The present disclosure relates to magnetic assemblies, and more specifically, to a compact magnetic assembly that efficiently interconnects high frequency and high current magnetic devices.
High-density and low-loss assembly and interconnection of magnetic devices present various concerns when operating in a power range of tens of kilowatts, a current range of hundreds of amperes, and a frequency range of tens of kilohertz. The various concerns include the number of winding terminations, electromagnetic interference (EMI). High-density and low-loss assembly and interconnection of magnetic devices also invite an interest in solving issues related to interconnecting one or more subassemblies, and cooling the magnetic devices. Skin effect losses in high current conductors and leakage inductance can increase the overall power dissipation and lead to high EMI. Therefore, shielding and interconnect methods for reducing EMI are required, which add significant volume and weight to the conventional magnetic assembly. These issues are exacerbated for power converters comprising assemblies with multiple magnetics.
Typically, high frequency magnetic assemblies utilize one or more multi-stranded “Litz” wires for creating electrical connections to high frequency, high current magnetic devices. However, leakage inductance occurs when high frequency, high current flows through the Litz wire connection point, thereby increasing the radiated magnetic field and associated EMI. Consequently, additional shielding is required at the connection points. As a result, a magnetic assembly having a large number of Litz wire connection points requires an increased amount of EMI shielding, thereby preventing fabrication of a compact magnetic assembly.
According to one embodiment, a magnetic assembly to receive current having a high current and high frequency comprises a transformer, at least one first inductor, and at least one second inductor. The first inductor is in electrical communication with the transformer, and the second inductor is in electrical communication with the first inductor. The magnetic assembly further includes at least one conductor having a first end coupled to the second inductor and a second end coupled to the transformer. The conductor extends continuously between the first and second ends without terminating to form an auxiliary winding of the second inductor, a resonant winding of the first inductor, and at least one primary winding of the transformer.
According to another embodiment, a method of forming a magnetic assembly to receive current having a high current and high frequency comprises disposing a first end of a conductor at a first contact point of a first inductor and disposing a second end of the conductor at a second contact point of a transformer. The method further includes extending the conductor continuously between the first and second contact points without terminating the conductor therebetween. The method further includes forming an auxiliary winding of a first inductor using a first portion of the conductor, forming a resonant winding of a second inductor using a second portion of the conductor, and forming at least one primary winding of the transformer using a third portion of the conductor.
According to yet another embodiment, a method of electrically connecting an interconnect conductor to a continuously extending conductor that forms at least one winding of a magnetic assembly comprises determining cross-section area size of single bonds for bonding the interconnect conductor. The method further includes determining a target impedance and a total contact area of the interconnect conductor. The method further includes determining a bonding pattern to electrically connect the interconnect conductor to the conductor of the magnetic assembly. The method further includes bonding the interconnect conductor to the conductor of the magnetic assembly according to the bonding pattern thereby forming an electrically conductive contact point without terminating the conductor.
Additional features are realized through the techniques of the present invention. Other embodiments and aspects of the invention are described in detail herein and are considered a part of the claimed invention. For a better understanding of the invention with the features, refer to the description and to the drawings.
For a more complete understanding of this disclosure, reference is now made to the following brief description, taken in connection with the accompanying drawings and detailed description, wherein like reference numerals represent like parts:
To mitigate skin effect losses and leakage inductance in high current conductors, at least one embodiment of the disclosure provides a magnetic assembly included with one or more conductors that extend continuously without terminating to form a winding of one or more independent magnetic devices. The magnetic assembly according to at least one embodiment described herein may be utilized to construct various magnetic hardware devices. Referring to
According to at least one exemplary embodiment, the SRC module 100 may be switched at 100 kHz to generate a galvanically-isolated output of 500 VDC at 62,500 W. The SRC module 100 includes a primary bridge unit 102 and a secondary bridge unit 104. The primary bridge unit 102 includes the magnetic assembly 200. The magnetic assembly 200 includes, for example, five independent magnetic devices: a transformer T1, two first inductors (e.g., resonant inductors) Lr1 and Lr2, and two second inductors (e.g., auxiliary inductors) La1 and La2. It can be appreciated that a resonant inductor may be referred to as a second inductor and an auxiliary inductor may be referred to as a first inductor.
Each resonant inductor Lr1, Lr2, includes respective resonant windings, and each auxiliary inductor La1, La2 includes respective auxiliary windings. The transformer T1 includes two primary windings T1-1, T1-2. The secondary bridge unit 104 may include a secondary winding T1-3 that electrically communicates with the primary windings T1-1, T1-2 via an electromagnetic field. The full load and high input line correspond to the highest continuous currents of the independent magnetic devices. In the exemplary embodiment shown in
Based on the current parameters described above, a conventional SRC module would require excessively large terminals to connect each individual magnetic device, thereby increasing the overall size of the SRC module. Further, the large terminals would increase the gap between the two conductors forming the transformer windings, which carry current in opposite directions, thereby increasing leakage inductance. However, the magnetic assembly 200 according to at least one exemplary embodiment provides at least one conductor that continuously extends between the first and second ends thereof without terminating, and forms the auxiliary winding of at least one auxiliary inductor, the resonant winding of at least one resonant inductor, and at least one primary winding of the transformer. The conductor may be formed as a electrically conductive “Litz wire”, for example,
A magnetic assembly 200 according to an exemplary embodiment of the disclosure is illustrated in
The first and second resonant inductors Lr1, LR2 may be connected to the transformer T1 in various manners. For example, the first and second resonant inductors Lr1, Lr2 may each be connected in parallel with the transformer T1, as illustrated in
Each of the windings corresponding to the transformer T1, the resonant inductors Tr1, Tr2 and the auxiliary inductors Ta1, Ta2 are formed by a continuous conductor. Referring to
The second conductor 204 has a first end coupled 214 to the first auxiliary inductor and a second end 216 coupled to the first node of the transformer T1. The second conductor 204 extends continuously between the first and second ends 214, 216 without terminating to form a second auxiliary winding portion (i.e., winding La1-2) of the first auxiliary inductor La1, a second resonant winding portion (i.e., winding Lr1-2) of the first resonant inductor Lr1, and a second portion of a first primary winding (i.e., winding T1-1.2) of the transformer T1.
The third conductor 206 has a first end 218 coupled to the second auxiliary inductor La2 and a second end 220 coupled to a second node of the transformer T1. The third conductor 206 extends continuously between the first and second ends 218, 220 without terminating to form a first auxiliary winding portion (i.e., winding La2-1) of the second auxiliary inductor La2, a first resonant winding portion (i.e., winding Lr2-1) of the second resonant inductor Lr2, and a first portion of a second primary winding (i.e., T1-2.1) of the transformer T1.
The fourth conductor 208 has a first end 222 coupled to the second auxiliary inductor La2 and a second end 224 coupled to the second node of the transformer T1. The fourth conductor 208 extends continuously between the first and second ends 222, 224 without terminating to form a second auxiliary winding portion (i.e., winding La2-2) of the second auxiliary inductor La2, a second resonant winding portion (i.e., winding Lr2-2) of the second resonant inductor Lr2, and a second portion of a second primary winding (i.e., winding T1-2.2) of the transformer T1.
The magnetic assembly 200 according to at least one exemplary embodiment further includes one or more contact points (A-F) located on one or more of the conductors 202-208. The first end 210 of the first conductor 202 and the first end 214 of the second conductor 204 may be coupled to one another at a contact point A. The second end 212 of the first conductor 202 and the second end 216 of the second conductor 204 may be coupled to one another at a contact point C. The first end 218 of the third conductor 206 and the first end 222 of the fourth conductor 208 may be coupled to one another at a contact point F. The second end 220 of the third conductor 206 and the second end 224 of the fourth conductor 208 may be coupled to one another at a contact point D. Accordingly, at least one embodiment of the disclosure described above provides a magnetic assembly 200 including one or more conductors that extend continuously without terminating to form windings of one or more independent magnetic devices. The magnetic assembly 200, therefore, may operate under high current and high frequency conditions while mitigating skin effect losses and leakage inductance in the conductors.
At least one interconnect conductor may also be coupled to at least one of the conductors 202-208 at a respective contact point A-F without terminating the conductor 202-208 between the respective first and second ends, as discussed in greater detail below. According to at least one embodiment, the at least one conductor and the at least one interconnect conductor are formed from Litz wires comprising a plurality of electrically conductive strands. The strands may be braided according to various patterns to reduce the impact of both skin effect and proximity effect.
Referring to
The interconnect conductor 300 and the continuous conductor 302 are formed from Litz wires comprising a plurality of electrically conductive strands, and are bonded to one another using, for example, a laser welding process. Although a laser welding process will described going forward, other bonding methods may be used including, but not limited to, resistance welding, spot welding, ultrasonic welding, and wire fusion.
Still referring to
Referring now to
Referring now to
The corresponding structures, materials, acts, and equivalents of all means or step plus function elements in the claims below are intended to include any structure, material, or act for performing the function in combination with other claimed elements as specifically claimed. The description of the present invention has been presented for purposes of illustration and description, but is not intended to be exhaustive or limited to the invention in the form disclosed. Many modifications and variations will be apparent to those of ordinary skill in the art without departing from the scope and spirit of the invention. The embodiments were chosen and described in order to best explain the principles of the invention and the practical application, and to enable others of ordinary skill in the art to understand the invention for various embodiments with various modifications as are suited to the particular use contemplated.
While the preferred embodiments to the invention have been described, it will be understood that those skilled in the art, both now and in the future, may make various improvements and enhancements which fall within the scope of the claims which follow. These claims should be construed to maintain the proper protection for the invention first described.
This invention was made with Government support under Contract No.: N00014-09-D-0726 awarded by United States Navy. The Government has certain rights in this invention.
Number | Name | Date | Kind |
---|---|---|---|
3043000 | Hatfield et al. | Jul 1962 | A |
4268957 | Sbuelz | May 1981 | A |
4623771 | Sakino | Nov 1986 | A |
5517755 | Wright | May 1996 | A |
5545966 | Ramos et al. | Aug 1996 | A |
5808535 | Delucia | Sep 1998 | A |
6349044 | Canales-Abarca et al. | Feb 2002 | B1 |
6384703 | Ramos et al. | May 2002 | B1 |
6885268 | Choi | Apr 2005 | B2 |
7002443 | Ness et al. | Feb 2006 | B2 |
7142085 | Phadke | Nov 2006 | B2 |
7489226 | Chignola et al. | Feb 2009 | B1 |
8009004 | Ahangar et al. | Aug 2011 | B2 |
20110038181 | Yan et al. | Feb 2011 | A1 |
20120042588 | Erickson, Jr. | Feb 2012 | A1 |
20130103023 | Monson et al. | Apr 2013 | A1 |
20130154781 | Cho | Jun 2013 | A1 |
20140153293 | Chang et al. | Jun 2014 | A1 |
Number | Date | Country |
---|---|---|
EP000402831 | Dec 1990 | DE |
Entry |
---|
Prasai et al., “Utilizing Stray Capacitances of a Litz Wire”, 40th Industry Applications Conference, 2005, vol. 3, pp. 1876-1883. |
Skutt et al., “Leakage Inductance and Termination Effects in a High-Power Planar Magnetic Structure”, Ninth Annual Applied Power Electronics Conference and Exposition, vol. 1, 1994, pp. 295-301. |
Sullivan, “Optimal Choice for Number of Strands in a Litz-Wire Transformer Winding”, IEEE Transactions on Power Electronics, vol. 14, No. 2, Mar. 1999, pp. 283-291. |
Tang et al., “Stranded Wire with Uninsulated Strands as a Low-Cost Alternative to Litz Wire”, IEEE 34th Annual Power Electronics Specialist Conference, 2003, vol. 1, pp. 289-295. |
Number | Date | Country | |
---|---|---|---|
20150015356 A1 | Jan 2015 | US |