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ECE 8830 - Electric Drives

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Title: Microelectromechanical Devices Author: Ankineedu Maganti Last modified by: Pritpal Singh Created Date: 8/4/2003 1:49:55 AM Document presentation format – PowerPoint PPT presentation

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Title: ECE 8830 - Electric Drives


1
ECE 8830 - Electric Drives
Topic 10 Cycloconverters
Spring 2004
2
Introduction
  • Cycloconverters directly convert ac signals of
    one frequency (usually line frequency) to ac
    signals of variable frequency. These variable
    frequency ac signals can then be used to directly
    control the speed of ac motors.
  • Thyristor-based cycloconverters are typically
    used in low speed, high power (multi-MW)
    applications for driving induction and wound
    field synchronous motors.

3
Phase-Controlled Cycloconverters
  • The basic principle of cycloconversion is
    illustrated by the single phase-to-single phase
    converter shown below.

4
Phase-Controlled Cycloconverters (contd)
  • A positive center-tap thyristor converter is
    connected in anti-parallel with a negative
    converter of the same type. This allows
    current/voltage of either polarity to be
    controlled in the load.
  • The waveforms are shown on the next slide.

5
Phase-Controlled Cycloconverters (contd)

6
Phase-Controlled Cycloconverters (contd)
  • An integral half-cycle output wave is created
    which has a fundamental frequency f0(1/n) fi
    where n is the number of input half-cycles per
    half-cycle of the output. The thyristor firing
    angle can be set to control the fundamental
    component of the output signal. Step-up frequency
    conversion can be achieved by alternately
    switching high frequency switching devices (e.g.
    IGBTs, instead of thyristors) between positive
    and negative limits at high frequency to generate
    carrier-frequency modulated output.

7
Phase-Controlled Cycloconverters (contd)
  • 3? to single phase conversion can be achieved
    using either of the dual converter circuit
    topologies shown below

8
Phase-Controlled Cycloconverters (contd)
  • A Thevenin equivalent circuit for the dual
    converter is shown below

9
Phase-Controlled Cycloconverters (contd)
  • The input and output voltages are adjusted to
    be equal and the load current can flow in either
    direction. Thus,
  • where Vd0 is the dc output voltage of each
    converter at zero firing angle and ?p and ?N are
    the input and output firing angles. For a 3?
    half-wave converter Vd0 0.675VL and Vd0
    1.35VL for the bridge converter (VL is the rms
    line voltage).

10
Phase-Controlled Cycloconverters (contd)
  • Voltage-tracking between the input and output
    voltages is achieved by setting the sum of the
    firing angles to ?. Positive or negative voltage
    polarity can be achieved as shown below

11
Phase-Controlled Cycloconverters (contd)
  • A 3? to 3? cycloconverter can be implemented
    using 18 thyristors as shown below

12
Phase-Controlled Cycloconverters (contd)
  • Each phase group functions as a dual converter
    but the firing angle of each group is modulated
    sinusoidally with 2?/3 phase angle shift -gt 3?
    balanced voltage at the motor terminal. An
    inter-group reactor (IGR) is connected to each
    phase to restrict circulating current.

13
Phase-Controlled Cycloconverters (contd)
  • An output phase wave is achieved by sinusoidal
    modulation of the thyristor firing angles.

14
Phase-Controlled Cycloconverters (contd)
  • A variable voltage, variable frequency motor
    drive signal can be achieved by adjusting the
    modulation depth and output frequency of the
    converter.
  • The synthesized output voltage wave contains
    complex harmonics which can be adequately
    filtered out by the machines leakage inductance.

15
Phase-Controlled Cycloconverters (contd)
  • A 3? to 3? bridge cycloconverter (widely used
    in multi-MW applications) can be implemented
    using 36 thyristors as shown below

16
Phase-Controlled Cycloconverters (contd)
  • The output phase voltage v0 can be written as
  • where V0 is the rms output voltage and ?0 is
    the output angular frequency. We can also write
  • where the modulation factor, mf is given by

17
Phase-Controlled Cycloconverters (contd)
  • From these equations, we can write
  • and
  • Thus for zero output voltage, mf0 and
  • ?P ?N ?/2. For max. phase voltage,
  • mf1 gt ?P0, ?N ?. See below figure
  • for ?P and ?N values for mf0.5 and 1.

18
Phase-Controlled Cycloconverters (contd)
  • The phase group of a cycloconverter can be
    operated in two modes
  • 1) Circulating current mode
  • 2) Non-circulating current (blocking) mode
  • In the circulating current mode, the current
    continuously circulates between the ve and -ve
    converters. Although the fundamental output
    voltage waves of the individual converters are
    equal, the harmonics will cause potential
    difference which will result in short-circuits
    without an IGR.

19
Phase-Controlled Cycloconverters (contd)
  • The equivalent circuit of a phase group with
    an IGR is shown below.
  • The inclusion of an IGR leads to self-induced
    circulating current as illustrated in the next
    slide.

20
Phase-Controlled Cycloconverters (contd)

21
Phase-Controlled Cycloconverters (contd)
  • At t0, ve load current is taken by the ve
    converter only (iPi0).
  • From 0-gt?/2, rising ve load current will
    create a ve voltage drop (vLLdi0/dt) in the
    primary winding of the IGR. This creates a -ve
    voltage drop in the secondary winding of the IGR
    -gt DN reverse biased. ? no current flow in
    the -ve converter.
  • At ?/2, i0 peaks at Im-gt vL0. After this vL
    tends to reverse polarity inducing current in the
    -ve converter. Voltage across IGR becomes clamped
    to 0 -gt self-induced circulation current between
    ve and -ve converters.

22
Phase-Controlled Cycloconverters (contd)
  • The ve and -ve converter currents can be
    expressed as
  • The self-induced circulating current is simply
    iP-iN.
  • In practice, the waves will not be pure sine
    waves but include a ripple current. Practical
    waveforms are shown on the next slide.

23
Phase-Controlled Cycloconverters (contd)

24
Phase-Controlled Cycloconverters (contd)
  • Advantages of circulating current mode of
    operation, over blocking mode include
  • Output phase voltage wave has lower harmonic
    content than in blocking mode.
  • Output frequency range is higher.
  • Control is simple.
  • Disadvantages
  • Bulky IGR increases cost and losses.
  • Circulating current increases losses in
    thyristors.
  • Over-design increases cost.

25
Phase-Controlled Cycloconverters (contd)
  • In the blocking mode of operation, no IGR is
    used and only one converter is conducting at any
    time.
  • Zero current crossing detection can be used to
    select ve or -ve converter conduction as shown
    below

26
Phase-Controlled Cycloconverters (contd)
  • Since the cycloconverter is usually connected
    directly to a motor, the harmonics from the
    converter will induce torque pulsations and
    machine heating resulting in increased machine
    losses. Also, since the cycloconverter is
    essentially a matrix of switches without energy
    storage (neglecting IGR) PinPout . Thus
    distortions in the output voltage waveform
    reflect back into the line input. See text for a
    discussion of the load voltage and line
    harmonics.

27
Phase-Controlled Cycloconverters (contd)
  • A major disadvantage of cycloconverters is
    poor DPF (displacement power factor). To
    calculate DPF, consider a phase group of an
    18-thyristor cycloconverter shown below.

28
Phase-Controlled Cycloconverters (contd)
  • Assume the ve converter is operating in
    continuous conduction and is connected to a high
    inductance load and assume that the
    cycloconverter is operating at low frequency.
    Segments of the output current and voltage waves
    are as shown below

29
Phase-Controlled Cycloconverters (contd)
  • The Fourier series of the line current is given
    by
  • where i0 is the load current and ? is the
    supply frequency. The current wave has a dc
    component and a fundamental component with a
    lagging phase angle, ?P.

30
Phase-Controlled Cycloconverters (contd)
  • Since the supplys active and reactive power
    components are contributed only by the
    fundamental current, the instantaneous active Pi
    and reactive power Qi for the positive converter
    is given by
  • where Vs rms line voltage.

31
Phase-Controlled Cycloconverters (contd)
  • These equations can be rewritten as
  • If the firing angle is constant, the converter
    acts as a rectifier and VdVd0cos?P and i0Id.
  • In a cycloconverter ?P and i0 vary
    sinusoidally and so Pi and Qi are also
    modulated. We need to average these parameters to
    determine loading on the source.

32
Phase-Controlled Cycloconverters (contd)

33
Phase-Controlled Cycloconverters (contd)
  • The expression for the average reactive power
    contributed by the line, Qi, is given by
  • where ? load power factor angle.
  • Performing the integration above yields
  • where P0, Q0 are the real and reactive output
    power per phase, respectively.

34
Phase-Controlled Cycloconverters (contd)
  • P0 and Q0 are given by
  • and
  • Since the real output power real input
    power, we can write
  • The input DPF can be expressed as
  • DPF cos?i

35
Phase-Controlled Cycloconverters (contd)
  • ? DPF
  • where tan? Q0/Pi (Q0/P0)

36
Phase-Controlled Cycloconverters (contd)
  • This equation for DPF applies when additional
    phase groups are added or if a 36-thyristor
    implementation is considered.
  • mf1 was assumed in this derivation. For
    mf ?1
  • The maximum value of line DPF is 0.843.

37
Phase-Controlled Cycloconverters (contd)
  • See Bose text pp. 180-184 for methods to
    improve DPF.

38
Phase-Controlled Cycloconverters (contd)
  • The control of a cycloconverter is very
    complex. A typical variable speed constant
    frequency (VCSF) system is shown below

39
Phase-Controlled Cycloconverters (contd)
  • Generator bus with regulated voltage but
    variable frequency (1333-2666 Hz) is fed to the
    cycloconverter phase groups. (A generator speed
    variation of 21 is assumed). The dual converter
    in each phase group uses a low-pass filter to
    generate a sinusoidal signal.
  • ? modulator receives biased cosine waves from
    generator bus voltage and sinusoidal control
    signal voltages to generate thyristor firing
    angles.

40
Phase-Controlled Cycloconverters (contd)
  • 3? sinusoidal control signals are generated
    through the vector rotator. The feedback voltage
    Vs is generated from the output phase voltages.

41
Phase-Controlled Cycloconverters (contd)
  • Details of ? modulator are shown below

42
Matrix Converters
  • These types of cycloconverters use
    high-frequency, self-controlled ac switches (e.g.
    IGBTs). A 3? to 3? converter is shown below

43
Matrix Converters (contd)
  • A matrix of nine switches where any input
    phase can be connected to any output phase. The
    switches are controlled by PWM to fabricate an
    output fundamental voltage whose amplitude and
    frequency can be varied to control an ac motor.
  • The output waveform synthesis is shown on the
    next slide.

44
Matrix Converters (contd)

45
Matrix Converters (contd)
  • Matrix converters offer the advantage over
    thyristor cycloconverters of being able to
    produce unity PF line current.
  • However, compared to PWM voltage-fed
    converters, the parts count is significantly
    higher.

46
High-Frequency Cycloconverters
  • See Bose text pp. 186-189
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