JPH0521244A - Thin transformer - Google Patents

Thin transformer

Info

Publication number
JPH0521244A
JPH0521244A JP3173559A JP17355991A JPH0521244A JP H0521244 A JPH0521244 A JP H0521244A JP 3173559 A JP3173559 A JP 3173559A JP 17355991 A JP17355991 A JP 17355991A JP H0521244 A JPH0521244 A JP H0521244A
Authority
JP
Japan
Prior art keywords
coil
plane
coils
thin transformer
loss
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP3173559A
Other languages
Japanese (ja)
Inventor
Kazuhiko Sakakibara
一彦 榊原
Naoki Murakami
直樹 村上
Toshiaki Yanai
利明 谷内
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP3173559A priority Critical patent/JPH0521244A/en
Publication of JPH0521244A publication Critical patent/JPH0521244A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To reduce loss of a plane coil caused by skin effect in use at high frequency in a thin transformer which is formed by laminating a plane coil. CONSTITUTION:A coil part of a thin transformer is constituted of at least three plane coils 2a, 2b, 3. The plane coil 3 is held between two plane coils 2a, 2b, the plane coils 2a, 2b are made one coil and the plane coil 3 is made the other coil. Here, magnetmotive force by a current flowing to one coil is reduced by connecting the plane coils 2a, 2b in parallel. Influence of skin effect is reduced by reduction of the magnetmotive force, and loss caused thereby is reduced.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、スイッチング電源等に
おいて、電力変換,絶縁などに用いられる薄形トランス
の改良に関し、特にコイル部の損失を低減する薄形トラ
ンスに関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an improvement of a thin transformer used for power conversion, insulation, etc. in a switching power supply and the like, and more particularly to a thin transformer for reducing loss of a coil portion.

【0002】[0002]

【従来の技術】従来技術で構成された薄形トランスの構
造を図6(a),(b)に示す。図6において、(a)
は一部分を破断した斜視図、(b)はその破断部Aの断
面図であり、θ,Z,rは空間の座標軸である。この従
来例の構成において、101は内部にリング状の空間S
を形成するための凹部を有する一対のフェライト磁心、
102は平面コイルで構成された一方のコイル、103
は同じく平面コイルで構成されたもう一方のコイルであ
る。コイル102とコイル103の巻数比は自在に設計
できるが、図例では4:1の場合を示している。コイル
102とコイル103とは、一対のフェライト磁心10
1同士で形成される内部空間S内において、充填材10
4により互いに絶縁され積層されて固定されている。
2. Description of the Related Art The structure of a conventional thin transformer is shown in FIGS. 6 (a) and 6 (b). In FIG. 6, (a)
Is a partially broken perspective view, (b) is a sectional view of the broken portion A, and θ, Z, and r are coordinate axes of the space. In the structure of this conventional example, 101 is a ring-shaped space S inside.
A pair of ferrite magnetic cores having recesses for forming
102 is one coil composed of a planar coil, 103
Is the other coil which is also composed of a planar coil. Although the winding ratio of the coil 102 and the coil 103 can be designed freely, the case of 4: 1 is shown in the illustrated example. The coil 102 and the coil 103 are a pair of ferrite magnetic cores 10.
In the internal space S formed by one member, the filler 10
They are insulated from each other by 4 and laminated and fixed.

【0003】スイッチング電源のトランスは高周波で使
用されるので、そのコイルには表皮効果が現れる。この
ため、上記薄形トランスでは、各平面コイル102,1
03の厚さh′は、その平面コイル102,103に加
工されている導電板のスキンディプス(表皮効果の深
さ)δとほとんど同じ値に設計されていた。このスキン
ディプスδは、その導電板の導電率をσ、透過率を
μ0、平面コイル102,103に流れる電流の周波数
をfとして、次式で計算される値である。
Since the transformer of the switching power supply is used at a high frequency, a skin effect appears in its coil. Therefore, in the thin transformer, the planar coils 102, 1
The thickness h'of 03 was designed to be almost the same as the skin depth (depth of skin effect) δ of the conductive plate processed in the planar coils 102 and 103. The skin depth δ is a value calculated by the following equation, where the conductivity of the conductive plate is σ, the transmittance is μ 0 , and the frequency of the current flowing through the planar coils 102 and 103 is f.

【0004】[0004]

【数1】 [Equation 1]

【0005】このような平面コイルの厚さをスキンディ
プスとほとんど同じ値にした薄形トランスの設計例は、
A.F.ゴールドバーク、J.G.カサキアン、M.
F.シュレヒトの各氏による「イシューズ リレイテッ
ド ツウ 1−10MHZ トランスフォーマ デザイ
ン」(IEEE Trans.onPower Ele
ctron.,4,January 1989)や「フ
ァイナイト エレメント アナリシス オブ カッパー
ロス イン 1−10MHZ トランスフォーマ」
(IEEE Trans.on Power Elec
tron.,4,April 1989)等の論文に紹
介されている。
A design example of a thin transformer in which the thickness of such a plane coil is almost the same as the skin depth is as follows.
A. F. Gold Burke, J.M. G. Kasakian, M.A.
F. "Lee shoes Rireiteddo-to-1-10MH Z transformer design" by Messrs Shurehito (IEEE Trans.onPower Ele
ctron. , 4, January 1989) and "finite element analysis of Copper loss-in-1-10MH Z transformer"
(IEEE Trans. On Power Elec
tron. , 4, April 1989) and the like.

【0006】[0006]

【発明が解決しようとする課題】しかしながら、上記従
来の技術における薄形トランスでは、平面コイルの厚さ
をスキンディプス以上としてもコイルの損失を減少でき
ないため、その損失を低減することが課題として残って
いた。図7は平面コイルの厚さを変えたときのコイルの
損失を示す計算図であり、平面コイルの厚さにはその損
失を最小とする値hoptが存在し、それ以上巻線の厚さ
を増加しても効果の無いことが示されている。
However, in the thin transformer of the above-mentioned conventional technique, the loss of the coil cannot be reduced even if the thickness of the plane coil is more than the skin depth. Therefore, the reduction of the loss remains a problem. Was there. FIG. 7 is a calculation diagram showing the loss of the coil when the thickness of the plane coil is changed. There is a value h opt that minimizes the loss in the thickness of the plane coil, and the thickness of the winding is more than that. It is shown that there is no effect even if is increased.

【0007】本発明は、上記課題を解決するために創案
されたもので、その目的は、表皮効果を生ずる平面コイ
ルの損失を低減できる薄形トランスを提供することにあ
る。
The present invention was devised to solve the above problems, and an object of the present invention is to provide a thin transformer capable of reducing the loss of the planar coil that causes the skin effect.

【0008】[0008]

【課題を解決するための手段】上記の目的を達成するた
めに、本発明の薄形トランスの構成においては、導電板
をスパイラル形状に加工した平面コイルを少なくとも3
個積層したコイル部と、このコイル部を挟み込む一対の
偏平なフェライト磁心とを備え、前記3個の平面コイル
の内、上下に配置された平面コイルが中間に配置された
平面コイルを挟み込む構造を有し、前記上下の平面コイ
ルを電気的に並列接続または直列接続して一方のコイル
とし、中間の平面コイルをもう一方のコイルとしたこと
を特徴としている。
In order to achieve the above object, in the structure of the thin transformer of the present invention, at least three plane coils each obtained by processing a conductive plate into a spiral shape are used.
A structure is provided in which a coil portion that is laminated individually and a pair of flat ferrite cores that sandwich the coil portion are provided, and among the three planar coils, the planar coils that are arranged above and below sandwich the planar coil that is arranged in the middle. The upper and lower flat coils are electrically connected in parallel or in series to form one coil, and the intermediate flat coil is the other coil.

【0009】[0009]

【作用】本発明は、平面コイルの構成とその平面コイル
の損失との関係を解析し、その解析結果に基づいて、平
面コイルの損失を最小にするコイルの構成を提示するも
のであって、薄形トランスを構成するコイルの少なくと
も一方を他方のコイルを挟む2個の平面コイルとし、こ
の2個の平面コイルを並列または直列に接続して1個の
コイルに流れる電流による起磁力を減少させる。この起
磁力の減少により、各コイルの厚さ方向に変化する磁束
の大きさを減少させ、コイルの表皮効果の影響を少なく
して、それによる損失を低減している。
The present invention analyzes the relationship between the configuration of a plane coil and the loss of the plane coil, and based on the analysis result, presents a configuration of a coil that minimizes the loss of the plane coil. At least one of the coils constituting the thin transformer is made into two plane coils sandwiching the other coil, and these two plane coils are connected in parallel or in series to reduce the magnetomotive force due to the current flowing in one coil. .. Due to this decrease in the magnetomotive force, the magnitude of the magnetic flux changing in the thickness direction of each coil is reduced, the influence of the skin effect of the coil is reduced, and the loss due to it is reduced.

【0010】[0010]

【実施例】以下、本発明の実施例を図面に基づいて詳細
に説明する。
Embodiments of the present invention will now be described in detail with reference to the drawings.

【0011】図1(a),(b)は本発明の薄形トラン
スの第1の実施例を示す構成図であり、(a)は薄形ト
ランスの断面図、(b)はコイルの接続図である。本実
施例の構成において、1は内部にリング状の空間Sを形
成するための凹部を有する一対のフェライト磁心、2
a,2b(以下、代表するときは2と記す)はそれぞれ
導電板をスパイラル状に加工して6ターンの平面コイル
とした一対のコイル、3は同じく導電板をスパイラル状
に加工して3ターンの平面コイルとしたコイル、4は充
填材である。一対の平面コイル2a,2bは、平面コイ
ル3を上下から挟み込むように配置され、平面コイル2
aと平面コイル2bとは図1(b)に示すように、外部
において電気的に並列接続されている。したがって、平
面コイル2と平面コイル3の巻数比は、6:3となる
が、この巻数比は自在に設計できることは言うまでもな
い。フェライト磁心1は薄形の円板状に形成され、その
一対の凹部同士が向い合わさって形成される内部空間S
内にコイル2a,2bとコイル3とが挟み込まれて、充
填材4により任意の厚さで絶縁され積層状態で固定され
る。
1A and 1B are configuration diagrams showing a first embodiment of a thin transformer according to the present invention. FIG. 1A is a sectional view of the thin transformer, and FIG. 1B is a coil connection. It is a figure. In the configuration of the present embodiment, 1 is a pair of ferrite magnetic cores each having a recess for forming a ring-shaped space S therein, 2
a and 2b (hereinafter referred to as "2" when represented) are a pair of coils each made into a flat coil of 6 turns by processing a conductive plate into a spiral shape, and 3 are 3 turns by similarly processing a conductive plate into a spiral shape. The coil 4 is a plane coil, and 4 is a filler. The pair of plane coils 2a and 2b are arranged so as to sandwich the plane coil 3 from above and below.
The a and the planar coil 2b are electrically connected in parallel externally as shown in FIG. 1 (b). Therefore, the turn ratio of the plane coil 2 and the plane coil 3 is 6: 3, but it goes without saying that this turn ratio can be designed freely. The ferrite core 1 is formed in a thin disk shape, and an internal space S formed by a pair of recesses facing each other.
The coils 2a, 2b and the coil 3 are sandwiched therein, and are insulated in a desired thickness by the filling material 4 and fixed in a laminated state.

【0012】以上のように構成した第1の実施例の作用
とその効果を説明する。
The operation and effect of the first embodiment constructed as above will be described.

【0013】本実施例は、2個の平面コイル2a,2b
を1個の平面コイル3の上下に配置し、その2個の平面
コイル2a,2bを並列接続して、2個の平面コイル2
a,2bに流れる電流を2等分し、1個の平面コイル2
aまたは2bに流れる電流による起磁力を減少すること
を目的にしている。このように起磁力を減少することに
よって、各コイルの厚さ方向に変化する磁束の大きさも
同時に減少できるので、コイルの表皮効果の影響を少な
くすることが可能である。
In this embodiment, two plane coils 2a and 2b are used.
Are arranged above and below one plane coil 3, and the two plane coils 2a and 2b are connected in parallel to form two plane coils 2
The current flowing in a and 2b is divided into two, and one flat coil 2
The purpose is to reduce the magnetomotive force due to the current flowing through a or 2b. By reducing the magnetomotive force in this way, the magnitude of the magnetic flux that changes in the thickness direction of each coil can also be reduced at the same time, so that the effect of the skin effect of the coil can be reduced.

【0014】以下に、コイルの表皮効果による損失の増
加を交流抵抗(コイルに実効値電流1Aを流した時の損
失と等価)で評価し、上記実施例の効果を説明する。計
算に使用した薄形トランスの形状と比較した巻線構造を
図2(a)〜(g)に示す。(g)は巻線部分を破断し
た斜視図、(a)〜(f)はその破断面Aの断面図であ
り、巻線の形状や構成を変えた6種類(以下、(a)〜
(f)構造と記す)についてコイル部のみを拡大して示
している。(g)の断面図において、1は内部にリング
状の空間Sを形成するための凹部を有する一対のフェラ
イト磁心(コア)、2は導電板をスパイラル状に加工し
て4ターンの平面コイルとした一次コイル、3は同じく
導電板をスパイラル状に加工して1ターンの平面コイル
とした二次コイルである。なお、空間Sは充填材で満た
されている。巻線構造において、(a)構造が前記論文
に記載された基本構造、(b)構造が本実施例による構
造、(c)〜(f)構造が起磁力を弱めることにより交
流抵抗の減少を狙った構造である。
The increase in loss due to the skin effect of the coil will be evaluated by the AC resistance (equivalent to the loss when an effective value current of 1 A is passed through the coil), and the effect of the above embodiment will be described below. The winding structure in comparison with the shape of the thin transformer used for the calculation is shown in FIGS. (G) is a perspective view in which a winding portion is broken, and (a) to (f) are cross-sectional views of the fractured surface A, showing six types (hereinafter, (a) to
Regarding (f) structure, only the coil portion is shown in an enlarged manner. In the cross-sectional view of (g), 1 is a pair of ferrite magnetic cores (cores) each having a recess for forming a ring-shaped space S therein, 2 is a flat coil having four turns by processing a conductive plate into a spiral shape. The primary coil 3 and the secondary coil 3 are similarly secondary coils each formed by processing a conductive plate into a spiral shape to form a one-turn flat coil. The space S is filled with the filler. In the winding structure, (a) structure is the basic structure described in the above-mentioned paper, (b) structure is the structure according to the present embodiment, and (c) to (f) structures reduce the magnetomotive force to reduce the AC resistance. This is the targeted structure.

【0015】計算の条件を表1に示す。表中のWは平面
コイル3の導電板の幅、Dは同じく平面コイル3の導電
板の間隔、Hは導電板の厚さである。
Table 1 shows the calculation conditions. In the table, W is the width of the conductive plate of the planar coil 3, D is the distance between the conductive plates of the planar coil 3, and H is the thickness of the conductive plate.

【0016】[0016]

【表1】 [Table 1]

【0017】導電板のスキンディプスの値は周波数50
0kHzで93μmとなり、導電板の厚さHとほぼ等し
く、2MHzではHの半分に減少する。スキンディプス
の値が導電板の厚さ以下になると各巻線構造による表皮
効果の値が顕著になるので、計算を行う周波数は2MH
zとした。計算には市販の有限要素法のプログラム「マ
クスウェル」(Ansoft Corp.)を使用し
た。各巻線構造(a)〜(f)の交流抵抗を一次コイル
を例に取って計算し、直流抵抗で規格化した結果を図3
に示す。(a)構造に比べて本実施例の(b)構造で
は、直流抵抗の増加率(Rac/Rdc)を減少でき
る。しかし、それ以外の巻線構造では交流抵抗の増加率
を低減できないことが分かる。これは、(c)〜(e)
構造のように磁束を分散させたり、磁束の流れを妨げる
巻線を入れると漏れ磁束や一部に集中する磁束により、
渦電流損失が増加するためである。また、(f)構造の
ように導電板を分割しても電流はインピーダンスの低い
一次コイル2と二次コイル3の境界に集中して流れ、交
流抵抗を減少できない。従って、本実施例以外の方法で
は、交流抵抗(コイルの損失)を減少することはできな
い。
The value of the skin depth of the conductive plate is 50
It becomes 93 μm at 0 kHz, which is almost equal to the thickness H of the conductive plate and decreases to half of H at 2 MHz. When the skin depth is less than the thickness of the conductive plate, the value of the skin effect due to each winding structure becomes remarkable, so the frequency for calculation is 2 MH.
z. A commercially available finite element method program "Maxwell" (Ansoft Corp.) was used for the calculation. The AC resistance of each winding structure (a) to (f) was calculated by using the primary coil as an example, and the result normalized by the DC resistance is shown in FIG.
Shown in. In the structure (b) of this embodiment, the increase rate (Rac / Rdc) of the DC resistance can be reduced as compared with the structure (a). However, it can be seen that the rate of increase in AC resistance cannot be reduced with other winding structures. This is (c)-(e)
When magnetic flux is dispersed like a structure or a winding that blocks the flow of magnetic flux is inserted, leakage flux or magnetic flux concentrated in a part causes
This is because the eddy current loss increases. Further, even if the conductive plate is divided as in the case of (f) structure, the current concentrates on the boundary between the primary coil 2 and the secondary coil 3 having low impedance, and the AC resistance cannot be reduced. Therefore, the AC resistance (coil loss) cannot be reduced by any method other than this embodiment.

【0018】次に、本発明の第2の実施例を説明する。Next, a second embodiment of the present invention will be described.

【0019】図4(a),(b)は、その構成を示す図
であって、(a)は部分断面図、(b)はコイルの電気
的な接続図である。この実施例は、第1の実施例の平面
コイル2a,2b,3からなるコイル部の内、中間の平
面コイル3を上下の平面コイル2a,2bで挟み込み、
上下の平面コイル2a,2bを直列接続して一方のコイ
ル部とし、中間の平面コイル3を他方のコイル部とした
薄形トランスを示している。これらのコイル部は、第1
の実施例と同様に一対の偏平なフェライト磁心1内の空
間Sに挾まれて充填材4により積層されて固定される。
4 (a) and 4 (b) are views showing the structure thereof, FIG. 4 (a) is a partial sectional view, and FIG. 4 (b) is an electrical connection diagram of a coil. In this embodiment, an intermediate flat coil 3 is sandwiched between upper and lower flat coils 2a and 2b in the coil portion composed of the flat coils 2a, 2b and 3 of the first embodiment.
A thin transformer in which the upper and lower flat coils 2a and 2b are connected in series to form one coil portion and the intermediate flat coil 3 serves as the other coil portion is shown. These coil parts are
Similar to the above embodiment, the flat ferrite magnetic core 1 is sandwiched between the flat ferrite magnetic cores 1 and stacked and fixed by the filler 4.

【0020】このように構成された第2の実施例におい
ては、各コイル部の損失を第1の実施例と同様の作用で
減少することができるとともに、コイル2a,2bを直
列に接続しているので第1の実施例より大きなインダク
タンスを得ることができる。
In the second embodiment thus constructed, the loss of each coil portion can be reduced by the same action as in the first embodiment, and the coils 2a and 2b are connected in series. Therefore, a larger inductance can be obtained than in the first embodiment.

【0021】次に、本発明の第3の実施例を説明する。Next, a third embodiment of the present invention will be described.

【0022】図5(a),(b),(c)は、その構成
を示す図であって、(a)は部分断面図、(b)および
(c)はコイルの電気的な接続図である。この実施例
は、コイル部が4個以上の平面コイルを積層して形成さ
れる場合の一例として、5層の平面コイルで構成される
場合を示している。本実施例のコイル部は、平面コイル
3aを平面コイル2a,2bで上下から挟み込み、さら
にこのうちの一つの平面コイル2bと平面コイル2cで
もう一つの平面コイル3bを挟み込んで、平面コイル2
a,2b,2cを一方のコイル部とし、平面コイル3
a,3bを他方のコイル部としている。これらのコイル
部は、第1の実施例と同様に一対の偏平なフェライト磁
心1内の空間Sに挟まれて充填材4により積層されて固
定される。本実施例は、各コイル部における接続のし方
によって、図5(b)に示すように平面コイル2a,2
b,2cの組および平面コイル3a,3bの組毎に並列
接続した場合と、図5(c)に示すように上記各組毎に
直列接続した場合の2種に構成できる。
5 (a), 5 (b), and 5 (c) are views showing the structure, (a) is a partial sectional view, and (b) and (c) are electrical connection diagrams of coils. Is. In this embodiment, as an example of the case where the coil portion is formed by laminating four or more plane coils, a case where the coil portion is composed of five layers of plane coils is shown. In the coil portion of this embodiment, the plane coil 3a is sandwiched between the plane coils 2a and 2b from above and below, and the plane coil 2b and the plane coil 2c are sandwiched between the plane coil 2a and the plane coil 3b.
a, 2b, 2c as one coil part, and the planar coil 3
a and 3b are used as the other coil portion. Similar to the first embodiment, these coil portions are sandwiched between the spaces S in the pair of flat ferrite magnetic cores 1 and stacked and fixed by the filler 4. In this embodiment, as shown in FIG. 5B, the planar coils 2a, 2 are
It is possible to configure two types, that is, a group of b and 2c and a group of planar coils 3a and 3b are connected in parallel, and a series of each group is connected as shown in FIG. 5C.

【0023】以上の第3の実施例の構成において、
(b)の接続による構成は第1の実施例に対応し、
(c)の接続による構成は第2の実施例に対応してお
り、それぞれ同様の効果が得られることは明らかであ
る。ただし、各コイル部を構成する平面コイル数が多い
分、その効果をより一層高めることができる。
In the configuration of the above third embodiment,
The configuration by the connection of (b) corresponds to the first embodiment,
It is clear that the configuration by the connection of (c) corresponds to the second embodiment, and the same effects can be obtained respectively. However, since the number of plane coils forming each coil portion is large, the effect can be further enhanced.

【0024】なお、本発明の薄形トランスの形状は、上
記の実施例に限られるものではなく、数々の形状の場合
に適用可能であることは当然である。このように、本発
明はその主旨に沿って種々に応用され、種々の実施態様
を取り得るものである。
The shape of the thin transformer of the present invention is not limited to the above-mentioned embodiment, and it goes without saying that it can be applied to various shapes. As described above, the present invention can be applied in various ways in accordance with its gist and can take various embodiments.

【0025】[0025]

【発明の効果】以上の説明で明らかなように、本発明の
薄形トランスによれば、平面コイルの厚さをスキンディ
プス程度として従来構造の平面コイルよりも、コイル部
の損失を小さくすることができ、スイッチング電源の小
形化、経済化が図られる利点が得られる。
As is apparent from the above description, according to the thin transformer of the present invention, the thickness of the plane coil is set to about skin depth to reduce the loss of the coil portion as compared with the plane coil of the conventional structure. It is possible to obtain the advantage that the switching power supply can be made compact and economical.

【図面の簡単な説明】[Brief description of drawings]

【図1】(a),(b)は本発明の第1の実施例を示す
構成図
1A and 1B are configuration diagrams showing a first embodiment of the present invention.

【図2】(a),(b)は上記第1の実施例の効果を明
らかにするためにコイルの損失を比較した巻線構造図
2A and 2B are winding structure diagrams in which coil losses are compared in order to clarify the effect of the first embodiment.

【図3】上記第1の実施例のコイル損失が従来例と比較
して減少できることを示した説明図
FIG. 3 is an explanatory diagram showing that the coil loss of the first embodiment can be reduced as compared with the conventional example.

【図4】(a),(b)は本発明の第2の実施例を示す
構成図
4A and 4B are configuration diagrams showing a second embodiment of the present invention.

【図5】(a),(b),(c)は本発明の第3の実施
例を示す構成図
5A, 5B and 5C are configuration diagrams showing a third embodiment of the present invention.

【図6】(a),(b)は従来例の構成を示す構成図6A and 6B are configuration diagrams showing a configuration of a conventional example.

【図7】上記従来例の導電板の厚さと損失の関係を示す
説明図
FIG. 7 is an explanatory diagram showing the relationship between the thickness and the loss of the conductive plate of the conventional example.

【符号の説明】[Explanation of symbols]

1…フェライト磁心、2a,2b,2c…一方のコイル
部を構成する平面コイル、3,3a,3b…他方のコイ
ル部を構成する平面コイル、4…充填材。
DESCRIPTION OF SYMBOLS 1 ... Ferrite magnetic core, 2a, 2b, 2c ... The plane coil which comprises one coil part, 3, 3a, 3b ... The plane coil which comprises the other coil part, 4 ... Filler.

Claims (1)

【特許請求の範囲】 【請求項1】 導電板をスパイラル形状に加工した平面
コイルを少なくとも3個積層したコイル部と、このコイ
ル部を挟み込む一対の偏平なフェライト磁心とを備え、 前記3個の平面コイルの内、上下に配置された平面コイ
ルが中間に配置された平面コイルを挟み込む構造を有
し、前記上下の平面コイルを電気的に並列接続または直
列接続して一方のコイルとし、中間の平面コイルをもう
一方のコイルとしたことを特徴とする薄形トランス。
Claim: What is claimed is: 1. A coil portion, in which at least three planar coils obtained by processing a conductive plate into a spiral shape are laminated, and a pair of flat ferrite magnetic cores sandwiching the coil portion. Among the plane coils, the plane coils arranged above and below have a structure sandwiching the plane coils arranged in the middle, and the top and bottom plane coils are electrically connected in parallel or in series to form one coil, A thin transformer characterized by using the flat coil as the other coil.
JP3173559A 1991-07-15 1991-07-15 Thin transformer Pending JPH0521244A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3173559A JPH0521244A (en) 1991-07-15 1991-07-15 Thin transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3173559A JPH0521244A (en) 1991-07-15 1991-07-15 Thin transformer

Publications (1)

Publication Number Publication Date
JPH0521244A true JPH0521244A (en) 1993-01-29

Family

ID=15962798

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3173559A Pending JPH0521244A (en) 1991-07-15 1991-07-15 Thin transformer

Country Status (1)

Country Link
JP (1) JPH0521244A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000058346A (en) * 1998-08-10 2000-02-25 Sumitomo Wiring Syst Ltd Ignition coil for internal combustion engine and manufacture thereof
JP2001217126A (en) * 1999-11-22 2001-08-10 Fdk Corp Laminated inductor
JP2009212370A (en) * 2008-03-05 2009-09-17 Denso Corp Transformer
JP2011018795A (en) * 2009-07-09 2011-01-27 Fuji Electric Systems Co Ltd Electromagnetic induction apparatus
JP2017117908A (en) * 2015-12-24 2017-06-29 Tdk株式会社 Coil component and electronic circuit using the same
WO2018220627A1 (en) * 2017-05-29 2018-12-06 Thin Energy Ltd. Thin transformer and method of production of same

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000058346A (en) * 1998-08-10 2000-02-25 Sumitomo Wiring Syst Ltd Ignition coil for internal combustion engine and manufacture thereof
JP2001217126A (en) * 1999-11-22 2001-08-10 Fdk Corp Laminated inductor
JP2009212370A (en) * 2008-03-05 2009-09-17 Denso Corp Transformer
JP2011018795A (en) * 2009-07-09 2011-01-27 Fuji Electric Systems Co Ltd Electromagnetic induction apparatus
JP2017117908A (en) * 2015-12-24 2017-06-29 Tdk株式会社 Coil component and electronic circuit using the same
WO2018220627A1 (en) * 2017-05-29 2018-12-06 Thin Energy Ltd. Thin transformer and method of production of same
CN110914937A (en) * 2017-05-29 2020-03-24 稀薄能源有限公司 Thin transformer and method of manufacturing the same
EP3631822A4 (en) * 2017-05-29 2021-03-10 Thin Energy Ltd. Thin transformer and method of production of same

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