The present invention relates to an electro-magnetic coil with coolant permeability, an insulated wire building up such electromagnetic coils, as well as a method of producing such an electro-magnetic coil with coolant permeability.
Electromagnetic coils are a basic component of a vast array of modern technologies. High-power electromagnetic coils in particular are used extensively in the fields of medicine, particle physics, micromanipulation, and many others. Such coils comprise electromagnetic coil windings that are often actively cooled with a fluid to allow the winding to withstand high current density without overheating.
Various strategies exist to make this cooling maximally effective. Generally speaking, it is advantageous to increase the rate of coolant flow and the area of the wire in contact with the coolant, while at the same time maximizing proximity of wire and coolant, i.e. any heat conducted to the coolant should have to traverse as short a distance through the wire as possible. Also, it is of course preferable to use standard wires and winding techniques if possible.
A number of designs and configurations for electromagnetic coil windings have been proposed in the literature, the most relevant of which are described here.
U.S. Pat. No. 2,710,947 describes a coil wound with two strips of material simultaneously—the first being an un-insulated conductor, and the second being a corrugated insulator—such that the corrugated insulating strip forms axial cooling channels in the coil structure.
EP 2,330,603 describes a transformer coil wound with two conductive strips, at least one of which is corrugated in order to form axially-extending coolant channels.
U.S. Pat. No. 8,284,006 describes an air-cooled transformer coil having spacer elements between winding layers that form axial passages for air to flow.
Many different approaches to create cooling channels by embedding different spacer elements within the winding are known. One example is U.S. Pat. No. 7,023,312 disclosing thermoplastic ducts spaced between the layers of conductive winding.
U.S. Pat. No. 3,579,162 describes a transformer coil having axial cooling ducts around which the coil wires are wound.
U.S. Pat. No. 2,632,041 describes a transformer having winding sections separated by axial spacer elements, thus forming radial cooling channels.
U.S. Pat. No. 3,056,071 describes an electromagnetic coil formed with a wire having shallow groove-shaped cutouts that form axial cooling channels.
The electro-magnetic coils described in the prior art require complex wire geometries and/or winding techniques.
In light of the aforementioned prior art and the limitations thereof, it is inter alia an object of this invention to provide a coil whose coolant permeability emerges intrinsically.
An electro-magnetic coil with coolant permeability according to the invention is wound using insulated wire, comprising a plurality of radially arranged layers and a plurality of axially arranged turns of the insulated wire per layer, wherein the insulated wire has a plurality of sections along its length with different cross-sections for any pair of two adjacent sections.
A coil according to the invention comprises a coil whose coolant permeability emerges intrinsically as a result of the wire's varying cross-sectional shape. The difference of the cross-section of adjacent section can comprise a variation of height or a variation of width or a variation of both dimensions. Such an embodiment according to the invention is characterized by combined axial and radial cooling channels providing a coil winding with coolant permeability in both the axial and radial directions.
It is a further object of the invention to provide a coolant permeable coil that can be formed from standard, readily available insulated wires using common coil winding techniques.
According to an embodiment of the invention, a coil is wound from a wire having periodically varying cross-sectional shape and/or area along its length. This wire can be formed by drawing a standard insulated wire with uniform cross-section through a forming tool, which periodically compresses sections of the wire along its height, width or both. As the wire is wound in multiple rows over multiple layers, the varying cross-sections form coolant channels in both axial and radial directions. The shape and periodicity of the cross-sections can be optimized for various purposes. For instance, if it was advantageous for the majority of coolant to flow in the radial direction, the cross-sectional parameters of the wire could be adjusted to form primarily radial coolant channels, and vice versa.
The coil according to the inventions results in a large heat transfer area with coolant distributed throughout the winding volume. It does not require separate spacer elements which simplifies the winding process and allows maximal packing density (volume copper/total volume) to achieve maximum magnetic field generation per given input power. The optimization is related to both the coil itself and the method of winding it. The fact that it does not require spacers and can be wound using standard practices is related to the method, but the realization of optimal packing density is a property of the winding configuration itself, regardless of how it is actually achieved.
The coil preferably comprises a housing with at least one inlet and at least one outlet, connected to gaps in axial and/or radial directions of the coil creating channels for a coolant fluid, wherein the inlet(s) and outlet(s) are adapted to be connected to a coolant circuit to pump a coolant fluid through the channels of the coil to cool the coil.
The inlet(s) and outlet(s) can be provided in longitudinal direction at opposite sides of the housing of the coil, e.g. at the same radial direction from the core of the coil, wherein the coolant is moved through the winding in axial direction by applying an axial pressure gradient and the radial cooling channels are used to distribute flow evenly over radial flow cross-section.
The inlet(s) and outlet(s) can also be provided in different radial distances from the core of the coil, then the coolant is moved through the winding in radial direction (inward or outward) by applying a radial pressure gradient and the axial cooling channels are used to distribute flow evenly over axial flow cross-section.
It is a further object of the invention to provide an insulated wire to build-up an improved coil with coolant permeability.
Such an insulated wire has an initial round shape before deformation for optimal price of the raw material. It can also have an initial rectangular, especially square shape. If the wire used is approximately rectangular before deformation then an optimum packing density results.
An insulated wire used to form a coolant-permeable electro-magnetic coil comprises alternating sections of round or rectangular shaped wire and deformed sections compressed along the height or width of the wire. The cross-section reduction along the height and the width of the wire can be anti-aligned, wherein the wire is wide where it is flat or wherein the wire is narrow where it is high, achieving an approximate constant total wire cross-section of the wire.
Alternatively, the wire deformation along the height and the width of the wire can be aligned, wherein the wire is wide where it is high and wherein the wire is narrow where it is flat to achieve the best fluid permeability.
It is a further object of the invention to provide an improved method of producing a coil with coolant permeability.
This object is achieved by a method to produce a coil comprising the steps of compressing the wire using a wire-forming tool consisting in one embodiment of two wheels that have profiled surfaces corresponding to the desired wire thickness.
This method allows winding a coil from a single, continuous, insulated wire in traditional manner, but without requiring the use of additional spacing elements. The deformation process of an ordinary insulated wire takes place at the same time as winding by pressing and deforming the wire right before winding it.
According to one embodiment, the parameters of the wire taken from the group including thickness, deformation periodicity, deformed section length, deformed section width and inner diameter of the winding are chosen at random. This allows creating coolant channels which form stochastically. While the resultant channels will still be very effective, they will likely not be optimal.
According to another embodiment, a relationship between the wire parameters and the resulting coil is defined beforehand that ensure the channels will continue to align with themselves over multiple layers, in order to realize an ideal channel configuration. One such relationship comprises in its simplest form to set L=2*pi*t, where L is the length of the periodic pattern, and t is the maximum thickness (height) of the wire, with pi being Ludolph's number. At the same time the circumference of the core on which the wire is wound is chosen to be a multiple of length L so that deformed and un-deformed sections between windings in the same layer align. In other words L is a divisor of the value of the circumference of the core on which the wire is wound. This alignment is still essentially achieved for a high number of layers increasing the diameter of the wound wire layers.
The coolant channels can be formed from the group encompassing radial coolant channels between subsequent layers of wires, axial coolant channels between adjacent turns of wires, and cross-section coolant channels between two adjacent turns and between two subsequent layers.
The cross-section of the wire can change between undeformed circular sections and two different deformed section, i.e. oval or elliptic sections with the longer axis direction in either layer or turn orientation.
An electromagnetic coil winding according to the invention has intrinsically emerging radial and axial coolant channels. The coil is wound from a wire with varying cross-sectional shape, said wire consisting of alternating deformed and undeformed sections that collectively form into axial and radial coolant channels as the wire is wound around a core.
Preferred embodiments of the invention are described in the following with reference to the drawings, which are for the purpose of illustrating the present preferred embodiments of the invention and not for the purpose of limiting the same. In the drawings,
The initial wire 310 can be rectangular or oblong/elliptical, especially it can be an initial wire which is insulated. The cross-section of the deformed section 13 of
Of course it is possible to start with a wire 11 having a rectangular cross-section and deform it into an essentially square one. The deformation process is not intended to damage the insulation. It is possible that the main part of the deformation is exerted within the insulation coating.
b and 2c show a second embodiment 20 of a wire with varying cross-section in a top view, a side view and a perspective view, respectively. The wire 21 is a commercially available insulated wire. At first the wire 21's cross-section is uniform throughout its length. As the wire 21 is wound onto the magnet core, it is periodically deformed such that untouched areas 22 having substantially the original cross-section alternate with deformed areas 23 having a new cross-section. The cross-section of the deformed section 23 is both flatter and narrower than the original section 22, i.e. it is compressed to a smaller cross-section area. In other words, the tool used to deform the wire 21 deforms the wire 21 along both its height and width.
Between the sections 22 and 23 are present deformed upper shoulders 201 and side shoulders 202, mainly comprising inclined surfaces between the corresponding adjacent surfaces. Adjacent shoulders 201 and 202 have an inclination directed into the same direction, i.e. reducing the cross-sectional area from a section 22 to a section 23 and increasing the cross-sectional area from section 23 to section 22.
When a second layer of windings (here four turns 19) is arranged on the first layer 29 shown in
End caps 75 and 76 form the structural support for the winding, and together with outer tube 77 form a sealed volume around winding 72. Coolant is pumped as represented by inlet flow 200 through inlet(s) 73 in the endcap 75 and out through outlet(s) 74 in the endcap 76 as outlet flow 212. As the coolant enters the winding, it disperses radially and flows axially as axial flow 211 to outlet 74. Variations of the design are possible such as where inlet 73 and outlet 74 are on the same side of the magnet 71 by either segmenting the wire volume to form a U-shaped flow path that returns to the inlet side or by embedding flow channels to lead the coolant back to the inlet side at endcap 75 either through the core 71 or around the winding.
Finally,
This application is the United States national phase of International Application No. PCT/EP 2020/052019 filed Jan. 28, 2020, the disclosure of which is hereby incorporated by reference in its entirety.
Filing Document | Filing Date | Country | Kind |
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PCT/EP2020/052019 | 1/28/2020 | WO |