Patent Application
20150332841
The present invention relates to a litz wire coil suitable for a non-contact power supplying system of an electromagnetic induction type.
In recent years, as a means for charging electric vehicles (EVs), a non-contact power supplying system of an electromagnetic induction type using coils has been studied. A non-contact power supplying system includes an electricity-feeding side coil (primary coil) to which a power is supplied from an alternating current power source, and an electricity-receiving side coil that is disposed to face the electricity-feeding side coil and is magnetically coupled to the electricity-feeding side coil. In a non-contact power supplying system for electric vehicles, an electricity-feeding side coil is disposed outside the vehicle (floor surface), and an electricity-receiving side coil is disposed inside the vehicle.
As an electricity-feeding side coil and an electricity-receiving side coil, a plane coil that is formed by spirally winding, for example, an enameled wire (a line material configured by covering a conducting body with an insulation film) on one plane is used. A plane coil is manufactured by, for example, fixing an end of the line material to a winding frame, and rotating the winding frame while applying an appropriate tensile force to the line material. When a single-core enameled wire is used for a coil line material, variations of electrical characteristics such as inductance are small, and mass-manufacturing can be achieved in a practical range.
In addition, when a large current of high frequency is required to be supplied to transmit a large power as in the case of a non-contact power supplying system for electric vehicles, a plane coil (hereinafter referred to as “litz wire coil”) formed by winding a litz wire configured by twisting together multiple enameled wires (element wires) is used. One reason for this is that increase in alternating-current resistance due to the skin effect and the proximity effect specific to high frequency can be limited when a litz wire is used.
Conventionally, a litz wire coil has been proposed in which a litz wire is rolled in a tape form in such a manner as to work the wire into a rectangular shape in cross section, and then the wire is spirally wound, thereby increasing the space factor (for example, PTL 1). In the litz wire coil disclosed in PTL 1, the space factor is increased, and therefore the electric resistance is enhanced and the coil size is stabilized, and consequently, variations of inductance can be limited.
PTL 1
Japanese Patent Application Laid-Open No. 2000-215972
For the use in vehicles, household electrical appliances and the like, a litz wire coil used for a non-contact power supplying system is required to have high electrical characteristics (high inductance and low resistance) even with a limitation of the size, and it is required that variations of inductance be small. The coil inductance of a litz wire can be increased by increasing the external diameter of the coil. However, when the cross sectional flatness ratio (long side/short side) of a litz wire is excessively large as in PTL 1, the number of turns required for obtaining a desired coil external diameter is significantly large. As a result it is difficult to increase the inductance, and moreover increase in alternating-current resistance results. As described, today, a litz wire coil that is enough for general use and has high electrical characteristics while satisfying size requirement has not been achieved.
An object of the present invention is to provide a litz wire coil which has high electrical characteristics and is suitable for a non-contact power supplying system.
A litz wire coil according to an embodiment of the present invention is configured by spirally winding a litz wire on one plane by a predetermined number of turns, the litz wire being configured by twisting together a plurality of enameled wires which are each formed by baking an insulating film on a conducting body. The litz wire has a cross-sectional shape of a substantially rectangular shape, and has a flatness ratio (long side/short side) in cross section of 1.10 to 1.60.
A litz wire coil according to an embodiment of the present invention can limit variations of electrical characteristics and reduce alternating-current resistance. Therefore, the litz wire coil according to the embodiment of the present invention is suitable for a non-contact power supplying system.
In the following, an embodiment of the present invention is described in detail with reference to the drawings.
Litz wire coil 1 illustrated in
Litz wire 11 is configured by twisting together a plurality of enameled wires (element wires) which are each formed by baking an insulating film on a conducting body. The conducting body of the enameled wire is preferably copper or copper alloy, and it is also possible to use aluminum, aluminum alloy, a clad metal of copper and aluminum, and the like. In addition, the insulation film of the enameled wire is preferably made of a resin material which is melt by soldering of a high temperature when terminal metal fittings (not illustrated) are connected to end portions 11a and 11b of litz wire 11 by soldering, and examples of such a resin material include poly urethane, poly vinyl formal, poly urethane nylon, poly ester, poly ester nylon, poly ester imide, polyamide imide, poly ester imide/polyamide imide, polyimide and the like.
In addition, as illustrated in
By appropriately setting the winding condition, pressing condition, and coil design including selection of litz wire 11, it is possible to control the cross-sectional flatness ratio of litz wire 11 to fall within the above-mentioned range.
As viewed in cross section, the long side of litz wire 11 preferably extends along the radial direction of the coil. With this configuration, it is possible to achieve stable electrical characteristics and a low alternating-current resistance, and moreover, a large diameter of litz wire coil 1, that is, high inductance.
It is to be noted that a low alternating-current resistance and stable electrical characteristics can be achieved also with a configuration in which the long side of litz wire 11 in cross section extends along the thickness direction of the coil.
Preferably, litz wire coil 1 has coil internal diameter Din of 150 to 250 mm and coil external diameter Dout of 350 to 600 mm, and the number of turns is 5 to 50 turns. Preferably, in litz wire 11, the diameter of the element wire is 0.04 to 0.25 mm, and the number of twisted wires is 300 to 4,000. With this configuration, stable electrical characteristics can be achieved, which is favorable for use in a non-contact power supplying system for electric vehicles.
The size of litz wire coil 1 (coil internal diameter Din, coil external diameter Dout, and the number of turns) is properly designed such that a desired transmission efficiency is achieved in a non-contact power supplying system, and the configurations including the diameter of the element wire, the number of twisted wires, the insulating material of litz wire 11 and the like are properly selected according to litz wire coil 1 to be manufactured.
Litz wire coil 1 can be manufactured by the following method for example.
As illustrated in
It suffices that the strength of winding frame 2 is a strength that prevents damage at a second step (pressure shaping step) described later. For example, winding frame 2 is made of an aluminum alloy or iron. The same applies to pressing member 3 for example. The size of winding frame 2 is set in accordance with litz wire coil 1 to be manufactured. That is, the external diameter of internal diameter restriction part 23 corresponds to the internal diameter of litz wire coil 1, and the internal diameter of external diameter restriction part 22 corresponds to the external diameter of litz wire coil 1.
On plane part 21, mark lines serving as marks for the winding are formed at intervals that correspond to the number of turns of litz wire coil 1. By disposing litz wire 11 along mark lines 24, it is possible to confirm whether litz wire 11 is being wound as desired, and consequently it is possible to easily achieve a designed number of turns.
At the first step, litz wire 11 in a tensionless state is fed to winding frame 2, and litz wire 11 is spirally wound on plane part 21 by a predetermined number of turns in such a manner that litz wire 11 does not overlap. To be more specific, one end of litz wire 11 is fixed to the inner periphery side (or the outer periphery side) of winding frame 2, and winding frame 2 is rotated by a predetermined rotational speed. At this time, litz wire 11 is fed in accordance with the circumferential velocity of the winding position of litz wire 11. With this configuration, litz wire 11 is fed in a tensionless state. At the first step, it is also possible to wound litz wire 11 from the 1 outer periphery side of litz wire coil to feed litz wire 11 at a tensionless state.
When the external diameter of litz wire 11 is substantially equal to the interval of mark lines 24, litz wire 11 is wound and aligned in a substantially close contact state as illustrated in
When the external diameter of litz wire 11 is smaller than the interval of mark lines 24, a gap is formed between adjacent parts of litz wire 11 when litz wire 11 is wound as illustrated in
As illustrated in
It is to be noted that the external diameter of litz wire 11 may be greater than the interval of mark lines 24. In this case, as illustrated in
In addition, it is preferable to change the feeding position of litz wire 11 in accordance with the state of progress of winding of litz wire 11. To be more specific, the feeding position of litz wire 11 can be correctly controlled by using a traversing apparatus.
The winding position of litz wire 11 changes as the number of turns increases, and therefore, when the feeding position of litz wire 11 is fixed, a tensile force may be exerted on litz wire 11. In the present embodiment, the feeding position of litz wire 11 is changed in accordance with the state of progress of the winding, and thus litz wire 11 can be surely fed in a tensionless state.
In addition, it is preferable to dispose a bonding part that temporarily fixes litz wire 11 on plane part 21 of winding frame 2. For example, a belt-shaped bonding tape serving as the bonding part is radially disposed on plane part 21. With this configuration, litz wire 11 wound on plane part 21 is temporarily fixed at that position without being displaced, and thus litz wire 11 can be easily wound as designed.
In addition, as illustrated in
In the state where litz wire 11 has been wound at a first step (winding step), deviation of litz wire 11, a gap between litz wire 11, separation of litz wire 11 and the like still remain. That is, such a state is a state where many defects remain as a coil, and is not a state of a flat and stable coil shape. Therefore, a second step (pressure shaping) is performed to obtain a desired shape of litz wire coil 1.
As illustrated in
The pressing force at the second step is adjusted in accordance with a required coil accuracy. For example, when the pressing force at the second step is set to 0.1 MPa or greater, the irregularity and gap between parts of the element wire can be eliminated. In addition, when the pressing force is set to 0.5 MPa or greater, the entire coil can be sufficiently planarized. Furthermore, when the pressing force is set to 5.0 MPa or greater, it is possible to cause plastic deformation of a part of the element wire so as to increase the space factor.
In order to maintain the coil shape of pressure-shaped litz wire coil 1, a predetermined process is performed on litz wire coil 1.
For example, as described above, a belt-shaped bonding tape is wound in the radial direction of the coil to fix the coil shape.
In addition, for example, it is possible to adopt a configuration in which litz wire 11 is composed of a self-welding line (an enameled wire having a surface layer that exhibits a bonding force at the time of heating), and a heat at a fusing temperature of the self-welding line is applied at the time of the pressure shaping, or after the pressure shaping, to firmly fix the litz wire.
In addition, it is also possible to apply an adhesive agent to the entirety of litz wire coil 1 to fix the coil shape for example. In this case, it is preferable to preliminary apply a releasing agent to winding frame 2.
In addition, for example, it is also possible to immerse litz wire coil 1 in impregnation varnish to fix the coil shape.
As described, the method of manufacturing litz wire coil 1 according to the present embodiment includes a first step (winding step) and a second step (pressure shaping step). In the first step, litz wire 11 in a tensionless state is fed to winding frame 2 that includes annular plane part 21, internal diameter restriction part 23 formed in a cylindrical shape or a columnar shape at the center of plane part 21, and external diameter restriction part 22 uprightly formed at the outer peripheral edge to spirally wound litz wire 11 on plane part 21 by a predetermined the number of turns. In the second step, by pressing member 3 having a shape corresponding to plane part 21, litz wire 11 wound on plane part 21 is pressure-shaped in the thickness direction with a predetermined pressure.
With this manufacturing method, the coil shape is highly accurately controlled, and thus it is possible to stably mass-manufacture litz wire coil 1 suitable for a non-contact power supplying system for electric vehicles in which variations of electrical characteristics (inductance, in particular) are significantly small. In addition, since the coil is entirely integrated, the coil can be easily handled when it is incorporated in a predetermined apparatus (for example, a non-contact power supplying system for electric vehicles).
In Examples, under the condition where coil internal diameter is 200 mm and the number of turns is 35 turns, a litz wire was wound by the manufacturing method of the embodiment to produce a litz wire coil. The external diameter of the coil was adjusted such that the flatness ratio of the litz wire in cross section is 1.10 to 1.60. In Example 1, a litz wire in which the diameter of the element wire is 0.20 mm and the number of twisted is 400 (cross-sectional area: 12.6 mm2) was used. In Example 2, a litz wire in which the diameter of the element wire is 0.11 mm and the number of twisted wires is 1,300 (cross-sectional area: 12.4 mm2) was used.
In comparative examples, under the condition where the coil internal diameter is 200 mm and the number of turns is 35 turns, a litz wire was wound by the manufacturing method of the embodiment to produce a litz wire coil. The external diameter of the coil was adjusted such that the flatness ratio of the litz wire in cross section does not fall within a range of 1.10 to 1.60. In addition, in addition to the litz wire used in the above-mentioned Examples, a litz wire in which the diameter of the element wire is 0.14 mm and the number of the twisted wires is 600 (cross-sectional area: 9.2 mm2) was used.
In each of litz wire coils produced in Examples and Comparative Examples, the alternating-current resistance value and the inductance at 50 kHz were measured to evaluate the electrical characteristics. Evaluations are shown in Tables 1 to 3.
It is to be noted that the alternating-current resistance values in Tables 1 to 3 are each the average value (mΩ) of 10 litz wire coils produced in the same manner. In addition, variations of inductance are values (%) obtained by computing {(Maximum value)−(Minimum value)}/(Average value) based on results of measurement of 10 litz wire coils produced in the same manner. Further, since variations of inductance is required to be 1% or below for mass-manufacturing, 1% is used as an evaluation criteria.
As shown in Tables 1 to 3, when the flatness ratio of the litz wire in cross section is 1.10 to 1.60, the alternating-current resistance was low, and variations of inductance was 1% or below (Examples 1 and 2). In particular, when the flatness ratio of the litz wire in cross section is 1.20 to 1.40, the alternating-current resistance was especially low (Examples 1-2 to 1-5, and 2-2 to 2-5), and further, when the flatness ratio of the litz wire in cross section is 1.25 to 1.35, the variations of inductance were further reduced (Examples 1-3, 1-4, 2-3 and 2-4).
While the invention made by the present inventor has been specifically described based on the preferred embodiments, it is not intended to limit the present invention to the above-mentioned preferred embodiments but the present invention may be further modified within the scope and spirit of the invention defined by the appended claims.
For example, the shape of the litz wire coil is not limited to the annular shape, and may be an elliptical annular shape or a square-annular shape.
The embodiment disclosed herein is merely an exemplification and should not be considered as limitative. The scope of the present invention is specified by the following claims, not by the above-mentioned description. It should be understood that various modifications, combinations, sub-combinations and alterations may occur depending on design requirements and other factors in so far as they are within the scope of the appended claims or the equivalents thereof.
This disclosure of Japanese Patent Application No. 2012-274578, filed on Dec. 17, 2012, including the specification, drawings and abstract, is incorporated herein by reference in its entirety.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2012-274578 | Dec 2012 | JP | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2013/007234 | 12/9/2013 | WO | 00 |
