Inductor core

Abstract

An inductor core including a two separate inductor core components which, when assembled with each other, together form the inductor core and define a common axis; wherein the inductor core components form at least one magnetic flux barrier, the magnetic flux barrier having a width in the circumferential direction relative to the common axis; wherein the width is adjustable by rotating the inductor core components relative to each other around the common axis.

Claims

1. An inductor core comprising two separate inductor core components which, when assembled with each other, together form the inductor core and define a common axis; wherein the inductor core components form at least one magnetic flux barrier, the magnetic flux barrier having a width in the circumferential direction relative to the common axis; wherein said width in the circumferential direction is configured to be adjustable in a range from a position in which a first one of the two conductor core components contacts a second one of the two conductor core components to a position in which the first conductor core component is out of contact with the second conductor core component by rotating the inductor core components relative to each other around the common axis; wherein a first one of the two inductor core components comprises a first set of projections and a second one of the two inductor core components comprises a second set of projections; wherein the projections of the second set interleave the projections of the first set so as to define a respective flux barrier between each projection of the second set and a respective adjacent projection of the first set; and wherein the first set of projections comprise at least three projections.

2. The inductor core of claim 1, wherein the two inductor core components have the same shape and size.

3. The inductor core of claim 1, wherein the inductor core components are made of a soft magnetic powder material.

4. A method of adjusting a width of a magnetic flux barrier of an inductor core as defined in claim 1; the method comprising rotating the inductor core components relative to each other around a common axis so as to adjust a width of the magnetic flux barrier.

5. The inductor core of claim 1, wherein the first inductor core component comprises a first base member, wherein the second inductor core component comprises a second base member, and wherein the inductor core comprises at least a first axially extending core member shaped and sized to provide a magnetic flux path between the first and second base members.

6. The inductor core of claim 1, wherein the magnetic flux barrier extends in a direction that is parallel with the common axis.

7. The inductor core of claim 1, wherein the projections of the first and second set of projections are rectangular-shaped.

8. The inductor core of claim 1, wherein the first inductor core component comprises a first base member, wherein the second inductor core component comprises a second base member; wherein the inductor core further comprises an inner core member and an outer core member, each axially extending between the first and second base members and providing respective magnetic flux paths between the first and second base members; wherein the outer core member at least partly surrounds the inner core member, thereby defining an outer circumference of a space around the inner core member for accommodating a winding between the inner and the outer core members; and wherein at least one of the inner and outer core members comprise said at least one magnetic flux barrier.

9. The inductor core of claim 8, wherein the outer core member comprises the first and second sets of projections defining a respective gap between each projection of the second set and a respective adjacent projection of the first set.

10. The inductor core of claim 9, wherein each projection has a radial width that varies along the circumferential direction.

11. The inductor core of claim 8, wherein a flux conducting cross-sectional area of the outer core member exceeds a flux conducting cross-sectional area of the inner core member.

12. The inductor core of claim 1, wherein the first set of projections each comprise a first lateral side face and a second lateral side face and wherein for at least one of the first set of projections, the first lateral side face is broader in a radial direction than the second lateral side face.

13. The inductor core of claim 12, wherein the second set of projections each comprise a first lateral side face and a second lateral side face, wherein for at least one of the second set of projections, the first lateral side face is broader in a radial direction than the second lateral side face, wherein the first lateral side face of the at least one of the first set of projections faces the first lateral side face of the at least one of the second set of projections.

14. An inductor core comprising two separate inductor core components which, when assembled with each other, together form the inductor core and define a common axis; wherein the inductor core components form at least one magnetic flux barrier, the magnetic flux barrier having a width in the circumferential direction relative to the common axis; wherein said width in the circumferential direction is configured to be adjustable in a range from a position in which a first one of the two conductor core components contacts a second one of the two conductor core components to a position in which the first conductor core component is out of contact with the second conductor core component by rotating the inductor core components relative to each other around the common axis, wherein the inductor core comprises a first and a second base member and at least a first axially extending core member shaped and sized to provide a magnetic flux path between the first and second base members; wherein the first core member comprises a first set of projections axially extending from the first base member towards the second base member and a second set of projections axially extending from the second base member towards the first base member; where the projections of the second set interleave the projections of the first set so as to define a respective flux barrier between each projection of the second set and a respective adjacent projection of the first set.

15. The inductor core of claim 14, wherein a first one of the two separate inductor core components comprises the first base member and the first set of projections, and a second one of the two inductor core components comprises the second base member and the second set of projections.

16. The inductor core of claim 14, further comprising a second axially extending core member shaped and sized to provide a magnetic flux path between the first and second base members.

17. The inductor core of claim 16, wherein each of the two inductor core components comprises a part of the second core member.

18. The inductor core of claim 14, wherein the first set of projections each comprise a first lateral side face and a second lateral side face and wherein for at least one of the first set of projections, the first lateral side face is broader in a radial direction than the second lateral side face.

19. The inductor core of claim 18, wherein the second set of projections each comprise a first lateral side face and a second lateral side face, wherein for at least one of the second set of projections, the first lateral side face is broader in a radial direction than the second lateral side face, wherein the first lateral side face of the at least one of the first set of projections faces the first lateral side face of the at least one of the second set of projections.

20. An inductor core comprising two separate inductor core components which, when assembled with each other, together form the inductor core and define a common axis; wherein the inductor core components form at least one magnetic flux barrier, the magnetic flux barrier having a width in the circumferential direction relative to the common axis; wherein said width in the circumferential direction is configured to be adjustable in a range from a position in which a first one of the two conductor core components contacts a second one of the two conductor core components to a position in which the first conductor core component is out of contact with the second conductor core component by rotating the inductor core components relative to each other around the common axis; wherein a first one of the two inductor core components comprises a first set of projections and a second one of the two inductor core components comprises a second set of projections; wherein the projections of the second set interleave the projections of the first set so as to define a respective flux barrier between each projection of the second set and a respective adjacent projection of the first set, and wherein the first set of projections each comprise a first lateral side face and a second lateral side face and wherein for at least one of the first set of projections, the first lateral side face is broader in a radial direction than the second lateral side face.

21. The inductor core of claim 20, wherein the second set of projections each comprise a first lateral side face and a second lateral side face, wherein for at least one of the second set of projections, the first lateral side face is broader in a radial direction than the second lateral side face, wherein the first lateral side face of the at least one of the first set of projections faces the first lateral side face of the at least one of the second set of projections.

22. The inductor core of claim 20, wherein the two inductor core components have the same shape and size.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) Embodiments of the various aspects disclosed herein, as well as additional objects, features and advantages of the present inventive concept, will be described in more detail in the following illustrative and non-limiting description of embodiments of the aspects disclosed herein with reference to the appended drawings, where like reference numerals refer to like elements unless stated otherwise, wherein:

(2) FIG. 1 shows a schematic exploded view of an embodiment of an inductor.

(3) FIGS. 2a-b are illustrations of an inductor core in assembled condition.

(4) FIG. 3 shows a schematic view of another embodiment of an inductor core component.

(5) FIG. 4 is an illustration of an inductor core in assembled condition.

(6) FIGS. 5-6 show further embodiments of an inductor core.

(7) FIG. 7 illustrates examples of an inductor core configured to have an inductance that changes with the current loading.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

(8) FIG. 1 is a schematic exploded view of an embodiment of an inductor comprising an inductor core and a winding 109. The inductor core is formed by two separate inductor core components 101a and 101b, respectively.

(9) A first one (101a) of the two inductor core components comprises a base member 103a, an inner core member 105a, and a set of projections 102a. The base member 103a has the form of a circular disc defining a periphery 104a. The inner core member section 105a extends axially from a center of the base member 103a. In the present example, the inner core member section has a cylindrical shape. However, it will be appreciated that the inner core member section may have a different shape, e.g. a polygonal cross-section. The base inner core member section 105a is arranged coaxially with the base member 103a. The projections 102a extend axially from the base member 103a and are distributed along the periphery 104a of the base member 103a, leaving a radial gap between the inner core member section 105a and the projections 102a. The projections 102a extend in the same direction as the inner core member section 105a. The projections 102a are spaced apart from each other in the circumferential direction, thus defining gaps between adjacent projections, the gaps being delimited by the lateral side faces 107a of the projections. In the example of FIG. 1, the projections 102a all have the same shape and size and they are uniformly distributed along the periphery 104a, i.e. all gaps between adjacent projections have the same size. The set of projections 102a thus together form a part of an outer core member surrounding the inner core member section 105a. The inner core member section 105a and the set of projections 102a together define a space between the inner core member section 105a and the set of projections 102a for accommodating the winding 109. Each projection 102a is formed as a segment of a tubular wall, so that the set of projections together form a tubular wall having axially extending slots. The axial length of the inner core member section 105a is shorter than the axial length of the projections 102a.

(10) It will be appreciated that, in alternative embodiments, the shape and/or arrangement of the various parts of the inductor core component 101a may be different. For example, the projections may have a different shape, they may have shapes and/or sizes different from each other, the gaps between adjacent projections may not all have the same size, etc.

(11) In the example of FIG. 1, the second inductor core component 101b has the same shape and size as the first inductor core components 101a, i.e. the second inductor core component 101b comprises a base member 103b, an inner core member section 105b, and a set of projections 102b extending from a periphery 104b of the base member 103b, all as described in connection with the first inductor core component 101a. It will be appreciated however, that other embodiments of an inductor core may comprise two inductor core components of different shapes. For example, only one of the components may comprise an inner core member section which then may be sufficiently long so as to axially extend all the way to the base member of the other inductor core component in the assembled inductor core. Alternatively or additionally, the projections of the two components may have different shapes and sizes.

(12) The two inductor core components 101a and 101b are adapted to be assembled axially aligned and with their respective inner core member sections 105a,b facing each other and such that the projections extend into the gaps formed by the projections of the other component, i.e. such that the projections of one component are interleaved with the projections of the other component.

(13) The inner core member sections 105a and 105b may touch each other with their respective front faces 106a and 106b in the assembled indictor core so as to form an inner core member extending all the way between the base members 103a and 103b, respectively. In some embodiments, the inner core member sections 105a,b may define an axial flux barrier, e.g. in the form of an axially extending gap between them and/or in the form of a part of one or both inner core member sections comprising a material of lower permeability.

(14) Together, the interleaved projections 102a,b of the two inductor core components 101a,b form an outer core member having the form of an outer tubular wall that surrounds the inner core member thereby forming a radially and axially extending space between the inner core member and the outer core member, which space is for accommodating the winding 109.

(15) The winding 109 has a tubular shape and is sized such that it surrounds the inner core member and fits in the space between the inner and outer core member. The inductor core may further comprise a winding lead-through and/or other features (not shown so as to simplify the illustration). The lead-through may be arranged e.g. in the outer core member or in one of the base members.

(16) The inductor core components 101a and 101b may each be made of compacted magnetic powder material. The material may be soft magnetic powder. The material may be ferrite powder. The material may be surface-insulated soft magnetic powder, e.g. comprising iron particles provided with an electrically insulating coating. The resistivity of the material may be such that eddy currents are substantially suppressed. As a more specific example, the material may be a soft magnetic powder, e.g. from the product family Somaloy (e.g. Somaloy® 110i, Somaloy® 130i or Somaly® 700HR) from Hoeganaes AB, S-263 83 Hoeganaes, Sweden.

(17) The soft magnetic powder may be filled into a die and compacted. The material may then be heat treated, e.g. by sintering (for powder materials such as ferrite powder) or at a relatively low temperature so as not to destroy an insulating layer between the powder particles (for soft magnetic composites). During the compaction process a pressure may be applied in a direction corresponding to the axial direction of the respective member. In the radial and circumferential directions the dimension of the components are defined by the cavity walls of the mold. Each component may thus be manufactured using uniaxial compaction with a tighter tolerance in the radial and circumferential directions than in the axial direction.

(18) Alternatively, the inductor core components may be made from a different material of a sufficiently high permeability, higher than the permeability of air, and/or assembled from a plurality of individual pieces rather than formed in a single piece.

(19) FIGS. 2a-b are illustrations of an inductor core in assembled condition. Once the inductor core is assembled, the interleaved projections 102a,b of the two inductor core components 101a,b form a tubular wall having axially extending slots 210 and 211 between respective projections of one of the two inductor core components and an adjacent one of the projections of the other inductor core component. These slots are formed, because the projections of each component have a width d, measured in the circumferential direction, that is smaller than width D (also measured in the circumferential direction) of the gap between adjacent projections of the respective other component.

(20) Depending on the angular position of the two inductor core components 101a,b relative to each other, the slots cause the magnetic flux through the outer core member from one base member to the other to cross a flux barrier in the form of an air gap, where the size of the air gap (in the circumferential direction) depends on the relative angular position of the inductor core components with respect to each other.

(21) In the example of FIG. 2a, the inductor core components are oriented such the each projection 102a of one inductor core component touches an adjacent projection 102b of the other inductor core component, i.e. respective lateral surfaces 107a,b of the projections touch each other. Consequently, a magnetic flux path exists between the base members through the outer core member such that the entire flux path extends through the material of the inductor core members, as indicated by the arrow 212 in FIG. 2a. As can be seen, the flux path crosses the touching surfaces between two of the projections.

(22) FIG. 2b shows the inductor core where the inductor core components 101a,b are rotated to a different relative angular position with respect to each other such that each projection is separated from both its adjacent projections of the other inductor core component by respective gaps 210, 211. Consequently, the magnetic flux between the base members through the outer core member has to cross a gap between adjacent projections, as indicated by arrow 213.

(23) The size of the smallest gap which the flux has to cross may be continuously varied by rotating the inductor core components 101a,b relatively to each other around their common axis. It will be appreciated that the smallest gap size may be varied between 0 mm (as in the example of FIG. 2a) and a maximum gap size equal to (D−d)/2 which occurs when each projection is positioned exactly in the center between two adjacent projections of the respective other inductor core component. Typical maximal gap sizes may range between 1 mm and 8 mm. However, other gap sizes may be possible, depending on the desired properties of the inductor. It will be appreciated that when the gaps formed on respective sides of a projection have different width, the magnetic flux will predominantly flow across the narrower one of the gaps. Hence, the effective gap width is normally defined by the smallest one of the gaps.

(24) As can most clearly be seen in FIG. 2a, in this example the inner core member sections 105a and 105b touch each other in the assembled inductor core (for reasons of simplicity of the illustration, in FIGS. 2a-b the inductor core is shown without the winding). Furthermore, the projections 102a,b have an axial length small enough so as to cause them to only partially extend towards the base member of the respective other inductor core component when the inductor core components are assembled with their inner core member sections touching. Hence a gap 214 is formed between a free end 108a,b of each projection and the respective other inductor core component. This gap may have a width L (measured in the axial direction). It will thus be appreciated that the maximum obtainable gap size between the inductor core components may be the smaller of L and (D−d)/2.

(25) In the assembled condition, the inductor core of FIGS. 1 and 2a-b thus provides a closed loop flux path extending axially from one base member to the other through the inner core member, radially inwards within one of the base members, radially outwards within the other base member, and axially and partially circumferentially in the outer core member. The closed loop flux path crosses a flux barrier formed by the gap(s) 201 and/or 211 between adjacent projections where the gap width of the gap is adjustable by rotating the inductor core components relatively to each other around their common axis.

(26) Hence, inductors having different inductance properties may be manufactured using the same inductor core components. To this end, during manufacture, the inductor core components and the winding may be assembled, the inductor core components may be rotated relatively to each other so as to adjust the gap size to a desired value, and by securing the inductor core components in their desired position relative to each other, e.g. by gluing the components together, by filling the gaps with a desired curable material of sufficiently low permeability, and/or the like. Generally, the gaps 210, 211 and/or 214 may be filled with air, wherein the magnetic flux barrier is formed as an air gap. Alternatively, some or all of the gaps may be filled with a material presenting a significantly reduced magnetic permeability compared to the material of the indictor core components. By way of example, the material may be a plastic material, a rubber material or a ceramic material.

(27) As will be understood by those skilled in the art, it is much more feasible to accurately adjust the size of the gaps 210 and 211 by rotating the inductor core components relatively to each other than to reduce the acceptable manufacturing tolerance interval of the components in the axial direction.

(28) Furthermore, as mentioned above, the tolerance interval in the circumferential direction may be made relatively tight. Thus, also the circumferential width of the projections and the circumferential width of the gaps between them may be accurately defined. Since the inductance of a final inductor depends on the total length of the flux path and the size of the flux barrier, the design according to the inductor core enables manufacturing of inductors presenting a precise inductance.

(29) FIG. 3 shows a schematic view of another embodiment of an inductor core component. The inductor core component 301a of FIG. 3 is similar to the indictor core component 101a shown in FIG. 1 in that it comprises a base member 303a, and inner core member section 305a, and a set of projections 302a, all as described in connection with the inductor core component 101a of FIG. 1, except that the base member 303a and the projections 302a have a different shape. In particular the base member 303a is a plate defining a circumference that has alternating convex and concave portions. Furthermore, the projections 302a have a radial width that varies in the circumferential direction, i.e. the projections have a narrow lateral side 315 having a smaller radial width than the other, broader lateral side 316.

(30) FIG. 4 is an illustration of an inductor core in assembled condition where that inductor core comprises two inductor core components 301a and 301b, each as described in connection with FIG. 3. In particular, FIG. 4a shows a 3D view of the assembled inductor core, while FIG. 4b shows a cross sectional view of the inductor core. The inductor core components 301a and 301b have the same size and shape, each comprising a base member 303a,b, respectively, projections 302a,b, respectively, and inner core member sections together forming an inner core member 305. Consequently in the assembled inductor core the inductor core components may be arranged such that the air gap 310 having the smallest reluctance is formed by two adjacent projections facing each other with their respective broad lateral side surface 316. The opposite, narrow lateral side face 315 of each projection thus faces a narrow side face of another projection. However, the gap 311 between the narrow side faces may be selected to be larger than the gap between two broad side faces. Consequently, the reluctance of the gap defined between the narrow side faces is considerably larger than the reluctance of the gap between the broad side faces. Consequently, the reluctance of the inductor may be controlled more accurately, and flux leakage is reduced.

(31) FIG. 5 shows another embodiment of an inductor core. The inductor core of FIG. 5 is similar to the inductor core of FIG. 1 in that the inductor core comprises two separate inductor core components 501a and 501b, respectively. Both inductor core components comprise a base member 503a,b, respectively, an inner core member section (not explicitly shown), and a set of projections 502a,b, respectively, all as described in connection with FIG. 1. However, the embodiment of FIG. 5 differs from the embodiment of FIG. 1 in that the inductor core components 501a,b have different shapes. In particular, the projections 502a of one of the inductor core components 501a are longer than the projections 502b of the other inductor core component 501b.

(32) FIG. 6 shows yet another embodiment of an inductor. The inductor of FIG. 6 is similar to the inductor of FIG. 1 in that the inductor comprises a tubular winding 609 and an inductor core formed by two separate inductor core components 601a and 601b, respectively. In the example of FIG. 6, the inductor core component 601a is similar to the inductor core components of FIG. 1 in that it comprises a base member 603a, an inner core member section 605a, and a set of projections 602a. The base member 603a has the form of a circular disc. The inner core member 605 extends axially from a center of the base member 603a. A tubular circumferential wall 645 extends axially from a periphery of the base member 603a leaving a radial gap between the inner core member 605 and the wall 645. The wall defines a periphery 604 facing away from the base member. Axial projections 602a are distributed along the periphery 604. The projections 602a extend in the same direction as the inner core member 605. The projections 602a are spaced apart from each other in the circumferential direction, thus defining gaps between adjacent projections. The wall 645 and the set of projections 602a thus together form an outer core member surrounding the inner core member 605. The axial length of the inner core member section 605 is shorter than the axial length of the wall 645 including the projections 602a. The second inductor core component 601b is formed as a disc 603b having radial projections 602b extending radially outward from the periphery of the disc. The inductor core component 601b thus forms a lid of the inductor core component 601a where the axial projections 602a interleave the radial projections 602b and axially extend into the gaps formed between the radial projections of the inductor core component 601b. When assembled, the inner core member 605a touches the disc 603b.

(33) The circumferential width of the radial projections 602b is smaller than the size of the gaps formed between adjacent axial projections 602a. Furthermore, the radial length of the projections 602b is larger than the radial wall thickness of the axial projections 602b. Consequently, when the inductor core component 601b is assembled with the inductor core component 601a, an air gap is formed between the radial projections 602b and the axial projections 602a. In particular, a tangential air gap is formed between each radial projection 602b and the side walls of the adjacent axial projections 602a. By rotating the inductor core component 601a relative to the inductor core component 601b around their common axis, the width of the tangential gap may be adjusted in a similar fashion as described in connection with the previous embodiments.

(34) Even though both components of the inductor core of FIG. 6 may be made of compacted soft magnetic powder, they may also be made of different material. For example, the disc-shaped component 601b may be made of laminate. In such an embodiment, the disc-shaped component 601b may be formed as an annular disc having a central hole for receiving the inner core member section 605 which, in turn is shaped and sized to extend through the central hole. Hence, in such an embodiment, the annular disc-shaped component mainly provides a two-dimensional flux path in the radial and circumferential directions.

(35) FIG. 7 illustrates examples of an inductor core configured to have an inductance that changes with the current loading; such an arrangement is also referred to as a ‘swinging choke’. The change of inductance is caused by partial saturation of the magnetic core due to the core geometry. The dimensions of the core, in particular the size of the projections and the tangential and axial gaps between the inductor core components, may be selected to provide a partial low reluctance path that will establish the high initial low load inductance. This low reluctance path will typically start to saturate as the current loading is increased. As the flux path saturates there will be alternative paths for the flux that is now directed to a higher reluctance that will reduce the inductance. It is possible to stabilize these two induction levels with an appropriate design of the air-gap sections.

(36) FIGS. 7a-b schematically show parts of an inductor core, e.g. the inductor core of FIG. 1, comprising inductor core components 101a,b from which respective tooth-like projections 102a,b extend. The projections 102a,b define tangential air gaps 210 between them and respective gaps 214 between an end portion of the teeth and a base member 103a,b of the respective other inductor core component. The tangential gaps 210 are narrower than the axial gaps 214.

(37) FIG. 7a illustrates a low reluctance path 725 crossing the tangential air gap 210 between adjacent projections 102a, b. As illustrated in FIG. 7b, when the current load is increased, the core material through which the low conductance path passes at least partially saturates, causing the flux to be forced to on a different path 726 which crosses the gap 214 and has a higher reluctance, as the gap 214 dominates the reluctance. Consequently with increasing current load, the inductance of the inductor decreases, e.g. as schematically illustrated in FIG. 7c. The inductance decreases between a high-inductance, low-power mode “A” where the inductance is dominated by the flux path 725 and a low-inductance, high-power mode “B” where the inductance is dominated by flux path 726.

(38) One reason for using a swinging choke is to provide further harmonic reduction when the inductor is operated at low power in an application like e.g. a switch mode power electronic circuit.

(39) It will be appreciated that, in alternative embodiments, alternative flux paths may be provided by suitable arrangement of projections and air gaps of different sizes, e.g. as illustrated in FIG. 7d. FIG. 7d schematically shows parts of an inductor core as illustrated in FIG. 7a. However in this example, the set of projections comprises one or more narrow projections 702a,b having a smaller tangential width than the remaining projections 721a,b and forming a smaller air gap 710 between them than the corresponding tangential air gaps 731 between the remaining projections 721a,b. As in the example of FIGS. 7a-b, this inductor provides a low-power flux path 725 through the narrow projections 702a,b and crossing the narrow air gap 710. At higher currents, saturation of the narrow projections occurs, and the flux will increasingly follow the path 726 through the broader projections 721a, b and the wider air gap 731.

(40) Although some embodiments have been described and shown in detail, the invention is not restricted to them, but may also be embodied in other ways within the scope of the subject matter defined in the following claims. In particular, it is to be understood that other embodiments may be utilised, and that structural and functional modifications may be made without departing from the scope of the present invention. For example, in the above, inductor cores presenting a cylindrical geometry have been disclosed. However, the inventive concept is not limited to this geometry. For example, the inductor cores may present an oval, triangular, square or polygonal cross section. Similarly, in the embodiments described above, the lateral side faces of the adjacent projections that define the air gap have been shown to be parallel to each other, i.e. the side faces have been shown to be axially-radially oriented. It will be appreciated, however, that the side faces may be chosen not to be parallel to each other, thus providing an air gap having a varying width. Other variations are possible as well, e.g. side faces having a step, so as to provide an air gap having two different widths. Such air gaps having varying widths are also referred to as swing choke and allow the design of inductors having desired inductance properties at different currents.

(41) Embodiments of the inductor core described herein may be used in a variety of applications including photovoltaic applications, in power conversion units, voltage control units, filter units such as LC or LCL filters, etc. Embodiments of the inductor core described herein may be used in systems operating at a variety of power levels, e.g. larger than 500 W such as larger than 1 kW. In particular, when embodiments of the inductor core described herein are used in a multi-phase system, e.g. a 3-phase system, inductors used in different phases may accurately and conveniently be configured to have as similar properties as desirable.

(42) In device claims enumerating several means, several of these means can be embodied by one and the same structural component. The mere fact that certain measures are recited in mutually different dependent claims or described in different embodiments does not indicate that a combination of these measures cannot be used to advantage.

(43) It should be emphasized that the term “comprises/comprising” when used in this specification is taken to specify the presence of stated features, integers, steps or components but does not preclude the presence or addition of one or more other features, integers, steps, components or groups thereof.