumed to be equal to those of synchronous machine and then the stator and the rotorcurrents will be compared in order to study the steady state behavior of them according tothe outcome of simulations and calculations and after that the input power of the rotorwill be evaluated. It should be noted that only the results of the calculations are presentedhere.Pre-defined values of the stator output power and the power ratio are as 1.6 MW and 0.8,

    respectively.According to these values, the results of simulations and calculations of DFIG andsynchronous machine are as follows:

    (a) (b)

    Fig. 6: Stator current in equal stator output power and power ratio (a) synchronousmachine (b) DFIG.

    Table (6) stator current in equal stator output power and power ratio

    Is calculation simulation

    synchronous 1673.2 1658.8

    DFIG 1673.2 1658.8

    As it is shown in Figure 6 for equal stator output and power ratio, stator current of DFIGand synchronous machine in steady state can be assumed equal with a very good accuracy.

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    9/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 56

    (a) (b)Fig.7: Rotor current in equal stator output power and power ratio (a) Synchronous

    machine (b) DFIG.Table 7: The results of simulation and calculation of rotor current in equal stator output

    power and power ratio

    Ir,If calculation simulation

    synchronous 5235.5 5233

    DFIG 2063.5 2092.3

    As it is shown above, in an equivalent condition rotor effective current in DFIG machine is

    less comparing with synchronous machine which is because of the smaller gap in DFIG

    machine and consecutively less maximum flux density on teeth comparing with synchronous

    machine. It should be mentioned that in table (3) excitation current of synchronous machine

    in rotor reference is DC and rotor current of DFIG machine is AC which is transmitted to

    stator (effective value is presented). Considering the transformation ratio the difference in

    rotor current will be about 500A.

    (a) (b)

    Fig. 8: The results of simulation and calculation of rotor active power in equal stator output

    power and power ratio (a) Synchronous machine (b) DFIG machine.

    Table 8: rotor active power in equal stator output power and power ratio

    Ir,If calculation simulation

    synchronous -4319 -4321

    DFIG 4.424e4 4.434e4

    As it is shown in figure (8), whereas rotor circuit in DFIG machine produces some additional

    power and transmits it to transmission network according to the results of the simulation it

    produces 44.24 KW of extra active power while 4.319 KW of active power is wasted in

    synchronous machine.

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    10/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 57

    (a) (b)

    Fig. 9: Active power transmitted to network in equal stator output power and power ratio (a)

    Synchronous machine (b) DFIG machine.

    Table 9: Active power transmitted to network in equal stator output power and power ratio

    Qg calculation simulation

    synchronous 1.2e6 1.199e6

    DFIG 1.322e6 1.325e6

    (a) (b)

    Fig. 10: transmission of reactive power to network in equal stator output power and power

    ratio (a) Synchronous machine (b) DFIG machine.

    Table 10: Reactive power transmitted to network in equal stator output power and power

    ratio

    Qg calculation simulation

    synchronous 1.2e6 1.199e6

    DFIG 1.322e6 1.325e6

    If we relinquish wasted power in rotor of synchronous machine due to its small amount thetransmitted active power to network (Pg) will be equal to stator active output power (Ps)

    while in DFIG machine transmitted active power to network (Pg) will be equal to the sum ofstator and rotor active power (Ps + Pr). If so for equal stator output power, DFIG machine candefinitely transmit more active and also reactive power even with less rotor current incomparison with synchronous machine.So we can manufacture DFIG machine in smaller dimension and less cost which leads tocondone larger size of DFIG machine in comparison with synchronous machine in equalcondition that concluded in design paragraph.

    8. Conclusion:

    Application of variable speed generation using DFIG in pump storage hydro power plants isstudied in this paper. Comparing to conventional applications with fixed-speed synchronous

  • 7/31/2019 5_IJPAST-192-V7N1.57224426

    11/11

    Int. J. Pure Appl. Sci. Technol., 7(1) (2011), 48-58. 58

    machine having the same stator, the paper concludes that, in viewpoint of structure, the DFIGmachine should have a slightly bigger volume because of 3 phased rotor with AC currents.Regarding the steady state performances of both machines, the results show that DFIG candeliver more active and reactive power to network with less rotor current because of the extrapower delivered by the rotor. . DFIG machine can therefore be manufactured in smaller

    dimension with less cost for the same needed power. The ability of faster response to networkdemand for active and reactive powers in case of DFIG is also a remarkable advantage whichcan be utilized for enhancing the network stability under perturbations.

    References

    [1] Y. Pannatier, C. Nicolet, B. Kawkabani, J. J. Simond and Ph. Allenbakh, Dynamic behaviorof a 2 variable speed pump-turbine power plant, International Conference on Electrical

    Machines, ICEM 2008, September 6-9, 2008, Vilamoura, Portugal.[2] Franois BONNET, Luc LOWINSKY, Maria PIETRZAK-DAVID and Paul-tienne VIDAL,

    Doubly fed induction machine speed drive for hydro-electric power station, Toulouse Cedex7, France, EPE 2007 - Aalborg.

    [3] J. K. Lung, Y. Lu, W. L. Hung and W. S. Kao, Modeling and dynamic simulation of doublyfed adjustable speed pumped storage units,IEEE Transactions on Energy Conversion, 22 (2)(June 2007).

    [4] T. Kuwabara, A. Shibuya and H. Furuta, Design and dynamic response characteristics of400MW adjustable speed pumped storage unit for ohkawachi power, IEEE Transaction on

    Energy Conversion, 11 (2) (Jun 1996).[5] N. Chayawatto, E. Ortjohbann and S. Chatratana, Dynamic behaviour of doubly fed induction

    machine with generator-side converter under abnormal condition, Sustainable Energy andEnvironment (SEE), 2004.

    [6] Y. S. Lai, Machine modeling and universal controller for vector-controlled inductionmotor drives,IEEE Trans. Energy Convers, 18 (1) (Mar. 2003), 2332.

    [7] N.P. Quang, A. Dittrich and A. Thieme, Doubly-fed induction machine asgenerator:control algorithms with decoupling of torque and power factor, Electrical

    Engineering, 80 (1997), 325-335.[8] F. Blaschke, The principle of field orientation as applied to the new TRANSVECTOR closed

    loop control system for rotating field machines, Siemens Rev., 34 (1972), 217220.[9] R. Pena, J.C. Clare and G.M. Asher, Doubly fed induction generator using back-to-back

    PWM converters and its application to variable-speed wind-energy generation, IEEProc.-Electr. Power Appl., 143 (3) (1996), 231-241.

    [10] A. Sapin, A. Hodder, J.J. Simond and D. Schafer, Doubly-fed asynchronous machine with -level VSI for variable speed pump storage,ICEM2000.

    [11] S. Furuya et al, Successful achievement in a variable speed pumped storage powersystem at YAGISAWA power plant,IEEE Con. Power Conversion, Yokohama 1993.

    [12] A. Boquel and J. Janning, Analysis of a 300 MW variable speed drive for pump-storage plantapplications,EPE 2005, Dresden.

    [13] A. Schwery, E. Fass, J.M. Henry, W. Bach and A. Mirzaian, Pump storage power plant:ALSTOM's long experience and technological innovation(www.ALSTOM.com).