Arrangement for Current Sharing of Parallel-Connected Converters

Information

  • Patent Application
  • 20240429833
  • Publication Number
    20240429833
  • Date Filed
    June 18, 2024
    6 months ago
  • Date Published
    December 26, 2024
    7 days ago
Abstract
Current sharing between the plurality of parallel-connected ARCP or hard-switching converter legs is balanced by a control arrangement. The control arrangement senses a leg output current in each of the parallel-connected converter legs and have an individual autonomous leg-specific switching instant adjustment for the main switches of each of the parallel-connected converter legs to shift the first mode A commutation of the respective converter leg later in time and to shift the second mode B commutation of the respective converter leg earlier in time by a variable timestep proportional to the value of the sensed leg current of the respective converter leg. In other words, if the value of the sensed leg output current in one converter leg is larger than in the other converter leg, then in mode A, the higher-current leg will commutate later than the leg with less current, and in mode B, the higher-current leg will commutate earlier than the leg with less current.
Description
TECHNICAL FIELD

The present invention relates to parallel-connected power converters and more particularly to a current sharing of parallel-connected power inverters and rectifiers.


BACKGROUND

A dc-ac or ac-dc converter, also known as an inverter or a rectifier respectively, converts power from dc to ac or ac to dc system at desired voltages and frequencies. The inverter therefore can be operated as an adjustable-frequency voltage source. The dc power input to the inverter may be obtained from an existing power supply network through a rectifier or from a battery, fuel cell, photovoltaic array, etc. The filter capacitor(s) across the input terminals of the inverter provides a fairly constant dc-link voltage. A configuration of ac to dc rectifier and dc to ac inverter may be called a dc-link converter.


In some situations, a power inverter with an increased output power capability is implemented by connecting a plurality of inverter units in parallel with one another to feed the same load. The parallel-connected inverter units may receive simultaneous and similar control signals to provide a desired output of the power inverter. However, due to parameter differences of switch components and differing impedances in parallel branches, the currents between the units can be unequal in magnitude. Such a current imbalance can stress the components unevenly and wear switch components with higher current prematurely. A higher current in a switch component can result in a higher dissipated power and, further, a higher temperature of the component.


Current imbalance has been addressed by modifying switch control pulses in order to balance the currents. The control pulses can be modified by delaying a turn-on time instant for a switch that has the highest current or by delaying turn-off time instants for a switch that has the smallest current. One such method is disclosed in EP0524398. In these solutions, the conducting times of the parallel components are modified to equalize stresses to the switch components on the basis of measured inverter unit currents.


U.S. Pat. No. 8,432,714 discloses a method for balancing load between parallel-connected inverter modules wherein temperatures of each output leg of each inverter module are determined and the switching instructions for one or more of the parallel inverter modules are modified for controlling the temperatures of the output legs.


WO2017/079125A1 discloses a method wherein the output voltages of all the parallel connected power devices are measured, and the measuring results are used for mitigating timing differences during output voltage state changes caused e.g. by gate driver circuit and switching component parameter tolerances.


U.S. Pat. No. 7,068,525 discloses a method of operating multiple parallel-connected inverters by regulating the individual currents of the inverters separately.


SUMMARY

An object of the present invention is to provide an improved power converter system having two or more parallel-connected converter legs. The power converter system is recited in the independent claim. Preferred embodiments are disclosed in the dependent claims.


An aspect of the invention is a power converter system, comprising

    • two or more converter legs connected in parallel between a common dc system and a common ac system or between two common dc systems, wherein each of said converter legs comprises a first controllable main switching device with a first antiparallel diode and a second controllable switching device with a second antiparallel diode connected in series between a first DC voltage rail and a second DC voltage rail to alternatively connect the first and second dc-link rails to a converter leg output or input,
    • wherein each parallel-connected converter leg comprises a mode A of commutation wherein a leg current commutates from the first or second antiparallel diode to the second or first controllable main switching device, respectively, and a mode B of commutation wherein the leg current commutates from the first or second controllable main switching device to the second or first antiparallel diode, respectively,
    • wherein commutations of the parallel-connected converter legs are initiated by essentially simultaneous commutation commands,
    • a control arrangement configured to sense the leg current in each of the parallel-connected inverter legs, and wherein the control arrangement is configured to balance a current sharing between the parallel-connected inverter legs by means of having an individual autonomous leg-specific switching instant adjustment for the main switches of each of the parallel-connected converter legs to shift the mode A commutation of the respective converter leg later in time and to shift the mode B commutation of the respective converter leg earlier in time by a variable timestep proportional to the value of the sensed leg current of the respective converter leg.


In an embodiment, each individual autonomous leg-specific switching instant adjustment is configured to shift a start of a leg voltage swing during the mode A commutation of the respective converter leg later in time and to shift a start of a leg voltage swing during the mode B commutation of the respective converter leg earlier in time by a variable timestep proportional to the value of the sensed leg current of the respective converter leg.


In an embodiment, the size of the variable timestep of an individual shift later in time during an individual mode A commutation and the size of the variable timestep of an individual shift earlier in time during an individual mode B commutation are configured to be dependent on the value of the sensed leg current of the respective converter leg in such a way that the size of the variable timestep of individual shift in time increases with the increasing value of the sensed leg current and decreases with the decreasing value of the sensed leg current.


In an embodiment, each individual autonomous leg-specific switching instant adjustment of the main switching devices has a first predetermined dependence on the value of the sensed leg current of the respective converter leg in mode A commutation and a second predetermined dependence in the mode B commutation, and wherein optionally the predetermined first and second dependences of different parallel-connected converter legs having different nominal leg current ratings are selected to scale the current sharing between the between the parallel-connected converter legs according to nominal leg currents of the parallel-connected converter legs.


In an embodiment, the parallel-connected converter legs are auxiliary resonant commutated pole (ARCP) converter legs, particularly ARCP half-bridge legs, and wherein the control arrangement is configured to advance each ARCP mode B commutation sequence and delay each ARCP mode A commutation sequence in time in such a way that the size of the variable timestep increases with the increasing value of the sensed leg current and decreases with the decreasing value of the sensed leg current-of the respective converter leg.


In an embodiment, the ARCP commutation sequence includes a sequence from a turn-on instant of at least one auxiliary switching device to a turn-off instant of the main switching device that has been conducting.


In an embodiment, the control arrangement is configured to delay both the turn-on instance of the at least one auxiliary switching device and the turn-off instant of the main switching device in the mode A commutation by a first variable timestep twA which increases with the increasing value of the sensed leg current and decreases with the decreasing value of the sensed leg current of the respective converter leg, and the control arrangement is configured to delay both the turn-on instance of the at least one auxiliary switching device and the turn-off instant of the main switching device in the mode B commutation by a second variable timestep twB which decreases with the increasing value of the sensed leg current and increases with the decreasing value of the sensed leg current of the respective converter leg, thereby advancing the turn-off instant of the main switching device proportionally to the value of the sensed leg current.


In an embodiment, the control arrangement is configured to delay the turn-off instant of the main switching device in the mode A commutation by adding the first variable timestep twA to a reference turn-off instant of the main switching device, and wherein the control arrangement is configured to advance the turn-off instant of the main switching device in the mode B commutation by adding the second variable timestep twB to a reference turn-off instant of the main switching device.


In an embodiment, the first variable timestep is twA=kA|Io|, where Io is the value of the sensed leg current sample of the respective converter leg, and kA is a constant, kA being equal for all converter legs with equal nominal leg current ratings, and the second variable timestep is twB=tc−kB|Io|, where twB≥0, Io is the value of the sensed leg current sample of the respective converter leg, tc is a constant time, and kB is a constant, kB being equal for all converter legs with equal nominal leg current ratings.


In an embodiment, the parallel-connected converter legs have different nominal leg current ratings, and wherein the constants kA and/or kB in the parallel-connected converter legs are selected to scale with nominal leg currents of the converter legs such that a product of the constant kA and the nominal leg current IN is same in all parallel-connected converter legs and a product of the constant kB and the nominal leg current IN is essentially same in all parallel-connected converter legs.


In an embodiment, the parallel connected converter legs are hard-switching converter legs, particularly half-bridge legs, and wherein the control arrangement is configured to delay a turn-off instant of the main switching device that has been conducting in the mode B commutation by a first variable timestep td,off which decreases with the increasing value of the sensed leg current and increases with the decreasing value of the sensed leg current of the respective converter leg, and the control arrangement is configured to delay a turn-on instant of the main switching device that will start conducting in the mode A commutation by a second variable timestep td,on which increases with the increasing value of the sensed leg current and decreases with the decreasing value of the sensed leg current of the respective converter leg.


In an embodiment, the first variable timestep td,off decreases with the increasing value of the sensed leg current according to koff*|Io|, where Io is the value of the sensed leg current of the respective converter leg and kB is a constant, kB being equal for all converter legs with equal nominal leg current ratings, and the second variable timestep td,on increases with the increasing value of the sensed leg current according to kon*|Io|, where Io is the value of the sensed leg current of the respective converter leg, and kon is a constant, kon being equal for all converter legs with equal nominal leg current ratings.


In an embodiment, the first variable timestep is td,off=tc−koff|Io|, where tc is a constant time defining an adjustment range, and wherein the second variable timestep is td,on=tD+kon|Io|, where, tD is an optional constant turn-on delay to avoid simultaneously conducting main switch devices.


In an embodiment, the parallel connected converter legs have different nominal leg current ratings, and wherein the constants kon or koff in the parallel-connected connector legs are selected to scale with nominal leg currents of the converter legs such that a product of the constant kon and the nominal leg current IN is same in all parallel-connected converter legs and a product of the constant koff and the nominal leg current IN is same in all parallel-connected converter legs.


In an embodiment, the control arrangement comprises a leg-specific controller for each of the two or more parallel-connected converter legs to adjust the switching instants of the main switching devices.


In an embodiment, the power inverter system comprises two or more converters, each of the converters comprising one or more converter phase legs, wherein the parallel-connected converter legs are the corresponding converter phase legs of the two or more converters connected in parallel.


In an embodiment, the control arrangement comprises converter-specific switching controllers for the two or more converters, each of the converter-specific switching controllers being configured to provide the autonomous adjustment of switching instants for each of the converter phase legs of the respective converter.





BRIEF DESCRIPTION OF THE DRAWINGS

In the following the invention will be described in greater detail by means of exemplary embodiments with reference to the attached drawings, in which



FIG. 1 is a block diagram that schematically illustrates an exemplary inverter system having a plurality of parallel-connected inverters;



FIG. 2 is a schematic of an exemplary inverter system having two parallel-connected hard-switching inverters;



FIG. 3 is a schematic block diagram of an exemplary ARCP inverter system having a plurality of parallel-connected inverters;



FIG. 4 is a schematic block diagram of an ARCP switching controller having a PWM modulator and ARCP control functions;



FIGS. 5A-5F are diagrams illustrating an example of mode A commutation;



FIGS. 6A-6D are diagrams illustrating an example of mode B commutation;



FIG. 7 is a flow diagram illustrating an exemplary operation of the control arrangement according to an aspect of the invention;



FIGS. 8A-8C are timing diagrams illustrating an example of shifting switching instants in a single converter leg;



FIGS. 9A and 9B show timing diagrams illustrating a simulated operation of the method according to embodiments of the invention for negative output current; and



FIG. 10 shows a timing diagram illustrating an exemplary simulation for two parallel-connected ARCP converter legs dimensioned for nominal currents in ratio 2:1.





DETAILED DESCRIPTION

A dc-ac or ac-dc converter, also known as an inverter or a rectifier respectively, converts power from dc to ac or ac to dc power system at desired voltages and frequencies. Further, a dc-dc converter, such as a dc chopper, converts power from dc to dc power system. Although embodiments are described using inverters and inverter systems as examples, the invention is similarly applicable to rectifiers and rectifier systems as well as dc-dc converters. Inverter and rectifier can be exactly similar in structure and the control operations can be similar, the difference being the direction of a power flow. When a converter operates as an inverter (dc/ac converter), it converts the power from a dc system to an ac system, i.e., the ac side of the converter is referred as an output side and the dc side is considered as an input side. When a converter operates as a rectifier (ac/dc converter), it converts power from an ac system to a dc system, i.e., the ac side of the converter is considered as an input side and the dc side is considered as an output side. Further, connecting ac/dc and dc/dc converters in back-to-back configuration, i.e. dc-sides connected together, between two ac systems, one of the converters is operating in rectifier mode and the other in inverter mode, depending on the power flow direction. Operation modes of the converters may vary during the operation, as power flow may vary.



FIG. 1 shows a block diagram that schematically illustrates an exemplary inverter system having a plurality of (i.e., two or more) inverters INV1, INV2, . . . , INVN connected in parallel from their DC side (e.g., DC link) terminals (e.g., dc+, dc−) and their AC side terminals (e.g., U1, V1, W1, U2, V2, W2). In the illustrated example, the inverters INV1 and INV2 are three-phase inverters providing three phase outputs U1, V1, W1 and U2, V2, W2, but it should be appreciated that parallel-connected inverters may be implemented as single-phase inverters, or generally include any number of inverter phases or phase legs. The parallel-connected inverters are fed by a common DC voltage source 4 with voltage Udc, and inverters are feeding a common AC load 6. A typical application area of the parallel-connected inverters fed by a common DC voltage source 4 is an electric motor drive having an AC electric motor as a common load 6. There is a non-zero impedance at each phase output of each inverter, represented by inductances Lo in FIG. 1. The output inductances Lo may be intentionally implemented (e.g., a coil, a choke, etc.) or it may be just some leakage impedance of practical components and materials, such as cabling. The output inductances Lo may be substantially equal, but it must not necessarily be so. The corresponding phase outputs U1, U2, V1, V2, and W1, W2 of the parallel-connected inverters INV1 and INV2 are connected through the output inductances Lo to the common phase outputs U, V, and W, respectively. The corresponding phase outputs U1, U2, V1, V2, and W1, W2 of the parallel-connected inverters INV1 and INV2 may be connected together right after the output inductances Lo, and a single cable or multiple cables per phase U, V, and W may be used to connect the phase outputs to the load 6. Alternatively, each parallel-connected inverters INV1 and INV2 can be connected by means of its own cabling to the load 6, and the phase outputs U1, U2, V1, V2, and W1, W2 can be connected in parallel first at the terminals of the load 6. Output phase current Io of each phase U, V, W supplied to the load 6 is formed by combining phase output currents Io1 and Io2 of the respective phase outputs U1, U2, V1, V2, and W1, W2 of the parallel-connected inverters INV1 and INV2. The common DC supplied parallel-connected inverter modules INV1 and INV2 can be controlled to act like one high power inverter. This can be achieved by controlling the parallel inverter units with essentially same control commands.


Each inverter module INV1 and INV2 may have one or more bridge circuits (a full bridge or a half bridge), one bridge circuit for each inverter phase or phase leg. The bridge circuits of the same phase of different inverter modules are connected in parallel with one another. Each bridge circuit can include a plurality of controllable electronic switching elements or devices (e.g. insulated gate bipolar transistors (IGBTs) that operate in a switch mode, meaning that that they are controlled to transition from a blocking state (OFF state) to a conducting state (ON state), and vice-versa, by providing control pulses (often called switching control signals or gating signals) at a high switching frequency. In a PWM modulation scheme, the width of control pulses provided to the control inputs of the switching devices is varied to provide a desired output of the inverter. The parallel-connected inverter modules INV1 and INV2 may have a common switching control that provides switching signals or gating signals to operate switching devices of all inverter modules, or more preferably, each parallel-connected inverter module INV1 and INV2 may have a dedicated switching control unit 81 and 82 that provides switching signals or gating signals to operate switching devices of the respective inverter module, as illustrated in FIG. 1. Alternatively, the control may be distributed among a common switching control unit and inverter module-specific switching control units. In the latter cases, the inverter modules may be normal inverter modules (i.e., that can be used as single units) that can be connected in parallel as such. In embodiments, the switching control(s) 81 and 82 of the parallel-connected inverter modules INV1 and INV2 may be controlled by a higher-level control system 86 with simultaneous and essentially similar control signals or commands.


In embodiments, the higher-level control system 86 may be an electric motor control or similar. It can also include a common PWM generation function (for example, a PWM modulator) for all system elements and phases.


The schematic of an exemplary inverter system (e.g., single-phase inverter system) having two so-called hard-switching inverters INV1 and INV2 connected in parallel is illustrated in FIG. 2 and described herein in order to alleviate comprehending operation and configuration of embodiments of the invention in relation to exemplary basic parallel-connected inverters. It is not intended to limit embodiments of the invention to the described and illustrated exemplary inverters. It shall be appreciated that the current sharing control according to embodiments of the invention is universally applicable to any number of parallel inverters, any type of inverters and their derivates and modifications regardless the specific design, configuration, and operation variations of an inverter from the exemplary inverter.


The parallel-connected inverters INV1 and INV2 may preferably be identical inverters having the same configuration and operation. The inverters INV1 and INV2 comprise power switching sections 10, such as half-bridge circuits, and dc-link rails 22 (positive dc-link potentials P) are connected to a first voltage terminal Udc+ of the common DC power source 4, and dc-link rails 24 (negative dc-link potentials N) are connected to a second voltage terminal Udc− of the common DC power source 4. The DC link may be implemented in a similar manner as a DC link 2 discussed below with reference to FIG. 3. The output node 110 of each power switching section 10 can be connected through the corresponding output inductance Lo1 and Lo2 to the corresponding phase terminal of an ac load 6, such as an ac motor or ac grid or any applicable electric load, and thereby the corresponding phase outputs 110 of the inverters INV1 and INV2 (e.g., phase legs U1 and U2) are connected in parallel via Lo1 and Lo2. It should be appreciated that although a half-bridge inverter is illustrated as an example herein, the inverter may have other configurations, particularly a full-bridge configuration.


The exemplary half-bridge power section 10U of the inverter INV1 illustrated in FIG. 2 includes a pair of main or power switching devices S11 and S21 coupled in parallel to the dc-link rails 22 and 24. The first (upper) main switching device S11 may have a first terminal electrically coupled to the positive dc-link rail 22 and a second terminal electrically coupled to an output node 110. The second (lower) main switching device S21 having a first terminal coupled to output node 110 and a second terminal coupled to the negative dc-link rail 24. Across the upper main switching device S11 between the positive dc-link rail 22 and the output node 110 is connected a first antiparallel diode D11, and across the lower main switching device S21 between the output node 110 and the negative dc-link rail 24 is connected a second antiparallel diode D21. The upper main switching device S21 is operable to turn on and turn off, and thereby to respectively connect and disconnect the dc-link rail 22 and the output node 110, in response to control signal(s) G11 received from a control and driver circuitry, such as an inverter-specific switching controller 81 illustrated in FIG. 2. The lower main switching device S21 is operable to turn on and turn off, and thereby to respectively connect and disconnect the dc-link rail 24 and the output node 110, in response to control signal(s) G21 received from the control and driver circuitry, such as the switching controller 81. Similarly, the exemplary half-bridge power section 10U of the inverter INV2 illustrated in FIG. 2 includes a pair of main or power switching devices S12 and S22, a first antiparallel diode D12, a second antiparallel diode D22, and switching control signals G12 and G22 from a control and driver circuitry, such as an inverter-specific switching controller 82. In embodiments, the switching devices S11, S12, S21 and S22 may be insulated gate bipolar transistors (IGBT), or other type of semiconductor switching devices, such as integrated gate-commutated thyristors (IGCT), metal-oxide-semiconductor field-effect transistors (MOSFET), or silicon carbide (SiC) MOSFETs to name several examples.


Electronic switching devices, e.g., IGBTs, have a finite switching time, i.e. they they cannot instantly switch from the conductive to the blocking state and vice versa. During this transition interval (commutation), the switch neither completely blocks nor fully conducts, and therefore, neither the voltage across the switch nor the current through the switch is zero. In other words, there is a considerable overlap between voltage and current waveforms. This simultaneous presence of voltage across the switch and current through it means that, during this overlapping period, power is being dissipated within the device. This power loss, called “a switching loss”, reduces efficiency of the inverter, and when dissipated in the switch causes a major thermal stress on the switching device. The ability of a switching device to remove heat is limited. As the heat load increases, temperature rises which, in turn, degrades performance.


Conventional PWM inverters, such as the exemplary inverters in FIG. 2, are operated under such “hard switching” conditions, where the voltages across the switches and currents through the switches are changed abruptly from high values to zero and vice versa at a high switching frequency fs, with an overlap between the voltage and current waveforms, causing switching losses and generating a substantial amount of electro-magnetic interference. The switching losses are proportional to the switching frequency fs and thereby limit the maximum switching frequency. A high level of EMI is caused due to a wide spectrum of harmonics contained in rectangular PWM waveforms.


Soft-switching techniques aim to eliminate the switching losses by forcing a zero-voltage or a zero-current condition on the switch during a switching event. Switching at zero-voltage crossing is called zero-voltage switching (ZVS) whereas switching at zero-current crossing is called zero-current switching (ZCS). The auxiliary resonant commutated pole (ARCP) inverter is one of the most promising approaches for soft-switching inverters and has distinct potential benefits in a motor drive application. The ARCP inverter can be implemented using various topologies, which all perform essentially similarly. The output voltage wave form during commutation can be shaped to be motor friendly via suitable resonant circuit parameter selections. The stress in motor insulation and bearings is thus reduced. The basic configuration and operation of ARCP is described, for example, an article “The auxiliary resonant commutated pole converter”, IEEE-IAS Conference Proceedings 1990, pp. 1228-35, and in U.S. Pat. No. 5,047,913 by R. W. De Doncker et al.


According to an aspect of the invention, the inverter system is an auxiliary resonant commutated pole (ARCP) inverter system, comprising a plurality of (i.e., two or more) ARCP inverters INV1, INV2, . . . , INVN connected in parallel from their DC side (e.g. DC link) input terminals and their AC side output terminals (e.g., U1, V1, W1, U2, V2, W2). In embodiments, an ARCP inverter comprises series-connected dc-link capacitances of equal size between the negative (N) and the positive (P) dc-link rails of the dc-link side of the inverter. At a midpoint, called a neutral point (NP), of capacitances there is provided a neutral point potential UNP that essentially corresponds to half of the voltage Udc between the dc rails. Each phase of the inverter is associated with at least one resonant capacitor to force zero-voltage turn-off switching conditions. Further, an auxiliary branch comprising a resonant inductor and auxiliary switching device(s) is connected between the neutral point and a phase output to operate under zero current switching conditions. In the ARCP, the commutation is accomplished through the auxiliary circuitry in a finite amount of time. The auxiliary circuit is only used when the output is required to commutate from one voltage rail to the other. In order to ensure that the inverter output voltage at least reaches the positive and negative dc rail voltages during each resonant commutation cycle, a boost current is added to the resonant current by appropriately controlling the conduction times of the auxiliary switching devices. A predetermined boost current level in the inductor adds sufficient energy to the resonant operation to ensure that the output voltage attempts to overshoot the respective converter antiparallel diode and clamping the output voltage to the respective rail voltage. Ideally, the main switches turn on and off in a zero-voltage condition, and the auxiliary switch(es) in zero-current condition, which reduce the occurring switching losses. Consequently, the switching frequency can be increased without a considerable loss penalty. Low acoustic noise of such a drive is appreciated in many applications. High switching frequency also enables higher fundamental output frequencies with low distortion, making the ARCP topology attractive for high-speed drive applications.


The schematic of an exemplary ARCP inverter system having a plurality of (i.e., two or more) inverters INV1, INV2, . . . , INVN connected in parallel is illustrated in FIG. 3 and described herein in order to alleviate comprehending operation and configuration of embodiments of the invention in relation to an exemplary basic ARCP. It is not intended to limit embodiments of the invention to the described and illustrated exemplary ARCP(s) with only two parallel inverters. It shall be appreciated that the current sharing control according to embodiments of the invention is universally applicable to any type of ARCP inverters and their derivates and modifications regardless the specific design, configuration, and operation variations of an inverter from a basic ARCP inverter.


The parallel-connected ARCP inverters INV1 and INV2 may preferably be identical modules having the same configuration and operation. The exemplary ARCP inverter INV1 illustrated in FIG. 3 includes a DC-link 2 comprising a first dc-link rail 22, and a second dc-link rail 24, a first dc-link capacitor Cd11 coupled with the first dc-link rail 22 and a dc-link midpoint, called a neutral point NP1, and a second dc-link capacitor Cd12 coupled with the second dc-link rail 24 and the neutral point NP1. During operation, the first dc-link rail 22 is at a first voltage, so called positive (P) dc-link potential, and the second dc-link rail 24 is at a second voltage lower than the first DC voltage, so called negative (N) dc-link potential, and the dc-link midpoint NP1 is at a midpoint voltage, so called neutral point voltage UNP. The capacitances of the dc-link capacitors Cd11 and Cd21 are substantially equal, for example Cd11=Cd21=2Cdc, so that the voltages U11 and U21 provided across the dc-link capacitors Cd1 and Cd2 series-connected between the dc-link rails 22 and 24 are substantially equal, i.e. a half of a dc-link voltage Udc=U11+U21 between the dc-link rails 22 and 24. Thus, also the neutral point voltage or potential UNP essentially corresponds to half of the voltage Udc, in other words UNP=Udc/2. The exemplary ARCP inverter INV2 includes a similar DC link 2 having dc-link rails 22 and 24, dc-link capacitors Cd21 and Cd22, voltages U21 and U22, and dc-link midpoint NP2.


The dc-link rails 22 of the parallel-connected ARCP inverters (positive dc-link potentials P) are connected to each other and to a first voltage terminal Udc+ of the common DC power source 4. The dc-link rails 24 of ARCP inverter modules (negative dc-link potentials N) are connected to each other and to a second voltage terminal Udc− of the common DC power source 4. Further, the neutral points NP1 and NP2 of the parallel-connected ARCP inverter modules may be connected to each other as shown in FIG. 3. The connection of the neutral points NP1 and NP2 is not essential to this invention, and they may as well be not connected to each other.


The common dc power input to the parallel-connected ARCP or hard-switching inverter modules INV1 and INV2 may be obtained from any kind of a dc power source 4, such as from an existing power supply network through a rectifier, or from a battery, fuel cell, photovoltaic array, etc. It shall be appreciated that dc-link 2 may be provided in a number of forms and may have a number of voltages and other attributes. It shall also be appreciated that the voltage difference between positive and negative dc-link rails is flexible, depending on how the dc-link 2 is charged or how the dc-link 2 is discharged by the connected circuits. For example, some embodiments may use a front-end isolation transformer and rectifier connected to the dc-link with the positive and negative rails floating and the differential voltage typically in the range of 50V-1500V, but in principle in other voltages outside this range as well. In other embodiments, the positive rail, mid-point, or negative rail may be grounded to earth. Preferably, the positive and negative rails are balanced. For example, if the dc-link neutral point NP is at 0 VDC, dc-link rail 22 would be at a positive voltage (e.g., in the range of +25 VDC to +500 VDC, the range of in the range of +150 VDC to +400 VDC or other positive voltage ranges) and dc-link rail 24 would be at a negative voltage corresponding to the positive voltage (e.g., in the range of −25 VDC to −500 VDC, the range of in the range of −150 VDC to −400 VDC or other negative voltage ranges corresponding to the other positive voltage ranges). It shall be appreciated that the foregoing examples are few of many voltage values and polarities that may be present in or associated with the operation of dc-link 2. It shall be additionally appreciated that the voltage values of the foregoing examples may be subject to fluctuation, margins of error, tolerance, and other variations and may not be rigidly fixed to the precise example values stated. It shall be further appreciated the term bus may be utilized in place of the term link such that, for example, references to a dc-link are understood to encompass a dc-bus and vice versa.


The exemplary ARCP inverters INV1 and INV2 illustrated in FIG. 3 may be three-phase bridge ARCP inverters including a power section 10U, 10V, and 10W for each phase or phase leg U1, U2, V1, V2, W1 and W2, respectively. Operation and configuration of the inverters INV1 and INV2 are illustrated and described in more detail primarily with respect to one phase or phase leg U1 and U2 herein, but the other phases or phase legs V1, V2, W1 and W2 of the inverters INV1 and INV2 can have identical operation and configuration. In the ARCP inverter INV1, the power sections 10U, 10V, and 10W of phase legs U1, V1 and W1 may be connected to the positive dc-link rail 22, the neutral point NP1, and the negative dc-link rail 24 of the common dc-link 2, and thereby to the negative (N), the neutral point (NP) and the positive (P) dc-link potentials, as illustrated in FIG. 2. The output node 110 of each power section 10U, 10V, and 10W is connected to the corresponding phase of an ac load 6, such as an ac motor or ac grid or any applicable electric load, via a non-zero impedance (presented generally by an output inductance Lo1 herein), which can consist of the impedance of connecting cable or busbar and it can also have additional elements if needed. In the ARCP inverter INV2, the power sections 10U, 10V, and 10W of phase legs U2, V2 and W2 may be connected to the common dc-link 2 of the inverter INV2 in a similar manner as in the inverter INV1. The phase output node 110 of each power section 10U, 10V, and 10W of the inverter INV2 is connected to the corresponding phase of the ac load 6 via a non-zero impedance (presented generally by an output inductance Lo2 herein), and thereby each phase output of the inverter INV2 is connected in parallel with the corresponding phase output of the inverter INV1. It should be appreciated that although a three-phase ARCP inverter is illustrated as an example herein, an ARCP inverter may be implemented as a single-phase inverter, or generally include any number of inverter phases or phase legs. Moreover, although a half-bridge ARCP inverter is illustrated as an example herein, the ARCP inverter may have other configurations, particularly a full-bridge configuration.


The exemplary half-bridge power section 10U of the ARCP inverter INV1 illustrated in FIG. 3 includes a pair of main or power switching devices S11 and S21 coupled in parallel to the dc-link rails 22 and 24 of the dc-link 2. The first main switching device S11 may have a first terminal electrically coupled to the positive dc-link rail 22 and a second terminal electrically coupled to an output node 110. The second main switching device S21 having a first terminal coupled to output node 110 and a second terminal coupled to the negative dc-link rail 24. Across the first main switching device S11 between the positive dc-link rail 22 and the output node 110 is connected a first antiparallel diode D11, and across the second main switching device S21 between the output node 110 and the negative dc-link rail 24 is connected a second antiparallel diode D21. Further, a first resonant capacitor C11 is operationally connected (i.e., directly or via additional components, such as an active or passive damping circuit series connected with the resonant capacitor) in parallel with the first main switching device S11, and a second resonant capacitor C21 is operationally connected in parallel with the second main switching device S21. More generally, there may be one or more resonant capacitors connected in such manner that at least one terminal of the resonant capacitor(s) is connected to one of the dc-link rails (P, NP, N) and the other terminal(s) is (are) operationally connected to the phase output node 110. The first main switching device S11 is operable to turn on and turn off, and thereby to respectively connect and disconnect the dc-link rail 22 and the output node 110, in response to control signal(s) G11 received from a control and driver circuitry, such as an inverter-specific ARCP switching controller 81 illustrated in FIG. 3. The second main switching device S21 is operable to turn on and turn off, and thereby to respectively connect and disconnect the dc-link rail 24 and the output node 110, in response to control signal(s) G21 received from the control and driver circuitry, such as the ARCP switching controller 81. All power sections 10U, 10V, and 10W of phase legs U1, V1 and W1 in the ARCP inverter INV1 may be controlled by the same inverter-specific switching controller 81. Similarly, the exemplary half-bridge power section 10U of the ARCP inverter INV2 illustrated in FIG. 3 includes a pair of main or power switching devices S12 and S22, a first antiparallel diode D12, and a first resonant capacitor C12, a second antiparallel diode D22, a second resonant capacitor C22, and switching control signals G12 and G22 from a control and driver circuitry, such as an inverter specific ARCP switching controller 82. All power sections 10U, 10V, and 10W of phase legs U2, V2 and W2 in the ARCP inverter INV2 may be controlled by the same inverter-specific switching controller 82. In embodiments, the switching devices S11, S12, S21 and S22 may be an insulated-gate bipolar transistor (IGBT), or another type of semiconductor switching device, such as an integrated gate-commutated thyristor (IGCT), a metal-oxide-semiconductor field-effect transistor (MOSFET), or a silicon carbide (SiC) MOSFET to name several examples.


In operation, when the first main switch S11/S12 is turned on (to a conductive state), a first switch current Is11/Is12 can flow between the dc-link rail 22 and the output node 110. Similarly, when the second main switching device S21/S22 is turned on (to a conductive state), a second switch current Is21/Is22 can flow between the output node 110 and the dc-link rail 24. On the other hand, when the first main switching device S11/S12 is turned off (to a non-conductive state), the first switch current Is11 will not flow in the switch-forward direction between the dc-link rail 22 and the output node 110, although a current Id11/Id12 may flow in the switch-reverse direction through the first anti-parallel diode D11/D12 of the first main switching device S11/S12. Similarly, when the second main switching device S21/S22 is turned off (to a non-conductive state), the second switch current Is21/Is22 will not flow in the switch-forward direction between the output node 110 and the dc-link rail 24, although a current Id21/Id22 may flow in the switch-reverse direction through the anti-parallel diode D21/D22 of the second switching device S21/S22. Thus, by turning on and off the first main switching device S11/S12 and the second main switching device S21/S22, the output voltage at the output node 110 will be controlled or commutated to be either the voltage P from the dc-link rail 22 or the voltage N from the dc-link rail 24. The purpose of the resonant capacitors C11/C12 and C21/C22 is to limit the voltage slew rate of the output node; this ensures that the voltages Uc11/Uc12 and Uc21/Uc22 across the main switching devices S11/S12 and S21/S22 do not significantly change during turn-off such that the main switching devices are turned off at essentially zero-voltage.


The exemplary half-bridge power section 10U of the ARCP inverter INV1 illustrated in FIG. 3 further includes an auxiliary circuit comprising a resonant inductor L1 and a bidirectional auxiliary switch Saux1 connected in series between the neutral point NP1 and the output node 110. The auxiliary switch Saux1 is operable to turn on and turn off, and thereby to respectively connect and disconnect the neutral point and the output node 110, in response to control signals received from the control and driver circuitry, such as the ARCP switching controller 81. The auxiliary switch Saux1 can behave like a bidirectional thyristor: it can be triggered into conduction, and it turns off if or before the current tries to reverse its direction. In embodiments, the bidirectional auxiliary switch Saux1 may be implemented with a pair of ordinary switching devices connected back-to-back, for example in a common-emitter or common-collector configuration and provided with anti-parallel diodes. FIG. 3 illustrates an exemplary auxiliary switch Saux1 comprising a first auxiliary switching device Sa11 and a second auxiliary switching device Sa21 in a common-emitter series connection, a first anti-parallel diode Da11 connected across the first auxiliary switching device Sa11, and a second antiparallel diode Da21 connected across the second auxiliary switching device Sa21. One of the two auxiliary switching devices Sa11 and Sa21 is turned on and conducting at a time, as is one of the two antiparallel diodes Da11 and Da21, in response to control signals Ga11 and Ga21 received from a control and driver circuitry, such as an ARCP switching controller 81 illustrated in FIG. 3. In each case, the auxiliary current Ia1 will flow through one diode in series with one switch. The auxiliary switching devices in the auxiliary circuit are turned on and off at zero-current. When the first auxiliary switching device Sa11 is turned on and the second switching device Sa21 is turned off, the auxiliary current Ia1 will flow in one direction through Sa11 and Da21. When the first auxiliary switching device Sa11 is turned off and the second switching device Sa21 is turned on, the auxiliary current Ia1 will flow in the opposite direction through Sa21 and Da11. The auxiliary circuit is only used when the output node 110 is required to commutate from one voltage rail to the other. The auxiliary circuit functions by creating a pulse of current that, in combination with the resonant capacitors, is used to slew the output voltage on the output node 110. Similarly, the exemplary half-bridge power section 10U of the ARCP inverter INV2 illustrated in FIG. 3 further includes an auxiliary circuit comprising a resonant inductor L2 and a bidirectional auxiliary switch Saux2 connected in series between the neutral point NP2 and the output node 110. In embodiments, the auxiliary switch Saux2 may be implemented with a pair of ordinary switches and antiparallel diodes in a similar manner as the auxiliary switch Saux1. FIG. 3 illustrates an exemplary auxiliary switch Saux2 comprising a first auxiliary switching device Sa12 and a second auxiliary switching device Sa22 in a series connection, a first anti-parallel diode Da12 connected across the first auxiliary switching device Sa12, and a second antiparallel diode Da22 connected across the second auxiliary switching device Sa22. One of the two auxiliary switching devices Sa12 and Sa22 is turned on and conducting at a time, as is one of the two antiparallel diodes Da12 and Da22, in response to control signals Ga21 and Ga22 received from a control and driver circuitry, such as an ARCP switching controller 82 illustrated in FIG. 3.


The switching control 81 . . . 8n illustrated in FIGS. 1, 2 and 3 refers generally to any control functions, logic, hardware, firmware, software, etc. required to control switching devices in the hard-switching or ARCP phase leg(s) based on a PWM signal or PWM signals. Given a PWM signal, a standard hard-switching inverter does not need too much additional logic to form a complete inverter drive system. At a minimum, the direct PWM signal is sent to one switch while the complement of the PWM input signal is sent to the other switch in that phase. The ARCP on the other hand, requires more than the PWM modulation and control: it requires an additional more complex control, particularly due to the auxiliary circuit and the auxiliary switch(es).



FIG. 4 is a schematic block diagram of an exemplary embodiment of an ARCP switching controller 81 having a PWM modulator 82 and ARCP control functions 84 separated. In the illustrated example, the ARCP control 84 may include a dedicated ARCP control module 841U, 841V, and 841W adapted to provide control signals, such as G11, G21, Ga11 and Ga21 to each ARCP phase leg U1, V1 and W1, respectively, based on a respective PWM signal PWMU, PWMV and PWMW received from the PWM modulator 82. The ARCP control 84, or the respective ARCP control module 841U, 841V, and 841W, may have to provide for instance the following functions for each phase leg U1, V1 and W1: Activation of the correct auxiliary switch before commutating the main switches, controlling the boost time, ensuring that the main switches are switched at essentially zero-voltage, ensuring that the auxiliary switches are switched at zero-current, initially starting the switching sequence upon power up, etc. Depending on a selected ARCP control strategy, various sensing feedbacks (FB) may be required to implement the control algorithms, such as feedback from main switch zero-voltage sensors, auxiliary switch zero-current sensors, an auxiliary current sensor, an output (load) current sensor, a dc-link voltage sensor, a dc-link capacitor sensor(s), a neutral point voltage sensor, etc.


As used herein, the mode of commutating the output current Io from a diode to a switch (e.g., the current Io1 from the diode D21 to the switch S11) in ARCP is called mode A and the mode of commutating the output current Io from a switch to a diode (e.g., the current Io1 from the switch S11 to the diode D21) is called mode B, when the auxiliary circuit is involved in commutation and a boost current is provided. The mode of commutating high output current Io from a switch to diode, when the output current Io itself is sufficient to drive the output voltage from one dc-link rail to another and the auxiliary circuit is not involved, is called mode O herein. The terms mode A and mode B are used herein also for hard-switching commutations from a diode to switch and switch to diode, respectively, e.g. in inverters illustrated in FIG. 2.


Mode A commutation: If the output current Io is positive (Io>0) and the output voltage Uo swings from the potential N (the dc-link 24) to the potential P (the dc-link 22), the lower diodes D21 and D22 commutate their currents (Id21 and Id22, respectively) to upper switches S11 and S12, respectively. If the output current Io is negative (Io<0) and the output voltage Uo swings from the potential P (the dc-link 22) to the potential N (the dc-link 24), the upper diodes D11 and D12 commutate their currents (Id11 and Id12, respectively) to lower switches S21 and S22, respectively.


Mode B commutation: If the output current Io is positive (Io>0) and the output voltage Uo swings from the potential P (the dc-link 22) to the potential N (the dc-link 24), the upper switches S11 and S12 commutate their currents to lower diodes D21 and D22, respectively. If the output current Io is negative (Io<0) and the output voltage Uo swings from the potential N (the dc-link 24) to the potential P (the dc-link 22), the lower switches S21 and S22 commutate their currents to diodes D11 and D12, respectively.


In the following, examples of typical ARCP commutation in modes A and B are briefly described for a single phase, e.g., the ARCP phase V1, of the ARCP inverter INV1. The commutation modes A and B of the corresponding the ARCP phase V2 of the ARCP inverter INV2 are similar.


As an example of the mode A, a commutation of the positive output current Io1 (Io>0) from the lower diode D21 to the upper main switch S11 and the output voltage Uo from N to P will described with reference to FIGS. 5A-5F.

    • The diode D21 is conducting the output current Io1 (=Id21), the diode D21 supplying the output current Io (FIG. 5A) and switches S11, Sa11 and Sa21 not conducting (turned off); during the commutation S21 turns off and S11 turns on.
    • The command for commutation arrives at time instant tAo. The auxiliary switch Sa11 is turned on (at zero current) after a time interval twA1, which marks the start of the boosting interval tbA1. The neutral point voltage UNP1 is applied across the resonant inductor L1, which causes the auxiliary current Ia1 through the resonant inductor L1 to ramp up linearly (FIG. 5C), and the current Id21 in diode D21 decreases accordingly as Id21=Io1−Ia1 (FIG. 5A). In order to turn the diode D21 off, the auxiliary current Ia1 must increase to the level of the output current Io1 and even beyond (by a boosting current IbA1), so that finally Ia1=Io1+IbA1. The boosting current portion IbA1 of the total inductor current Ia1 is diverted to the switch S21 parallel to the diode D21 (FIG. 5B) while the load 6 takes its own, i.e., the output current Io1.
    • The switch S21 is turned off after a time interval tbA1 (FIG. 5B), which marks the end of the boosting interval tba1, and the commutation swing of the output voltage Uc21 from N (zero) to P (the full Udc) starts. The boosting current IbA1 must be large enough to force the output potential swing from N to P, charging the capacitor C21 and discharging the capacitor C11. If there is a slight unbalance of the dc link voltage halves so that U21<U11, more boosting current is needed, and if U21>U11, less boosting current suffices.
    • The interval for the swing of UC21 from zero to Udc has duration tsA1.










t

sA

1


=




L
1


C


[



cos

-
1


(



U

c

21


-

U
dc






L
1

/
C




I
pA



)

-
β

]





(
1
)







where

    • IpA1 is the peak value of the resonant part of the inductor current










I

pA

1


=




CU

c

21

2


L
1


+

I

bA

1

2







(
2
)









    • β is a phase angle












β
=


sin

-
1


(


I
bA

/

I
pA


)





(
3
)









    • and C=C11+C21 in the exemplary topology shown in FIG. 3. The voltage change rate average is du/dt=Udc/tsA1.





When Uc21 reaches Udc and Uc11 reaches zero after a time interval tsA1 (FIG. 5D), the portion of the auxiliary current Ia1 exceeding the output current Io1 turns on the diode D11 and is called ItA1 (FIGS. 5C and 5D). The switch S11 may be turned on as soon as Uc21 has reached Udc. The boosting time tbA1 may preferably be set to a value that minimizes the current ItA1 close to zero. This way the losses and the reverse recovery current of D11 will be minimized, as well as the duration of the commutation. This strategy narrows the window ttAx. Thus, the precise timing of S11 turn-on is critical.

    • Because the diode D11 and the switch S11 clamp the output voltage to the positive dc potential P, the inductor current Ia1 decays linearly to zero during a time interval is ttA (FIG. 5C).
    • The current Id11 decays first from ItA1 to zero in time ttAx, whereafter the switch current Is11 increases linearly from zero to the load current level Io1 (FIG. 5F) while Ia1 continues to decrease from Io1 towards zero (FIG. 5C), after which the auxiliary diode Da21 turns off and the commutation sequence is finished.
    • The total duration of the commutation from the turn-on of the auxiliary switch Sa21 to completion in mode A is tA=tbA1+tsA1+ttA1. There is a current in the auxiliary branch during this time interval.


As an example of the mode B, a commutation of the positive output current Io1 (Io>0) from the upper main switch S11 to the lower diode D21 and a swing of the output voltage Uo from N to P will described with reference to FIGS. 6A-6D.

    • The switch S11 is conducting the output current Io1 (Io1=Is11) (FIG. 6A) and switches S21, Sa11 and Sa21 not conducting (turned off); during the commutation the upper switch S11 turns off and the lower diode D21 turns on.
    • The command for commutation arrives at time instant tB0. After a waiting time twB1, the auxiliary switch Sa21 is turned on, and boosting current IbB1 (in negative direction in the inductor L1, positive direction in S11) is linearly built up for a time tbB1 (FIG. 6B).
    • The boosting current adds on top of the load current in the switch S11, which turns off a total current of Is11=Io1+IbB1 at the end of tbB1 (FIG. 6A). The swing of Uc11 from zero to Udc starts (FIG. 6C). The output potential swing from P to N is a combination of the linear portion caused by Io1 and a resonant portion caused by IbB1. The duration of the swing is tsB1










t

sB

1


=




L
1


C


[



cos

-
1


(



U

c

11


-

U
dc






L
1

/
C




I

pB

1




)

-

π
2

-
γ

]





(
4
)







where

    • IpB1 is the peak value of the resonant part of the inductor current,










I

pB

1


=




CU

c

11

2


L
1


+


(


I

o

1


-

I

bB

1



)

2







(
5
)









    • γ is a phase angle,












γ
=


tan

-
1


(




C
/

L
1





U

c

11





-

I

o

1



+

I

bB

1




)





(
6
)









    • and C=C11+C21. The voltage change rate average is du/dt=Udc/tsB1.

    • The remaining current Ia1 in the inductance at the end of the swing adds initially on top of the output current Io1 in the diode D21 so that Id21=Io1+ItB. The diode current decays linearly to the final value Io, as the inductor current reaches zero again after time ttB (FIGS. 6B and 6D). The total duration of the commutation in mode B from the triggering of Sa to completion is tB=tbB+tsB+ttB.





The descriptions above for modes A and B assumed a positive direction of Io. The operation for a negative Io (Io<0) is identical, just the roles of S11 and S21, D11 and D21, and Uc11 and Uc21 are swapped from mode A to mode B, and vice versa.


The commutation for a corresponding phase in the plurality of parallel-connected inverters can be initiated by similar commutation commands at the same time instant. For example, the ARCP commutation for the ARCP phase V1 of the ARCP inverter INV1 and the ARCP phase V2 of the ARCP inverter INV2 can be initiated by similar commutation commands at the time instant tAo for mode A commutation and at the time instant tBo for mode B commutation. In an ideal case, the output currents Io1 and Io2 of the parallel-connected ARCP inverter would be equal. However, the ideal behavior during commutations would require that the corresponding switches, e.g., S11 and S12, in the parallel operated inverter turn on at the same instant when commutating the output potential Uo, for example from N to P. Likewise, they should turn off at the same instant when commutating the output potential from P to N. Unfortunately, the parallel operated inverters do not behave similarly, for example due to parameter differences of switch components and differing impedances in parallel branches, the output currents from the parallel inverters can be unequal in value. In other words, there can be uneven current sharing between the inverters. Due to thermal and economic reasons, it is of utmost importance that the parallel-connected inverters share the load current as evenly as possible.


According to an aspect of the invention, current sharing between the plurality of parallel-connected ARCP or hard-switching converter legs is balanced by a control arrangement, such as the switching controls functions 84 or switching control module 841U, 841V, and 841W. FIG. 7 shows a flow diagram illustrating an exemplary operation of the control arrangement. The control arrangement may sense the leg output current Io in each of the parallel-connected converter legs (step 72) and have an individual autonomous leg-specific switching instant adjustment for the main switches of each of the parallel-connected converter legs to shift the first mode A commutation of the respective converter leg later in time and to shift the second mode B commutation of the respective converter leg earlier in time by a variable timestep proportional to the value of the sensed leg current of the respective converter leg (step 74). In other words, if the value of the sensed leg output current in one converter leg is larger than in the other converter leg, then in mode A, the higher-current leg will commutate later than the leg with less current, and in mode B, the higher-current leg will commutate earlier than the leg with less current.


Ideally, when the current sharing is in balance, the output currents of the parallel-connected converter legs (e.g., phase legs U1 and U2 in FIG. 3) are equal and their difference or a differential output current Ido is zero, (e.g., Ido=Io1−Io2=0). For example, if the sensed leg output currents of the parallel-connected converter legs had equal values, the autonomous switching instant adjustments of the parallel-connected legs would (independently from each other, each based on its own sensed leg output current only) result in commutating their output voltage swings to start approximately simultaneously. On the other hand, if the sensed leg output currents of the parallel-connected legs had different values, the autonomous switching instant adjustments of the legs would (independently from each other) result in commutating their output voltage swings to start differently, i.e. earlier or later, each depending on its own sensed leg output current value in manner (in a direction) that a differential output current (e.g., Ido=Io1−Io2) is reduced. In other words, these differences in the starting instant of the output voltage swings (e.g., Uc21 and Uc22, referred to the N potential in FIG. 3) would create an effective volt-second difference to the loop inductance (ΔL=Lo1+Lo2) in a direction that tends to reduce the output current difference Ido. The shifting of the output voltage swing in time may also be called as pulse shifting. Thereby, the control arrangement can fine tune the switching instants so that a commutation-induced output current difference between the parallel-connected inverter legs towards zero, while the switching instants may otherwise be generated in a conventional manner.


Advantageously, the parallel inverter legs do not need to know about each other's currents or the differential current, but the balanced current sharing by adjusting boost current can be embodied relying only on information that is readily available separately in each of the parallel-connected legs, i.e. output current value (e.g., Io1 or Io2). The benefit of an autonomous (or distributed or decentralized) control stems from avoiding the need for information exchange between higher-level control and lower-level control entities or between the lower-level control entities, such as the switching controls 81 and 82. The autonomous control system is usually also simpler and more modular compared to a centralized one, thus it easier to understand and maintain. Further, to keep the implementation cost effective, it would be preferable that there would not be any extra requirements for component selection or communication needs between the parallel-connected inverter units, i.e., the normal “single inverter units”, such as the inverters INV1 and INV2, could be parallel as such. The challenge on the other hand is obvious: the autonomous units must operate with a limited information. This challenge is overcome with embodiments of the present invention.


In a typical case the the parallel-connected converter legs have similar nominal leg current ratings. In embodiments, the autonomous leg-specific switching instant adjustment of all parallel-connected converter legs have the same first predetermined dependence on the value of the sensed leg current of the respective converter leg in mode A commutation and a same second predetermined dependence in the mode B commutation.


However, the the autonomous leg-specific switching instant adjustment of the invention can be applied also in a case the parallel connected phase legs have different nominal current ratings. In embodiments, predetermined first and second dependences of different parallel-connected converter legs having different nominal leg current ratings are selected to scale the current sharing between the between the parallel-connected converter legs according to nominal leg currents of the parallel-connected converter legs.


Let us examine an example of an autonomous leg-specific switching instant adjustment according to principles of the invention applied in an ARCP converter system, such as the system illustrated in FIG. 3. Generally, turn-on instants of the auxiliary switches and turn-off instants of the main switches are both shifted by a same amount, applicable both in mode A and mode B. This means that each ARCP commutation sequence is shifted as such in time. The amount of shifting is determined autonomously in the parallel connected legs 1 and 2, based on their respective leg output currents Io1 and Io2. The durations of boosting times and boosting current levels are not affected by the shifting due to the autonomous leg-specific switching instant adjustment according to the embodiments of the invention. It should be appreciated that the boosting currents might have been manipulated if some other control methods relying on such manipulation were applied simultaneously. The example presented herein assumes that both converter legs aim for identical boost currents, reference values for the boost currents being IbA1,r1=IbA,r2 for mode A, and IbB,r1=IbB,r2 for mode B.



FIGS. 8A-8C show an exemplary timing diagram that schematically illustrates the principle of the shifting for a single converter leg. In the illustrated timing diagram, FIG. 8A shows a PWM signal as providing commutation commands that are simultaneously applied to each of the parallel-connected converter legs to initiate the commutations. In the illustrated example, a leading (rising) edge of the incoming PWM signal initiates a Mode B commutation at the instant tB0 and a trailing (falling) edge initiates a Mode A commutation the time instant tA0. FIG. 8B shows schematically the timing of the auxiliary current Ia of a single converter leg. For simplicity, the auxiliary current Ia is shown only for the boosting periods tbB and tbA. FIG. 8C shows schematically the timing of the capacitor voltage VC2, i.e. the output voltage swing. Again, for simplicity, the swing times of the voltage VC2 are reduced to zero. In the illustrated example the mode B commutation is advanced, and the mode A commutation is delayed in proportion to the sensed value of the output current Io. The output current Io is assumed to be of negative polarity in FIGS. 8A-8B, but Io should be interpreted as the absolute value of Io as will be discussed in in equations below. Therefore, the polarity of the output current does not affect on the basic principles of the autonomous leg-specific switching instant adjustment method according to embodiments of the invention.


Let us assume that leg output current Io is positive, and that Io1>Io2 so that the differential output current Id>0. In mode A, the turn-off instant toffS21 of the lower main switch S21 starts the voltage swing in the APCP inverter leg INV1 and the turn-off instant toffS22 of the lower main switch S22 starts the voltage swing in the APCP inverter leg INV2. In mode B, the turn-off instant of upper main switch S11 starts the voltage swing in the APCP inverter leg INV1 and the turn-off instant toffS12 of the lower main switch S12 starts the voltage swing in the APCP inverter leg INV2.


In an exemplary embodiment, let us define the difference in the turn-off instants of the main switches in mode A as follows










Δ


t

S

2



=


t

offS

21


-

t

offS

22







(
7
)







In mode B the difference in the turn-off instants is defined as










Δ


t

S

1



=


t

offS

11


-

t

offS

12







(
8
)







where toffS21 and toffS22 are the turn-off instants in mode A for S21 and S22, respectively. Likewise, toffS11 and toffS12 are the turn-off instants in mode B for S11 and S12, respectively.


Allowing for the possibly unequal swing intervals tsA1 and tsA2 in mode A, the effective total timing difference during the commutation is










Δ


t
A


=

-

(


Δ


t

S

2



+



t

sA

1


-

t

sA

2



2


)






(
9
)







Likewise, allowing for the possibly unequal swing intervals tsB1 and tsB2 in mode B, the effective total timing difference during the commutation is










Δ


t
B


=


Δ


t

S

1



+



t

sB

1


-

t

sB

2



2






(
10
)







Under the assumption of positive output current Io, a positive ΔtA or ΔtB will increase the differential current Id=(Io1−Io2)/2 by










Δ


I

d

A



=


Δ


t
A



U
dc



L
d






(
11
)







in mode A, and by










Δ


I
dB


=


Δ


t
B



U
dc



L
d






(
12
)







in mode B.


In mode A, if the converter leg INV1 turns off its lower switch S21 later than the converter leg INV2 turns off its lower switch S22, the difference ΔtS2 in the turn-off instants will be positive. Hence ΔtA in the equation (9) will have a negative term, which will make the differential current ΔIdA in the equation (11) definitely negative, provided the swing times tsA1 and tsA2 are equal (i.e. boost currents IbA1=IbA2, which practically means for the equivalent boost time intervals tbA1=tbA2).


If the whole commutation sequence from the turn-on of the auxiliary switch to the turn-off of the main switch in mode A is adjusted to happen later in the converter leg that has higher output current value, the differential current ΔIdA will be decreased. To achieve this desired behavior, the turn-on instants tonSa1 of the auxiliary switches Sa1 can be delayed from the instant tA0 in both legs by individual variable increments or timesteps










t

wA

1


=


k
A





"\[LeftBracketingBar]"


I

o

1




"\[RightBracketingBar]"







(
13
)








and









t

wA

2


=


k
A






"\[LeftBracketingBar]"


I

o

2




"\[RightBracketingBar]"


.






(
14
)







The boosting times tbA1 and tbA2 are not altered. The factor proportional control gain kA is a design parameter (a positive constant) that should be equal for both legs if their nominal current ratings are equal. In order to shift the whole commutation sequence in time, the reference values for turn-off instants of S21 and S22 will be delayed as well by individual variable increments or timesteps twA1 and twA2.










t


offS

21

,
r


=


t

wA

1


+

t

bA
,
r







(
15
)













t


offS

22

,
r


=


t

wA

2


+

t

bA
,
r







(
16
)







where it is assumed that the reference boosting times tbA,r (and the corresponding reference boosting currents IbA,r) are equal in the legs.


Since |Io1|>|Io2|, the autonomous leg-specific switching instant adjustment method makes the lower switch S21 in the converter leg INV1 turn off later than the lower switch S22 in the converter leg INV2










Δ


k


S

2

,
r



=



t


offS

21

,
r


-

t


offS

22

,
r



=


k
A

(




"\[LeftBracketingBar]"


I

o

1




"\[RightBracketingBar]"


-



"\[LeftBracketingBar]"


I

o

2




"\[RightBracketingBar]"



)






(
17
)







This way a term kA(|Io1|−|Io2|) will be added to the difference ΔtS2 in the turn-off instants of the main switches, which tends to make the difference ΔtS2 more positive (since |Io1|>|Io2|), thereby reducing the differential current Id. In embodiments, the factor kA may conveniently have units in [ns/A] and may perhaps attain a value of 0.5 . . . 2, so that a differential current of 50 A, for example, would make a 50 ns . . . 200 ns change in the timing difference ΔtS2.


Similar reasoning can be applied to mode B, but now the converter leg with higher current must shift its commutation sequence earlier in time. Because the incoming PWM edge that provides the command to start commutation cannot be advanced in time, the incoming PWM edge is, in embodiments, first conceptually “delayed” by a constant time tc from the instant tB0 for both converter legs. Thereby an adjustment range is provided to allow advancing in time from this “delayed” command. In embodiments, in each parallel-connected converter leg, the turn-on instant tonSa2 of the auxiliary switch Sa2 will happen after a variable waiting interval or time step twB from the incoming PWM edge (the instant tB0) according to










t

w

B


=


t
c

-


k
B





"\[LeftBracketingBar]"


I

o

1




"\[RightBracketingBar]"








(
18
)







where kB is the advancement factor (a positive constant). The turn-off instant toffS1 of the upper main switch S1 is










t

offS

1


=


t

w

B


+

t

b

B







(
19
)







As the output current Io gets higher, the waiting interval twB gets smaller, and because the boosting time tbB is not altered, the turn-off instant toffS1 will get advanced in time, which was the goal.


In the illustrated example, the parallel connected legs INV1 and INV2 would accordingly calculate their respective waiting times to be










t

wB

1


=


t
c

-


k
B





"\[LeftBracketingBar]"


I

o

1




"\[RightBracketingBar]"








(
20
)








and









t

wB

2


=


t
c

-


k
B





"\[LeftBracketingBar]"


I

o

2




"\[RightBracketingBar]"








(
21
)







so that the reference values for turn-off instants for the switches S11 and S12 will be










t


offS

11

,
r


=


t

wB

1


+

t


b

B

,
r







(
22
)








and









t


offS

12

,
r


=


t

wB

2


+

t


b

B

,
r







(
23
)







where it is assumed that the reference boosting times tbB,r (and the reference boosting currents IbB,r) are equal in the legs.


Since |Io1|>|Io2|, the autonomous leg-specific switching instant adjustment method makes the upper switch S11 in the converter leg INV1 turn off earlier than the upper switch S12 in the converter leg INV2:










Δ


t


S

1

,
r



=



t


offS

11

,
r


-

t


offS

12

,
r



=

-


k
B

(




"\[LeftBracketingBar]"


I

o

1




"\[RightBracketingBar]"


-



"\[LeftBracketingBar]"


I

o

2




"\[RightBracketingBar]"



)







(
24
)








FIGS. 9A and 9B show timing diagrams for exemplary simulations that illustrate the operation of the autonomous leg-specific switching instant adjustment method according to embodiments of the invention for negative output current Io. The bottom traces Io1 and Io2 that converge close to each other represent the output currents of the parallel converter legs. Factors kA and kB in equations (13)-(14) and (20)-(21) were set at 1 ns/A. The square-wave signal PWM represents an incoming PWM command and the higher amplitude sloping signals represent a leg output voltage Uo referenced to the N potential. Note that the effective voltage pulse length of U0 increases as the total output current increases. This is a drawback of the method as it will cause current-dependent distortion, which, however, can be compensated with state-of-the art methods. FIGS. 9A and 9B also illustrate a behavior of the auxiliary current Ia in modes A and B. Auxiliary current pulses Ia are positive for mode B and negative for mode A.


In FIG. 9A, the total output current Io=Io1+Io2 of the parallel-connected converter legs was −200 A, but it was initially shared unevenly between the converter legs INV1 and INV2, the leg output current Io1 of the leg INV1 being −90 A and the leg output current Io2 of the leg INV2 being −110 A. When the output current is relatively low in FIG. 9A, the auxiliary current Ia is large in mode B and small in mode A. Since |Io2|>|Io1|, the method causes the mode B commutation of the leg INV2 to start earlier than the leg INV1, and thereby the auxiliary current Ia2 of the leg INV2 and the output voltage swing Uo are started (i.e. the main switch S2 turned off) slightly earlier than the Ia1 and the Uo of the leg INV1. As a result, the output currents Io1 and Io2 converge towards each other and are aligned already after mode B commutation, as illustrated in FIG. 9A. In an ideal case, when the output currents Io1 and Io2 are now equal, also the auxiliary currents and the output voltage swings of the parallel-connected legs are now approximately aligned in subsequent commutations.


In FIG. 9B, the total output current Io=Io1+Io2 of the parallel-connected converter legs was −1800 A, but it was initially shared unevenly between the converter legs INV1 and INV2, the leg output current Io1 of the leg INV1 being −720 A and the leg output current Io2 of the leg INV2 being −980 A. As the output current increases in FIG. 9B as compared with FIG. 9A, the auxiliary current Ia decreases in mode B and increases in mode A. In mode B, the output current speeds up the voltage swing in the resonant capacitors, hence there is less time for the auxiliary current to develop in the resonant inductor at higher output currents. In mode A, the auxiliary current must always be larger than the output current before the output voltage swing can start (i.e., main switch S2 is turned off.) In FIG. 9B, since |Io2|>|Io1|, the method causes the mode B commutation of the leg INV2 to start earlier than the leg INV1, and thereby the auxiliary current Ia2 of the leg INV2 and the output voltage swing Uo are started (i.e. the main switch S2 turned off) earlier than the Ia1 and the Uo of the leg INV1. As a result, although the output currents Io1 and Io2 converge towards each other during the first mode B commutation, they are still unequal, as illustrated in FIG. 9A. In the subsequent mode A commutation, as |Io2|>|Io1|, the method causes the mode A commutation of the leg INV2 to start later than the leg INV1, and thereby the auxiliary current Ia2 of the leg INV2 and the output voltage swing Uo are started (i.e. the main switch S2 turned off) later than the Ia1 and the Uo of the leg INV1. Now, the output currents Io1 and Io2 converge towards each other and are aligned during mode B commutation, as illustrated in FIG. 9B. In an ideal case, the output currents Io1 and Io2 as well as the auxiliary currents and the output voltage swings of the parallel-connected legs are now approximately aligned in subsequent commutations.


The autonomous leg-specific switching instant adjustment method can be applied to parallel connected hard-switching (HS) converter legs, such as the HS legs shown in FIG. 2. In that case, the mode A corresponds to a turn-on of a main switch that will start conducting (the current is commutated from a diode to the switch), and the mode B corresponds to turn-off of a switch that has been conducting (the current is commutated from the switch to a diode).


Let us examine exemplary cases for balance a current sharing between the parallel-connected HS inverter legs shown in FIG. 2 according to embodiments of the invention.


First, an exemplary commutation from the upper dc-rail 22 (UDC+) to the lower dc-rail 24 (UDC−), i.e. the turn-off sequence of the upper main switch S11 and turning on the lower main switch S21 in INV1 and respectively the turn-off sequence of the upper main switch S12 and turning on the lower main switch S22 in INV2 is described:


HS1) The upper switch S11 respectively S12 is on and the leg output 110 is connected to the upper dc-rail 22 (UDC+).


HS1.pos) If the current is positive, Io>0, the upper switch S11 respectively S12 carries the current and the turn-off event is similar to a Mode B (from the switch to a diode) commutation in the ARCP converter:

    • a) Similar to the ARCP mode B commutation, the converter leg with higher current must shift its commutation sequence earlier in time. Because the incoming PWM edge that provides the command to start commutation cannot be advanced in time, the incoming PWM edge is, in embodiments, first conceptually “delayed” by a constant time tc from the instant tB0 for both converter legs. Thereby an adjustment range is provided to allow advancing in time from this “delayed” command, i.e. the total delay decreases with the increasing leg output current. According to embodiments, the turn-off event of the upper switch S11 respectively S12 is advanced by a variable timestep td,off=tc−koff*|Io|, where koff is the advancement factor (a positive constant) corresponding to the KB1 in the ARCP mode B.
    • b) The output current Io1 respectively Io2 commutates to the lower diode D21 respectively D22.
    • c) In embodiments, the lower main switch S21 respectively S22 may be turned on after a predetermined turn-on delay tD, which is typically used in the art to prevent simultaneous conducting of upper and lower switches, i.e. to avoid DC-link short, in hard-switching converters.
    • d) The leg output 110 is connected to the lower dc-rail 24 (UDC−).
    •  HS1.pos) If the current is negative, Io<0, the upper diode D11 respectively D12 carries the current Io1 respectively Io2 and the turn-off event is similar to Mode A (from diode to switch) commutation in the ARCP converter:
    • a) According to embodiments, the turn-off event of upper switch S11 respectively S12 is not delayed at all, it can happen immediately. The upper diode D21 respectively D22 remains conducting.
    • b) Similar to the ARCP mode A commutation, the commutation is delayed in proportion to the sensed value of the output current Io1 respectively Io2 of the leg. In embodiments, the turn-on event of the lower switch S21 respectively S22 is delayed by a variable timestep td,on=tD+Kon*|Io|, where tD is the predetermined turn-on delay and Kon is a factor proportional control gain (a positive constant) corresponding to kA in the ARCP mode A.
    • c) The current Io1 respectively I02 commutates to lower switch S21 respectively S22 and the leg output 110 is connected to the lower dc-rail 24 (UDC−).


Similarly, commutation from the lower dc-rail 24 (UDC−) to the upper dc-rail 22 (UDC+), turn-off sequence of the lower switch S21 respectively S22 and turning on the upper switch S11 respectively S12:


HS2) The lower switch S21 is on in the leg INV1 and respectively the lower switch S22 is on in the leg INV2 and the leg output 110 is connected to the lower dc-rail 24 (UDC−) in each leg.


HS2.pos) If the current is positive, Io>0, the lower diode D21 respectively D22 carries the current and the turn-off event is similar to Mode A (from diode to switch) commutation in the ARCP converter:

    • a) According to embodiments, the turn-off event of lower switch S21 respectively S22 is not delayed at all, it can happen immediately. The lower diode D21 respectively D22 remains conducting.
    • b) Similar to the ARCP mode A commutation, the commutation is delayed in proportion to the sensed value of the output current Io1 respectively Io2 of the leg. In embodiments, The turn-on event of the upper switch S11 respectively S12 is delayed by a variable timestep td,on=tD+kon*|Io|, where tD is the predetermined turn-on delay and kon is a factor proportional control gain (a positive constant) corresponding to kA in the ARCP mode A.
    • c) The current Io1 respectively Io2 commutates to upper switch S11 respectively S12 and the leg output 110 is connected to the upper dc-rail 22 (UDC+).


HS2.neg) If the current is negative, Io<0, the lower switch S21 respectively S22 carries the current and the turn-off event is similar to Mode B (from switch to diode) commutation in the ARCPI converter:

    • a) Similar to the ARCP mode B commutation, the converter leg with higher current must shift its commutation sequence earlier in time. In embodiments, the turn-off event of lower switch S21 respectively S22 is delayed by a variable timestep td,off=tc−koff*|Io|, where, tc is the constant delay time for both converter legs from the incoming PWM edge that provides the command to start commutation, similar to instant tB0 in case of ARCP, and koff is the advancement factor (a positive constant) corresponding to the kB1 in the ARCP mode B.
    • b) The current Io1 respectively Io2 commutates to the upper diode D11 respectively D12.
    • c) Upper switch S11 respectively S12 is turned on after a predetermined turn-on delay tD, which is typically used to prevent simultaneous conducting of upper and lower switches, i.e. to avoid DC-link short, in hard-switching converters.
    • d) The leg output 110 is connected to the upper dc-rail 22 (UDC+).


The the autonomous leg-specific switching instant adjustment according to the invention can be applied also in a case the parallel connected phase legs having different nominal current ratings. Due to thermal and economic reasons, it is of utmost importance that the legs are loaded as close to their respective nominal ratings as possible.


In case of different nominal ratings, IN1 and IN2, the desired current share should be








I

o

1



I

o

2



=




I

N

1



I

N

2





or




I

o

1



I

N

1




=


I

o

2



I

N

2








Let us denote the ratio Io1/IN1 by r1 and the ratio Io2/IN2 by r2. Because Io1 and Io2 are time-varying quantities (typically sinusoidal), the ratios r1 and r2 are also time-varying. In an ideal current sharing, obviously r1=r2.


Let us examine connecting ARCP converter legs of different nominal current ratings in parallel. In mode B, the load current Io is participating in the voltage swing in charging and discharging the resonant capacitors C11 and C12. This feature provides a natural current balancing mechanism in parallel connected ARCP legs, because the leg with higher ratio r will have a faster voltage swing, which tends to make the difference r1−r2 smaller in value. It can be shown that the natural balancing in mode B tends to make the voltage swing slopes in the parallel ARCP legs identical during the commutation. (Provided that there are no deviations in the turn-off instants of the main switches.)


Let us assume the resonant capacitances C11/C21 and C12/C22 of the converter legs INV1 and INV2 are substantially different, e.g. 1 μF in total in the leg INV1, but only 500 nF in total in the leg INV2. This would be the case if the leg INV1 was dimensioned for twice the nominal current of the leg INV2 so that IN1=2IN2. Accordingly, the resonant inductance L1 in the leg INV1 would be dimensioned to be one half the resonant inductance L2 in the leg INV2, so that the resonant frequencies in both legs would be equal. It will turn out that under such circumstances the leg INV1 tends to have twice the output current of the leg INV1. Otherwise, the voltage slopes would not be identical. Under these conditions, mode B forces the parallel-connected legs towards sharing their currents in a ratio of 2:1. This takes place without any control, it is just a natural feature of the circuit. Deviations in timing and elsewhere act against this ideal situation, but the effect is quite strong.


In embodiments, the factors kA and kB in equations (13), (14) and (20), (21) are selected to scale with the nominal current in both legs INV1 and INV2 according to kA1IN1=kA2IN2 and kB1IN1=kB2IN2, where kA1 and kB1 are factors and IN1 is the nominal current of the leg INV1, and kA2 and kB2 are factors and IN2 is the nominal current of the leg INV2. The scaling can be applied to any number of parallel legs. In the special case where the parallel-connected converter legs have equal nominal leg currents, i.e. IN1=IN2 . . . =INN, also the factors kA and kB are equal for all converter legs, i.e. kA1=kA2 . . . =kAN and kB1=kB2 . . . =kBN.



FIG. 10 shows a timing diagram for an exemplary simulation that illustrates a situation, where two ARCP converter legs dimensioned for nominal currents in ratio 2:1 are connected in parallel. The dimensions for the ARCP leg INV1 were C11=C21=500 nF, L1=625 nH, kA1=1, kB1=1, Lo1=625 nH, IbA,r1=IbB,r1=150 A. The dimensions for the ARCP leg INV2 were C12=C22=250 nF, L2=1250 nH, kA2=2, kB2=2, Lo2=1250 nH, IbA,r2=IbB,r2=75 A. Thus, the targeted current sharing between the converter legs was 2:1. The autonomous current balancing was applied for both converter legs INV1 and INV2. Total output current is −1350 A, initially shared evenly −675 A and −675 A. Furthermore, the main switch turn-off instants were delayed 50 ns in the leg INV2, and auxiliary switch turn-on instants were delayed 100 ns in the leg INV2 in the simulation to show the balancing algorithm effectiveness in case of practical non-idealities. The initial condition had equal current sharing, which was wildly off the target as the leg INV1 should take −900 A and the leg INV2 should take −450 A. Two carrier periods in this simulation were enough to pull the leg output currents Io1 and Io2 very close to the desired values. This happens despite the errors introduced in the switching instants and mismatch of the main switch and diode characteristics.


Similarly, the autonomous leg-specific switching instant adjustment according to the invention can be applied also in a case the parallel connected hard-switching converter legs having different nominal current ratings. In embodiments, the factors kon or koff in the parallel-connected hard-switching legs are selected to scale with nominal leg currents IN1 and IN2 of the converter legs INV1 and INV2 such that a product of the constant kon and the nominal leg current IN is same in both parallel-connected converter legs and a product of the constant koff and the nominal leg current IN is same in both parallel-connected converter legs, i.e. kon1IN1=kon2IN2 and koff1IN1=koff2IN2. The scaling can be applied to any number of parallel legs. In the special case where the parallel-connected converter legs have equal nominal leg currents, i.e. IN1=IN2 . . . =INN, also the factors kon and koff are equal for all converter legs, i.e. kon1=kon2 . . . =konN and koff1=koff2 . . . =koffN.


The switching control and current sharing techniques described herein may be implemented by various means. For example, these techniques may be implemented in hardware (one or more devices), firmware (one or more devices), software (one or more modules), or combinations thereof. For a firmware or software, implementation can be through modules (e.g., procedures, functions, and so on) that perform the functions described herein. The software codes may be stored in any suitable, processor/computer-readable data storage medium(s) or memory unit(s) and executed by one or more processors/computers. The data storage medium or the memory unit may be implemented within the processor/computer or external to the processor/computer, in which case it can be communicatively coupled to the processor/computer via various means as is known in the art. Additionally, components of systems described herein may be rearranged and/or complimented by additional components in order to facilitate achieving the various aspects, goals, advantages, etc., described with regard thereto, and are not limited to the precise configurations set forth in a given figure, as will be appreciated by one skilled in the art.


The description and the related drawings are only intended to illustrate the principles of the present invention by means of examples. Various alternative embodiments, variations and changes are obvious to a person skilled in the art on the basis of this description. The present invention is not intended to be limited to the examples described herein but the invention may vary within the scope and spirit of the appended claims.

Claims
  • 1. A power converter system, comprising two or more converter legs connected in parallel between a common dc system and a common ac system or between two common dc systems, wherein each of said converter legs includes a first controllable main switching device with a first antiparallel diode and a second controllable switching device with a second antiparallel diode connected in series between a first DC voltage rail and a second DC voltage rail to alternatively connect the first and second dc-link rails to a converter leg output or input,wherein each parallel-connected converter leg includes a mode A of commutation wherein a leg current commutates from the first or second antiparallel diode to the second or first controllable main switching device, respectively, and a mode B of commutation wherein the leg current commutates from the first or second controllable main switching device to the second or first antiparallel diode, respectively,wherein commutations of the parallel-connected converter legs are initiated by essentially simultaneous commutation commands,a control arrangement configured to sense the leg current in each of the parallel-connected inverter legs, and wherein the control arrangement is configured to balance a current sharing between the parallel-connected inverter legs by means of having an individual autonomous leg-specific switching instant adjustment for the main switches of each of the parallel-connected converter legs to shift the mode A commutation of the respective converter leg later in time and to shift the mode B commutation of the respective converter leg earlier in time by a variable timestep proportional to the value of the sensed leg current of the respective converter leg.
  • 2. The power converter system as claimed in claim 1, wherein each individual autonomous leg-specific switching instant adjustment is configured to shift a start of a leg voltage swing during the mode A commutation of the respective converter leg later in time and to shift a start of a leg voltage swing during the mode B commutation of the respective converter leg earlier in time by a variable timestep proportional to the value of the sensed leg current of the respective converter leg.
  • 3. The power converter system as claimed in claim 1, wherein the size of the variable timestep of an individual shift later in time during an individual mode A commutation and the size of the variable timestep of an individual shift earlier in time during an individual mode B commutation are configured to be dependent on the value of the sensed leg current of the respective converter leg in such a way that the size of the variable timestep of individual shift in time increases with the increasing value of the sensed leg current and decreases with the decreasing value of the sensed leg current.
  • 4. The power converter system as claimed in claim 1, wherein each individual autonomous leg-specific switching instant adjustment of the main switching devices has a first predetermined dependence on the value of the sensed leg current of the respective converter leg in mode A commutation and a second predetermined dependence in the mode B commutation, and wherein optionally the predetermined first and second dependences of different parallel-connected converter legs having different nominal leg current ratings are selected to scale the current sharing between the between the parallel-connected converter legs according to nominal leg currents of the parallel-connected converter legs.
  • 5. The power converter system as claimed in claim 1, wherein the parallel-connected converter legs are auxiliary resonant commutated pole (ARCP) converter legs, particularly ARCP half-bridge legs, and wherein the control arrangement is configured to advance each ARCP mode B commutation sequence and delay each ARCP mode A commutation sequence in time in such a way that the size of the variable timestep increases with the increasing value of the sensed leg current and decreases with the decreasing value of the sensed leg current-of the respective converter leg.
  • 6. The power converter system as claimed in claim 5, wherein the ARCP commutation sequence includes a sequence from a turn-on instant of at least one auxiliary switching device to a turn-off instant of the main switching device that has been conducting.
  • 7. The power converter system as claimed in claim 5, wherein the control arrangement is configured to delay both the turn-on instance of the at least one auxiliary switching device and the turn-off instant of the main switching device in the mode A commutation by a first variable timestep twA which increases with the increasing value of the sensed leg current and decreases with the decreasing value of the sensed leg current of the respective converter leg, and wherein the control arrangement is configured to delay both the turn-on instance of the at least one auxiliary switching device and the turn-off instant of the main switching device in the mode B commutation by a second variable timestep twB which decreases with the increasing value of the sensed leg current and increases with the decreasing value of the sensed leg current of the respective converter leg, thereby advancing the turn-off instant of the main switching device proportionally to the value of the sensed leg current.
  • 8. The power converter system as claimed in claim 7, wherein the control arrangement is configured to delay the turn-off instant of the main switching device in the mode A commutation by adding the first variable timestep twA to a reference turn-off instant of the main switching device, and wherein the control arrangement is configured to advance the turn-off instant of the main switching device in the mode B commutation by adding the second variable timestep twB to a reference turn-off instant of the main switching device.
  • 9. The power converter system as claimed in claim 7, wherein the first variable timestep is twA=kA|Io|, where Io is the value of the sensed leg current sample of the respective converter leg, and kA is a constant, kA being equal for all converter legs with equal nominal leg current ratings, and wherein the second variable timestep is twB=tc−kB|Io|, where twB≥0, Io is the value of the sensed leg current sample of the respective converter leg, tc is a constant time, and kB is a constant, kB being equal for all converter legs with equal nominal leg current ratings.
  • 10. The power converter system as claimed in claim 9, wherein the parallel-connected converter legs have different nominal leg current ratings, and wherein the constants kA and/or kB in the parallel-connected converter legs are selected to scale with nominal leg currents of the converter legs such that a product of the constant kA and the nominal leg current IN is same in all parallel-connected converter legs and a product of the constant kB and the nominal leg current IN is essentially same in all parallel-connected converter legs.
  • 11. The power converter system as claimed in claim 1, wherein the parallel connected converter legs are hard-switching converter legs, particularly half-bridge legs, and wherein the control arrangement is configured to delay a turn-off instant of the main switching device that has been conducting in the mode B commutation by a first variable timestep td,off which decreases with the increasing value of the sensed leg current and increases with the decreasing value of the sensed leg current of the respective converter leg, and the control arrangement is configured to delay a turn-on instant of the main switching device that will start conducting in the mode A commutation by a second variable timestep td,on which increases with the increasing value of the sensed leg current and decreases with the decreasing value of the sensed leg current of the respective converter leg.
  • 12. The power converter system as claimed in claim 11, wherein the first variable timestep td,off decreases with the increasing value of the sensed leg current according to koff*|Io|, where Io is the value of the sensed leg current of the respective converter leg and kB is a constant, kB being equal for all converter legs with equal nominal leg current ratings, and wherein the second variable timestep td,on increases with the increasing value of the sensed leg current according to kon*|Io|, where Io is the value of the sensed leg current of the respective converter leg, and kon is a constant, kon being equal for all converter legs with equal nominal leg current ratings.
  • 13. The power converter system as claimed in claim 11, wherein the first variable timestep is td,off=tc−koff|Io|, where tc is a constant time defining an adjustment range, and wherein the second variable timestep is td,on=tD+kon|Io|, where, tD is an optional constant turn-on delay to avoid simultaneously conducting main switch devices.
  • 14. The power converter system as claimed in claim 12, wherein the parallel connected converter legs have different nominal leg current ratings, and wherein the constants kon or koff in the parallel-connected connector legs are selected to scale with nominal leg currents of the converter legs such that a product of the constant kon and the nominal leg current IN is same in all parallel-connected converter legs and a product of the constant koff and the nominal leg current IN is same in all parallel-connected converter legs.
  • 15. The power converter system as claimed in claim 1, wherein the control arrangement comprises a leg-specific controller for each of the two or more parallel-connected converter legs to adjust the switching instants of the main switching devices.
  • 16. The power converter system as claimed in claim 1, wherein the power inverter system comprises two or more converters, each of the converters having one or more converter phase legs, wherein the parallel-connected converter legs are the corresponding converter phase legs of the two or more converters connected in parallel.
  • 17. The power inverter system as claimed in claim 16, wherein the control arrangement comprises converter-specific switching controllers for the two or more converters, each of the converter-specific switching controllers being configured to provide the autonomous adjustment of switching instants for each of the converter phase legs of the respective converter.
Priority Claims (1)
Number Date Country Kind
23180670.4 Jun 2023 EP regional