6
CAPACITOR SIZE REDUCTION FOR MULTIPLE INVERTER SYSTEMS G.I. Orfanoudakis*, S.M. Sharkh* and M.A. Yuratich *University of Southampton,UK, [email protected], [email protected] †TSL Technology Ltd, UK, [email protected] Keywords: Multiple inverter systems, DC-link capacitors. Abstract Multiple inverter systems are examined from the aspect of their DC-link capacitors. A common capacitor is assumed and its current spectrum is derived for single and three-phase inverter systems. The effect of introducing a phase shift between the inverter reference or carrier waveforms is investigated, to reveal potential reductions in DC-link capacitor rms (ripple) current. It is shown that significant reductions of 40% - 50% in the capacitor rms current can be achieved, especially for three-phase inverter systems. The results are verified by simulations using MATLAB-Simulink. 1 Introduction During the last decade, multiple inverter systems have been extensively incorporated in high-power applications. In addition to high-power electric motor drives, comprising multiple inverters that share the total drive current, multiple inverter systems have been used to drive multi-phase motors, or different motors in multiple motor applications. Key examples of such applications are conveyor belts and electric vehicles with direct drive wheel motors. This study examines multiple inverter systems from the perspective of their DC-link capacitors, which are sensitive elements of an inverter and a common source of failures, and should therefore be selected and treated carefully. The DC- link capacitor current contains harmonics (ripple) which give rise to capacitor voltage fluctuations as well as capacitor losses. Voltage and thermal stresses induced, respectively, from these effects are the main factors that shorten the capacitor lifetime. In order to mitigate them, additional capacitors have to be connected in parallel. In a conventional multiple inverter system, each inverter is connected to its own DC-link. The present study investigates potential reduction in overall capacitor size and losses that can be achieved in multiple inverter systems, by using a common DC-link capacitor as shown in Figure 1. The study covers a range of cases for multiple inverter systems, defined by the number of inverters (N ), the number of inverter phases (1φ/3φ), and the phase angles of the inverter reference waveforms. Figure 1: Block diagram of multiple inverter system with N inverters sharing a common DC-link capacitor. 2 DC-link Capacitor Selection The selection of DC-link capacitors is determined by the required capacitance, voltage and ripple current ratings. The capacitance is selected according to the expected low- frequency capacitor current harmonics (I h at frequency f h , for h = 1, 2, ...) and the maximum affordable amplitude of DC voltage oscillations (ΔV dc /2). Each current harmonic results in a respective voltage harmonic at the DC-link. Assuming that, in the worst case, all current harmonics (or equivalently all peaks of voltage harmonics) can be in phase, the required capacitance is given by Equation (1): Δ h h h dc f I V C π 2 2 / 1 (1) According to this equation, high-frequency capacitor current harmonics, which appear due to the switching (PWM) operation of the inverter, have a small effect on the capacitor voltage ripple. However, they contribute to the DC-link capacitor losses and internal heat dissipation, thus increasing the required capacitor ripple current rating. The voltage rating is typically higher than the operating DC voltage of the inverter, to account for voltage oscillations and other effects such as input (grid) voltage fluctuations and regenerative operation of the inverter.

Capacitor Size Reduction for Multiple

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CAPACITOR SIZE REDUCTION FOR MULTIPLEINVERTER SYSTEMS

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  • CAPACITOR SIZE REDUCTION FOR MULTIPLE INVERTER SYSTEMS

    G.I. Orfanoudakis*, S.M. Sharkh* and M.A. Yuratich

    *University of Southampton,UK, [email protected], [email protected] TSL Technology Ltd, UK, [email protected]

    Keywords: Multiple inverter systems, DC-link capacitors.

    Abstract

    Multiple inverter systems are examined from the aspect of their DC-link capacitors. A common capacitor is assumed and its current spectrum is derived for single and three-phase inverter systems. The effect of introducing a phase shift between the inverter reference or carrier waveforms is investigated, to reveal potential reductions in DC-link capacitor rms (ripple) current. It is shown that significant reductions of 40% - 50% in the capacitor rms current can be achieved, especially for three-phase inverter systems. The results are verified by simulations using MATLAB-Simulink.

    1 Introduction

    During the last decade, multiple inverter systems have been extensively incorporated in high-power applications. In addition to high-power electric motor drives, comprising multiple inverters that share the total drive current, multiple inverter systems have been used to drive multi-phase motors, or different motors in multiple motor applications. Key examples of such applications are conveyor belts and electric vehicles with direct drive wheel motors.

    This study examines multiple inverter systems from the perspective of their DC-link capacitors, which are sensitive elements of an inverter and a common source of failures, and should therefore be selected and treated carefully. The DC-link capacitor current contains harmonics (ripple) which give rise to capacitor voltage fluctuations as well as capacitor losses. Voltage and thermal stresses induced, respectively, from these effects are the main factors that shorten the capacitor lifetime. In order to mitigate them, additional capacitors have to be connected in parallel.

    In a conventional multiple inverter system, each inverter is connected to its own DC-link. The present study investigates potential reduction in overall capacitor size and losses that can be achieved in multiple inverter systems, by using a common DC-link capacitor as shown in Figure 1. The study covers a range of cases for multiple inverter systems, defined by the number of inverters (N), the number of inverter phases (1/3), and the phase angles of the inverter reference waveforms.

    Figure 1: Block diagram of multiple inverter system with Ninverters sharing a common DC-link capacitor.

    2 DC-link Capacitor Selection

    The selection of DC-link capacitors is determined by the required capacitance, voltage and ripple current ratings. The capacitance is selected according to the expected low-frequency capacitor current harmonics (Ih at frequency fh, for h = 1, 2, ...) and the maximum affordable amplitude of DC voltage oscillations (Vdc/2). Each current harmonic results in a respective voltage harmonic at the DC-link. Assuming that, in the worst case, all current harmonics (or equivalently all peaks of voltage harmonics) can be in phase, the required capacitance is given by Equation (1):

    h h

    h

    dc f

    I

    VC

    22/1

    (1)

    According to this equation, high-frequency capacitor current harmonics, which appear due to the switching (PWM) operation of the inverter, have a small effect on the capacitor voltage ripple. However, they contribute to the DC-link capacitor losses and internal heat dissipation, thus increasing the required capacitor ripple current rating.

    The voltage rating is typically higher than the operating DC voltage of the inverter, to account for voltage oscillations and other effects such as input (grid) voltage fluctuations and regenerative operation of the inverter.

  • 3 Harmonic Analysis of Capacitor Current

    Methods are available in the literature for analyzing the DC-link capacitor current of a single inverter, with respect to both its rms value [2, 4, 8, 10] and its harmonic components [1, 5]. A study on the DC-link capacitor rms current of a two-inverter system can also be found in [7]. Expressions giving the capacitor current rms value can be used for estimating capacitor losses, given the capacitor Equivalent Series Resistance (ESR). The derivation, however, of the amplitude, frequency and phase for each capacitor current harmonic, provides additional capabilities. Regarding DC-link capacitor selection, harmonic analysis can give an accurate estimate of the required capacitance, according to Equation (1).Moreover, it offers a more accurate approximation of capacitor losses, in cases where the capacitor ESR varies with frequency [4, 6]. Pertaining to multiple inverter systems, harmonic analysis additionally offers the basis for examining the possible capacitor current harmonic reductions or cancellations that can be achieved by connecting two or more inverters to a common DC-link.

    Section 3.1, below, summarizes the results of the DC-link capacitor current harmonic analysis, for single and three-phase inverters (Figure 2). The effect of connecting multiple inverters to a common DC-link is discussed in section 3.2. It has to be noted that the contribution of the systems front-end, commonly a rectifier, on the DC-link capacitor current is not examined in this study. The current harmonics due a 6-pulse rectifier can be calculated as shown in [9], and superimposed onto the inverter harmonics to obtain the complete capacitor current spectrum.

    3.1 Single inverter DC-link capacitor current harmonics

    The DC-link capacitor current harmonics of a three-phase, two-level inverter were initially analyzed in [1]. The authors based their calculations on the Geometric Wall Model technique, which has been extensively applied in [3] for the harmonic analysis of inverter (PWM) output voltage waveforms. Using this technique, the DC-link capacitor current is expressed as a Fourier series, with Fourier coefficients corresponding to individual current harmonics. A different approach, which takes advantage of the known output phase voltage spectrum of the two-level inverter, was adopted in [5], giving the same result. In both cases, the first step of the derivation was the analysis of the current through the IGBT/diode module V1, shown in Figure 2. Assuming naturally sampled sine-triangle modulation (triangular carrier and sinusoidal reference waveforms), the Fourier coefficients of this current are derived in [1, 5]. After some manipulation and conversion to their complex form, these coefficients are given by Equations (2) for baseband, and (3) for carrier-sideband harmonics. Superscripts m and n denote the order of the harmonic, defining its frequency as fh = mfc + nf0, where fcand f0 are the inverter carrier (switching) and fundamental frequencies, respectively. The symbols IL, M and stand for the peak output current, inverter modulation index and load power angle, respectively.

    Figure 2: Single-phase H-bridge and three-phase two-level inverter topologies.

    Baseband harmonics (m = 0, n = 1 or 2):

    =

    ==

    2for ,4

    1for ,2

    10

    nej

    MI

    nej

    I

    ijL

    jL

    Vn

    (2)

    Carrier (m 0, n = 0) and sideband (m 0, n 0) harmonics:

    ( )

    +=

    + MmJeMmJe

    nmm

    Ieji

    nj

    nj

    L

    jmn

    Vmn

    22

    2cos

    11

    2

    1

    (3)

    A current harmonic, hmn , in the above complex form, can be expressed in the time domain using Equation (4):

    ( ) [ ] [ ]( ) mnccmnmn tmtnhth +++= 00cos ,{ }{ }

    = h

    hmn

    mnmn

    ReIm

    tan 1 (4)

    where c and 0 are the carrier and fundamental angular frequencies, equal to 2fc and 2f0, while c and 0 are the phase angles of the carrier and reference waveforms, respectively [3].

  • By convention, the phase angles c and 0 are set to zero for module V1 (c,V1 = 0,V1 = 0). Use of other than zero values for c and 0 introduces a shift of mc + n0 to the phase of the mnth harmonic. An equivalent way of introducing the same phase shift is multiplying the complex form by a rotating factor, r, given by Equation (5):

    ( )0 nmj cer += (5)

    This factor will be used below, to derive the DC-link capacitor current harmonic coefficients for a single-phase and a three-phase inverter, as well as for a multiple inverter system with a common DC-link.

    3.1.1 Single-phase H-bridge inverter

    Under the assumption that the inverter is supplied by a source providing purely DC current, Idc, the DC-link ripple (AC) current is totally carried by the capacitor (Figure 2). Apart from its DC component, the positive DC-link current, id, is therefore equal and opposite to the capacitor current, iC, at any instant. Neglecting the negative sign, the current harmonics of id and iC are then the same, and can be found by adding the respective harmonic coefficients for modules V1 and V2. The two modules are switched using the same carrier waveform (c,V2 = 0), while the reference waveform for V2 is shifted by 180 deg (0,V2 = ). Thus, the harmonic coefficients for the capacitor current are given by Equation (6), below:

    ( )

    =+= oddfor,0

    evenfor,21 111,

    n

    nieii V

    mnjn

    Vmn

    Cmn

    (6)

    According to Equations (2) and (6), the DC-link capacitor current of an H-bridge inverter contains a baseband harmonic (m = 0, n = 2) at twice the fundamental frequency:

    jL

    C ej

    MIi

    21,02 = (7)

    3.1.2 Three-phase two-level inverter

    The harmonic coefficients for the DC-link capacitor current of a three-phase, two-level inverter can be derived following a similar procedure. The positive DC-link current is now the sum of the currents of modules V1, V3 and V5. A common carrier waveform is used for all modules (c,V3 = c,V5 = 0), while the reference waveforms for V3 and V5 are shifted by -120 deg (0,V3 = -2/3) and 120 deg (0,V5 = 2/3), respectively. The harmonic coefficients for the three-phase inverter capacitor current are given by Equation (8). No baseband harmonics remain in this case.

    ( )

    =

    =

    ++=

    03modfor ,0

    03modfor ,3

    1

    1

    3/23/213,

    n

    ni

    eeii

    Vmn

    njnjV

    mnC

    mn

    (8)

    3.2 Common DC-link capacitor current harmonics

    This section discusses the effect of introducing a carrier phase shift between the inverters of an N-inverter system. It is assumed that the kth inverter (1 k N) has its own carrier waveform, shifted by c,k compared to the 1

    st inverter (c,1 = 0), and that this waveform is used to switch all its phase legs. Moreover, the reference waveform for module V1 of the kth

    inverter is assumed to be shifted by 0,k in relation to the respective waveform of the 1st inverter (0,1 = 0). The reference waveforms for the other modules are shifted accordingly, as explained in sections 3.1.1 and 3.1.2. According to Equation (5), the rotating factors, rk, for the harmonics of the kth inverter will be:

    ( )kkc nmjk er

    ,0, += (9)

    Hence, the harmonic coefficients of the common DC-link capacitor current will be given by Equation (10), below:

    =

    kkC

    mnC

    mn rii 3/1, (10)

    4 System cases - Results

    Different multiple inverter systems configurations are examined in this section. The aim is to investigate whether the required DC-link capacitor size can be reduced by the introduction of an appropriate phase shift to the inverter reference or carrier waveforms. Given that the capacitor voltage rating is primarily determined by the system specifications and therefore cannot be decreased, a reduction to the capacitor size can arise from a reduction of the capacitance or the ripple current requirements. As explained in sections 2 and 3, the required capacitance is mainly affected by the low-frequency capacitor current harmonics, while the ripple current rating is determined by the capacitor current rms value. With reference to the presented harmonic analysis, the low-frequency harmonics will be considered to be the baseband harmonics, while the capacitor rms current will be calculated using Equation (11), below:

    =m n

    Cmn

    rmsC

    iI

    2

    ,2

    (11)

    Multiple inverter systems with two (N = 2) and three (N = 3) inverters will be examined. The inverter loads are assumed to be identical, having a power factor cos = 0.85, which is a typical value for motors. The phase shifts 0,k of the inverter reference waveforms are fixed to different values to represent different system configurations. Then, the carrier phase shift is varied, to determine the value that yields the optimum (minimum) capacitor rms current. The optimal current value is finally compared to the conventional practice of using the same carrier for all inverters. The analytically derived current rms values are verified by simulations in MATLAB-Simulink. The simulated results are shown as points in the relative figures.

  • 0 30 60 90 120 150 1800

    0.2

    0.4

    0.6

    0.8

    1

    c

    Rm

    s cu

    rren

    t rat

    io

    M = 1M = 0.8M = 0.6

    0 0.2 0.4 0.6 0.8 10

    0.2

    0.4

    0.6

    0.8

    M

    Nor

    m. r

    ms

    curr

    ent

    IC,rms|90

    IC,rms|0

    Figure 3: Capacitor rms current versus c and M for single-phase inverter system with N = 2, 0 = 90 deg.

    4.1 Single-phase inverter systems

    The DC-link capacitor current of a single-phase H-bridge inverter contains a baseband harmonic, described by Equation (7). According to Equation (10), the coefficient for this harmonic in a multiple inverter system will be given by:

    =k

    jjLC

    keej

    MIi ,0202

    2 (12)

    It can be noticed that the above expression is only dependent on the inverter reference phase shifts, 0,k. Given that 0,1 isdefined to be zero, the baseband harmonic can be eliminated for N = 2 if 0,2 = 90 deg, while for N = 3 if 0,2 = 60 deg and 0,3 = -60 (or 120 and -120) deg.

    These two cases of interest are examined with respect to their capacitor rms current, in Figures 3 and 4, respectively. The upper plots illustrate how the capacitor rms current varies with c. If IC,rms|c is the common capacitor rms current when the inverter carriers are shifted by c, then the variation is shown by plotting the ratio IC,rms|c /IC,rms|0 for different values of c. The optimal value for c, c,opt, proves to be equal to 90 and 60 deg for N = 2 and N = 3, respectively. Adopting c,optas a carrier phase shift for each case, the resulting capacitor rms current, IC,rms|c,opt, is subsequently plotted together with IC,rms|0 against the inverters modulation index, M. The rms values are normalized to the output rms current.

    The ripple current rating of the inverter DC-link capacitors is determined by the maximum rms current that the capacitors may have to carry within the inverter operating range. For the two cases presented in Figures 3 and 4, the maximum(normalized) rms current values are given in Table 1.

    0 30 60 90 120 150 1800

    0.2

    0.4

    0.6

    0.8

    1

    c

    Rm

    s cu

    rren

    t rat

    io

    M = 1M = 0.8M = 0.6

    0 0.2 0.4 0.6 0.8 10

    0.2

    0.4

    0.6

    0.8

    1

    MN

    orm

    . rm

    s cu

    rren

    t

    IC,rms|60

    IC,rms|0

    Figure 4: Capacitor rms current versus c and M for single-phase inverter system with N = 3, 0 = 60/120 deg.

    N 0 (deg) c,opt (deg) max IC,rms|c,opt max IC,rms|0 Decr.23

    9060/120

    9060/120

    0.6 0.68

    0.71 1

    15.5%32%

    Table 1: Summary of results for the examined single-phase inverter systems.

    The above analysis can be extended to systems incorporating inverters with other values of 0. The carrier phase shift, c,opt,that minimizes the required ripple current rating of the DC-link capacitor can be determined for each value of 0. It is assumed that 0,2 = -0,3 = 0 and c,2 = -c,3 = c. In the case of single-phase inverter systems, the study showed that c,optdoes not change with 0: for N = 2, c,opt is 90 deg and for N = 3, 60/120 deg. However, the maximum capacitor rms current varies significantly with 0, as shown in Figure 5, below.

    0 30 60 90 120 150 1800

    0.5

    1

    1.5

    2

    0

    Max

    nor

    m. r

    ms

    curr

    ent

    IC,rms|c,opt

    IC,rms|0

    Figure 5: Maximum capacitor rms currents IC,rms|c,opt and IC,rms|0 versus 0, for single-phase inverter systems with N = 2and N = 3 (bold lines).

  • 0 30 60 90 120 150 1800

    0.2

    0.4

    0.6

    0.8

    1

    c

    Rm

    s cu

    rren

    t rat

    io

    M = 1M = 0.8M = 0.6

    0 0.2 0.4 0.6 0.8 10

    0.5

    1

    1.5

    M

    Nor

    m. r

    ms

    curr

    ent

    IC,rms|90

    IC,rms|0

    Figure 6: Capacitor rms current versus c and M for three-phase inverter system with N = 2, 0 = 30/90 deg.

    4.2 Three-phase inverter systems

    Assuming a balanced operation, the DC-link current of a three-phase, two-level inverter does not contain any baseband harmonics. Under the same assumption, no baseband harmonics appear in the DC-link of a multiple three-phase inverter system either.

    The case of 0 = 30 deg is examined as an example in Figures 6 and 7, for systems with N = 2 and N = 3, respectively. The value of c,opt and the maximum capacitor rms current for each case are shown in Table 2. The results are the same for 0 = 90 deg.

    Further investigation, regarding other values of 0, yields different optimal phase shifts in the case of three-phase inverter systems. Figure 8 illustrates how c,opt varies with 0and plots the corresponding values of the maximum capacitor rms current.

    According to section 4.1 and Figures 5 and 8, a carrier phase shift of approximately 90 deg is optimal, for both single and three-phase inverter systems with N = 2. For systems with N= 3, the optimal phase shift is 60 or 120 deg. It is therefore indicated that these phase shifts affect certain carrier and sideband harmonics similarly to the single-phase inverter baseband harmonic, according to Equation (12). Other carrier and sideband harmonics may be increased when using the specific phase shifts. Nevertheless, the overall capacitor current rms value is decreased. A mathematical analysis that could theoretically examine this effect is beyond the scope of the present study.

    0 30 60 90 120 150 1800

    0.2

    0.4

    0.6

    0.8

    1

    c

    Rm

    s cu

    rren

    t rat

    io

    M = 1M = 0.8M = 0.6

    0 0.2 0.4 0.6 0.8 10

    0.5

    1

    1.5

    MN

    orm

    . rm

    s cu

    rren

    t

    IC,rms|60

    IC,rms|0

    Figure 7: Capacitor rms current versus c and M for three-phase inverter system with N = 3, 0 = 30/90 deg.

    N 0 (deg) c,opt (deg) max IC,rms|c,opt max IC,rms|0 Decr.23

    30/90 30/90

    9060

    0.65 0.78

    1.07 1.51

    39.3%48.3%

    Table 2: Summary of results for the examined three-phase inverter systems.

    0 30 60 90 1200

    30

    60

    90

    120

    150

    180

    0

    c,o

    pt

    0 30 60 90 1200

    0.5

    1

    1.5

    2

    0

    Max

    nor

    m. r

    ms

    curr

    ent

    IC,rms|c,opt

    IC,rms|0

    Figure 8: Optimal carrier phase shift and maximum capacitor rms currents IC,rms|c,opt and IC,rms|0 versus 0, for three-phase inverter systems with N = 2 and N = 3 (bold lines).

  • 5 Discussion

    This section discusses a number of considerations regarding the applicability of the outcomes from this study.

    The first relates to the power factor of the inverter loads. A power factor of 0.85 was assumed in section 4, and was used as a constant throughout the study. The capacitor current of a multi-inverter system was therefore treated as a function of the inverter output current and modulation index, as well as of the angles 0 and c. A preliminary investigation, however, indicated that the optimal phase shifts and current rms values are significantly different for low load power factors, below 0.5. The presented results are therefore valid when the inverter systems are used as motor drives, but have to be rederived in case of low power factor applications.

    A second comment refers to the effect of the inverter modulation strategy. The naturally sampled sine-triangle strategy was assumed for this study because analytical derivation of harmonic coefficients is intricate for other modulation strategies. For these strategies, the harmonic amplitudes can be calculated by numerical convolution of the output phase voltage and current spectra, according to [5]. The effect of using a modulation strategy other than SPWM on the presented results will depend on the degree of resemblance between their two capacitor current spectra.

    Furthermore, it was assumed that 0 is fixed, as it happens for example in a multi-phase machine, and therefore the carrier phase shift can be set to the corresponding c,opt. However, there are applications where 0 varies with time. In such cases, the carrier phase shift should be controlled to the respective optimum value. On the other hand, if there is freedom to select the value of 0, this should be done along with c,opt, to minimize the capacitor rms current according to Figures 5 and 8.

    A final note refers to the physical layout of the studied multiple inverter systems. It is well known that a low-inductance connection, typically a flat bus bar, should be present between the DC-link capacitor and the switching modules of an inverter. A common DC-link capacitor was used in the examined multiple inverter systems, therefore assuming that all inverters can be laid physically close (in the same cabinet) to the capacitor and to each other.

    6 Conclusions

    This study investigated the effect of introducing a reference or carrier waveform phase shift to multiple inverter systems using a common DC-link capacitor. It was based on an analytical derivation of the capacitor current harmonics and the mathematical representation of introducing a reference/carrier phase shift. The study covered single and three-phase systems, comprising two (N = 2) or three (N = 3) inverters. Regarding the single-phase inverter systems, it was shown that for N = 2 and N = 3, a decrement in the capacitor rms current of approximately 15% and 35%, respectively, can be achieved by selecting an appropriate carrier phase shift for

    each case. For three-phase inverter systems, the potential decrements were in the order of 40% and 50%, respectively. The results were verified by simulations using MATLAB-Simulink.

    Acknowledgements

    We would like to thank EPSRC and TSL Technology Ltd for funding this research as part of a PhD studentship.

    References

    [1] M. H. Bierhoff and F. W. Fuchs, DC-link harmonics of three-phase voltage-source converters influenced by the pulsewidth-modulation strategy-An analysis, IEEE Transactions on Industrial Electronics, vol. 55, no. 5, pp. 2085 2092, (May 2008).

    [2] P. A. Dahono, Y. Sato and T. Kataoka, Analysis and minimization of ripple components of input current and voltage of PWM inverters, IEEE Transactions on Industry Applications, vol. 32, no. 4, pp. 945 950, (Jul./Aug. 1996).

    [3] D. G. Holmes and T. A. Lipo, Pulse Width Modulation for Power Converters, IEEE press series on power engineering. Piscataway, NJ: IEEE Press, (2003).

    [4] J. W. Kolar and S. D. Round, Analytical calculation of the RMS current stress on the DC-link capacitor of voltage-PWM converter systems, IEE Proceedings in Electrical Power Applications, vol. 153, no. 4, pp. 535 543, (July 2006).

    [5] B. P. McGrath and D. H. Holmes, A general analytical method for calculating inverter DC-link current harmonics, IEEE Transactions on Industry Applications, vol. 45, no. 5, pp. 1851 1859, (Sep./Oct. 2009).

    [6] G. I. Orfanoudakis, S. M. Sharkh and M. A. Yuratich, Analysis of DC-link capacitor losses in three-level neutral-point-clamped and cascaded H-bridge voltage source inverters, IEEE International Symposium on Industrial Electronics, Bari, Italy, (July 2010).

    [7] K. M. Rahman et al, Multiple inverter system with low power bus system, U.S. Patent 6 864 646, (Mar. 2005).

    [8] F. Renken, DC-Link Capacitor Current in Pulsed Single-Phase H-Bridge Inverters, 11th EPE Meeting,Dresden, Germany, (2005).

    [9] M. Sakui and H. Fujita, An Analytical Method for Calculating Harmonic Currents of a Three-Phase Diode-Bridge Rectifier with dc Filter, IEEE Transactions on Power Electronics, vol. 9, no. 6, pp. 631 637, (1994).

    [10] B. A. Welchko, Analytical Calculation of the RMS Current Stress on the DC Link Capacitor for a VSI Employing Reduced Common Mode Voltage PWM, European Conference on Power Electronics and Applications, pp. 1 8, (2007).

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