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JP5923916B2 - Contactless power supply - Google Patents
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JP5923916B2 - Contactless power supply - Google Patents

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JP5923916B2
JP5923916B2 JP2011219417A JP2011219417A JP5923916B2 JP 5923916 B2 JP5923916 B2 JP 5923916B2 JP 2011219417 A JP2011219417 A JP 2011219417A JP 2011219417 A JP2011219417 A JP 2011219417A JP 5923916 B2 JP5923916 B2 JP 5923916B2
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coil
metal heat
heat conductor
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metal
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有二 成瀬
有二 成瀬
花村 昭宏
昭宏 花村
皆川 裕介
裕介 皆川
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Nissan Motor Co Ltd
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Description

本発明は、非接触給電装置に関するものである。   The present invention relates to a non-contact power feeding device.

送電コイルを有する充電器と、受電コイルを有する本体機器とを具備し、両コイル間の電磁誘導により非接触で電力を伝送する非接触電力伝送機器の本体機器側において、受電コイルとして、巻線部を薄型の平面状に形成した平面コイルを備えるとともに、該平面コイルの少なくとも一面側において巻線部の全てに接触する熱伝導層を備える非接触電力伝送機器が知られている(特許文献1)。   Winding as a receiving coil on the main device side of a non-contact power transmission device that includes a charger having a power transmission coil and a main device having a power receiving coil, and transmits power in a non-contact manner by electromagnetic induction between the two coils. There is known a non-contact power transmission device including a planar coil in which a portion is formed in a thin planar shape, and a heat conductive layer that is in contact with all of the winding portions on at least one side of the planar coil (Patent Document 1). ).

特開2009−4513号公報JP 2009-4513 A

上記従来の構造ではコイルの上面全体に塊状の熱伝導層を設けているが、コイルに磁束が流れることによってコイルとコイル上面全体に設けた熱伝導層との間で渦電流が発生し、これにより発熱量が増加するという問題がある。   In the conventional structure described above, a massive heat conduction layer is provided on the entire top surface of the coil. However, eddy currents are generated between the coil and the heat conduction layer provided on the entire top surface of the coil when magnetic flux flows through the coil. There is a problem that the calorific value increases.

本発明が解決しようとする課題は、コイルの発熱を抑制できる非接触給電装置を提供することである。   The problem to be solved by the present invention is to provide a non-contact power feeding device capable of suppressing heat generation of a coil.

本発明は、コイルをその巻回方向で見たときに巻回されたコイル間に跨って配置され、跨って配置された延在方向の長さが跨っていない方向の長さよりも長い非磁性金属熱伝導体を設けることによって、上記課題を解決する。 The present invention is arranged so that the coil is disposed between the wound coils when viewed in the winding direction, and the non-magnetic length is longer than the length in the direction in which the extending direction is not straddled. By providing a metal heat conductor, the above-described problems are solved.

本発明によれば、跨って配置された延在方向の長さが跨っていない方向の長さよりも長い金属熱伝導体をコイル間に跨るように設けると、当該金属熱伝導体は磁束の直交方向に対して縦横比が大きいため、発生する渦電流が小さくなる。これにより、コイルの発熱を抑制することができる。   According to the present invention, when a metal heat conductor that is longer than the length in the direction in which the extending direction is not straddled is provided so as to straddle between the coils, the metal heat conductor is orthogonal to the magnetic flux. Since the aspect ratio is large with respect to the direction, the generated eddy current is small. Thereby, the heat_generation | fever of a coil can be suppressed.

本発明の一実施の形態に係る非接触給電装置を示す要部断面図である。It is principal part sectional drawing which shows the non-contact electric power feeder which concerns on one embodiment of this invention. 図1の受電コイルのうちコイル及び金属熱伝導体を示す平面図である。It is a top view which shows a coil and a metal thermal conductor among the receiving coils of FIG. 本発明の他の実施の形態に係る非接触給電装置の受電コイルを示す断面図である。It is sectional drawing which shows the receiving coil of the non-contact electric power supply which concerns on other embodiment of this invention. 本発明のさらに他の実施の形態に係る非接触給電装置の受電コイルを示す平面図である。It is a top view which shows the receiving coil of the non-contact electric power feeder which concerns on other embodiment of this invention. 図4のO−A線に沿う断面図である。It is sectional drawing which follows the OA line of FIG. 図4のO−B線に沿う断面図である。It is sectional drawing which follows the OB line of FIG. 本発明のさらに他の実施の形態に係る非接触給電装置の受電コイルのうちコイル及び金属熱伝導体を示す平面図である。It is a top view which shows a coil and a metal thermal conductor among the receiving coils of the non-contact electric power feeder which concerns on further another embodiment of this invention. 図6のVII−VII線に沿う断面図である。It is sectional drawing which follows the VII-VII line of FIG. 本発明に係る非接触給電装置のコイルの抵抗−周波数特性及びインダクタンス−周波数特性を示すグラフである。It is a graph which shows the resistance-frequency characteristic and inductance-frequency characteristic of the coil of the non-contact electric power supply which concern on this invention. 本発明の比較例に係る非接触給電装置のコイルの抵抗−周波数特性及びインダクタンス−周波数特性を示すグラフである。It is a graph which shows the resistance-frequency characteristic and inductance-frequency characteristic of the coil of the non-contact electric power feeder which concerns on the comparative example of this invention. コイル付近の温度を見積もるためのモデルを示す図である。It is a figure which shows the model for estimating the temperature of the coil vicinity. 金属熱伝導体に発生するジュール熱を見積もるためのモデルを示す図である。It is a figure which shows the model for estimating the Joule heat which generate | occur | produces in a metal heat conductor. 金属熱伝導体の厚さとコイル近傍温度及び発熱量の関係を示すグラフである。It is a graph which shows the relationship between the thickness of a metal heat conductor, coil vicinity temperature, and emitted-heat amount.

図1は本発明の一実施の形態を適用した非接触給電装置であり、所定のギャップ空間30を介して位置する受電コイル10と送電コイル20とを備え、給電スタンドなどに設置される送電装置40から、車両などに搭載されるバッテリ50などの負荷に非接触で電力を供給し、充電するシステムなどに適用することができる。   FIG. 1 is a non-contact power feeding apparatus to which an embodiment of the present invention is applied, and includes a power receiving coil 10 and a power transmitting coil 20 positioned via a predetermined gap space 30, and is installed in a power feeding stand or the like. The present invention can be applied to a system in which electric power is supplied in a non-contact manner to a load such as a battery 50 mounted on a vehicle or the like and charged.

受電コイル10は、銅などの導体からなるコイル11を備える。本例のコイル11は、少なくともxy平面上に巻回された偏平状コイルであり、図2に示すようにxy平面上に1重(1段)で巻回されたもののほか、z軸方向に複数重(複数段)巻回されたものも含まれる。また本例のコイル11は、図2に示すように平面視において渦巻状に巻回されたもののほか、平面視において楕円形状に巻回されたもの、正方形や長方形などの矩形状に巻回されたもの、或いは8の字形状に交差して巻回されたものも含まれる。本例のコイル11は、互いに短絡しないように導体の表面が絶縁被覆され、その両端はそれぞれバッテリ50の入力端子に接続されている。   The power receiving coil 10 includes a coil 11 made of a conductor such as copper. The coil 11 of this example is a flat coil wound at least on the xy plane, and is wound in a single (one step) on the xy plane as shown in FIG. Also included are those that are wound in multiple layers. In addition to the coil 11 wound in a plan view as shown in FIG. 2, the coil 11 of this example is wound in an elliptical shape in a plan view, or a rectangular shape such as a square or a rectangle. Also included are those which are wound around the shape of figure 8 or intersecting with the figure 8 shape. The surfaces of the conductors of the coil 11 of this example are insulated so as not to short-circuit each other, and both ends thereof are connected to the input terminals of the battery 50, respectively.

さらに図2に、平面視において渦巻状に3回転だけ巻回した本例のコイル11を示す。内側の端部のポイントP1から反時計回りにポイントP2までが1回転目、このポイントP2から反時計回りにポイントP3までが2回転目、ポイントP3から反時計回りに外側の端部のポイントP4までが3回転目となる。ただし、巻回数は図示するものに限定されず、給電使用に応じて適宜設定することができる。   Further, FIG. 2 shows the coil 11 of this example wound three times in a spiral shape in plan view. From the inner end point P1 to the point P2 counterclockwise is the first rotation, from the point P2 to the point P3 counterclockwise is the second rotation, and from the point P3 to the outer end point P4. Up to the third rotation. However, the number of windings is not limited to that shown in the figure, and can be appropriately set according to the use of power feeding.

図1に戻り、コイル11の背面には、絶縁部13を介して、送電コイル20からの磁界を調整する磁性コア14がコイル11の全面にわたって設けられている。さらに磁性コア14の背面には、受電コイル10および送電コイル20からの磁界が受電コイル10の背面側に及ぶのを抑制する磁気遮蔽板15が設けられている。なお、受電コイル10の全体を保護するために、当該受電コイル10の全体を覆うカバー16が設けられているが、後述する金属熱伝導体12の一部はカバー16からギャップ空間30へ露出している。この点については後述する。   Returning to FIG. 1, a magnetic core 14 that adjusts the magnetic field from the power transmission coil 20 is provided over the entire surface of the coil 11 on the back surface of the coil 11 via the insulating portion 13. Further, on the back surface of the magnetic core 14, a magnetic shielding plate 15 that suppresses the magnetic fields from the power receiving coil 10 and the power transmitting coil 20 from reaching the back side of the power receiving coil 10 is provided. In order to protect the entire power receiving coil 10, a cover 16 that covers the entire power receiving coil 10 is provided. However, a part of the metal thermal conductor 12 described later is exposed from the cover 16 to the gap space 30. ing. This point will be described later.

本例の受電コイル10のコイル11の間(コイル線の間)には、金属熱伝導体12が設けられている。本例の金属熱伝導体12には、アルミニウムなどの熱伝導率が高い金属を用いることができる。金属熱伝導体12とコイル11との間、および隣接する金属熱伝導体12同士を絶縁するため、金属熱伝導体12の表面は絶縁被覆されている。   A metal thermal conductor 12 is provided between the coils 11 of the power receiving coil 10 of this example (between the coil wires). For the metal thermal conductor 12 of this example, a metal having high thermal conductivity such as aluminum can be used. In order to insulate between the metal heat conductor 12 and the coil 11 and between the metal heat conductors 12 adjacent to each other, the surface of the metal heat conductor 12 is coated with insulation.

本例の金属熱伝導体12は、コイル11をその巻回方向で見た場合に、巻回されたコイル11の間に跨って配置されて、好ましくはコイル11と直交する方向に配置されている。ここでコイル11の間に跨って配置されるとは、図2のコイル11の平面視において金属熱伝導体12の両端が少なくとも巻回されて隣接する2つのコイル11のそれぞれに熱的に接していることを意味する。換言すれば、電磁誘導作用によりコイル11に生じた熱が金属熱伝導体12に伝わり、ここから受電コイル10の外部へ放熱させる機能を司ることができる意味である。   When the coil 11 is viewed in the winding direction, the metal thermal conductor 12 of this example is disposed between the wound coils 11 and preferably disposed in a direction orthogonal to the coil 11. Yes. Here, the term “arranged between the coils 11” means that the two ends of the metal thermal conductor 12 are at least wound in the plan view of the coil 11 in FIG. 2 and are in thermal contact with the two adjacent coils 11. Means that In other words, it means that the heat generated in the coil 11 due to the electromagnetic induction action is transmitted to the metal heat conductor 12 and can be used to radiate heat from here to the outside of the power receiving coil 10.

金属熱伝導体12は、図2に示すようにコイル11の巻回方向に沿って任意の間隔で配置することができるほか、コイル11の巻回方向に沿って連続して積層するように配置してもよい。金属熱伝導体11を連続して積層するように配置する場合には、隣接する金属熱伝導体11は互いに絶縁する。   As shown in FIG. 2, the metal heat conductor 12 can be arranged at an arbitrary interval along the winding direction of the coil 11, and is arranged so as to be continuously laminated along the winding direction of the coil 11. May be. When arrange | positioning so that the metal heat conductor 11 may be laminated | stacked continuously, the adjacent metal heat conductor 11 is insulated from each other.

金属熱伝導体12は、2つのコイルの間に跨って配置された延在方向の長さが、跨っていない方向の長さよりも長く形成されている。つまり、図1のxyz座標でいうと、跨って配置された延在方向がy軸方向に相当し、跨っていない方向がx軸方向(コイル11の巻回方向に沿う方向)に相当し、したがってy軸方向の長さがx軸方向の長さよりも長く形成されている。なお、z軸方向の長さはコイル11の厚さに、後述するカバー26からの露出分を加えた長さとされている。このような条件を満たす金属熱伝導体11の形状例として、コイル11の巻回方向に薄い薄板を挙げることができる。 The metal heat conductor 12 is formed so that the length in the extending direction disposed between the two coils is longer than the length in the non-stretching direction. That is, in terms of the xyz coordinates in FIG. 1, the extending direction arranged across the road corresponds to the y-axis direction, and the non-crossing direction corresponds to the x-axis direction (the direction along the winding direction of the coil 11). Therefore, the length in the y-axis direction is longer than the length in the x-axis direction. Note that the length in the z-axis direction is a length obtained by adding the exposure from the cover 26 described later to the thickness of the coil 11. As an example of the shape of the metal thermal conductor 11 that satisfies such conditions, a thin thin plate can be cited in the winding direction of the coil 11.

金属熱伝導体12は、図1に示すようにその下面がギャップ空間30に向かってカバー16から露出するように設けられている。この露出した部分から金属熱伝導体12に伝わったコイル11からの熱をギャップ空間30へ放熱することができる。   As shown in FIG. 1, the metal heat conductor 12 is provided such that its lower surface is exposed from the cover 16 toward the gap space 30. Heat from the coil 11 transmitted from the exposed portion to the metal heat conductor 12 can be radiated to the gap space 30.

本例の金属熱伝導体12は、コイル11間を跨ぐ方向(y軸方向)に長く、コイル11の巻回方向(図1のx軸方向)に薄い薄板状の金属で構成され、換言すれば磁束直交方向に対して縦横比が大きく互いに絶縁されているため、発生する渦電流が小さく、近接効果によるコイル11の抵抗、薄板である金属熱伝導体12自体の発熱等、電磁気的な影響は少ない。また、高熱伝導率の金属熱伝導体12をコイル11に接触して配置できるため、樹脂を充填した場合に比べてコイルからの放熱性が高い。例えば、アルミの熱伝導率は約200W/(mK)に対し、高熱伝導樹脂は、1〜2W/(mK)であり、アルミニウムの薄板である金属熱伝導体12を用いることで大幅な熱伝導率の向上が期待できる。   The metal heat conductor 12 of this example is made of a thin plate-like metal that is long in the direction straddling the coils 11 (y-axis direction) and thin in the winding direction of the coil 11 (x-axis direction in FIG. 1). For example, since the aspect ratio is large and insulated from each other in the direction perpendicular to the magnetic flux, the generated eddy current is small, the resistance of the coil 11 due to the proximity effect, the heat generation of the thin metal heat conductor 12 itself, and other electromagnetic influences. There are few. Moreover, since the metal thermal conductor 12 with high thermal conductivity can be disposed in contact with the coil 11, heat dissipation from the coil is higher than when the resin is filled. For example, the thermal conductivity of aluminum is approximately 200 W / (mK), whereas the high thermal conductive resin is 1 to 2 W / (mK), and a large thermal conductivity is achieved by using the metal thermal conductor 12 that is a thin aluminum plate. The rate can be expected to improve.

図8に、本例に係るコイル11間に積層状のアルミニウム製金属熱伝導体12を配置した場合の抵抗およびインダクタンスの測定結果を示す。図中、◆はコイル11間にアルミニウム製金属熱伝導体12を配置しない場合の抵抗−周波数特性及びインダクタンス−周波数特性を示し、□はコイル11間にアルミニウム製金属熱伝導体12を配置した場合の抵抗−周波数特性及びインダクタンス−周波数特性を示す。積層状のアルミニウム製金属熱伝導体12の有無による抵抗及びインダクタンスの変化は見られない。   FIG. 8 shows measurement results of resistance and inductance when a laminated aluminum metal heat conductor 12 is arranged between the coils 11 according to this example. In the figure, ♦ indicates resistance-frequency characteristics and inductance-frequency characteristics when the aluminum metal heat conductor 12 is not disposed between the coils 11, and □ indicates the case where the aluminum metal heat conductor 12 is disposed between the coils 11. The resistance-frequency characteristics and the inductance-frequency characteristics are shown. Changes in resistance and inductance due to the presence or absence of the laminated aluminum metal heat conductor 12 are not observed.

一方、図9の上図に示すようにコイル11間にアルミニウム製金属熱伝導体を配置した場合には、同図の下左右図に示すように、コイル11の抵抗が増加し、またインダクタンスの低下が観察された。これはアルミニウム製金属熱伝導体12´の上下面及び側面を通過する磁束によりアルミニウム製金属熱伝導体12´に渦電流が発生し、近接効果と磁束遮蔽効果が引き起こされたためと考えられる。このため、アルミニウムなどの金属熱伝体をコイル11の近傍に配置する場合には、このような渦電流が発生しない配置が必要になる。 On the other hand, when an aluminum metal heat conductor is disposed between the coils 11 as shown in the upper diagram of FIG. 9, the resistance of the coil 11 increases as shown in the lower left and right diagrams of FIG. A decrease was observed. This is presumably because an eddy current is generated in the aluminum metal heat conductor 12 'by the magnetic flux passing through the upper and lower surfaces and the side surfaces of the aluminum metal heat conductor 12', causing a proximity effect and a magnetic flux shielding effect. Therefore, when arranging a metal thermal conduction material such as aluminum in the vicinity of the coil 11, is arranged such eddy current is not generated becomes necessary.

次に金属熱伝導体12の最適化される形状について検討する。熱伝導率を高めるためには、金属熱伝導体12のコイル11に接する部分の厚みを大きくすることが有効であるが、一方において、金属熱伝導体12の渦電流を抑えるには、厚みを周波数に応じて薄くして互いに絶縁する必要がある。まず、図10に示すように、コイル11の付近の温度Tは、熱抵抗1/KA、単位長さあたり定常発熱量Q、周囲温度Tとして、

Figure 0005923916
で表される。ここで、熱抵抗は、金属熱伝導体12の厚さと単位長さ当たりの層数による等価熱伝導率を用いる。金属熱伝導体12の厚み(アルミニウムと樹脂との混合率)を上げることにより、コイル付近の温度を低減できる。 Next, the optimized shape of the metal heat conductor 12 will be considered. In order to increase the thermal conductivity, it is effective to increase the thickness of the portion of the metal thermal conductor 12 that is in contact with the coil 11. On the other hand, to suppress the eddy current of the metal thermal conductor 12, the thickness is reduced. It is necessary to insulate from each other by thinning according to the frequency. First, as shown in FIG. 10, the temperature T 2 in the vicinity of the coil 11 has a thermal resistance 1 / KA, a steady heat generation amount Q per unit length, and an ambient temperature T 1 .
Figure 0005923916
It is represented by Here, the thermal resistance uses an equivalent thermal conductivity according to the thickness of the metal thermal conductor 12 and the number of layers per unit length. By increasing the thickness of the metal heat conductor 12 (mixing ratio of aluminum and resin), the temperature near the coil can be reduced.

一方、図11に示すように、金属熱伝導体12は縦aX,横X,高さLの平板とされ、これに垂直にBsinωtの磁束が鎖交している場合に金属熱伝導体12の平板に発生するジュール熱を見積もる。縦ax,横xの領域を鎖交する磁束φ(t,x)は、鎖交磁束密度B,角周波数ω,金属熱伝導体12の導電率σ,金属熱伝導体12の透磁率μとして、

Figure 0005923916
発生する起電圧V(t,x)と実効値Veffは、それぞれ下記のようになる。
Figure 0005923916
On the other hand, as shown in FIG. 11, the metal thermal conductor 12 is a flat plate having vertical aX, horizontal X, and height L, and when the magnetic flux of B 0 sin ωt is linked perpendicularly to the metal thermal conductor 12 The Joule heat generated in 12 flat plates is estimated. The magnetic flux φ (t, x) interlinking the longitudinal ax and lateral x regions is the interlinkage magnetic flux density B 0 , the angular frequency ω, the electrical conductivity σ of the metal thermal conductor 12, and the magnetic permeability μ of the metallic thermal conductor 12. As
Figure 0005923916
The generated electromotive voltage V (t, x) and effective value V eff are as follows.
Figure 0005923916

幅dx,adxの周回経路に上記起電圧による電流が発生しているとすると、その部分の抵抗dr(x)は、

Figure 0005923916
となり、金属熱伝導体12に発生するジュール熱は、上記電流によるジュール熱を平板領域で積分(0〜x〜X)することにより、下記のようになる。
Figure 0005923916
Assuming that a current due to the electromotive voltage is generated in the circulation path of the widths dx and adx, the resistance dr (x) at that portion is
Figure 0005923916
Thus, the Joule heat generated in the metal thermal conductor 12 is as follows by integrating (0 to x to X) the Joule heat generated by the current in the flat plate region.
Figure 0005923916

ここで、周波数が十分高い場合には、電流の発生する厚さLは、表皮厚で代表される。

Figure 0005923916
Here, when the frequency is sufficiently high, the thickness L at which the current is generated is represented by the skin thickness.
Figure 0005923916

以上のことから、結局、1枚の平板で発生するジュール熱は以下のように見積もれる。

Figure 0005923916
From the above, after all, the Joule heat generated in one flat plate can be estimated as follows.
Figure 0005923916

金属熱伝導体12である薄板間の絶縁層の厚さを0.1mmとし、アルミニウムと樹脂との混合率を薄板厚さに応じて変化させて、(例えば混合率50%であれば、薄板厚さも絶縁層と同じ0.1mmとする)、ジュール熱と合わせてプロットすると、図12のようになる。例えば、金属熱伝導体12のジュール熱の総和を定常出力Pの1/kとなるように a の値を決めると、(nは薄板の層数)

Figure 0005923916
より、
Figure 0005923916
ただし、
Figure 0005923916
The thickness of the insulating layer between the thin plates as the metal heat conductor 12 is set to 0.1 mm, and the mixing ratio of aluminum and resin is changed according to the thickness of the thin plate (for example, if the mixing ratio is 50%, the thin plate The thickness is also set to 0.1 mm, which is the same as the insulating layer), and plotted together with Joule heat, the result is as shown in FIG. For example, when the value of a is determined so that the total Joule heat of the metal heat conductor 12 becomes 1 / k of the steady output P, (n is the number of thin plates)
Figure 0005923916
Than,
Figure 0005923916
However,
Figure 0005923916

上記数9式を満たすaで最大のものを選ぶことで、熱性能と電磁気性能を両立させることができる。   By selecting the largest value a that satisfies the above formula 9, it is possible to achieve both thermal performance and electromagnetic performance.

図1に戻り、送電コイル20についても上述した受電コイル10と同じ構造とされている。受電コイル10のコイル11、金属熱伝導体12、絶縁部13、磁性コア14、磁気遮蔽板15及びカバー16にそれぞれ対応する部材として、送電コイル20は、コイル21、金属熱伝導体22、絶縁部23、磁性コア24、磁気遮蔽板25及びカバー26を備える。なお、本発明の金属熱伝導体12,22は少なくとも受電コイル10又は送電コイル20の一方に設ければよい。   Returning to FIG. 1, the power transmission coil 20 has the same structure as that of the power reception coil 10 described above. As members corresponding to the coil 11, the metal heat conductor 12, the insulating portion 13, the magnetic core 14, the magnetic shielding plate 15, and the cover 16 of the power receiving coil 10, the power transmission coil 20 includes the coil 21, the metal heat conductor 22, and the insulation. A portion 23, a magnetic core 24, a magnetic shielding plate 25, and a cover 26 are provided. Note that the metal thermal conductors 12 and 22 of the present invention may be provided in at least one of the power receiving coil 10 or the power transmitting coil 20.

以上のように、本例の非接触給電装置1によれば、金属熱伝導体12は、コイル11間を跨ぐ方向(y軸方向)に長く、コイル11の巻回方向(図1のx軸方向)に薄い薄板状の金属で構成され、換言すれば磁束直交方向に対して縦横比が大きく互いに絶縁されているため、発生する渦電流が小さく、近接効果によるコイル11の抵抗、薄板である金属熱伝導体12自体の発熱等、電磁気的な影響は少ない。   As described above, according to the non-contact power feeding device 1 of the present example, the metal thermal conductor 12 is long in the direction across the coils 11 (y-axis direction), and the winding direction of the coil 11 (x-axis in FIG. 1). In other words, it has a large aspect ratio with respect to the direction perpendicular to the magnetic flux and is insulated from each other. Therefore, the generated eddy current is small, the resistance of the coil 11 due to the proximity effect, and the thin plate. There are few electromagnetic influences, such as heat_generation | fever of the metal heat conductor 12 itself.

また、上記数9式を満たすaで最大のものを選ぶことで、熱性能と電磁気性能を両立させることができる。   Further, by selecting the largest value a that satisfies the above formula 9, it is possible to achieve both thermal performance and electromagnetic performance.

さらに、金属熱伝導体12の一部が、コイル11のギャップ空間30側に露出していることにより、ギャップ空間30の外気との自然対流による熱交換あるいはファン等による強制空冷により効果的にコイル11の抜熱が可能となる。   Further, since a part of the metal heat conductor 12 is exposed to the gap space 30 side of the coil 11, the coil can be effectively subjected to heat exchange by natural convection with the outside air of the gap space 30 or forced air cooling by a fan or the like. 11 can be removed.

図3は、本発明の他の実施の形態に係る受電コイル10を示す断面図であり、本例ではギャップ空間30に露出した金属熱伝導体12の一部が連結部12aにて連結されている。こうすることで、金属熱伝導体12をコイル11の上面及び両側面で接触できるため、コイル11の熱抵抗を低減し、放熱効果を増すことができる。また、金属熱伝導体12によってコイル11の位置決めをすることができる。さらに、非接触給電装置1に力が加わった場合にコイル11を保護することができる。すなわち、一般にコイル11の抵抗値は周波数とともに増大するが、その値はコイル11の巻き方(並列のコイルの撚り方等)や配置(コイル間のクリアランス)によっても影響される。所定の巻き方でコイル11を巻いた後、外部から力がかかった場合にも位置が変わらないよう、従来例では樹脂で固めるなどしているが、本例によれば従来に比べて大きな放熱効果が期待できる。   FIG. 3 is a cross-sectional view showing a power receiving coil 10 according to another embodiment of the present invention. In this example, a part of the metal thermal conductor 12 exposed in the gap space 30 is connected by a connecting portion 12a. Yes. By carrying out like this, since the metal thermal conductor 12 can be contacted by the upper surface and both sides | surfaces of the coil 11, the thermal resistance of the coil 11 can be reduced and the heat dissipation effect can be increased. Further, the coil 11 can be positioned by the metal heat conductor 12. Furthermore, the coil 11 can be protected when a force is applied to the non-contact power feeding device 1. That is, the resistance value of the coil 11 generally increases with frequency, but the value is also affected by how the coil 11 is wound (such as how to twist parallel coils) and arrangement (clearance between the coils). After winding the coil 11 in a predetermined winding method, the conventional example is hardened with resin so that the position does not change even when a force is applied from the outside. The effect can be expected.

図4は、本発明のさらに他の実施の形態に係る受電コイル10を示す平面図、図5Aは図4のO−A線に沿う断面図、図5Bは図4のO−B線に沿う断面図である。本例では、2本のコイル11を並列で用いた場合であり、共振の鋭さを示すQ値を増加させるためにコイル11を撚って配置した場合である。この場合において、周方向のコイル11の電線間のクリアランスは角度とともに変化するため、図5A及び図5Bに示すように、そのクリアランスにあわせて金属熱導電体12のコイル11に直交する辺の長さW,Wを変えている。このように、コイル11の電線に接するような形状の金属熱導電体12を配置ことが放熱上有効となる。 4 is a plan view showing a power receiving coil 10 according to still another embodiment of the present invention, FIG. 5A is a cross-sectional view taken along line OA in FIG. 4, and FIG. 5B is taken along line OB in FIG. It is sectional drawing. In this example, two coils 11 are used in parallel, and the coils 11 are twisted to increase the Q value indicating the sharpness of resonance. In this case, since the clearance between the wires of the coil 11 in the circumferential direction changes with the angle, as shown in FIGS. 5A and 5B, the length of the side perpendicular to the coil 11 of the metal thermal conductor 12 is matched to the clearance. W A and W B are changed. Thus, the arrangement of the metal thermal conductor 12 shaped so as to be in contact with the wire of the coil 11 is effective in terms of heat dissipation.

図6は、本発明のさらに他の実施の形態に係る受電コイル10を示す平面図、図7は図6のVII−VII線に沿う断面図である。本例では、ギャップ空間30に露出した複数の金属熱伝導体12の一面に、これらを連結し、コイル11の巻回方向に延在する他の金属熱伝導体17が配置されている。この他の金属熱伝導体17を設けることで、金属熱伝導体12の放熱面積を大きくすることができ、放熱効果を高めることができる。また、コイル11から離れたギャップ空間30に平板状の金属熱伝導体17を配置することにより、近接効果によるコイル抵抗の上昇を抑えることができる。   FIG. 6 is a plan view showing a power receiving coil 10 according to still another embodiment of the present invention, and FIG. 7 is a cross-sectional view taken along the line VII-VII in FIG. In this example, the other metal heat conductors 17 that are connected to one surface of the plurality of metal heat conductors 12 exposed in the gap space 30 and extend in the winding direction of the coil 11 are arranged. By providing the other metal heat conductor 17, the heat radiation area of the metal heat conductor 12 can be increased, and the heat radiation effect can be enhanced. Further, by arranging the flat metal heat conductor 17 in the gap space 30 away from the coil 11, an increase in coil resistance due to the proximity effect can be suppressed.

上記受電コイル10又は送電コイル20は本発明に係るコイルに相当する。   The power receiving coil 10 or the power transmitting coil 20 corresponds to a coil according to the present invention.

1…非接触給電装置
10…受電コイル
11…コイル
12…金属熱伝導体
12a…連結部
13…絶縁部
14…磁性コア
15…磁気遮蔽板
16…カバー
17…他の金属熱伝導体
20…送電コイル
21…コイル
22…金属熱伝導体
23…絶縁部
24…磁性コア
25…磁気遮蔽板
26…カバー
30…ギャップ空間
DESCRIPTION OF SYMBOLS 1 ... Non-contact electric power feeder 10 ... Power receiving coil 11 ... Coil 12 ... Metal thermal conductor 12a ... Connection part 13 ... Insulation part 14 ... Magnetic core 15 ... Magnetic shielding board 16 ... Cover 17 ... Other metal thermal conductors 20 ... Power transmission Coil 21 ... Coil 22 ... Metal thermal conductor 23 ... Insulating part 24 ... Magnetic core 25 ... Magnetic shielding plate 26 ... Cover 30 ... Gap space

Claims (7)

少なくとも一方のコイルが巻回して構成された一対のコイル間を非接触で給電する非接触給電装置において、
前記巻回して構成されたコイルをその巻回方向で見たときに、巻回されたコイルの間に跨って配置され、跨って配置された延在方向の長さが跨っていない方向の長さよりも長く形成された非磁性金属熱伝導体を備える非接触給電装置。
In a non-contact power feeding device that feeds power between a pair of coils formed by winding at least one coil in a non-contact manner,
When the coil formed by winding is viewed in the winding direction, the coil is disposed between the wound coils, and the length in the direction in which the length of the extending direction is not straddled is disposed. The non-contact electric power feeder provided with the nonmagnetic metal heat conductor formed longer than the length.
前記金属熱伝導体は、
薄板状に形成され、
前記跨って配置されたコイルと絶縁され、
前記跨って配置されたコイルに直交して配置されている請求項1に記載の非接触給電装置。
The metal heat conductor is
Formed into a thin plate,
Insulated with the coil arranged across,
The non-contact electric power feeder of Claim 1 arrange | positioned orthogonally to the coil arrange | positioned across the said straddle.
前記コイルに直交して配置された金属熱伝導体は、前記コイルの間隔に応じて前記コイルに接して設けられている請求項2に記載の非接触給電装置。   The non-contact electric power feeder of Claim 2 with which the metal heat conductor arrange | positioned orthogonally to the said coil is provided in contact with the said coil according to the space | interval of the said coil. 前記金属熱伝導体の一部が、前記一対のコイル間のギャップ空間に露出している請求項1〜3のいずれか一項に記載の非接触給電装置。   The contactless power feeding device according to any one of claims 1 to 3, wherein a part of the metal heat conductor is exposed in a gap space between the pair of coils. 前記ギャップ空間に露出した金属熱伝導体の一部が連結されている請求項4に記載の非接触給電装置。   The non-contact electric power feeder according to claim 4 with which a part of metallic heat conductor exposed to said gap space is connected. 前記ギャップ空間に露出した複数の金属熱伝導体の一面に、これらを連結し、前記コイルの巻回方向に延在する他の金属熱伝導体が配置されている請求項4又は5に記載の非接触給電装置。   The other metal heat conductor which connects these and is extended to the winding direction of the said coil is arrange | positioned on one surface of the some metal heat conductor exposed to the said gap space, The Claim 4 or 5 is arrange | positioned. Non-contact power feeding device. 前記薄板状の金属熱伝導体は、
金属熱伝導体の導電率をσ,金属熱伝導体の長辺の長さをX,金属熱伝導体の透磁率をμ,金属熱伝導体の積層数をn,給電電力の角周波数をω,鎖交磁束密度をB,金属熱伝導体の板厚/長辺の長さ比をaとしたときに、
−Ka−K<0
ただし、K={16P・√(σωμ/2)}/nkσ
を満たす請求項2〜6のいずれか一項に記載の非接触給電装置。
The sheet metal heat conductor is
The conductivity of the metal heat conductor is σ, the length of the long side of the metal heat conductor is X, the magnetic permeability of the metal heat conductor is μ, the number of metal heat conductors is n, and the angular frequency of the feed power is ω , When the flux linkage density is B 0 and the metal heat conductor plate thickness / long side length ratio is a,
a 3 −Ka 2 −K <0
However, K = {16P · √ (σωμ / 2)} / nkσ 2 B 0 2 X 4
The non-contact electric power feeder as described in any one of Claims 2-6 which satisfy | fills.
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