1. analysis of new step-up and step-down direct sysmmetric 18-pulse topologies for aircraft atru

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  • 8/8/2019 1. Analysis of New Step-up and Step-down Direct Sysmmetric 18-Pulse Topologies for Aircraft ATRU

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    This work made use of Engineering Research Center Shared Facilities supported by the National Science Foundation under NSF Award Number EEC-9731677 and the CPES Industry Partnership Program. Any opinions, findings and conclusions or recommendations expressed in this material are those of the

    author(s) and do not necessarily reflect those of the National Science Foundation. This work was conducted with the use of Saber Sketch, donated in kind by

    Synopsis Inc of the CPES Industry Partnership Program.

    Analysis of New Step-up and Step-down Direct

    Symmetric 18-pulse Topologies for Aircraft

    Autotransformer-Rectifier Units

    Alexander Uan-Zo-li, Rolando P. Burgos, Frederic Lacaux, Arman Roshan, Fred Wang and Dushan Boroyevich

    Center for Power Electronics Systems (CPES)

    Department of Electrical and Computer Engineering

    Virginia Polytechnic Institute and State UniversityBlacksburg, VA 24061-0111 USA

    AbstractAmong possible 18-pulse Autotransformer-

    Rectifier-Unit (ATRU) topologies, Direct Symmetric circuit (DS-

    ATRU) demonstrates relatively low complexity, it is insensitive to

    impedance mismatch and distortions of input voltage and has low

    common mode voltage. This paper proposes new step-up and step-

    down Direct Symmetric 18-pulse ATRU topologies for aircraftapplication. Serious study of proposed topologies was performed.

    The authors analyzed the kVA ratings, effects of leakage

    inductance on compliance with input current harmonic

    requirements, power sharing between diode bridges, common

    mode voltage and output ripple. The comparison is carried out for

    the full range of the input line frequency from 400 to 800Hz. Key

    analyses and results obtained with Saber simulations are

    presented for validation of the presented work. Some

    experimental results are shown.

    I. INTRODUCTION

    Today, the More Electric Aircraft (MEA) initiative aims for

    the replacement of Constant Frequency Generators (CFG) by

    variable frequency generators (VFG), which eliminates all thecomplexities associated with the integrated mechanicalfrequency controller of CFG [1], [2]. This approach was

    successfully proven on business jets (Bombardier Global

    Express), airliners (McDonnell Douglas MD-90), and is the

    selected technology for the Airbus A-380 [2], [3]. This in turnhas drastically changed aircraft electric power systems, which

    may now employ either variable frequency AC, DC, or a

    hybrid AC and DC system for power distribution [4], [5] and[6]. Aircraft power electronics have also been affected by this

    trend, as the need for conversion and driving equipment has

    become manifest. A number of static power converters havealready been studied and tested [3], [7], [8], [9], [10] and [11].

    The work on this area however is far from being mature; andnew technologies, structures, and topologies have yet to beestablished.

    Recently, the usage of AC-DC conversion has become a

    common feature upon the aircraft electric power distribution.For constant frequency systems for instance, Transformer

    Rectifier Units (TRUs) are employed to generate low voltage

    DC. For variable frequency systems, the AC-DC conversion isused to generate the DC bus, which supplies power to both

    DC-DC and DC/AC secondary converters. There exist two

    alternative types of AC/DC conversion techniques, the PWMactive front-ends and passive multi-pulse converters.

    Seemingly, the former approach still requires considerable

    development for aircraft applications given the stringent

    operational and reliability goals that must be met. The latter onthe contrary may be readily employed given its sheer

    simplicity and the vast existent knowledge in industry. Also,given that there is no need for isolation, the autotransformers

    have obvious advantages over transformers due to reduced

    kVA ratings, size and weight. Given the stringent requirements

    for the input harmonics and output voltage ripple of theAC/DC equipment, 18-pulse topologies are a natural choice for

    the aircraft application.A number of possible topologies and winding configurations

    were recently proposed [12], [13], [14], [15] and [16]. Among

    possible 18-pulse Autotransformer-Rectifier-Unit (ATRU)

    topologies, Direct Symmetric circuit (DS-ATRU) demonstrates

    relatively low complexity, is insensitive to impedancemismatch and distortions of the input voltage and has lowcommon mode voltage [17]. Due to these reasons, 18-pulse

    DS-ATRU is a logical choice for passive rectification for the

    aircraft application.

    This paper presents new step-up and step-down variations ofDS-ATRU. The proposed circuits are analyzed in order to

    assess the feasibility of employing them in electrical powersystems of aircrafts. Particular attention is given to their correct

    operation at relatively high and variable line frequency. The

    following items are chosen to be analyzed: KVA ratings, input

    harmonic distortion (harmonics and THD), DC voltageregulation, common-mode voltage, impact of impedance

    mismatch between converter paths, impact of harmonic voltagedistortion, and impact of leakage inductance on the operation

    of ATRUs at high frequency.

    II. DIRECT SYMMETRIC TOPOLOGY

    A. Operation of DS-ATRUThe block diagram of DS-ATRU is shown in Fig. 1 and the

    vector diagrams of three consecutive conduction intervals are

    demonstrated in Fig. 2. As can be observed, the

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    autotransformer is used to create two additional 3-phasesystems, one leading the input AC supply voltage by 40

    degrees, the other lagging by 40 degrees, with the amplitudes

    of the created phase voltages equal to the amplitude of the

    supply voltages. The three resultant three-phase systems arethen connected to the diode bridges (it is possible to use

    compensating inductors to counteract the impedance mismatch between conduction paths). The outputs of the rectifiers are

    directly fed to the load. At each moment, there are two bridgesconducting load current, with one rectifier producing positive

    current, and the other negative current. The angle between the

    utilized phase vectors is 160 degrees, so the line-to-line voltage

    used by rectifiers is 14% higher than the line-to-line voltage ofthe input line. In average, each rectifier bridge conducts one

    third of the total output power. Each bridge diode conducts fullload DC current for the duration of 40 degrees.

    AC Supply

    CompensatingInductors

    Autotransformer

    ForwardBridge

    LaggingBridge

    ThroughBridge

    Fig. 1 Block Diagram of DS-ATRU

    Vb

    Va

    Vap

    Vapp

    Vcpp

    Vbp

    Vc

    Vbpp

    Vb

    Va

    Vap

    Vapp

    Vcpp

    Vcp

    Vbp

    Vc

    Vbpp

    Vb

    Va

    Vap

    Vapp

    Vcpp

    Vcp

    Vbp

    Vc

    Fig. 2 Vector diagram of three consecutive conduction intervals

    B. Description of possible winding configurations andtheir comparison

    Fig. 3 shows three winding configurations of the DS-ATRU, accordingly T-Delta [15], Delta [15] and Polygon

    [18]. Fig. 4 demonstrates how each of the winding

    configurations creates three 3-phase systems shifted by 40

    degrees. Table 1 shows the comparison of the windingconfigurations based on autotransformer manufacturability

    (number of unconnected windings per 3-phase

    autotransformer leg) and power rating. It is clear that Deltaand T-Delta configurations offer the lowest possible power

    rating, which translates in smaller physical size of the

    autotransformer. It can be seen that Polygon has the

    smallest number of unconnected windings, whichtranslates in higher manufacturability and potentially the

    lowest leakage.

    Va

    Vap Vapp

    VbpVcpp

    Vb

    Vbpp

    Vc

    Vcp

    Va

    Vap Vapp

    VbpVcpp

    Vb

    Vbpp

    Vc

    Vcp

    VappVap

    VbppVcp

    VbpVcpp

    Va

    VbVc

    Fig. 3 T-Delta, Delta and Polygon winding configurations of DS-ATRU

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    k1

    k2

    VaVb

    Vc

    Vbpp Vap

    Vapp

    Vcpp

    Vbp

    Vcp

    k1

    k2

    VaVb

    Vc

    VbppVap

    Vapp

    Vcpp

    Vbp

    Vcp

    Vc

    Vbpp

    Vb

    Va

    Vap

    Vapp

    Vcpp

    Vcp

    Vbp

    k1

    k2

    Fig. 4 Vector Diagrams of T-ATRU, D-ATRU and P-ATRU windings

    Table 1 Comparison of DS winding configurations

    Parameter of

    Comparison\Winding

    T-

    Delta

    Delta Polygon

    Number of unconnected

    windings per transformerleg [#]

    5 3 2

    kVA Rating [%] 55.4 51.4 83

    C. Variations of Direct Symmetric Topology forincreased and decreased voltage

    In order to satisfy the requirements of the aircraft powersystem, it may become necessary to modify the existing

    topology of DS-ATRU in order to provide lower or highervalue of the output voltage [19]. Fig. 5 shows vector diagrams

    of some of the proposed step-down and step-up variations of

    the DS-ATRU, which are based on the Delta winding

    configuration. It is also possible to show the same variations

    for TS-ATRU. All proposed topologies feature very small

    increase in number of windings, while preserving thesymmetry between the created phases and providing required

    voltage. The main problem with the shown topologies is thatall created phases are at different angle to the input phase. This

    would create additional harmonics due to imbalance in

    impedances. The authors also looked at these topologies with

    more symmetric output vectors. Fig. 6 and Fig. 7 show thesimulated the input currents and the harmonic contents of the

    input current for the step-down Delta DS-ATRU with

    symmetric distribution of the AC vectors and input voltage of231V, 400Hz and 800Hz input line. SaberR Synopsis Simulator

    was used to obtain the simulation results. It can be easily

    noticed that the circuit exhibits the 18-pulse operation withrelatively small harmonic distortion of the input voltage. The

    leakage and parasitic parameters used for the simulation were

    obtained from the analysis of the existing ATRU technologies.

    Vb

    VaD

    Vap

    Vapp

    Vcpp

    Vcp Vbpp

    VbD

    Vbp

    40 40

    Va

    Vc

    VcD

    VaD

    Vapp

    Vapp

    Vcpp

    Vcp

    Vbpp

    VbD Vbp

    40

    40Va

    Vb

    Vc

    VcD

    Fig. 5 Vector Diagrams for step-down and step-up variations of Delta DS-ATRU

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    THD=5 .3%

    Fig. 6 ATRU Input current and its harmonic content at 400Hz, 231V input line

    T H D = 5 . 3 %T H D = 3 . 7 4 %

    Fig. 7 ATRU Input current and its harmonic content at 800Hz, 231V input line

    III. PERFORMANCE EVALUATION

    A serious study of DS-ATRU topologies was performed.

    The authors analyzed the kVA ratings, effects of leakage

    inductance on compliance with input current harmonic

    requirements, power sharing between diode bridges, commonmode voltage and output ripple using Synopsis Saber

    simulations on the switching models of the equipment.

    A. Effects of leakage coupling on the input current distortion

    Because the decreases in voltage with additional winding is

    normally relatively low, the authors studied the influence of

    coupling on the standard ATRU topologies, without the step

    down or step up capability. Fig. 8 shows detailed schematic ofthe winding configuration of the T-Delta DS-ATRU. Thistopology was evaluated by [20], but still some questions

    remained unanswered. In order to carefully analyze the effects

    of coupling, the authors propose to use a fully coupled model

    of the leakage, which takes into account the coupling betweenall leakages of all windings of the same autotransformer core

    leg. Such approach is rather complex, but it allows to observethe influence of all circuit leakage parameters, and provides

    invaluable aid to designers of the autotransformer [21]. Fig. 9

    shows the approach to modeling, for example, of the five

    windings of one autotransformer core leg where each leakageinductance (defined as inductance, which does not create flux

    coupled with windings positioned on the other legs) is coupled

    with all windings on the same leg [22]. Figs. 10-15 show somepreliminary data, demonstrating the effects of coupling of the

    winding of the same leg on the THD of the input current. As

    can be observed, such dependence is far from simple and someeffects were not expected.

    Based on the analysis of the relationship of THD of theATRU input currents and winding leakage coupling, the

    authors came up with the following preliminary conclusions:

    Only couplings of the windings on the same leg areimportant;

    Couplings between Nk1 windings are not important and

    can be ignored;

    Couplings between adjacent Nk1 and Nk2 are notimportant and can be ignored;

    Couplings between opposite windings Nk1 and Nk2 are

    important and must be modeled.

    B. Simulation and Assessment of normal ATRU OperatingConditions

    Figs. 16 and 17 show the harmonic content of the inputcurrent of the step-down D-ATRU supplied by balanced 3-

    phase voltage, 230V, 400Hz and 800Hz accordingly as afunction of output load. As one can see, the harmonics are

    relatively small. Fig. 18 shows the common mode voltage of

    the ATRU as a function of output load for balanced 3-phase

    voltage. Again, the proposed ATRU topology demonstrateslow common mode voltage, being less than 12V at maximum

    output power, while supplied by 230V, 800Hz supply.

    C. Simulation and Assessment of Abnormal ATRUOperating Conditions

    Figs. 19-24 show simulated input current, input voltage,output common mode voltage and output ripple for the cases of

    abnormal operating conditions. The results can be summarizedas follows:

    The step-down D-ATRU presents a minimum common-modevoltage with balanced power supply of 9V at 360 Hz and 3V

    at 800 Hz.

    With 6Vac unbalance, the common mode voltage is 62 V at

    360 Hz and 24 V at 800 Hz

    With 12 Vac unbalance the common mode voltage of the

    step-down D-ATRU is 118V at 360 Hz and 47V at 800 Hz

    The input voltage unbalance together with phase

    displacement introduces the 2nd order voltage and current

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    harmonics and affects the common-mode voltage, whichsurpassed 62V. Voltage modulation introduces current sub-

    harmonics, i.e., harmonics below fundamental frequency (360

    Hz in this case). That leads to low frequency harmonics on the

    DC voltage, i.e., between DC and 2nd order harmonics.Voltage harmonic distortion (5th harmonic injection) increases

    the ATRU input current distortion. Presence of the voltage

    unbalance and voltage modulation generates 3rd and evenorder harmonics of relatively high level. DC offset in the AC

    input voltage supply generates further power unbalance

    between phases. The combined effect of the dc offset,

    harmonic distortion, and phase unbalance and voltagemodulation can saturate the autotransformer core, even though

    a small gap was used to prevent saturation.

    Va

    Vap Vapp

    VbpVcpp

    Vb

    Vbpp

    Vc

    Vcp

    Nk1a

    Nk2a

    Nk1b

    Nk2b

    Np

    Fig. 8 Autotransformer winding configuration

    Rk1

    L NK1B

    L NK1A

    L NK2B

    L N K 2 A

    LNP

    Rk1

    Rk2

    Rk2

    RP

    Fig. 9 Modeling of the autotransformer core winding

    0

    0.01

    0.02

    0.03

    0.04

    0.05

    0.06

    0 0.2 0.4 0.5 0.8 1

    THD

    Fig. 10 THD as a function of the Nk1a-Nk1b

    coupling

    -0.005

    0.005

    0.015

    0.025

    0.035

    0.045

    0.055

    0.065

    0 0.2 0.4 0.5 0.8 1

    THD

    Fig. 11 THD as a function of the Nk2aNk2b

    coupling

    0.03

    0.035

    0.04

    0.045

    0.05

    0 0.2 0.4 0.5 0.8 1

    THD

    Fig. 12 THD as a function of the Nk2Np

    coupling

    -0.01

    0.01

    0.03

    0.05

    0.07

    0 0.2 0.4 0.5 0.8 1

    THD

    Fig. 13 THD as a function of the Nk1Np

    coupling

    0.03

    0.035

    0.04

    0.045

    0.05

    0.055

    0 0.2 0.4 0.5 0.8 1

    THD

    Fig. 14 THD as a function of the Nk1bNk2a

    coupling

    0

    0.02

    0.04

    0.06

    0.08

    0.1

    0.12

    0.14

    0 0.2 0.4 0.5 0.8 1

    THD

    Fig. 15 THD as a function of the Nk1aNk2

    coupling

    I-5I-7

    I-11I-13

    I-17I-19

    I-35I-37

    0%

    25%

    50%

    100%

    200%

    0.00

    0.50

    1.00

    1.50

    2.00

    2.50

    3.00

    3.50

    4.00

    4.50

    5.00

    [%]

    HarmonicOrder

    Load Current [%

    Fig. 16 Harmonic of Input Current as a function of

    output load, balanced supply400Hz, 230V

    I-5I-7

    I-11I-13

    I-17I-19

    I-35I-37

    0%

    25%

    50%

    100%

    200%

    0.00

    0.50

    1.00

    1.50

    2.00

    2.50

    3.00

    3.50

    4.00

    4.50

    5.00

    [%]

    HarmonicOrder

    LoadCurrent [%

    Fig. 17 Harmonic of Input Current as a function of

    output load, balanced supply400Hz, 230V

    0

    2

    4

    6

    8

    10

    12

    14

    0 100 200 300 400 500

    Volts

    Fig. 18 Output common mode voltage of th

    ATRU, balanced supply 400Hz and 800Hz,230Vrms

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    Fig. 19 Input Currents and voltage for 6Vac

    input unbalance

    Fig. 20 Common mode voltage for 6Vac

    input unbalance

    Fig. 21 Output voltage ripple for 6Vac input

    unbalance

    Fig. 22 Input Currents and voltage for 12Vac

    input unbalanceFig. 23 Common mode voltage for 12Vac

    input unbalanceFig. 24 Output voltage ripple for 12Vac

    input unbalance

    IV. EXPERIMENTALRESULTS

    In order to validate the proposed circuits, the authors built ascaled-down prototype of the step-down DS-ATRU with

    symmetric outputs. Figs. 25-27 show the input phase voltages

    Va, Vb and Vc and the created step-down voltages VaD, VbD,

    VcD, as well as the leading the input supply by 40 degreesvoltages Vap, Vbp and Vcp, and lagging by 40 degrees

    voltages Vapp, Vbpp and Vcpp under no load conditions.

    Figs. 28-29 show the voltages Va, VaD, Vap and Vapp under

    load conditions, supplied by 400Hz and 800Hz input line. Figs.30-31 show the currents flowing into the rectifier from the

    voltages VaD, Vap and Vapp, under load conditions when

    ATRU is supplied by 400Hz and 800Hz input line. Lastly,Figs. 32 and 33 show the input current of the ATRU under load

    at 400Hz and 800Hz supply. It can be seen that the ATRU

    demonstrates 18-pulse rectification of the input voltage, whileproviding necessary step-down of the input voltage.

    Fig. 25 Voltages Va, Vad, Vap, Vapp under noload conditions

    Fig. 26 Voltages Vb, VbD Vbp, Vbpp under no

    load conditions

    Fig. 27 Voltages Vb, VbD Vbp, Vbpp under no-

    load conditions

    Fig. 28 Voltages Va, Vad, Vap, Vapp, 400Hz,

    under load

    Fig. 29 Voltages Va, Vad, Vap, Vapp 800Hz,

    under load

    Fig. 30 Currents Iad, Iap, Iapp 400Hz, Voltage

    Va, under load

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    Fig. 31 Currents Iad, Iap, Iapp, Voltage Va,800Hz, under load

    Fig. 32 Currents Ia, Ib, Ic, Voltage Va, 400Hz,under load

    Fig. 33 Currents Ia, Ib, Ic, Voltage Va, 800Hz,under load

    CONCLUSION

    This paper proposes new step-up and step-down Direct

    Symmetric 18-pulse ATRU topologies for aircraft application.

    Also, it includes comparison of different types of the DS-Topologies and detailed analysis of new step-up and step-down

    versions of DS-ATRU. Some key figures and results were

    shown in this paper. The authors analyzed the kVA ratings,effects of leakage inductance on compliance with input current

    harmonic requirements, power sharing between diode bridges,

    common mode voltage and output ripple. The comparison is

    carried out for the full range of the input line frequency from400 to 800Hz. Key analyses and results obtained with Saber

    simulations are presented for validation of the presented work.

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