JPS61219114A - Inductance element - Google Patents
Inductance elementInfo
- Publication number
- JPS61219114A JPS61219114A JP6163485A JP6163485A JPS61219114A JP S61219114 A JPS61219114 A JP S61219114A JP 6163485 A JP6163485 A JP 6163485A JP 6163485 A JP6163485 A JP 6163485A JP S61219114 A JPS61219114 A JP S61219114A
- Authority
- JP
- Japan
- Prior art keywords
- copper wire
- amorphous metal
- inductance
- warp
- woof
- 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.)
- Granted
Links
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 claims abstract description 28
- 239000000835 fiber Substances 0.000 claims abstract description 19
- 239000005300 metallic glass Substances 0.000 claims abstract description 18
- 229910052802 copper Inorganic materials 0.000 claims description 13
- 239000010949 copper Substances 0.000 claims description 13
- 238000002955 isolation Methods 0.000 claims description 4
- 230000035699 permeability Effects 0.000 claims description 4
- 239000004744 fabric Substances 0.000 abstract description 3
- 239000004753 textile Substances 0.000 abstract description 3
- 239000012212 insulator Substances 0.000 abstract 3
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 4
- 239000002759 woven fabric Substances 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 239000000203 mixture Substances 0.000 description 3
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000004907 flux Effects 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 229910000679 solder Inorganic materials 0.000 description 2
- 229910000859 α-Fe Inorganic materials 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 1
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 1
- 238000005280 amorphization Methods 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 239000003990 capacitor Substances 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
- 239000011651 chromium Substances 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 239000010941 cobalt Substances 0.000 description 1
- 229910017052 cobalt Inorganic materials 0.000 description 1
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 238000005520 cutting process Methods 0.000 description 1
- 230000002500 effect on skin Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000010304 firing Methods 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 238000005304 joining Methods 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- WPBNNNQJVZRUHP-UHFFFAOYSA-L manganese(2+);methyl n-[[2-(methoxycarbonylcarbamothioylamino)phenyl]carbamothioyl]carbamate;n-[2-(sulfidocarbothioylamino)ethyl]carbamodithioate Chemical compound [Mn+2].[S-]C(=S)NCCNC([S-])=S.COC(=O)NC(=S)NC1=CC=CC=C1NC(=S)NC(=O)OC WPBNNNQJVZRUHP-UHFFFAOYSA-L 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- 229910052758 niobium Inorganic materials 0.000 description 1
- 239000010955 niobium Substances 0.000 description 1
- GUCVJGMIXFAOAE-UHFFFAOYSA-N niobium atom Chemical compound [Nb] GUCVJGMIXFAOAE-UHFFFAOYSA-N 0.000 description 1
- 239000003921 oil Substances 0.000 description 1
- 230000008520 organization Effects 0.000 description 1
- 229910052698 phosphorus Inorganic materials 0.000 description 1
- 239000011574 phosphorus Substances 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 229910052710 silicon Inorganic materials 0.000 description 1
- 239000010703 silicon Substances 0.000 description 1
- 238000009987 spinning Methods 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F17/00—Fixed inductances of the signal type
- H01F17/04—Fixed inductances of the signal type with magnetic core
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Coils Or Transformers For Communication (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は、高周波帯域で回路素子として使用されるイン
ダクタンス素子に関するものである。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an inductance element used as a circuit element in a high frequency band.
(従来技術および発明が解決しようとする問題点)従来
100KHz帯の周波数帯域で使用されるインダクタン
ス素子はフェライトの環状磁心を用いたものがほとんど
である。この種のインダクタ?−)m傾lv1+−+斗
布田国油紡亦丁羽小郡旦泊μl−7#堺するものであり
、インダクタの小型化には限界がある。なぜなら、周波
数が高くなると磁束の表皮効果のため、磁心の容積の割
には有効磁束が少なくインダクタンスが低下する。その
ため、所望のインダクタンス値を得るには、コイルの巻
数増加で対応せざるを得なく、どうしても小型のインダ
クタンス素子とするには限界がある。(Prior Art and Problems to be Solved by the Invention) Most inductance elements conventionally used in the 100 KHz frequency band use a ferrite annular magnetic core. This kind of inductor? -) m inclination lv1+-+Dufu Tian Oil Textile Co., Ltd. Dingba Kogun Danpaku μl-7 #Sakai, and there is a limit to the miniaturization of the inductor. This is because as the frequency increases, due to the skin effect of magnetic flux, the effective magnetic flux is small relative to the volume of the magnetic core, and the inductance decreases. Therefore, in order to obtain a desired inductance value, it is necessary to increase the number of turns of the coil, and there is a limit to how small an inductance element can be made.
一方、電子回路の他の素子の分野ではICからLSI化
等の半導体関係の進歩に伴って、より小型化、軽薄化が
望まれており、現に抵抗やコンデンサーは小型化の進歩
が著しくチップの自動装着技術の普及が広まっている。On the other hand, in the field of other elements of electronic circuits, with the progress in semiconductors such as the transition from ICs to LSIs, there is a desire for smaller, thinner and thinner resistors and capacitors. Automated attachment technology is becoming more popular.
ところが、インダクタンス素子だけが旧態依然として、
環状磁心と巻線との組合わせで構成されており、しかも
前述の如く小型化に限界かあるため、小型で軽薄型の新
規なインダクタンス素子の出現が業界では渇望されてい
た。However, only the inductance element remains in its old state.
The inductance element is composed of a combination of an annular magnetic core and a winding wire, and as mentioned above, there are limits to miniaturization, so the industry has been eager for a new small, light and thin inductance element.
近年、インダクタンス素子の小型化に対して、フェライ
トと導電体とを交互に積層し、焼成した外鉄型閉磁路ト
ロイダルよりなる積層チップインダクタが考案されてい
る。しかしながら、この積層チップインダクタは、尚厚
みが厚く薄型になっていないこと、焼成工程の管理が厳
しく安価な量産品が得られないこと等の欠点に加えて、
容積当たりのインダクタンス値が小さいという重大な欠
点を有している。In recent years, in order to reduce the size of inductance elements, a multilayer chip inductor has been devised, which is made of an outer iron type closed magnetic circuit toroidal in which ferrite and conductor are alternately laminated and fired. However, this multilayer chip inductor has drawbacks such as being too thick and not being thin enough, and the firing process is difficult to control, making it impossible to produce inexpensive mass-produced products.
It has a serious drawback of having a small inductance value per volume.
(問題点を解決するための手段)
本発明者らは、上記問題点を解決すべく、鋭意研究の結
果、高透磁率アモルファス金属繊維と絶縁被覆銅線とを
組合わせて、全く新規な構成体を形成せしめ、小型で薄
型の、しかも容積当たりのインダクタンス値の大きいイ
ンダクタンス素子を発明するに至った。(Means for Solving the Problems) In order to solve the above problems, the present inventors, as a result of intensive research, have created a completely new structure by combining high magnetic permeability amorphous metal fibers and insulated copper wires. We have succeeded in inventing an inductance element that is small, thin, and has a large inductance value per volume.
本発明は高周波帯域での使用、とりわけ100KHz以
上においてもそのインダクタンスが数μH以上の大きな
値を有する小型で薄型の安価なインダクタンス素子の提
供を目的とする。An object of the present invention is to provide a small, thin, and inexpensive inductance element whose inductance has a large value of several μH or more even when used in a high frequency band, particularly at frequencies above 100 KHz.
すなわち、本発明は、高透磁率アモルファス金属繊維と
絶縁被覆銅線とを交織した織物組織を有し、かつ該絶縁
被覆銅線が電気的に連続していることを特徴とするイン
ダクタンス素子である。That is, the present invention is an inductance element characterized by having a woven fabric in which high magnetic permeability amorphous metal fibers and insulating coated copper wires are interwoven, and the insulating coated copper wires are electrically continuous. .
本発明を図面に基づいて説明する。The present invention will be explained based on the drawings.
第1図に本発明の構成の一例を示す。第1図ではアモル
ファス金属繊維(図中、lで示す)をタテ糸とし、ヨコ
糸に絶縁被覆銅線(図中、2で示す)を使用した交織織
物の耳部でヨコ糸の絶縁被覆銅線を折り返して一本の連
続した銅線としたものである。本発明において、銅線を
流れる電流の方向が、アモルファス金属繊維の周囲を同
一円周方向に流れることが重要であり、従ってタテ糸と
ヨコ糸が逆の組合わせでもよい。また織物の組織につい
ても、平織、綾織、朱子織等いずれでも可であるが、タ
テ糸とヨコ糸の交差する点が最も多い平織組織が好まし
い。FIG. 1 shows an example of the configuration of the present invention. In Figure 1, amorphous metal fibers (indicated by l in the figure) are used as the warp yarns, and insulation-coated copper wires are used as the weft yarns at the edges of a mixed woven fabric (indicated by 2 in the figure). The wire is folded back to form one continuous copper wire. In the present invention, it is important that the direction of the current flowing through the copper wire is in the same circumferential direction around the amorphous metal fibers, so the warp and weft threads may be used in reverse combinations. Further, the structure of the woven fabric may be plain weave, twill weave, satin weave, etc., but plain weave structure in which the warp threads and weft threads intersect with each other in the greatest number of points is preferable.
絶縁被覆銅線は電気的な連続性が保持されておれば良く
、第1図のように折り返しても良いが、第2図の示す如
く、絶縁被覆銅線を織物耳部で折り返さずに、隣接する
銅線をハンダ等で接合(図中、3で接合部を示す)して
電気的に接続したものであっても、本発明の効果は具現
される。The insulated copper wire only needs to maintain electrical continuity, and may be folded back as shown in Fig. 1, but as shown in Fig. 2, the insulated copper wire may not be folded back at the selvage of the fabric. Even if adjacent copper wires are electrically connected by joining them with solder or the like (indicated by 3 in the figure), the effects of the present invention can be realized.
図において、アモルファス金属繊維および絶縁被覆銅線
は各々1本のみをタテ糸ヨコ糸として示しであるが、所
望のインダクタンス値を得るため、あるいは所望の使用
目的のため、各複数本束ねてタテ糸ヨコ糸として組織を
形成してもよい。例えばタテ糸としてアモルファス金属
繊維を2本以上集束したものを使用すれば高インダクタ
ンス値の素子となる。またヨコ糸として絶縁被覆銅線を
複数本集束したものを使用すれば、高周波の電流損失も
少なく、また高電流でも可能なインダクタンス素子が可
能であり、更には相互インダクタンスを利用して直流成
分をカットする目的の絶縁トランスとして使用可能であ
る。In the figure, only one amorphous metal fiber and insulated copper wire are shown as warp threads or weft threads, but in order to obtain a desired inductance value or for a desired purpose, multiple pieces of each are bundled and warp threads are used. The structure may be formed as a weft. For example, if a bundle of two or more amorphous metal fibers is used as the warp thread, an element with a high inductance value can be obtained. Furthermore, if a bundle of multiple insulated copper wires is used as the weft thread, there will be less current loss at high frequencies, and an inductance element that can handle high currents will be possible.Furthermore, by using mutual inductance, it will be possible to reduce the direct current component. Can be used as an isolation transformer for cutting purposes.
本発明の高透磁率アモルファス金属繊維とは、磁性を有
する金属成分(例えば、鉄、コバルト、ニッケルまたは
これらの混合物等)とアモルファス化に必要な半金属成
分(例えば、シリコン、ホウ素、リン、炭素またはこれ
らの混合物等)を主成分とする断面円形のアモルファス
状態の繊維である。また、特性安定化のためにクロム、
マンガン、ニオブ等を数原子%添加してもよい。通常は
回転液中紡糸法により得られる直径100μmから15
0μmのアモルファス金属繊維をそのまま使用するか、
もしくはダイス線引により、直径を細くしたもの、更に
は磁気特性向上のための熱処理を施したものを使用して
もよい。断面円形であることは織物組織を構成するに際
し、極めて加工性、操作性、可とう性等に優位に作用す
る。織物組織を構成することから、アモルファス金属繊
維の成分は零磁歪近傍が好ましい。The high magnetic permeability amorphous metal fiber of the present invention includes a magnetic metal component (for example, iron, cobalt, nickel, or a mixture thereof) and a semimetal component necessary for amorphization (for example, silicon, boron, phosphorus, carbon, etc.). or a mixture thereof, etc.) is an amorphous fiber with a circular cross section. In addition, chromium is added to stabilize the properties.
Several atomic percent of manganese, niobium, etc. may be added. The diameter is usually 100 μm to 15 μm obtained by spinning in a rotating liquid.
Either use 0 μm amorphous metal fiber as is, or
Alternatively, it is also possible to use a material whose diameter has been reduced by die drawing, or a material which has been subjected to heat treatment to improve magnetic properties. Having a circular cross section has an extremely advantageous effect on workability, operability, flexibility, etc. when constructing a textile structure. Since the amorphous metal fiber constitutes a woven structure, it is preferable that the components of the amorphous metal fiber have near zero magnetostriction.
本発明における絶縁被覆銅線としては、一般に使用され
ているエナメル線、ホルマール線等が挙げられ、裸銅線
に対して業界の常識的な絶縁被覆を施した銅線である。Examples of the insulating coated copper wire in the present invention include commonly used enamelled wires, formal wires, etc., and are copper wires that are made by applying an industry-common insulating coating to bare copper wires.
織物組織をより密にするにはタテ糸とヨコ糸の直径を同
一にするのが好ましい。In order to make the woven fabric denser, it is preferable that the warp and weft yarns have the same diameter.
(発明の実施例) 本発明を実施例により更に詳細に説明する。(Example of the invention) The present invention will be explained in more detail with reference to Examples.
実施例1
直径100μm1長さ15mmのアモルファス金属繊i
(組成CQea、+、F e4.ais !+z、 5
B Is:添字は原子%)5本1束にしたものを1本の
タテ糸として10本用いて、直径140μmのエナメル
被覆銅線をヨコ糸として耳部で折り返した平織組織のイ
ンダクタンス素子を作成した。アモルファス金属繊維1
束あたりの等価巻数は34ターンである。電流値]00
mAでの各周波数におけるインダクタンス値を測定した
。結果を第3図に示す。Example 1 Amorphous metal fiber i with a diameter of 100 μm and a length of 15 mm
(Composition CQea, +, Fe4.ais !+z, 5
B Is: Subscript is atomic %) A plain weave inductance element was created by using 10 strands of 5 wires bundled together as one warp thread and folding an enamelled copper wire with a diameter of 140 μm as a weft thread at the edge. did. Amorphous metal fiber 1
The equivalent number of turns per bundle is 34 turns. Current value]00
The inductance value at each frequency in mA was measured. The results are shown in Figure 3.
0.1〜100KHzまでは平坦な周波数特性を示し、
インダクタンスは約150μHと゛高い値を示す。また
100KHz以上ではインダクタンス値は単調に減少す
るが、IMHzでも約70μHの高い値を有している。Shows flat frequency characteristics from 0.1 to 100KHz,
The inductance shows a high value of about 150 μH. Further, the inductance value monotonically decreases above 100 KHz, but it has a high value of about 70 μH even at IMHz.
また150μHのインダクタンス値は単位容積あたりの
インダクタンスに換算すると約3μH/mm3と非常に
大きな値を有している。現在市販されている積層チップ
イングクタは最も高いインダクタンスのものでらL4μ
H/mm3である。Further, the inductance value of 150 μH has a very large value of about 3 μH/mm 3 when converted into inductance per unit volume. The multilayer chip inductor currently on the market has the highest inductance, L4μ.
H/mm3.
実施例2
直径80μm1長さ3 、5 mmのアモルファス金属
繊維1本をタテ糸として10本用い、直径70μmのエ
ナメル被覆銅線をヨコ糸として実施例1と同様にインダ
クタンス素子を作成した。単位容積あたりのインダクタ
ンス値は100KI−(zで7μH/mm’、1ooO
K、Hzで5μH/mm3の高い値を示す。Example 2 An inductance element was prepared in the same manner as in Example 1, using 10 amorphous metal fibers each having a diameter of 80 μm and a length of 3.5 mm as the warp yarn, and using an enamelled copper wire with a diameter of 70 μm as the weft yarn. The inductance value per unit volume is 100KI-(7μH/mm' at z, 1ooO
It shows a high value of 5 μH/mm3 at K and Hz.
実施例3
ヨコ糸として直径70μmのエナメル被覆銅線を2本使
用した以外は実施例2と同様なインダクタンス素子を作
成した。2本のヨコ糸の銅線を電気的に結線せず、各々
単独にインダクタンス値を測定すると10〜500KH
zの範囲で約11IHであった。この2本のヨコ糸を総
巻数が増加するように結線して電気的に連続した1本の
ヨコ糸とした場合のインダクタンス値は、同周波帯域で
約4μHであった。インダクタンスは概略巻数の2乗に
比例することが了解される。Example 3 An inductance element similar to Example 2 was produced except that two enamelled copper wires with a diameter of 70 μm were used as the weft threads. If you measure the inductance value of two weft copper wires individually without electrically connecting them, it will be 10 to 500 KH.
It was about 11 IH in the z range. When these two weft yarns were connected to increase the total number of turns to form one electrically continuous weft yarn, the inductance value was about 4 μH in the same frequency band. It is understood that inductance is approximately proportional to the square of the number of turns.
実施例4
実施例3と同じインダクタンス素子を用い、2本のヨコ
糸の銅線を各々変圧器の1次側、2次側として、1次側
にピーク電圧1,5V周波数10MHzのサイン波を人
力し、2次側の出力波形を観察した。その結果、2次側
出力は位相の遅れもなく、ピーク電圧値の一致したとこ
ろの、入力波形を完全に再現したものであった。Example 4 Using the same inductance element as in Example 3, two weft copper wires were used as the primary and secondary sides of the transformer, respectively, and a sine wave with a peak voltage of 1.5V and a frequency of 10MHz was applied to the primary side. I manually observed the output waveform on the secondary side. As a result, the secondary side output completely reproduced the input waveform without any phase delay and with the same peak voltage value.
即ち、本発明のインダクタンス素子を変圧器と同様な方
法で用いることにより、直流と交流との重畳した入力信
号より、交流信号のみを忠実に再現する、所謂、絶縁ト
ランスとして利用価値の高いものである。That is, by using the inductance element of the present invention in the same manner as a transformer, it can be used as a so-called isolation transformer, which can faithfully reproduce only an AC signal rather than a superimposed input signal of DC and AC. be.
(発明の効果)
本発明により、高インダクタンス値を有する小型で薄型
の安価で量産型のインダクタンス素子および直流成分を
カットし、高周波交流信号のみを再現する絶縁トランス
が提供される。(Effects of the Invention) The present invention provides a small, thin, inexpensive, and mass-produced inductance element having a high inductance value, and an isolation transformer that cuts a DC component and reproduces only a high-frequency AC signal.
第1図、第2図は本発明の構成組織の一例を示す図、第
3図は本発明のインダクタンス素子のインダクタンス値
の周波数特性を示す図である。
図中、lはアモルファス金属繊維、2は絶縁被覆銅線、
3は絶縁被覆銅線のハンダ結合部を示す。1 and 2 are diagrams showing an example of the structural organization of the present invention, and FIG. 3 is a diagram showing the frequency characteristics of the inductance value of the inductance element of the present invention. In the figure, l is amorphous metal fiber, 2 is insulated copper wire,
3 shows the solder joint portion of the insulated copper wire.
Claims (1)
交織した織物組織を有し、かつ該絶縁被覆銅線が電気的
に連続していることを特徴とするインダクタンス素子。 2、インダクタンス素子が絶縁トランスに用いられる特
許請求の範囲第1項記載のインダクタンス素子。[Claims] 1. An inductance element having a woven structure in which high magnetic permeability amorphous metal fibers and insulated copper wires are interwoven, and the insulated copper wires are electrically continuous. . 2. The inductance element according to claim 1, wherein the inductance element is used in an isolation transformer.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6163485A JPS61219114A (en) | 1985-03-25 | 1985-03-25 | Inductance element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6163485A JPS61219114A (en) | 1985-03-25 | 1985-03-25 | Inductance element |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS61219114A true JPS61219114A (en) | 1986-09-29 |
JPH0525161B2 JPH0525161B2 (en) | 1993-04-12 |
Family
ID=13176820
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP6163485A Granted JPS61219114A (en) | 1985-03-25 | 1985-03-25 | Inductance element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61219114A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0414803A (en) * | 1990-05-08 | 1992-01-20 | Miyota Kk | Mounting method of ultrathin inductance element |
JPH0696954A (en) * | 1991-06-14 | 1994-04-08 | Amorphous Denshi Device Kenkyusho:Kk | Micro-wire inductance element |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5435382A (en) * | 1993-06-16 | 1995-07-25 | Baltimore Aircoil Company, Inc. | Combination direct and indirect closed circuit evaporative heat exchanger |
JPH0743085A (en) * | 1993-07-30 | 1995-02-10 | Hitachi Air Conditioning & Refrig Co Ltd | Cross-flow cooling tower |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5529566U (en) * | 1978-08-17 | 1980-02-26 | ||
JPS5998506A (en) * | 1982-11-27 | 1984-06-06 | Matsushita Electric Works Ltd | Inductance element |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5529566B2 (en) * | 1973-02-13 | 1980-08-05 |
-
1985
- 1985-03-25 JP JP6163485A patent/JPS61219114A/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5529566U (en) * | 1978-08-17 | 1980-02-26 | ||
JPS5998506A (en) * | 1982-11-27 | 1984-06-06 | Matsushita Electric Works Ltd | Inductance element |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0414803A (en) * | 1990-05-08 | 1992-01-20 | Miyota Kk | Mounting method of ultrathin inductance element |
JPH0696954A (en) * | 1991-06-14 | 1994-04-08 | Amorphous Denshi Device Kenkyusho:Kk | Micro-wire inductance element |
Also Published As
Publication number | Publication date |
---|---|
JPH0525161B2 (en) | 1993-04-12 |
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