The present invention relates to an apparatus, system and method for load balancing between two inverters connected in parallel, and, in particular embodiments, to an apparatus, system and method for load balancing through a coupled inductor placed between parallel operated inverters and an output filter.
Magnetic devices include transformers, inductors and/or the like. A magnetic device typically includes a magnetic core formed of suitable magnetic materials such as ferrite, powder iron and/or the like. The magnetic device may further include a conductive winding or a plurality of conductive windings. The windings and the current flowing through the windings may generate a magnetic field, which is also known as magnetic flux. In a normal design, the magnetic core usually has a relatively high permeability in comparison with the surrounding medium (e.g., air). As a result, the magnetic flux is confined with the magnetic core, which forms a closed flux path. The magnetic flux provides a medium for storing, transferring or releasing electromagnetic energy.
Coupled inductors are widely used in the power electronics industry. A coupled inductor may comprise two windings magnetically coupled to each other. The two coupled windings may be wound on a same magnetic core (e.g., a toroid core). The first winding generates a first magnetic force, which drives a first magnetic field or flux. The flux generated by the first winding is confined with the magnetic core, which forms a closed flux path. Likewise, the second winding generates a second magnetic force, which drives a second magnetic field, which is confined with the magnetic core.
The magnetic material of the magnetic core of a coupled inductor may be of a magnetic permeability greater than that of a surrounding medium (e.g., air). However, the coupling between two windings of the coupled inductor is not perfect. There may be a leakage path between the winding and the surrounding medium having a lower magnetic permeability. The coupling between the winding the surrounding medium may generate leakage magnetic flux. In an equivalent circuit of a coupled inductor, the leakage magnetic flux is replaced by a leakage inductance.
These and other problems are generally solved or circumvented, and technical advantages are generally achieved, by preferred embodiments of the present invention which provide an apparatus, system and method for load current sharing in a direct current (DC) to alternating current (AC) power system.
In accordance with an embodiment, an apparatus comprises a magnetic core comprising a first side and a second side opposite the first side, a first winding comprising a first portion wound around the first side and a second portion wound around the second side, a second winding comprising a third portion wound around the first side and a fourth portion wound around the second side, wherein the second portion and the fourth portion are coupled to each other.
In accordance with another embodiment, a system comprises a first inverter, a second inverter, wherein the second inverter and the first inverter are connected in parallel, a coupled inductor having a first input and a second input connected to the first inverter and the second inverter respectively and an output filter coupled to the output of the coupled inductor.
The coupled inductor comprises a magnetic core comprising a first side and a second side opposite the first side, a first winding comprising a first portion wound around the first side and a second portion wound around the second side, a second winding comprising a third portion wound around the first side and a fourth portion wound around the second side, wherein the second portion and the fourth portion are coupled to each other.
In accordance with yet another embodiment, a method comprises winding a conductive wire at a first side of a magnetic core to form a first group of winding turns, extending the conductive wire from the first side to a second side of the magnetic core, winding the conductive wire at the second side of the magnetic core to form a second group of winding turns, winding the conductive wire at the second side of the magnetic core to form a third group of winding turns, extending the conductive wire from the second side to the first side of the magnetic core and winding the conductive wire at the first side of the magnetic core to form a fourth group of winding turns.
An advantage of an embodiment of the present invention is that the load currents of a plurality of inverters connected in parallel are balanced through a coupled inductor. Balanced load currents in different inverter modules of a power system help to improve the efficiency, reliability and cost of the power system.
The foregoing has outlined rather broadly the features and technical advantages of the present invention in order that the detailed description of the invention that follows may be better understood. Additional features and advantages of the invention will be described hereinafter which form the subject of the claims of the invention. It should be appreciated by those skilled in the art that the conception and specific embodiment disclosed may be readily utilized as a basis for modifying or designing other structures or processes for carrying out the same purposes of the present invention. It should also be realized by those skilled in the art that such equivalent constructions do not depart from the spirit and scope of the invention as set forth in the appended claims.
For a more complete understanding of the present invention, and the advantages thereof, reference is now made to the following descriptions taken in conjunction with the accompanying drawings, in which:
Corresponding numerals and symbols in the different figures generally refer to corresponding parts unless otherwise indicated. The figures are drawn to clearly illustrate the relevant aspects of the various embodiments and are not necessarily drawn to scale.
The making and using of the presently preferred embodiments are discussed in detail below. It should be appreciated, however, that the present invention provides many applicable inventive concepts that can be embodied in a wide variety of specific contexts. The specific embodiments discussed are merely illustrative of specific ways to make and use the invention, and do not limit the scope of the invention.
The present invention will be described with respect to preferred embodiments in a specific context, namely a coupled inductor structure for load current sharing in a direct current (DC) to alternating current (AC) power system having multiple inverters connected in parallel. The invention may also be applied, however, to a variety of DC/AC power systems. Furthermore, the invention may also be applied to a variety of current sharing applications. Hereinafter, various embodiments will be explained in detail with reference to the accompanying drawings.
The first inverter 102 and the second inverter 104 inverts a DC waveform received from the input DC power source 112 to an AC waveform. In some embodiments, the first inverter 102 and the second inverter 104 may comprise a plurality of switching elements such as insulated gate bipolar transistor (IGBT) devices. Alternatively, the first inverter 102 and the second inverter 104 may include other types of controllable devices such as metal oxide semiconductor field effect transistor (MOSFET) devices, bipolar junction transistor (BJT) devices, super junction transistor (SJT) devices, bipolar transistors and/or the like. The detailed operation and structure of the first inverter 102 and the second inverter 104 will be described below with respect to
The coupled inductor 110 may comprise two inductors magnetically coupled to each other. As shown in
It should be noted that the inverters 102 and 104 and the coupled inductor 110 shown in
The output filter 116 may comprise an inductor L1 coupled between the coupled inductor 110 and the output AC source 114. The output filter 116 may further comprise a plurality of output capacitors coupled between the common node of the coupled inductor 110 and the inductor L1 and ground. The plurality of output capacitors are collectively shown as a capacitor C1 in
The inductor L1 provides high impedance when high frequency noise tries to flow out of the inverters 102 and 104. At the same time, the capacitor C1 shunts the input of the output power source 114 and provides a low impedance channel for the high frequency noise generated from the inverters 102 and 104. As a result, the high frequency noise of the inverters 102 and 104 may be prevented from passing through the output filter 116.
It should further be noted that the inverter topologies, the output filter 116, the input DC power source 112 and the output AC power source 114 shown in
In some embodiments, the first inverter 102 may be of the same structure as the second inverter 104. For simplicity, only the detailed structure of the first inverter 102 will be described below.
The first inverter 102 comprises a pair of switching elements Q1 and Q2 connected in series. The common node of the switching elements Q1 and Q2 are coupled to ground through an isolation device formed by back-to-back connected switching elements Q5 and Q6. The back-to-back connected switching elements Q5 and Q6 are capable of completely isolating the common node of the switching elements Q1 and Q2 from ground. According to some embodiments, switching elements Q1, Q2, Q5 and Q6 are IGBT or IGBTs connected in parallel, series and any combinations thereof.
Switching elements Q1, Q2, Q5 and Q6 are so controlled that the output of the first inverter 102 generates a three level waveform. In particular, when switching element Q1 is turned on, the output of the first inverter 102 generates a positive voltage equal to one half of the voltage of the input DC power source 112. Likewise, when switching element Q2 is turned on, the output of the first inverter 102 generates a negative voltage equal to one half of the voltage of the input DC power source 112. When both switching elements Q1 and Q2 are turned off and switching elements Q5 and Q6 are turned on, the output of the first inverter 102 is coupled to ground. As such, the output of the first inverter 102 is a three-level voltage waveform. The frequency of the three-level voltage waveform is approximately 60 HZ according to an embodiment.
The first inverter 102 and the second inverter 104 shown in
The equivalent circuit of the coupled inductor 110 is shown in
The first resistor R1 represents the winding resistance of the first winding of the coupled inductor 110. Likewise, the second resistor R2 represents the winding resistance of the second winding of the coupled inductor 110.
The magnetic material of the magnetic core may be of a magnetic permeability greater than that of a surrounding medium (e.g., air). However, the coupling between two inductors of the coupled inductor 110 may be not perfect. The coupling between the winding and the surrounding medium may generate leakage magnetic flux. Both inductors of the coupled inductor 110 may generate leakage inductance through the coupling with the surrounding medium such as air. The leakage generated by the first inductor winding is defined as Llk1 and the leakage generated by the second inductor winding is defined as Llk2.
As shown in
According to some embodiments, the first leakage inductor Llk1 and second leakage inductor Llk2 help to achieve dynamic current sharing between the first inventor 102 and the second inverter 104. During a transition (e.g., from one output voltage level to another output voltage level), the impedance of the leakage inductors may become significant because the transition frequency is much higher than the normal operating frequency, which is about 60 Hz according to an embodiment. Such higher impedance can correct the unbalanced currents flowing through two sides of the transformer T1.
On the other hand, during normal operation mode or a static current sharing process, the resistors R1 and R2 may create a higher voltage drop in the conductive channel of the inverter, which is heavily loaded. In addition, the winding resistance is of a positive temperature coefficient. In other words, the winding resistance of highly loaded winding increases with increasing temperature caused by a higher load current. As a result, the load current is steered from the heavily loaded inverter to the lightly loaded inverter. Accordingly, static current sharing can be achieved. Both the dynamic current sharing and the static current share are well known in the art, and hence are not discussed in further detail herein.
It should be noted during a static current sharing process, the first leakage inductor Llk1 and second leakage inductor Llk2 may help to balance the load currents flowing through the first inventor 102 and the second inverter 104.
The coupled inductor may be wound around a magnetic core as shown in
The view 304 shows the coupled inductor comprises two winding coils 312 and 314 wound around a rectangular magnetic core. The first winding coil 312 is split into two portions N1 and N3. Likewise, the second winding coil 314 is split into two portions N2 and N4. As shown in
It should be noted that while
One advantageous feature of having multiple windings wound around the same magnetic core as shown in
The winding of first inductor L1 is split between a first side of the rectangular magnetic core and a second side of the rectangular magnetic core. In particular, there may be N1 turns located at the first side of the magnetic core and N3 turns at the second side of the magnetic core. Likewise, the winding of first inductor L2 is split between a first side of the rectangular magnetic core and a second side of the magnetic core. In particular, there may be N2 turns located at the first side of the magnetic core and N4 turns at the second side of the magnetic core. In some embodiments, N1, N2, N3 and N4 are equal.
Once the wire wraps N4 turns around the second side, the wire extends from the second side of the magnetic core to the first side of the magnetic core. The wire may wrap N2 turns around the first side and finish at Term B. It should be noted that N1, N2, N3 and N4 are wound in the same direction. In other words, the magnetic fields generated by windings N1, N2, N3 and N4 are in the same direction.
One advantageous feature of having a single wire winding structure shown in
It should be noted the windings N1, N2, N3 and N4 may be implemented by a single wire as described above. Alternatively, the winding N1, N2, N3 and N4 may be implemented by two wires. In particular, a first wire is employed to form windings N1 and N3. A second wire is employed to form windings N2 and N4. A first terminal of the first wire is a first input Term A of the coupled inductor. A first terminal of the second wire is a second input Term B of the coupled inductor. The second terminal of the first wire and the second terminal of the second wire are coupled together to form the output Term C of the coupled inductor.
Although embodiments of the present invention and its advantages have been described in detail, it should be understood that various changes, substitutions and alterations can be made herein without departing from the spirit and scope of the invention as defined by the appended claims.
Moreover, the scope of the present application is not intended to be limited to the particular embodiments of the process, machine, manufacture, composition of matter, means, methods and steps described in the specification. As one of ordinary skill in the art will readily appreciate from the disclosure of the present invention, processes, machines, manufacture, compositions of matter, means, methods, or steps, presently existing or later to be developed, that perform substantially the same function or achieve substantially the same result as the corresponding embodiments described herein may be utilized according to the present invention. Accordingly, the appended claims are intended to include within their scope such processes, machines, manufacture, compositions of matter, means, methods, or steps.
Number | Name | Date | Kind |
---|---|---|---|
4099066 | Beggs | Jul 1978 | A |
5379207 | Shah | Jan 1995 | A |
5422620 | Bitterli | Jun 1995 | A |
5737203 | Barrett | Apr 1998 | A |
6822546 | Jakab | Nov 2004 | B1 |
7398589 | Younger et al. | Jul 2008 | B2 |
7609536 | Brochu | Oct 2009 | B2 |
8203855 | Shimada et al. | Jun 2012 | B2 |
20020167388 | Usui | Nov 2002 | A1 |
20040257188 | Younger et al. | Dec 2004 | A1 |
20090134964 | Hebert | May 2009 | A1 |
20090289751 | Nagano | Nov 2009 | A1 |
20100164674 | Wu et al. | Jul 2010 | A1 |
Entry |
---|
Ferrite core, Google NPL. |
Li, Wuhua, et al., “Application Summarization of Coupled Inductors in DC/DC Converters,” IEEE, College of Electrical Engineering, Zhejiang University, 2009, pp. 1487-1491. |
Number | Date | Country | |
---|---|---|---|
20140152413 A1 | Jun 2014 | US |