JPH044771B2 - - Google Patents

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Publication number
JPH044771B2
JPH044771B2 JP59281689A JP28168984A JPH044771B2 JP H044771 B2 JPH044771 B2 JP H044771B2 JP 59281689 A JP59281689 A JP 59281689A JP 28168984 A JP28168984 A JP 28168984A JP H044771 B2 JPH044771 B2 JP H044771B2
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JP
Japan
Prior art keywords
line
ground electrode
distributed constant
electromagnetic delay
delay line
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Expired - Lifetime
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JP59281689A
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Japanese (ja)
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JPS61154210A (en
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Priority to JP28168984A priority Critical patent/JPS61154210A/en
Publication of JPS61154210A publication Critical patent/JPS61154210A/en
Publication of JPH044771B2 publication Critical patent/JPH044771B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、例えば立ち上がり時間1ns以下の超
高速信号を扱う分布定数型電磁遅延線に係り、特
に、導線路が誘電体を介して接地電極に対向して
なるインピーダンス線路を用いた分布定数型電磁
遅延線の改良に関する。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a distributed constant electromagnetic delay line that handles ultra-high-speed signals with a rise time of 1 ns or less, for example, and in particular, the present invention relates to a distributed constant electromagnetic delay line that handles an ultra-high-speed signal with a rise time of 1 ns or less, and in particular, the present invention relates to a distributed constant electromagnetic delay line that handles an ultra-high-speed signal with a rise time of 1 ns or less. This paper relates to improvements in distributed constant electromagnetic delay lines using impedance lines facing each other.

〔従来の技術〕[Conventional technology]

この種の分布定数型電磁遅延線としては、細長
い板状の接地電極の外周を誘電体で覆つて偏平で
細長いボビンを形成し、このボビンの外周に導体
を単層ソレノイド状にスペース巻きして導線路を
形成し、この導線路をその接地電極に対向させて
なる構成がある。
This type of distributed constant electromagnetic delay line is constructed by covering the outer periphery of an elongated plate-shaped ground electrode with a dielectric material to form a flat and elongated bobbin, and then winding a conductor around the outer periphery of this bobbin in the form of a single-layer solenoid. There is a configuration in which a conductive path is formed and this conductive path is opposed to the ground electrode.

このような分布定数型電磁遅延線は、超高速信
号に対して良好な遅延特性を得ることが容易であ
るが、本発明はこれに更に改良を加えたものであ
る。
Such a distributed constant type electromagnetic delay line can easily obtain good delay characteristics for ultrahigh-speed signals, but the present invention is a further improvement.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

本発明はこのような状況の下になされたもので
あり、出力波形、特に立ち上がり波形を改善した
分布定数型電磁遅延線を得るものである。
The present invention has been made under these circumstances, and is intended to provide a distributed constant electromagnetic delay line with improved output waveforms, especially rising waveforms.

〔問題点を解決するための手段〕[Means for solving problems]

このような問題点を解決するために本発明は、
導体が単層ソレノイド状にスペース巻きされてな
る偏平な導線路と、同じ厚みの誘電体を介して裏
表面側の導線路と対向するようにその誘電体に配
置された接地電極と、を具備する分布定数型電磁
遅延線であつて、その接地電極を各ターンの前記
導線路の一部と対向するように配置するととも
に、その接地電極と対向する導線路部分がその接
地電極と対向しない部分よりも広くなるようにそ
の接地電極を配置したものである。
In order to solve these problems, the present invention
Equipped with a flat conductor line in which a conductor is space-wound in the form of a single-layer solenoid, and a ground electrode placed on the dielectric so as to face the conductor line on the back surface side through a dielectric having the same thickness. A distributed constant type electromagnetic delay line in which the ground electrode is arranged to face a part of the conductive line of each turn, and the part of the conductive line that faces the ground electrode does not face the ground electrode. The ground electrode is arranged so that it is wider than the ground electrode.

〔作用〕[Effect]

このような手段を備えた本発明は、単層ソレノ
イド状にスペース巻きされた導線路の各ターンに
おいて、接地電極が部分的に導線路と対向しない
部分を有し、その部分では接地電極との間の容量
が減少し、導線路の途中にインダクタンス分が相
対的に大きな部分が直列に独立形成される。
In the present invention equipped with such a means, in each turn of the conductive line wound in a space in the form of a single-layer solenoid, the ground electrode has a part that does not face the conductive line, and in that part, there is no contact with the ground electrode. The capacitance between them decreases, and a portion with a relatively large inductance is formed independently in series in the middle of the conductive line.

〔実施例〕〔Example〕

以下本発明の実施例を説明する。 Examples of the present invention will be described below.

第1図および第2図は本発明の分布定数型電磁
遅延線の一実施例を示す正面図および側面図であ
る。
1 and 2 are a front view and a side view showing an embodiment of a distributed constant electromagnetic delay line of the present invention.

細長い板状の接地電極1の外周は例えばふつ素
樹脂等の誘電体2で覆われ、偏平で細長いボビン
3が形成されている。
The outer periphery of the elongated plate-shaped ground electrode 1 is covered with a dielectric material 2 such as fluororesin, and a flat and elongated bobbin 3 is formed.

このボビン3の外周には、1ピツチ分の長さと
途中に折れ曲がり部4を有する短冊状の単位導線
路5が、ボビン3の軸方向C−Cを横切るように
複数平行に圧着され、それら各単位導線路5が順
次直列接続されて単層ソレノイド状にスペース巻
きされた偏平な導線路6が形成されている。符号
7はそれら各単位導線路5の接続部である。
On the outer periphery of the bobbin 3, a plurality of rectangular unit conductive lines 5 having a length of one pitch and a bent part 4 in the middle are crimped in parallel so as to cross the axial direction C-C of the bobbin 3. Unit conductive lines 5 are connected in series to form a flat conductive line 6 space-wound in the shape of a single-layer solenoid. Reference numeral 7 indicates a connection portion between each of the unit conductive lines 5.

そして、本発明の分布定数型電磁遅延線におい
て、偏平に巻回された導線路6の内側に位置させ
た上記接地電極1が、ボビン3の幅W方向にて片
側に寄せて配置されている。
In the distributed constant electromagnetic delay line of the present invention, the ground electrode 1 located inside the flatly wound conductive line 6 is arranged to be shifted to one side in the width W direction of the bobbin 3. .

すなわち、第2図に示すように、接地電極1は
接続部7とは反対側(図中上側)の単位導線路5
の折れ曲がり部8側に寄せて配置されており、接
地電極1の一端(図中上端)と折れ曲がり部8内
側間の距離Bよりも、接地電極1の他端(図中下
端)と接続部7内側間の距離Dが大きくなつてい
る。なお、接地電極1の幅Aは距離Dより十分大
きくなつている。
That is, as shown in FIG. 2, the ground electrode 1 is connected to the unit conducting line 5 on the opposite side (upper side in the figure) from the connection part 7.
The distance between the other end of the ground electrode 1 (lower end in the figure) and the connection part 7 is longer than the distance B between one end of the ground electrode 1 (the upper end in the figure) and the inner side of the bent part 8. The distance D between the inner sides is increasing. Note that the width A of the ground electrode 1 is sufficiently larger than the distance D.

そのため、各ターンにおける表裏面側の単位導
線路5は、ほぼ等しい厚み誘電体2を介して大部
分が接地電極1とほぼ等しい間隔で対向し、接続
部7前後の部分では接地電極1から外れてこれと
対向しない構成となつている。
Therefore, most of the unit conducting paths 5 on the front and back sides of each turn face the ground electrode 1 at substantially equal intervals via the dielectric 2 having substantially the same thickness, and are separated from the ground electrode 1 in the portions before and after the connecting portion 7. The structure is such that it does not confront this.

このような本発明の分布定数型電磁遅延線は、
接地電極1を単位導線路5の折れ曲がり部8側へ
寄せるとともに、単位導線路5の接続部7側を空
けて配置しているから、第3図の実線のように、
出力パルス信号の立ち上がり部分が出力振幅の
100%まで所定の傾きで素早く立ち上がる。
Such a distributed constant electromagnetic delay line of the present invention is
Since the ground electrode 1 is placed closer to the bent portion 8 of the unit conductive line 5 and left open on the connecting portion 7 side of the unit conductive line 5, as shown by the solid line in Fig. 3,
The rising part of the output pulse signal is the output amplitude.
Quickly stand up to 100% at a specified tilt.

このような効果が得られる理由としては、以下
のようなことが考えられる。
The following may be considered as the reason why such an effect is obtained.

すなわち、導線路6は偏平に単層ソレノイド状
にスペース巻きされているから、各ターン毎に部
分的に接地電極1と対向しない個所が形成される
と、第4図の等価回路で示されるように、各ター
ンの導線路が、接地電極1に対して容量を持つた
マイクロストリツプ線路DLと、接地電極1と対
向せずに接地電極1に対して容量が殆どないイン
ダクタンスLを直列接続した構成となる。
In other words, since the conductive line 6 is space-wound in a flat single-layer solenoid shape, if a portion of each turn that does not face the grounding electrode 1 is formed, as shown in the equivalent circuit of FIG. The conductor line of each turn is connected in series with a microstrip line DL which has a capacitance with respect to the ground electrode 1, and an inductance L which does not face the ground electrode 1 but has almost no capacitance with respect to the ground electrode 1. The configuration is as follows.

各ターンの単位導線路5は、隣合う単位導線路
5、1つ置いた単位導線路5、……n番目の単位
導線路5、との間に各々M1,M2,……Mnの相
互誘導を持つており、各ターンではマイクロスト
リツプ線路DLの部分がインダクタンスLの部分
より大きいので、相互誘導は各マイクロストリツ
プ線路DL間で互いに形成されていると考え、イ
ンダクタンスLの部分を無視できる。
The unit conductor line 5 of each turn has mutual induction of M1, M2, ...Mn between the adjacent unit conductor line 5, one unit conductor line 5, ... n-th unit conductor line 5, respectively. In each turn, the part of the microstrip line DL is larger than the part of the inductance L, so it is assumed that mutual induction is formed between each microstrip line DL, and the part of the inductance L is Can be ignored.

もつとも、インダクタンスLの部分が大きくな
るような場合にはマイクロストリツプ線路DLに
含めて考えればよい。
However, if the inductance L is large, it may be included in the microstrip line DL.

なお、第4図中の相互誘導は、一番左端のマイ
クロストリツプ線路DLがそれより右側のマイク
ロストリツプ線路DLとの間に形成されるものだ
けを示したが、その左にも相互誘導があり、各マ
イクロストリツプ線路DLも同様に左右のマイク
ロストリツプ線路DLと結合している。
Note that the mutual induction in Figure 4 shows only the one formed between the leftmost microstrip line DL and the microstrip line DL on the right side; There is mutual induction, and each microstrip line DL is similarly coupled to the left and right microstrip lines DL.

ここで分布定数型電磁遅延線が、インダクタン
スLがなくマイクロストリツプ線路DLのみから
なる場合と、マイクロストリツプ線路DLおよび
インダクタンスLからなる場合について、各々電
気的特性を考えると、第5図に示すようになる。
Considering the electrical characteristics of the distributed constant electromagnetic delay line when it is composed of only a microstrip line DL without inductance L, and when it is composed of a microstrip line DL and an inductance L, the fifth The result will be as shown in the figure.

すなわち、周波数に対する出力振幅Vの関係
は、インダクタンスLがない分布定数型電磁遅延
線では、第5図破線のように、出力振幅Vが周波
数の増加とともにゆるやかな傾きで低下する。
これに対して、インダクタンスLも含む分布定数
型電磁遅延線は、ある周波数までは出力振幅Vが
平坦で、それ以上の周波数では比較的急速に低下
する傾向になる。
That is, regarding the relationship between the output amplitude V and the frequency, in a distributed constant electromagnetic delay line without an inductance L, the output amplitude V decreases with a gentle slope as the frequency increases, as shown by the broken line in FIG.
On the other hand, in a distributed constant electromagnetic delay line that also includes an inductance L, the output amplitude V tends to be flat up to a certain frequency, and decrease relatively rapidly at frequencies above that.

この場合、遮断周波数に着目すると、破線の特
性の方が周波数が高くなる。
In this case, when focusing on the cutoff frequency, the frequency is higher for the characteristic indicated by the broken line.

しかし、遮断周波数は、入力パルス信号の立ち
上がり時間が必要とする通過帯域以上に高い必要
はなく、むしろ、入力パルス信号の立ち上がり時
間が必要とする範囲では振幅特性の平坦な方が出
力パルス信号の波形は良好となる。
However, the cutoff frequency does not need to be higher than the passband where the rise time of the input pulse signal is required.In fact, it is better for the output pulse signal to have a flat amplitude characteristic in the range where the rise time of the input pulse signal is required. The waveform becomes good.

従つて、遮断周波数が入力パルス信号の立ち上
がり時間の必要とする範囲内にあれば、導線路6
がマイクロストリツプ線路DL部分とインダクタ
ンスL部分から形成されることにより、出力パル
ス信号の立ち上がり波形の改良が可能となる。
Therefore, if the cutoff frequency is within the range required by the rise time of the input pulse signal, the conductor line 6
By forming the microstrip line DL portion and the inductance L portion, it is possible to improve the rising waveform of the output pulse signal.

本発明の分布定数型電磁遅延線において、ボビ
ン3の幅Wに対する寸法BやDの割合は、その値
によつてかなり変化する。本発明者は、例えば厚
さ0.07mm、幅0.2mmの導体を、幅W=5mmのボビ
ン3にピツチ0.35mmで40ターン単層ソレノイド状
に形成し、第1図と同様な構成で遅延時間2ns、
特性インピーダンス100Ωの分布定数型電磁遅延
線を作つて実験した。
In the distributed constant type electromagnetic delay line of the present invention, the ratio of the dimensions B and D to the width W of the bobbin 3 varies considerably depending on their values. For example, the present inventor formed a conductor with a thickness of 0.07 mm and a width of 0.2 mm into a single layer solenoid shape with 40 turns at a pitch of 0.35 mm on a bobbin 3 with a width W of 5 mm. 2ns,
We created and experimented with a distributed constant electromagnetic delay line with a characteristic impedance of 100Ω.

すると、寸法DをBよりも幅Wに対して約5%
大きくすることにより、出力振幅Vの立ち上がり
が約8%改善され、上述した第3図の実線のよう
に出力振幅の略100%まで素早く立ち上げること
ができた。
Then, the dimension D is about 5% larger than the width W than B.
By increasing the value, the rise of the output amplitude V was improved by about 8%, and as shown by the solid line in FIG. 3 mentioned above, it was possible to quickly rise to about 100% of the output amplitude.

また、出力パルス信号の立ち上がり時間は
200psの超高速のものが得られたが、立ち上がり
部の傾斜は両者殆ど同じであり、結局本発明では
出力波形が改善された。
Also, the rise time of the output pulse signal is
Although an ultra-high speed of 200 ps was obtained, the slope of the rising part was almost the same in both cases, and the output waveform was improved in the present invention.

これに対して、ボビン3の幅方向WでDをBに
合せた場合、導線路6のターン数が例えば30ター
ン以上あるとすれば、出力パルス信号の立ち上が
り波形は、第3図の破線のように100%よりやや
低く立ち上がり、その後に次第に100%に達する
傾向にある。これは、導線路6のターンを増加し
て遅延時間を増加させると、その傾向が一層強く
なり、好ましくない。
On the other hand, if D is matched to B in the width direction W of the bobbin 3, and the number of turns of the conductive path 6 is, for example, 30 or more, the rising waveform of the output pulse signal will be as shown by the broken line in FIG. It tends to rise slightly below 100% and then gradually reach 100%. This tendency becomes even stronger when the number of turns in the conductive line 6 is increased to increase the delay time, which is not preferable.

本発明の分布定数型電磁遅延線は、接地電極1
を導線路6の折れ曲がり部8側に寄せて配置する
場合に限らず、逆に単位導線路5の接続部7側に
寄せてD<Bとしてもよい。
The distributed constant electromagnetic delay line of the present invention has a ground electrode 1
It is not limited to the case where D is placed closer to the bent portion 8 side of the conductive line 6, but it may be placed closer to the connecting portion 7 side of the unit conductive line 5 so that D<B.

なお、ボビン3の幅W寸法に対する寸法B,D
の割合すなわち接地電極1を一方へ寄せる割合
は、分布定数型電磁遅延線の構成や目的とする特
性に応じて最適の値に選定すればよい。
In addition, the dimensions B and D with respect to the width W dimension of the bobbin 3
The ratio, that is, the ratio at which the ground electrode 1 is moved to one side, may be selected to an optimal value depending on the configuration of the distributed constant electromagnetic delay line and the desired characteristics.

また、第6図に示すように、ボビン3の幅W方
向の中央部を外して2枚の接地電極9a,9bを
対向するよう長手方向に沿つて配置してもよい。
この構成の分布定数型電磁遅延線では、若干プリ
シユートが増加する傾向があるものの、本発明の
目的達成が可能である。
Alternatively, as shown in FIG. 6, the center portion of the bobbin 3 in the width W direction may be removed and the two ground electrodes 9a, 9b may be arranged along the longitudinal direction so as to face each other.
Although the distributed constant electromagnetic delay line having this configuration tends to have a slight increase in pre-cut, it is possible to achieve the object of the present invention.

さらに、本発明の分布定数型電磁遅延線は、第
7図に示すように、誘電体からなる偏平で細長い
ボビン10の外周に、第1図のような単層ソレノ
イド状の導線路6を形成し、その外周を誘電体1
1で覆うとともに、接続部7前後を除いて導線路
6と対向するように接地電極12を被せる構成も
可能である。
Furthermore, as shown in FIG. 7, the distributed constant electromagnetic delay line of the present invention has a single-layer solenoid-shaped conducting path 6 as shown in FIG. and the outer periphery is dielectric 1
1, and a configuration is also possible in which the ground electrode 12 is covered so as to face the conductive line 6 except for the front and back of the connection part 7.

このように本発明は、単層ソレノイド状にスペ
ース巻きされた偏平な導線路6における出力波形
の改善をその目的とすることから、接地電極1を
各ターンの導線路6の一部と対向するように配置
し、しかもその接地電極1と対向する導線路6部
分がその接地電極1と対向しない部分よりも広く
なるようにその接地電極1を配置すれば良い。
In this way, the present invention aims to improve the output waveform in the flat conductive line 6 space-wound in the form of a single-layer solenoid. Moreover, the ground electrode 1 may be arranged so that the portion of the conductive path 6 facing the ground electrode 1 is wider than the portion not facing the ground electrode 1.

本発明の分布定数型電磁遅延線にあつては、導
線路13の特性インピーダンスを調整するため
に、特に特性インピーダンスを増加させるため、
第8図に示すように、接地電極1に細いスリツト
14を多数分散して形成することも可能である。
ここでは連続する導体を単層ソレノイド状に巻い
て形成されている。
In the distributed constant electromagnetic delay line of the present invention, in order to adjust the characteristic impedance of the conducting line 13, in particular, to increase the characteristic impedance,
As shown in FIG. 8, it is also possible to form a large number of thin slits 14 in the ground electrode 1 in a distributed manner.
Here, a continuous conductor is wound into a single-layer solenoid shape.

この構成で接地電極1に分散形成されたスリツ
ト14は、導線路13の全体にわたつて静電容量
を低下させて特性インピーダンスを増加させるも
のであり、本発明のように各ターンにおいてマイ
クロストリツプ導線路とは別のインダクタンスL
をマイクロストリツプ線路と直列に形成するもの
とは異なる。
The slits 14 dispersedly formed in the ground electrode 1 in this configuration reduce the capacitance and increase the characteristic impedance over the entire conductive line 13, and as in the present invention, the slits 14 are formed in a microstrip in each turn. Inductance L separate from the conductor line
This is different from the one in which the microstrip line is formed in series with the microstrip line.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明の分布定数型電磁遅
延線は、導体が単層ソレノイド状にスペース巻き
されてなる偏平な導線路が、この表裏面側で同じ
厚みの誘電体を介して接地電極と対向する分布定
数型電磁遅延線において、各ターンの導線路の一
部と対向するように、かつその接地電極と対向す
る導線路部分がその接地電極と対向しない部分よ
りも広くなるようにその接地電極を配置している
から、導線路の各ターンではマイクロストリツプ
線路に対して略インダクタンスLのみの部分が直
列に形成され、周波数に対する振幅特性の平坦な
範囲が広がつて出力波形、特に立ち上がり波形が
改善される。
As explained above, in the distributed constant electromagnetic delay line of the present invention, a flat conductor path made of a conductor space-wound in the form of a single-layer solenoid is connected to a ground electrode via a dielectric material of the same thickness on the front and back sides. In the opposing distributed constant electromagnetic delay lines, the grounding is done so that it faces a part of the conductor line of each turn, and the part of the conductor line that faces the ground electrode is wider than the part that does not face the ground electrode. Because the electrodes are arranged, at each turn of the conductor line, a part with approximately only inductance L is formed in series with the microstrip line, and the flat range of the amplitude characteristic with respect to frequency is expanded, and the output waveform, especially The rising waveform is improved.

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

第1図および第2図は本発明の分布定数型電磁
遅延線の一実施例を示す正面図および側面図、第
3図は第1図に示す分布定数型電磁遅延線および
本発明の参考となる分布定数型電磁遅延線(図示
せず)の立ち上がり波形図、第4図は第1図の分
布定数型電磁遅延線の等価回路図、第5図は第1
図および本発明の参考となる分布定数型電磁遅延
線における周波数に対する出力振幅の関係を示す
図、第6図〜第8図は本発明の他の実施例を示す
側面図および正面図である。 1,9a,9b,12……接地電極、2,11
……誘電体、3,10……ボビン、5……単位導
線路、6,13……導線路、7……接続部、8…
…折れ曲がり部、14……スリツト、DL……マ
イクロストリツプ線路、L……インダクタンス。
1 and 2 are front and side views showing one embodiment of the distributed constant electromagnetic delay line of the present invention, and FIG. 3 is a front view and a side view showing an embodiment of the distributed constant electromagnetic delay line shown in FIG. Figure 4 is an equivalent circuit diagram of the distributed constant type electromagnetic delay line (not shown) shown in Figure 1.
6 to 8 are side views and front views showing other embodiments of the present invention. 1, 9a, 9b, 12...ground electrode, 2, 11
...Dielectric material, 3, 10... Bobbin, 5... Unit conducting line, 6, 13... Conducting line, 7... Connection part, 8...
...Bend portion, 14...Slit, DL...Microstrip line, L...Inductance.

Claims (1)

【特許請求の範囲】 1 導体が単層ソレノイド状にスペース巻きされ
てなる偏平な導線路と、 同じ厚みの誘電体を介して表裏面側の前記導線
路と対向するように前記誘電体に配置された接地
電極と、 を具備する分布定数型電磁遅延線において、 前記接地電極が各ターンの前記導線路の一部と
対向するように配置されるとともに、 前記接地電極と対向する前記導線路部分が前記
接地電極と対向しない部分よりも広くなるように
前記接地電極が配置されてなることを特徴とする
分布定数型電磁遅延線。
[Scope of Claims] 1. A flat conductive path formed by space-wound conductors in the form of a single-layer solenoid, and arranged on the dielectric so as to face the conductive path on the front and back sides through a dielectric having the same thickness. a distributed constant electromagnetic delay line comprising: a ground electrode arranged to face a portion of the conductive line of each turn; and a portion of the conductive line opposite to the ground electrode. The distributed constant electromagnetic delay line is characterized in that the ground electrode is arranged such that the ground electrode is wider than a portion not facing the ground electrode.
JP28168984A 1984-12-26 1984-12-26 Distribution constant type electromagnetic delay line Granted JPS61154210A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28168984A JPS61154210A (en) 1984-12-26 1984-12-26 Distribution constant type electromagnetic delay line

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28168984A JPS61154210A (en) 1984-12-26 1984-12-26 Distribution constant type electromagnetic delay line

Publications (2)

Publication Number Publication Date
JPS61154210A JPS61154210A (en) 1986-07-12
JPH044771B2 true JPH044771B2 (en) 1992-01-29

Family

ID=17642607

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28168984A Granted JPS61154210A (en) 1984-12-26 1984-12-26 Distribution constant type electromagnetic delay line

Country Status (1)

Country Link
JP (1) JPS61154210A (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4317544Y1 (en) * 1965-05-17 1968-07-20

Also Published As

Publication number Publication date
JPS61154210A (en) 1986-07-12

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