This patent application is related to the U.S. Patent Application entitled “Methods of Manufacturing and Assembling Electromagnetic Assemblies and Core Segments that Form the Same,” Attorney Docket No. 060286, filed concurrently herewith, the contents of which are incorporated by reference herein in their entirety.
The invention relates to electromagnetic assemblies, core segments that form the same, and their methods of manufacture.
Soft magnetic cores made from ceramic materials such as Mn—Zn ferrite, Ni—Zn ferrite, and other soft magnetic ferrite compositions, and from powdered metallic alloys such as Fe, Fe—Al—Si, Fe—Co, Fe—Co—V, Fe—Mn, Fe—P, Fe—Si, Ni—Fe, Ni—Fe—Mo, and other soft magnetic alloys, have been commercially available for decades. More recently, amorphous and nanocrystalline soft magnetic alloys made by a variety of rapid solidification techniques and reduced to powder form by atomization or comminution are becoming commercially available. Single-piece cores such as ring cores (toroids) are available in sizes up to about 150 mm diameter. Sizes beyond 150 mm diameter are uneconomical to produce, requiring very large high-tonnage presses to consolidate the ceramic or metal powders into the desired shapes. Commercially available presses capable of more than 1000 tons of compaction force are uncommon and expensive to purchase and operate. Typical pressing pressures required to consolidate many soft magnetic powders, such as Fe—Si and Fe—Si—Al powders which have very low ductility, can reach 150 tons per square inch (tsi) in order to achieve high target densities. High densities are important in fully developing optimum magnetic properties for any given material, and reductions in pressing pressure lead to inferior core performance.
For example, a 1000-ton press used to compact a powder requiring 150 tsi pressure will be limited to a pressing area of 6.67 square inches (1000 tons divided by 150 tsi). Pressing areas greater than 6.67 square inches will result in lower pressures and degraded core performance. For example, one commercially acceptable soft magnetic core formed with 150 tsi pressing area is a toroid of approximately 3.36″ outside diameter (OD) and 1.68″ inside diameter (ID), a 2:1 ratio of OD to ID being a common proportion for toroids. A typical powder compacting die to produce this part will consist of a cylindrical die cavity; a center core rod (a solid cylinder) positioned parallel to the axis of the cylindrical opening, and in the center of the opening thus creating an annular cavity; a bottom punch with an annular cross section that closely fits the die cavity; and a top punch with the same annular cross section as the bottom punch. These four pieces of tooling are held in proper alignment by attachment to a common structure, known as a tool set, and the tool set is provided with external attachment points to fit into an appropriate compacting press. The tool set allows the top and bottom punches to move longitudinally within the die cavity and also allows the top punch to travel vertically out of engagement with the die so the empty cavity is exposed and powder can be introduced into the cavity for each pressing cycle. Once filled with powder, the top punch re-enters the annular cavity and compresses the powder into a solid form. Therefore, to determine the maximum core size that can be produced on a press, one divides the maximum force the press can generate by the cross section of the annular face of the top punch.
In addition to toroidal shapes, mated pairs of coresare commonly used, with an E-shaped configuration being typical. Other cores used in mated pairs can be shaped to correspond to the letters U, I and C. Unlike toroids which have a closed magnetic pathway, E, U, I and C cores are open-ended and as such usually require mating with another core, open end-to-open end, to create a closed magnetic pathway. E-to-E, E-to-I, U-to-U, U-to-I, C-to-C and C-to-I core pairings are also common. Using a 1000-ton press and 150 tsi pressure limit, a common configuration of an E-core with typical proportions would be limited to approximate dimensions of 4.75 inches in length and 2.37 inches in height, or about 6.67 square inches.
In yet another example, an open-ended E, U, I or C core used by itself as a magnetic device would also be limited to the same dimensional limits as the mated pairs described above, since each core half, whether used as a mated pair or not, is pressed individually.
In a further example, reducing the pressing pressure to 40 tsi, a typical pressing pressure for more ductile materials such as powdered iron, and continuing to use a 1000-ton press, provides a maximum single piece toroid size of about 6.50 inches OD and 3.25 inches ID.
More restrictive limitations on maximum core sizes are imposed if more common and economical presses are employed, such as those presses with capacities of only 400 to 750 tons of pressing force.
Circuit designers thus have limits on the size of available cores made from these materials. For comparative illustration purposes, large magnetic cores of sizes beyond those examples provided herein are commercially available made from alloys such as Fe, Fe—Si, Fe—Co, Fe—Co—V, Fe—Mn, Fe—P, Ni—Fe, and Ni—Fe—Mo that have been rolled into thin ribbons. These cores are known as tape wound cores, and are created by building up multiple wraps of the magnetic ribbon on a pre-form, or mandrel, of the desired shape. Most common tape wound cores are in the form of a toroid, an oval toroid or rectangle, or several toroids or ovals which are assembled to create an E-core shape. These cores are labor intensive to manufacture in large sizes and have other important drawbacks that limit their use. They can be limited to use at lower frequencies, typically less than 100 kHz, due to high eddy current losses associated with and proportional to the ribbon thickness. To reduce eddy current losses, ribbon thickness can be reduced, but the practical lower limit is about 0.0005 inches. Thinner gages, down to 0.0000125 inches, are commercially available but are extremely expensive, and creating large cores from this delicate material is impractical. Fabricating long continuous lengths of ribbon at very thin gages that is also wide enough to create the desired final dimensions of the magnetic core is difficult and expensive. In addition, with each wrap of ribbon there is a laminar gap that cannot be reduced to zero; known in the trade as a “stacking factor.” A typical stacking factor for a core made from 0.0005″ thick ribbon is 60%. Accordingly, a core must be substantially larger than the arithmetic sum of the thicknesses of the wraps, leading magnetic cores that can be up to 50% larger for any given power output.
Tape wound cores are also limited to certain metal alloys whose ductility permits fabrication into ribbon form by rolling, or that can be cast to final gauge thickness directly. Ceramic magnetic materials cannot be formed into ribbons, and, thus, cannot be used in tape-wound configurations.
When the application requires cores larger than those commercially available, circuit designers have resorted to stacking smaller toroids, E, U, I or C cores together. This approach has limited benefit as the winding cross-section of the core, the area where the coil of wire resides, is not increased by stacking and therefore limits the amount of extra power such a stack can produce. For example, a toroid has a winding area limited by the size of the hole in the core. Stacking multiple toroids one upon another will geometrically increase the cross section of the magnetic material, which is capable of delivering more power, but the diameter of the hole remains the same. Because power (P) equals voltage (V) multiplied by current (I), and because any given circuit is confined to run at its specific designed voltage level, more power can only be generated by increasing the current in the windings. Therefore, the current in the windings is directly proportional to the cross section of the core for any desired output. Higher current densities, however, require heavier gauge wire to prevent overheating and excessive electromagnetic losses, and the hole in the stack of toroids will limit the wire size and number of turns of wire that can be wound. Therefore, the practice of stacking cores is of limited value when constructing large power inductors.
Alternatively, simple square or rectangular blocks of the aforementioned materials can be stacked and bonded together to make larger core shapes. One example of such a practice is disclosed in International Publication WO 2005/041221 A1. This approach limits the assemblies to rudimentary shapes and must rely on the skill of those assembling the pieces to achieve the necessary alignment of the segments. The uncured adhesive applied between segments can act as a lubricant, so clamping segments together for curing is a non-trivial task. Careful jigging or registration of the pieces is required until the adhesive cures to assure not only alignment of the segments, but that the gaps between segments are uniform and controlled. If the gaps between pieces are too large, the inductance of the assembly is reduced, and if the gap widths are too variable from assembly to assembly, the electrical properties will have excessive variation. This effect is described in Equation 1:
μeμo/(1+(gap/Ie)μo) Eq. 1
where μo is the permeability of the individual segments, Ie is the magnetic path length of the assembly, “gap” is the sum of the gap lengths between pieces, and μe is the effective permeability of the assembly. If the gap created by the adhesive (the glue line) varies excessively, the electrical properties of the assembled cores will be unacceptable. Depending on the permeability of the magnetic segments, the air gaps introduced by variations in the glue line thickness can have a large impact on the effective permeability of the final assembly. Using Equation 1, the change in effective permeability for a typical inductor material (60 permeability) and a typical transformer material (2500 permeability) are shown in
In inductor applications, low permeability material is required. Low permeability materials are created by taking the powder form of soft magnetic metal alloys and coating the particles with a non-magnetic coating. In effect, this creates a large number of very small air gaps between particles after the powder is compressed into a desired shape. Cores selected for inductor applications usually have a permeability of 300 or less. For example, many inductors use 60-perm material, and this material has its effective permeability reduced by nearly 8% if the sum total of all air gaps, created by the glue line thickness, around the magnetic path length is as little as 0.5 mm. Following the teachings of International Publication WO 2005/041221 A1 will naturally lead to the introduction of multiple air gaps. A review of commercially available inductor cores shows a guaranteed inductance value of, typically, +/−8% to +/−12% of nominal values. For example, Magnetics, a division of Spang & Company, Pittsburgh, Pa., discloses +/−8% tolerances for their molypermalloy (Fe—Ni—Mo) and High Flux (Fe—Ni) alloys, and +/−12% for their Kool Mu® (Fe—Al—Si) 60-perm materials. These published tolerances cover normal processing variations such as (i) particle size distribution of the pre-compacted powder, (ii) thickness variations in the non-magnetic coating typically applied to these powders, (iii) variations in chemistry of the alloy during manufacture, and (iv) variations in powder fill during pressing operations. The introduction of yet another source of variation, namely variation in air gaps in the assembled structure, would result in a core that has too broad of a range of inductance values within a production lot, and from lot to lot, and would be non-competitive in the marketplace. Any process that increases the tolerance on the inductor core is undesirable for one or more reasons: 1) the inductance of a wound core is directly proportional to the square of the number of turns of wire (See, Eq. 2); 2) inductors are usually wound to very specific inductance values; and 3) it is uneconomical to customize the number of turns of wire on a core-by-core basis to adjust for inductance variations resulting from variable air gap dimensions. Along with avoiding the aforementioned process variations, it is important to fully develop the electromagnetic properties of each material, regardless of its composition or assembly techniques.
In transformer applications where high inductance is required, materials such as ferrite are chosen due to their relatively high permeability ranging from about 500 to about 20,000. The permeability of a material directly affects the inductance of a core assembly, as described in Equation 2, where L is the inductance of the core (in Henries), N is the number of turns of wire on the core, μo is the permeability of the material, Ae is the effective cross section of the core, and Ie is the effective magnetic flux path length in the core.
L=((0.4πN2μoAe)/Ie)*10−8 Eq. 2
Unfortunately, cores made from high permeability materials suffer the largest drop in inductance with the introduction of air gaps, as shown in
Japanese Publication No. 04-165607 is said to teach improved manufacturing efficiency by adhering segments together in overlapping layers to form larger, useful magnetic assemblies. The teachings of this reference are similar to WO 2005/041221 A1, and discuss how segments are used as building blocks. However, Japanese Publication No. 04-165607 teach only simple shapes that have no means of establishing registration between segments, and no means to control inductance of the final assembly. Air gaps created by glue lines that interrupt the magnetic path length are uncontrolled and will lead to an undesirably high degree of variation in inductance from assembly to assembly. Similar teachings are offered in Japanese Publication Nos. 61-071612 and 59-178716, where magnetic materials in strip form are laminated into larger assemblies.
Accordingly, continuous efforts are needed to develop electromagnetic assemblies and their related methods of manufacture to further advance the technology of high power inductor and transformer cores made from these assemblies.
In one embodiment, a magnetic core segment is provided, comprising a first interlocking member configured to form an interlocking portion with a second interlocking member of a second magnetic core segment.
In another embodiment, a magnetic core assembly is provided, comprising a first segment and a second segment, at least a portion of the first segment configured to form an interlocking portion with at least a portion of the second segment.
In yet another embodiment, a stacked magnetic core assembly is provided, comprising first and second magnetic cores assemblies, the first and second magnetic core assemblies each further comprising an inter-layer interlocking member configured to form an inter-layer interlocking portion therebetween.
In another embodiment, a method of forming a magnetic core segment is provided, comprising forming a magnetic core segment comprising an interlocking member thereon, the interlocking member configured to form an interlocking portion with a second interlocking member of a second magnetic core segment.
In another embodiment, a method of forming a segmented magnetic core assembly is provided, comprising: contacting a first segment to a second segment, the first segment having an interlocking member configured to form an interlocking portion with a second interlocking member of the second magnetic core segment; and interlocking the first segment to the second segment to form the segmented magnetic core assembly.
In yet another embodiment, a method of forming a stacked magnetic core assembly is provided, comprising: placing a first magnetic core assembly over a second magnetic core assembly, the first and second magnetic core assemblies each comprising an inter-layer interlocking member configured to form an inter-layer interlocking portion therebetween.
In another embodiment, a method of forming a segmented magnetic core assembly is provided, comprising selecting individual interlocking segments based on a selected size and shape of the assembly.
It should be understood that this invention is not limited to the embodiments disclosed in this Summary, and it is intended to cover modifications that are within the spirit and scope of the invention, as defined by the claims.
The features and benefits presented in this invention are better understood through the detailed description of certain embodiments and the accompanying drawings, wherein:
Other than in the operating examples, or unless otherwise expressly specified, all of the numerical ranges, amounts, values and percentages, such as those denoting amounts of materials, times and temperatures of reaction, ratios of amounts, and others in the following portion of the specification, may be read as if prefaced by the word “about,” even though the term “about” may not expressly appear with the value, amount or range. Accordingly, unless indicated to the contrary, the numerical parameters set forth in the following specification and attached claims are approximations that may vary depending upon the desired properties sought to be obtained by the invention. At the very least, and not as an attempt to limit the application of the doctrine of equivalents to the scope of the claims, each numerical parameter should at least be construed in light of the number of reported significant digits and by applying ordinary rounding techniques.
Notwithstanding the fact that the numerical ranges and parameters setting forth the broad scope of the invention are approximations, the numerical values set forth in the specific examples are reported as precisely as possible. Any numerical values, however, inherently contain certain errors necessarily resulting from the standard deviation found in their respective testing measurements. Furthermore, when numerical ranges of varying scope are set forth herein, it is contemplated that any combination of these values inclusive of the recited values may be used.
Also, it should be understood that any numerical range recited herein is intended to include all sub-ranges subsumed therein. For example, a range of “1 to 10” is intended to include all sub-ranges between (and including) the recited minimum value of 1 and the recited maximum value of 10, that is, having a minimum value equal to or greater than 1 and a maximum value of equal to or less than 10. The terms “one,” “a,” or “an” as used herein are intended to include “at least one” or “one or more,” unless otherwise indicated.
Any patent, publication, or other disclosure material, in whole or in part, that is identified herein is incorporated by reference herein in its entirety, but is incorporated herein only to the extent that the incorporated material does not conflict with existing definitions, statements, or other disclosure material set forth in this disclosure. As such, and to the extent necessary, the disclosure as explicitly set forth herein supersedes any conflicting material said to be incorporated herein by reference. Any material, or portion thereof, that is said to be incorporated by reference herein, but which conflicts with existing definitions, statements, or other disclosure material set forth herein will only be incorporated to the extent that no conflict arises between that incorporated material and the existing disclosure material.
As used herein, the terms “registration” or “interlocking engagement” refer to the association between a first and second magnetic core assembly segment, wherein at least a portion of the first segment comprises a first member, such as, for example, a protrusion, complementary to a second member, such as, for example, an indention, of the second segment, such that when the first segment engages the second segment to form an interlocking portion, motion of the first segment relative to the second segment is at least partially constrained when a force is applied. The terms “interlocking portion” or “interlocking interface” refer to the contact region wherein adjacent interlocking members, such as a protrusion and corresponding indentation, are joined. As used herein, the term “protrusion” refers to the portion of a segment that projects beyond what would otherwise be a flat or blunt surface of the segment. The term “indentation” refers to the portion of the segment that is recessed from what would otherwise be a flat or blunt surface of the segment. The term “unstacked,” as used herein, refers to single-tiered or single-layered magnetic core assemblies, in contrast to “stacked” assemblies having portions of the assembly that overlap or overlay other portions to form regions that are multi-tiered or multi-layered.
There exists a need in the current state of the art for fabrication techniques, using both existing and future materials that have desirable properties when produced from pre-cursor powders, that permit creation of larger components than are currently commercially available, and to do so in a manner that produces improved and uniform electromagnetic properties in a cost-effective manner.
In this regard, the invention is directed to electromagnetic cores assemblies, core segments for those assemblies, and their methods of manufacture. The assemblies may be, for example, inductor and transformer cores made for high power applications. Such assemblies can be held together by physically restraining the segments relative to one another by using straps, bands, clamps, pre-forms, molds and other physical devices; or by bonding segments together using a compatible adhesive, paint or other conformal coating. As discussed in detail herein, surfaces, such as the proximal surfaces, and some embodiments ends, of the abutting segments may be formed or contoured to provide interlocking engagement therebetween that corresponds to substantially accurate meshing or mating of the segments while substantially eliminating potential variability in inductance caused by inconsistent glue line thickness.
By way of introduction, the invention provides a soft magnetic core segment comprising a first interlocking member configured to form an interlocking portion with a second interlocking member of a second magnetic core segment. In another embodiment, the invention provides a magnetic core assembly comprising a first segment and a second segment, at least a portion of the first segment configured to form an interlocking portion with at least a portion of the second segment. The invention also provides stacked magnetic core assemblies comprising at least one segmented magnetic core assembly as described herein.
In general terms, the segments may be formed into the desired shape by compacting soft magnetic powders at pressures ranging up to 150 tons per square inch into shapes being selected from a family of geometries that all possess commonality in terms of providing mechanical registration of the segments with respect to one another in an assembly. The registration may be uniform, predictable, repeatable and unaffected by operator methodology during assembly of the segments. The resultant assemblies provide sufficient strength to withstand the rigors of being wound with heavy conductors when used as high power components in power supplies, power factor correction circuits, and other circuitry where large magnetic cores are advantageous.
In general terms, methods of forming the magnetic core segments of the invention include forming the magnetic core segment comprising an interlocking member, the interlocking member configured to form an interlocking portion with a second interlocking member of a second magnetic core segment. In another embodiment, the invention provides a method of forming a segmented magnetic core, comprising: contacting a first segment to a second segment, the first segment having an interlocking member configured to form an interlocking portion with a second interlocking member of the second magnetic core segment; and interlocking the first segment to the second segment to form the segmented magnetic core. Embodiments of the invention also provide methods of forming a stacked magnetic core assembly, comprising placing a first magnetic core assembly over a second magnetic core assembly, the first and second magnetic core assemblies each comprising an inter-layer interlocking member configured to form an inter-layer interlocking portion therebetween.
The segments of the invention may be made from any suitable soft magnetic materials known to those of ordinary skill in the art for compaction and sintering to develop desired magnetic properties. Suitable examples include ferrite powders, such as Ni—Zn or Mn—Zn ferrite powders, and combinations thereof. It is also contemplated that the segments may be made from a variety of insulated soft magnetic metal alloy powders, the powders being formed into a desired shape and further processed to enhance magnetic properties. Examples of suitable metal alloy powders include, for example, Fe, Fe—Al—Si, Fe—Co, Fe—Co—V, Fe—Mn, Fe—P, Fe—Si, Ni—Fe, Ni—Fe—Mo, and combinations thereof, as well as amorphous and nanocrystalline alloys of various well known chemistries. Accordingly, one of ordinary skill in the art will recognize that the segments and assemblies of the embodiments set forth herein may be formed of any soft magnetic materials that can be compacted from powders that exhibit useful properties in a wide range of electromagnetic circuits. Accordingly, embodiments of the invention may employ a wide variety of commercially available soft magnetic materials, such as those made from insulated metal alloy powders, as well as pressed and sintered ceramic soft magnetic materials, such as ferrites, and combinations thereof, and should not be construed as being limited to the type of materials employed.
Referring to
The interlocking members 1a, 2a may have any cross sectional configuration to promote for efficient meshing between an adjacent segment. For example, and as discussed below, the protrusion and the indentation may each have a matching or mating cross-sectional configuration, such as, for example, a stepped-pyramidal, a square, a rectangular, a trapezoidal, triangular or conical, or arcuate cross section, and the like, or any combination thereof can be used. One of ordinary skill in the art will recognize that additional interlocking configurations other than those illustrated herein may also be employed. In addition, one of ordinary skill in the art will recognize that other assembly configurations other than those illustrated may be employed.
In addition, embodiments of the invention that employ the configuration set forth in
It is contemplated that segments of the invention, such as those of
As can be recognized by one of ordinary skill in the art, embodiments of the invention, such as those discussed herein, allow pre-formed coils of wire, such as a pre-wound bobbin, to be inserted onto the semi-assembled segments prior to completed assembly, and thereby reduce the costs normally associated with winding toroids. This is in contrast to conventional toroids, where wire must be wound directly onto the core using specialized winding equipment such as that manufactured by Gorman Machine Corp., Brockton, Mass., or Jovil Manufacturing Co., Danbury, Conn. Circuit designers most often choose toroid cores for inductor applications, however one drawback of using them is the extra cost associated with applying the winding. A toroid winding machine requires pre-winding the proper length of wire onto a spool before it is transferred to the core, making it slower than the bobbin winding process used with mated cores such as E-E, E-I, U-U, U-I, C-C and C-I configurations. Embodiments of the invention that employ segmented assemblies allow pre-wound wire to be placed over various segments without the need for special winding processes.
As shown in
In certain embodiments of the invention, careful placement of the profiles along the top and bottom faces of the segments allow spacing between profiles within each segment 70 that may be equal to the spacing between profiles on adjacent segments 72 that allow the layers to be stacked either directly on top of one another or to overlap those of the layer above and beneath, as illustrated. By overlapping segments in this way, additional strength of the assembly can be achieved by the inherently greater interfacial surface on which to apply adhesive. Any variation in glue line thickness in this plane will not affect permeability or other properties of the assembly. This is because the magnetic flux created in the wound and energized core is parallel to the circumference of the assembly. Magnetic flux is not impeded by air gaps that are parallel to it. The stacked segmented magnetic core assembly 60 allows a wire coil, such as a pre-wound bobbin (not shown) to be placed over at least one of a first segment of the magnetic core 65 and a second segment of the magnetic core 63.
The segments of embodiments of the invention may form assemblies that may be useful in a wide range of applications and configurations that employ large, economical cores such as, for example, in switching power supplies, flyback transformers, power factor correction circuits, high power transformers and high power inductors such as inductors for inverters, inductors for solar energy power conversion, inductors for wind energy power conversion, inductors for fuel cell power conversion, inductors for transportation power conversion applications, such as train traction and electric/hybrid vehicles.
The invention will be further described by reference to the following example. The following example is merely illustrative of the invention and are not intended to be limiting.
In the comparison both core assemblies are made from a 26-perm sendust (Fe—Al—Si) alloy. Both cores have essentially identical volumes of magnetic material (136 cm3, 138 cm3) and, therefore, the same energy storage capability when used as an inductor. The physical dimensions of the assemblies are used to calculate the effective core area (Ae), magnetic path length (Ie) and core volume (Ve) according to industry accepted standards published by the International Electrotechnical Commission, Geneva, Switzerland, publication IEC-205. Inserting these values into Equation 2, the inductance of each assembly is calculated and expressed in terms of nanohenries-per-turns-squared (nH/N2). Using each of these assemblies to create a 10 nH inductor at 100 amperes of current, the results are shown in the Table in
Embodiments of the invention set forth herein provide designs of magnetic core segments that provides accurate registration of each segment within an assembly. The registration can be both circumferential as well as inter-laminar. Because the interlocking members can take many profiles, the interlocking portion between the segments can be engineered to provide both interlocking engagement and at least one gap portion for receipt of a bonding material, such as an adhesive. The interlocking members provides the added benefit of restricting adhesive to certain areas of the abutting segment ends so as to provide the necessary strength of the final assembly. The interlocking portions can provide direct segment-to-segment contact in areas adjacent to the cavities so that the adhesive thickness does not affect the inductance of the final assembly. The assembly provides improved uniformity in inductance from assembly to assembly. The assembly can take many forms, including forms that combine different and individual segment cross sections together and form more complex assemblies. The individual interlocking segments may be selected based on a desired or selected size and shape of the assembly. Complex assemblies have the additional benefit of incorporating round cross section segments with rectilinear segments so as to reduce winding losses when the assembly is used in high power applications.
It will be appreciated by those skilled in the art that changes could be made to the embodiments described above without departing from the broad inventive concept thereof. It is understood, therefore, that this invention is not limited to the particular embodiments disclosed, but it is intended to cover modifications that are within the spirit and scope of the invention, as defined by the appended claims.