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JPH0650684B2 - High frequency air core transformer - Google Patents
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JPH0650684B2 - High frequency air core transformer - Google Patents

High frequency air core transformer

Info

Publication number
JPH0650684B2
JPH0650684B2 JP22307184A JP22307184A JPH0650684B2 JP H0650684 B2 JPH0650684 B2 JP H0650684B2 JP 22307184 A JP22307184 A JP 22307184A JP 22307184 A JP22307184 A JP 22307184A JP H0650684 B2 JPH0650684 B2 JP H0650684B2
Authority
JP
Japan
Prior art keywords
air
core
transformer
present
core transformer
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.)
Expired - Lifetime
Application number
JP22307184A
Other languages
Japanese (ja)
Other versions
JPS61102009A (en
Inventor
毅 池田
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP22307184A priority Critical patent/JPH0650684B2/en
Publication of JPS61102009A publication Critical patent/JPS61102009A/en
Publication of JPH0650684B2 publication Critical patent/JPH0650684B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F19/00Fixed transformers or mutual inductances of the signal type
    • H01F19/04Transformers or mutual inductances suitable for handling frequencies considerably beyond the audio range

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Multimedia (AREA)
  • Coils Or Transformers For Communication (AREA)

Description

【発明の詳細な説明】 〔従来技術とその問題点〕 トランス(変圧器ともいう)は、1つの回路から交流電
力を受けてこれと磁気的に結合している1以上の他の巻
線に電磁誘導作用によって変圧した出力を得る電気部品
ないし静止機器であり、その用途は電圧の変換、回路間
の絶縁、インピーダンス交換等の広範囲に及ぶ。
DETAILED DESCRIPTION OF THE INVENTION [PRIOR ART AND PROBLEMS] A transformer (also called a transformer) receives AC power from one circuit and is connected to one or more other windings magnetically coupled to the AC power. It is an electric component or a static device that obtains an output transformed by an electromagnetic induction action, and has a wide range of applications such as voltage conversion, insulation between circuits, and impedance exchange.

近年エレクトロニクスは産業用から玩具に至る家庭用品
まで広く使用されている。このエレクトロニクス回路は
半導体集積回路(IC,LSI,VLSI等)技術の進
歩に伴ない著しく小型化しており、その動作のための電
源も小型軽量であることを必要とする。そのために、電
源として一般にスイッチングレギュレーターが普及して
いる。スイッチングレギャレーターの小型軽量化及び高
効率化のためには、スイッチング周波数を高くすること
が考えられ、現在主流の50kHz級から、より高周波で
ある500kHzからMHz級のスイッチングレギャレータへ
の開発、努力がなされている。
In recent years, electronics have been widely used from industrial products to household items such as toys. This electronic circuit has been remarkably miniaturized along with the progress of semiconductor integrated circuit (IC, LSI, VLSI, etc.) technology, and the power supply for its operation needs to be small and lightweight. Therefore, a switching regulator is widely used as a power source. In order to reduce the size, weight and efficiency of switching regulators, it is conceivable to increase the switching frequency, and from the current mainstream of 50kHz to the higher frequency of 500kHz to MHz switching regulator. , Efforts are being made.

高周波スイッチングレギュレータを実現するためするた
めの技術的問題は、高速スイッチング素子(トランジス
タ等)及び特に高周波小型トランス等の開発にある、ス
イッチングレギュレータ用トランスにおいては十分な一
次、二次巻線間の絶縁耐圧を得るために、それぞれ一次
コイルと二次コイルを物理的に離して、または両コイル
間に十分な絶縁層を設けて重ねて巻回することを普通と
している。しかし、両コイル間のリーケージインダクタ
ンスを最小にしてエネルギーの伝達損失を最小にするた
め、両コイル間をフェライト等の高透磁率の磁路で磁気
的に結合している。磁芯を使用すると、トランスの小型
軽量化、さらに価格に限界があると共にMHz級の高周波
においても十分に使用できる高い透磁率や磁気飽和の少
ない磁気材料などを得ることが困難であった。
The technical problem for realizing a high-frequency switching regulator is the development of high-speed switching elements (transistors, etc.) and especially small high-frequency transformers. In transformers for switching regulators, sufficient insulation between primary and secondary windings is required. In order to obtain a withstand voltage, it is customary to physically separate the primary coil and the secondary coil, or to wrap them by providing a sufficient insulating layer between the coils. However, in order to minimize the leakage inductance between both coils and the energy transfer loss, the two coils are magnetically coupled by a magnetic path having a high magnetic permeability such as ferrite. When a magnetic core is used, it is difficult to obtain a magnetic material having high magnetic permeability and low magnetic saturation, which has a small size and light weight of a transformer, has a limit in price, and can be sufficiently used even in a high frequency of MHz class.

〔発明の目的〕[Object of the Invention]

本発明は、高周波スイッチングレギュレータ等に好適な
安価にして小型軽量のトランスを提供することを目的と
する。
An object of the present invention is to provide an inexpensive, compact and lightweight transformer suitable for a high frequency switching regulator and the like.

本発明の他の目的は、絶縁フィルムを介して相互に絶縁
した導電箔膜を一体に重合させ、磁芯を使用することな
く、即ち空芯状態で巻回することにより、安価にして小
型軽量、かつ、高効率の高周波で作動可能なトランスを
提供することである。
Another object of the present invention is to make the conductive foil films insulated from each other through an insulating film to be integrally polymerized, and to wind the coil without using a magnetic core, that is, in an air core state, thereby making it inexpensive, compact and lightweight. And to provide a highly efficient transformer that can operate at high frequency.

本発明の更に他の目的は、広い周波数範囲にわたり効率
が極めて高いトランスを提供することである。
Yet another object of the present invention is to provide a transformer that is extremely efficient over a wide frequency range.

〔発明の概要〕[Outline of Invention]

種々の形状のトランスについてエネルギー伝達特性の実
験を行なった結果、MHz級の高周波帯域においては、巻
線形状を工夫することにより磁芯を使用することなく、
即ち空芯で損失を実質的に排除して高効率のトランスが
得られることが判明した。即ち2枚の導電箔膜を絶縁体
を間挿して重合させ、空芯状態に巻回することにより高
周波におけるエネルギー伝達特性は極めて高くなること
が判明した。従来、トランスの巻線として断面がほぼ円
形の銅線等に代わって帯状または箔状導体を使用するこ
と、または箔状導体を絶縁フィルムを介して同時に磁芯
の回りに巻回するトランスは、既に提案されている(例
えば米国特許第2521513号明細書)が、本発明者
は、MHz級の高周波帯では空芯状態に巻線形状を工夫す
ることにより十分に高いエネルギー伝達特性が得られる
ことを実験により初めて認識した。
As a result of experiments on energy transfer characteristics of transformers of various shapes, in the high frequency band of MHz class, by devising the winding shape, without using a magnetic core,
That is, it was found that the air core substantially eliminates the loss to obtain a highly efficient transformer. That is, it has been found that the energy transfer characteristics at high frequencies become extremely high by superposing two conductive foil films by interposing an insulator between them and winding them in an air-core state. Conventionally, a strip-shaped or foil-shaped conductor is used as a winding wire of a transformer instead of a copper wire having a substantially circular cross section, or a transformer in which a foil-shaped conductor is wound around a magnetic core through an insulating film at the same time is Although already proposed (for example, US Pat. No. 2,521,513), the present inventor can obtain a sufficiently high energy transfer characteristic by devising the winding shape in the air core state in the high frequency band of MHz class. Was recognized for the first time by experiment.

従来、MHz級の高周波で作動可能なトランスを実現する
ために、あくまでも磁芯の改良にとらわれ、その高透磁
率化や高い飽和磁束密度化など磁芯の諸特性の改良に腐
心していた。しかし、本発明では高周波化への問題を、
空芯状態て巻線形状を工夫することにより解決したもの
で、高周波帯域においては、磁芯を使用する必要がない
というまったく従来のトランスとしての概念を基本的に
変革したものである。この本発明の空芯トランスを用い
てMHz級の高周波スイッチングレギュレータを超小型に
なし得ることを実証した。
Conventionally, in order to realize a transformer capable of operating at a high frequency of MHz class, we have been obsessed with the improvement of magnetic cores, and have been devoted to improving various characteristics of magnetic cores such as high permeability and high saturation magnetic flux density. However, in the present invention, the problem of increasing the frequency is
This was solved by devising the winding shape in the air core state, and it is a fundamental revolution of the concept of a conventional transformer in which it is not necessary to use a magnetic core in the high frequency band. It has been proved that a high frequency switching regulator of MHz class can be miniaturized by using the air core transformer of the present invention.

〔実施例(A)〕Example (A)

第1図は、本発明の一実施例による空芯トランスの構造
を示す概略図である。導電箔膜10,12は厚さ50μ
m、幅約10mm、長さ1650mmのアルミニウム箔であ
って、両端に適当な大きさ及び長さの錫めっき等を施し
た鉄線や銅線等の端子またはリード線18,20及び2
2,24を、例えば、電気溶接等の周知技法で固定す
る。この溶接に先立ちリード線の溶接部はプレス等によ
り平坦加工を施すことが好ましい。この導電箔膜10,
12はポリエチレン、マイラー等の高誘電率、かつ、高
絶縁耐圧を有するプラスチックフィルム14,16を介
して重ね合わせ、巻線機械を用いて空芯状態に密に巻回
する。この場合、絶縁体として14,16のマイラーフ
ィルムは、厚さ12μm、幅15mm、長さ約1650mm
であって、その幅を導電箔膜10,12より広くし両導
電箔膜間の絶縁耐圧を高めるのが好ましい。
FIG. 1 is a schematic diagram showing the structure of an air-core transformer according to an embodiment of the present invention. Conductive foil films 10 and 12 have a thickness of 50μ
m, width of about 10 mm, length of 1650 mm, and an aluminum foil having a suitable size and length at both ends, such as iron or copper wire, or terminals or lead wires 18, 20 and 2
2, 24 are fixed by a well-known technique such as electric welding. Prior to this welding, it is preferable that the welded portion of the lead wire be flattened by a press or the like. This conductive foil film 10,
12 is superposed through plastic films 14 and 16 having a high dielectric constant such as polyethylene and Mylar and a high withstand voltage, and is tightly wound in an air-core state using a winding machine. In this case, 14 and 16 mylar films as an insulator have a thickness of 12 μm, a width of 15 mm, and a length of about 1650 mm.
However, it is preferable that the width thereof is made wider than that of the conductive foil films 10 and 12 to increase the withstand voltage between the conductive foil films.

フィルム14,16の厚さは、必要とするトランスの巻
線間絶縁耐圧により決め、導電箔膜10,12の巻回数
は必要とするインダクタンスと巻数比により決めること
ができる。
The thickness of the films 14 and 16 can be determined by the required dielectric strength between windings of the transformer, and the number of turns of the conductive foil films 10 and 12 can be determined by the required inductance and the turn ratio.

以上の製法に基づいて作られた本発明の空芯トランスの
実施例(A)は、巻回数が52回で約16μHのインダク
タンスと約64nFの静電容量とQの値0.79が得られた。
In the embodiment (A) of the air-core transformer of the present invention manufactured based on the above manufacturing method, the number of windings was 52 and the inductance of about 16 μH, the capacitance of about 64 nF and the Q value of 0.79 were obtained.

第2図は、第1図の空芯トランスの等価回路図であり、
端子18−22間に一次巻線W1が導電箔膜10により形
成され、端子20−24間に二次巻線W2が導電箔膜12
により形成される。なお、両巻線W1,W2間にはその対向
する全長にわたりほぼ一定の分布静電容量C0が不可避的
に形成される。
FIG. 2 is an equivalent circuit diagram of the air-core transformer of FIG.
Primary winding W 1 between the terminals 18-22 is formed by the guide Denhakumaku 10, the secondary winding to the terminals 20-24 W 2 is electrically Denhakumaku 12
Is formed by. A substantially constant distributed electrostatic capacitance C 0 is unavoidably formed between the windings W 1 and W 2 over the entire length facing each other.

第3図は、本発明の空芯トランスの完成斜視図の一例で
あって、導電箔膜10,12と絶縁フィルムまたはテー
プ14,16とを巻回した後、そのまま使用するか、も
しくは適当な圧力を加えてほぼ楕円形に変形させると共
に、端子18〜24を除き全体を、例えばエポキシ等の
樹脂でコーティングして吸湿等による特性劣化を防止す
る。なお、磁芯が無いので押圧変形しやすく両巻線W1,W
2間の結合を一層密にして漏洩磁束による効率低下を防
止するのに大変有効である。
FIG. 3 is an example of a completed perspective view of the air-core transformer of the present invention, in which the conductive foil films 10 and 12 and the insulating films or tapes 14 and 16 are wound and then used as they are, or an appropriate one. The pressure is applied to deform it into a substantially elliptical shape, and the entire part except the terminals 18 to 24 is coated with a resin such as epoxy to prevent characteristic deterioration due to moisture absorption or the like. In addition, since there is no magnetic core, it is easy to be pressed and deformed. Both windings W 1 , W
It is very effective in making the coupling between the two more dense and preventing a decrease in efficiency due to magnetic flux leakage.

〔特性測定回路〕[Characteristics measurement circuit]

第4図は、本発明による空芯トランスの特性測定回路図
を示す。
FIG. 4 shows a characteristic measuring circuit diagram of the air-core transformer according to the present invention.

本発明による空芯トランスの一次巻線W1に50Ωの出力
抵抗Riを有する定振幅正弦波信号発生器(ソニー・テ
クトロニクス(株)製191型)28を接続し、二次巻
線W2に50Ωの負荷低抗R0を接続して両端電圧降下を1
0:1のプローブを介し、広帯域オシロスコープ(ソニ
ー・テクトロニクス(株)製2445型)30で測定す
る。
A constant amplitude sine wave signal generator (191 type manufactured by Sony Tektronix Co., Ltd.) 28 having an output resistance Ri of 50Ω is connected to the primary winding W 1 of the air-core transformer according to the present invention, and the secondary winding W 2 is connected to the secondary winding W 2 . Connect a 50 Ω load resistance R 0 to reduce the voltage drop across both ends to 1
A wideband oscilloscope (Model 2445 manufactured by Sony Tektronix Co., Ltd.) 30 is used for measurement through a 0: 1 probe.

〔周波数特性〕〔Frequency characteristic〕

第7図は、第4図の測定回路により、正弦波信号発生器
28の出力振幅を一定に維持して周波数を50kHzから
100MHzまで変化して出力電圧eoと入力電圧eiの比eo/
eiをオシロスコープで測定し、プロットしたものであ
る。
FIG. 7 shows the measurement circuit of FIG. 4 in which the output amplitude of the sine wave signal generator 28 is maintained constant and the frequency is changed from 50 kHz to 100 MHz to obtain the ratio eo / input voltage eo / input voltage ei.
This is a plot of ei measured with an oscilloscope.

上述の実施例(A)によるサンプル(一次,二次巻線の巻
数比は1対1である)では、第7図(A)に示す変圧特性
を示し、約2MHzまでは1以下であるが、2MHzより5MH
zまでは約1であり、それ以上では約100MHzまで1以
上の高い値を有することは注目に値する。この高周波特
性は、一次、二次巻線の結合度が全体にわたり極めて密
であること、及び誘導結合のみならず両巻線間に存在す
る大きな静電容量による静電結合によるものと考えられ
る。また高周波において1以上の変圧比が得られるの
は、この空芯トランスの比較的低いがなだらかなQによ
るものと推定される。
The sample according to the above-described embodiment (A) (the turns ratio of the primary and secondary windings is 1: 1) exhibits the transformation characteristic shown in FIG. 7 (A), which is less than 1 up to about 2 MHz. 5MHz from 2MHz
It is worth noting that it has a high value of 1 or more up to z and above 1 up to about 100 MHz. It is considered that this high-frequency characteristic is due to the fact that the degree of coupling between the primary and secondary windings is extremely dense as a whole and that not only inductive coupling but also electrostatic coupling due to a large capacitance existing between both windings. Further, it is presumed that the transformation ratio of 1 or more is obtained at a high frequency due to the relatively low but gentle Q of this air core transformer.

〔対比例(B)〕(Comparative (B))

次に、本発明と対比するために、実施例(A)と同じ材料
を用い、各巻線を別にして、巻回した試料を作った。す
なわち、第5図に示すように導電箔膜10′と12′に
厚さ50μm、幅10mm、長さ1650mmのアルミニウ
ム箔と、実施例(A)と同じマイラーフィルム14′,1
6′を用い、まず導電箔膜10′を先に66回巻回して
インダクタンス17μH、Q0.87を得て入力側とし、さ
らにその上から導電箔膜12′を33回巻回し、インダ
クタンス15.6μH、Q0.83を得たものを出力側としたサ
ンプルにつき、第4図の測定回路によって実施例(A)と
同様の実験を行なった結果、第7図(B)に示す特性を示
し、eo/eiが1以上の周波数は存在せず、1MHz付近と6
0MHz付近でeo/eiが0.6から0.7程度示したが、実施例
(A)に比べ全体的に比較にならないほどエネルギー伝達
特性の低いことが判明した。以上のように高周波帯域に
おいても実施例(A)のように重合させ、一体として巻回
しなければ、高周波で良好に作動することができないこ
とが判る。
Next, in order to compare with the present invention, the same material as that of the example (A) was used, and each winding was separated to prepare a wound sample. That is, as shown in FIG. 5, aluminum foil having a thickness of 50 μm, a width of 10 mm and a length of 1650 mm is formed on the conductive foil films 10 ′ and 12 ′, and the Mylar film 14 ′, 1 which is the same as the embodiment (A).
6 ', the conductive foil film 10' is first wound 66 times to obtain an inductance of 17 μH and Q0.87 to be the input side, and the conductive foil film 12 'is further wound 33 times to have an inductance of 15.6 μH. , Q0.83 was obtained on the output side, the same experiment as in Example (A) was conducted using the measurement circuit of FIG. 4, and as a result, the characteristics shown in FIG. There is no frequency where / ei is 1 or more, and around 1MHz and 6
Although eo / ei showed about 0.6 to 0.7 near 0 MHz,
It was found that the energy transfer characteristics were so low that they were incomparable as a whole compared to (A). As described above, it can be seen that even in the high frequency band, good operation at high frequencies cannot be achieved unless they are polymerized and integrally wound as in Example (A).

〔実施例(C)〕Example (C)

次に、本発明による空芯トランスの巻数の相違による特
性の比較を行なってみた。
Next, the characteristics of the air-core transformer according to the present invention are compared by the number of turns.

第1図に示す導電箔膜10,12を厚さ8μm、幅6mm
のアルミニウム箔と、絶縁体14,16として厚さ6μ
m、幅7mmのマイラーフィルムを用いて第1表に示した
サンプルを作成した。
The conductive foil films 10 and 12 shown in FIG. 1 are 8 μm thick and 6 mm wide.
Aluminum foil and insulators 14 and 16 with a thickness of 6μ
The samples shown in Table 1 were prepared using a Mylar film having a width of m and a width of 7 mm.

第4図に示す特性測定回路により実施例(A)と同様の実
験を行なった結果、巻数が増すと第1表から明らかなよ
うに、インダクタンス及び静電容量が増大し、第8図
(a)(b)(c)に示すように低周波帯域側にeo/eiの変圧比特
性が拡がることが判明し、使用周波数帯域を任意に選べ
ることが判明した。
As a result of conducting an experiment similar to that of the embodiment (A) using the characteristic measuring circuit shown in FIG. 4, as the number of turns increases, the inductance and the capacitance increase, as is apparent from Table 1, and FIG.
As shown in (a), (b) and (c), it was found that the transformation ratio characteristics of eo / ei spread to the low frequency band side, and it was found that the used frequency band can be arbitrarily selected.

〔直線性〕[Linearity]

次に第9図は、第4図の測定回路により実施例(A)の発
振器28の発振周波数を一定(5MHzと1MHz)にして、
入力電圧eiを0.1乃至5ボルトに変化した場合の出力電
圧eoをオシロスコープで測定プロットした直線性、即ち
ダイナミックレンジ特性曲線図である。第9図より明ら
かなように、実施例(A)の本発明の空芯トランスによる
と、広い入力電圧レンジにわたり極めて良好な直線性を
有する。なお、使用した試験器具の関係上、これ以上の
電圧につき実験できなかったが、空芯であり磁気飽和要
因は全く存在しないので、一層大入力についても線形出
力が得られることが容易に推定できる。
Next, FIG. 9 shows that the oscillation frequency of the oscillator 28 of the embodiment (A) is made constant (5 MHz and 1 MHz) by the measuring circuit of FIG.
It is the linearity which measured and plotted the output voltage eo in case the input voltage ei was changed to 0.1 to 5 volts by the oscilloscope, ie, a dynamic range characteristic curve diagram. As is clear from FIG. 9, the air-core transformer of the embodiment (A) of the present invention has extremely good linearity over a wide input voltage range. In addition, due to the test equipment used, it was not possible to experiment with higher voltage, but since it is an air core and there is no magnetic saturation factor, it can be easily estimated that a linear output can be obtained even for a larger input. .

〔変更、変形〕[Change, transformation]

以上、本発明の好適実施例につき説明したが、本発明
は、何らこの実施例のみに限定すべきでなく種々の変
更、変形が可能である。例えば相互に絶縁シートを介し
て3以上の導電箔膜を巻回して2以上の出力を得てもよ
い。例えば、第6図のように、2つの箔の一方は2つの
箔12″a,12″bに分割し、端部に夫々の端子20″a,
20″bを接続してもよい。各導電箔膜の厚さはそれを流
れる電流の大きさに応じて適宜選定でき、それによる特
性の顕著な違いのないことは第7図(A)と第8図(C)の比
較によっても確められた。さらに導体箔膜は、絶縁シー
トの両面または片面に無電解メッキや蒸着またはスパッ
タリング技法等により形成ることも可能である。
Although the preferred embodiment of the present invention has been described above, the present invention should not be limited to this embodiment at all, and various changes and modifications can be made. For example, two or more outputs may be obtained by winding three or more conductive foil films mutually via an insulating sheet. For example, as shown in FIG. 6, one of the two foils is divided into two foils 12 ″ a, 12 ″ b, and the terminals 20 ″ a,
20 ″ b may be connected. The thickness of each conductive foil film can be selected appropriately according to the magnitude of the current flowing through it, and there is no significant difference in characteristics due to that, as compared with FIG. 7 (A). It was also confirmed by the comparison of Fig. 8 (C) Further, the conductor foil film can be formed on both surfaces or one surface of the insulating sheet by electroless plating, vapor deposition or sputtering technique.

〔発明の効果〕〔The invention's effect〕

本発明の空芯トランスは、空芯、即ち、磁芯ないし鉄芯
を一切使用しないので極めて小型軽量化でき磁気飽和に
伴なう問題が生ずることなく、一定周波数以上では極め
て良好なエネルギー伝達特性を呈する。また、導電箔膜
を使用するので、密結合が可能であり、そのため漏洩磁
束も少なく同一円形断面積の銅線に比して十分大きい断
面積の箔が使用できるので、電流容量が増加でき、しか
も高周波においても表皮効果の影響を最少にすることが
できる。また、各巻線間は、任意厚さの絶縁フイルムを
用いて絶縁できるので、巻線間のアイソレーション、即
ち、絶縁耐圧が優れている。
Since the air-core transformer of the present invention does not use any air-core, that is, a magnetic core or an iron core, it can be made extremely small and lightweight without causing a problem with magnetic saturation, and has a very good energy transfer characteristic at a certain frequency or more. Present. Further, since the conductive foil film is used, tight coupling is possible, and therefore, there is little leakage flux, and a foil having a sufficiently large cross-sectional area can be used as compared with a copper wire having the same circular cross-sectional area, so that the current capacity can be increased, Moreover, the influence of the skin effect can be minimized even at high frequencies. Further, since each winding can be insulated by using an insulating film having an arbitrary thickness, the isolation between windings, that is, the withstand voltage is excellent.

従って、本発明の空芯トランスはMHz級の高周波で動作
するスイッチングレギュレータのトランスとして使用
し、その高効率化、小型軽量化する目的等において特に
有効であり、むろんスイッチングレギュレータ以外にア
イソレータその他高い絶縁耐圧を必要とする多くの目的
に使用可能であることはいうまでもない。
Therefore, the air-core transformer of the present invention is used as a transformer of a switching regulator that operates at a high frequency of MHz class, and is particularly effective for the purpose of improving its efficiency, downsizing, and weight reduction. It goes without saying that it can be used for many purposes requiring pressure resistance.

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

第1図は本発明による空芯トランスの一実施例の分解
図、第2図は本発明による空芯トランスの等価電気回路
図、第3図は、本発明の空芯トランスの一実施例の完成
斜視図、第4図は、本発明の空芯トランスの特性を測定
する回路図、第5図は、本発明の空芯トランスと対比す
べき他の形態の空芯トランスの要部を示す分解図、第6
図は、本発明による空芯トランスの他の実施例の要部を
示す分解図、第7図及び第8図は、本発明の空芯トラン
スの一実施例の周波数特性曲線図、第9図は、本発明の
空芯トランスの直線性及びダイナミックレンジの特性曲
線図である。 10,10′,10″,12,12′,12″a,12″b……導電箔膜 14,14′,14″,16,16′,16″……絶縁体 18,18′,18″,20,20′,20″a,20″b,22,22′,2
4,24′……端子
FIG. 1 is an exploded view of an embodiment of an air-core transformer according to the present invention, FIG. 2 is an equivalent electric circuit diagram of the air-core transformer according to the present invention, and FIG. 3 is an embodiment of an air-core transformer according to the present invention. FIG. 4 is a completed perspective view, FIG. 4 is a circuit diagram for measuring the characteristics of the air-core transformer of the present invention, and FIG. 5 shows a main part of another form of the air-core transformer to be compared with the air-core transformer of the present invention. Exploded view, No. 6
FIG. 7 is an exploded view showing a main part of another embodiment of the air-core transformer according to the present invention, FIGS. 7 and 8 are frequency characteristic curve diagrams of one embodiment of the air-core transformer of the present invention, and FIG. FIG. 4 is a characteristic curve diagram of linearity and dynamic range of the air-core transformer of the present invention. 10,10 ', 10 ", 12,12', 12" a, 12 "b ... Conductive foil film 14,14 ', 14", 16,16', 16 "... Insulator 18,18 ', 18 ″, 20,20 ′, 20 ″ a, 20 ″ b, 22,22 ′, 2
4,24 ′ …… Terminal

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】ポリエチレン、マイラー等の高誘電率の絶
縁層を介して相対向するように積層された2枚の帯状導
電薄膜を空芯状態に巻回して一体の空芯巻回体を形成
し、該空芯巻回体の前記帯状導電薄膜の両端近傍に夫々
1次側端子及び2次側端子を溶接接続し、前記空芯巻回
体を略楕円形とし、外周をエポキシ等でコーティングし
て形成されたことを特徴とする高周波用空芯トランス。
1. An air-core winding body is formed by winding two strip-shaped conductive thin films, which are laminated so as to face each other with an insulating layer having a high dielectric constant such as polyethylene or mylar, in an air-core state. Then, a primary side terminal and a secondary side terminal are welded and connected to the vicinity of both ends of the band-shaped conductive thin film of the air-core winding body, respectively, and the air-core winding body is formed into a substantially elliptical shape, and the outer periphery is coated with epoxy or the like. A high frequency air core transformer characterized by being formed by
JP22307184A 1984-10-25 1984-10-25 High frequency air core transformer Expired - Lifetime JPH0650684B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22307184A JPH0650684B2 (en) 1984-10-25 1984-10-25 High frequency air core transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22307184A JPH0650684B2 (en) 1984-10-25 1984-10-25 High frequency air core transformer

Publications (2)

Publication Number Publication Date
JPS61102009A JPS61102009A (en) 1986-05-20
JPH0650684B2 true JPH0650684B2 (en) 1994-06-29

Family

ID=16792373

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22307184A Expired - Lifetime JPH0650684B2 (en) 1984-10-25 1984-10-25 High frequency air core transformer

Country Status (1)

Country Link
JP (1) JPH0650684B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002111273A (en) * 2000-09-29 2002-04-12 Railway Technical Res Inst Magnetic shield transformer
CA3115916A1 (en) * 2018-03-07 2019-09-12 The Board Of Trustees Of The Leland Stanford Junior University Apparatuses and methods involving power conversion using multiple rectifier circuits

Also Published As

Publication number Publication date
JPS61102009A (en) 1986-05-20

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