Patent Application
20210407722
The present invention relates to a magnetic device with a high-permeability core having an air gap, that exhibits a low sensitivity to temperature changes.
Magnetic inductive component such as inductances, transformers, ad chokes often include, in their magnetic circuit, an air gap, in order to soften the saturation of the inductive components, achieve a desired magnetic reluctance or, in the case of inductances, increase the magnetic energy that can be stored in the component. A common shortcoming of such devices, however, is that the inductance of the component is very sensitive to the thickness of the air gap and even tiny deviations from the nominal values will translate in considerable changes in the inductance. To obviate his, it is known to include precise spacers and shims to control and keep constant the width of the air gap, but these measures cannot prevent ail changes, especially those of thermal origin.
Another device used in the art to limit this undesirable effect is the potting of the device in a compound or a glue having a low coefficient of thermal expansion, or CTE. This is not a completely satisfactory solution, however, and is not cost-effective.
Many applications, including those in the automotive sector require operation in an extended temperature range and with severe vibrations, together with a severe control of the tolerances and low thermal drifts. Magnetic devices with a lower sensitivity to temperature changes and mechanical influences that may alter the width of the air gaps are therefore highly desirable.
An aim of the present invention is the provision of a magnetic component that overcomes the shortcomings and limitations of the state of the art.
According to the invention, these aims are attained by the object of the attached claims, and especially by a magnetic shell for a magnetic device juxtaposable to another shell form a magnetic core, wherein at least part of the surfaces of the magnetic shells meet when the shells are juxtaposed and form at least an air gap, wherein the magnetic core expands and contracts under temperature changes along a main expansion direction at the air gap, characterized in that the surfaces of the magnetic shells that meet to form the air gap are at least in part disposed parallel to the main expansion direction at the air gap.
The invention relates also to a magnetic device comprising at least two magnetic shells as defined above juxtaposed and forming a magnetic core, and at least one electric winding for generating a magnetic flux in the magnetic core.
Dependent claims relate to important and potentially useful features of the invention that are not however essential, and include special shapes of the shell, that can be “E”-shaped to give a three-legged core, “C”-shaped, pot shaped, or have any suitable shape; stepped surfaces at the air gaps; and configuring the cores such that, when they are juxtaposed, the air gap can be zero width or another value of width defined by design where the surfaces are parallel to the main expansion direction.
With respect to what is known in the art, the magnetic cores assembled from the shell of the invention exhibit a magnetic reluctance that is less temperature-dependent than many cores of the prior art. They can be assembled in any suitable way, including by potting, but their favourable thermal properties do not depend on the use of special CTE compounds or adhesive. In the inductors and magnetic devices of the invention the series resistance introduced by fringe fields at the airgap may be lower than in similar devices known in the art.
Exemplar embodiments of the invention are disclosed in the description and illustrated by the drawings in which:
The juxtaposing of the shells forms a magnetic core with air gaps 30, 31 where the surfaces of the shells 20a, 20b come near. The width of the air gap can be determined by shims, separators, interposition of potting compound, or any other means. Importantly, the air gaps of the centre leg 30, 30 are oriented along two orthogonal direction. Part of the gap arises from the juxtaposing of surfaces 30 that are orthogonal to the axis of the leg—and to the general direction of the magnetic flux. Part of the air gap arises from the meeting of surfaces 31 that are aligned with the axis of the leg. This variety of directions arises from the special configuration of the centre leg 23 that is stepped. Side legs 22a and 22b have a butt end, in this variant. The axial air gaps 30 need not have the same width as the transversal air gap 31 and in fact, in the presented example, the transversal air gap 31 is considerably narrower and could reduce to zero, with the surfaces 30 in contact, in some realizations.
The invention is not limited to stepped legs with surfaces parallel and orthogonal to the leg axis and could include, in non-represented variants, legs with slanted or curved meeting surfaces.
When the temperature of the core changes, its material will expand and contract according to the temperature variations. The width of the air gap in the centre leg will change accordingly, and so will the reluctance of the magnetic core and the impedance of the coil 40. Thermal expansion will tend to move the shells 20a, 21a apart from one another, as indicated by the double arrow 28, especially if the assembly includes organic material such as adhesives, separators, or potting compound, which have a high coefficient of thermal expansion. The arrow 20 indicates the main expansion direction at the air gap, determined by the coefficients of thermal expansion of all the materials involved, including separators and adhesives.
Thermal expansion has opposite effects on the axial air gaps 30, that increase in width, and on the transversal air gap 31, whose width is essentially unchanged, while the transverse area of gap 31 is very slightly reduced. Thanks to these features, the reluctance of the core and the impedance of the coil 40 change less than in a standard E core where the centre leg and the side leg end with a flat transversal surface (vertical in the figures).
Note that the magnetic device can be an inductor, a choke, a transformer, or any other device. The final assembly will include at least one winding r coil, that can be made of enamel wire, litz wire, or any other type of conductor, including PCB tracks and rigid bars. The coil or coils can be wound around the centre leg, the side legs, or the top and bottom yokes, and can be split on different legs and parts of the magnetic circuit.
The air gap generates an amount of fringe field that radiates around the gap itself. This contributes to the increase of coil resistance at high frequency, due to local eddy currents in the conductors. In the invention, the fringe fields are at least in part rotated by 90 degrees and have a lesser impact on the high frequency resistance of the coil, because they are oriented parallel to the current direction.
| Number | Date | Country | Kind |
|---|---|---|---|
| 20183062.7 | Jun 2020 | EP | regional |
