JPH0376602B2 - - Google Patents
Info
- Publication number
- JPH0376602B2 JPH0376602B2 JP14744083A JP14744083A JPH0376602B2 JP H0376602 B2 JPH0376602 B2 JP H0376602B2 JP 14744083 A JP14744083 A JP 14744083A JP 14744083 A JP14744083 A JP 14744083A JP H0376602 B2 JPH0376602 B2 JP H0376602B2
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- pitch
- cable
- conductors
- core wire
- 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
Links
- 239000004020 conductor Substances 0.000 claims description 38
- 239000011295 pitch Substances 0.000 description 21
- 239000012212 insulator Substances 0.000 description 17
- 230000005855 radiation Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 230000005684 electric field Effects 0.000 description 1
- 238000005187 foaming Methods 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 230000001902 propagating effect Effects 0.000 description 1
- 238000004904 shortening Methods 0.000 description 1
- 125000006850 spacer group Chemical group 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q13/00—Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave
- H01Q13/20—Non-resonant leaky-waveguide or transmission-line antennas; Equivalent structures causing radiation along the transmission path of a guided wave
- H01Q13/203—Leaky coaxial lines
Landscapes
- Waveguide Aerials (AREA)
Description
【発明の詳細な説明】
発明の技術分野
本発明はらせん導体型漏洩ケーブルの構造に関
するものである。DETAILED DESCRIPTION OF THE INVENTION Technical Field of the Invention The present invention relates to the structure of a helical conductor type leaky cable.
従来技術と問題点
従来のらせん導体型漏洩ケーブルは、第1図に
示すように一対の導体1,2を一定のピツチPで
らせん状に撚り合せたもので、絶縁方式として
は、例えば第2図に示すように絶縁体3の中央に
導体1,2を埋め込んだ心線タイプや、第3図に
示すように絶縁体3に形成した溝に導体1,2を
挿入した所謂スペーサタイプが採用されている。Prior Art and Problems A conventional leaky spiral conductor cable is made by twisting a pair of conductors 1 and 2 in a spiral shape at a constant pitch P, as shown in Fig. 1. As shown in the figure, a core type in which the conductors 1 and 2 are embedded in the center of the insulator 3, and a so-called spacer type in which the conductors 1 and 2 are inserted into grooves formed in the insulator 3 as shown in Fig. 3 are adopted. has been done.
ところで、このようならせん導体型漏洩ケーブ
ルの放射周波数とピツチPとの間には次式で示
すような関係が成立する。 By the way, a relationship as shown in the following equation is established between the radiation frequency and pitch P of such a spiral conductor type leaky cable.
(c/p)・{Kλ/(1+Kλ)}</n<
(c/p)・{Kλ/(1−Kλ)} ……(1)
但し、cは光速、Kλは波長短縮率、nは自然
数である。 (c/p)・{Kλ/(1+Kλ)}</n<
(c/p)·{Kλ/(1−Kλ)} (1) where c is the speed of light, Kλ is the wavelength shortening rate, and n is a natural number.
(1)式において、Kλは絶縁体で定まり、通常0.5
〜0.95程度である。従つて、150MHz以下で使用
できるように設計すると、ピツチPは1〜2m以
上にせざるを得ない。この為、らせん角が極めて
小さくなり、均一なピツチで製造することが非常
に困難であつた。 In equation (1), Kλ is determined by the insulator and is usually 0.5
~0.95. Therefore, if it is designed to be used at frequencies below 150 MHz, the pitch P must be set to 1 to 2 m or more. For this reason, the helical angle becomes extremely small, making it extremely difficult to manufacture with uniform pitch.
発明の目的
本発明はこのような従来の欠点を改善したもの
であり、ピツチを長くとらなくても十分に低い放
射周波数が得られるらせん導体型漏洩ケーブルを
提供することを課題としている。OBJECTS OF THE INVENTION The present invention improves on these conventional drawbacks, and aims to provide a helical conductor type leaky cable that can obtain a sufficiently low radiation frequency without increasing the pitch.
発明の構成
本発明のらせん導体型漏洩ケーブルでは、ケー
ブルにP1,P2の異なる周期(二重周期)を持た
せるようにしたものである。Structure of the Invention In the spiral conductor type leaky cable of the present invention, the cable has different periods P 1 and P 2 (double period).
二対にP1,P2の異なるらせんピツチを持たせ
れば、らせんの向きが同じであれば、対同志の間
の相対ピツチPは
P=P1P2/(P1−P2) …(2)
となる。従つて、P2(又はP1)を変化させること
により、0<P<∞なる範囲の任意のピツチPを
実現することができる。 If two pairs have different helical pitches P 1 and P 2 , and if the directions of the helices are the same, the relative pitch P between the pairs is P = P 1 P 2 / (P 1 - P 2 )... (2) becomes. Therefore, by changing P 2 (or P 1 ), any pitch P in the range 0<P<∞ can be realized.
ケーブルを伝搬する電界及び、又は磁界の強
さ、即ち波源の強度分布はらせんピツチ以外でも
変化させることができるから、周期P1,P2は導
体のらせんピツチ以外に導体径や導体間隔などの
寸法、絶縁体の厚みや発泡度等ケーブルの構造に
関する任意のパラメータに持たせることができ
る。この際、ケーブルの有効な放射帯域幅を広げ
る為に各パラメータの変化は正弦波状であること
が好ましい。 Since the strength of the electric field and/or magnetic field propagating through the cable, that is, the intensity distribution of the wave source, can be changed other than the helical pitch, the periods P 1 and P 2 can be changed depending on factors other than the helical pitch of the conductor, such as the conductor diameter and conductor spacing. Any parameters related to the structure of the cable, such as dimensions, thickness of insulator, degree of foaming, etc., can be set. At this time, it is preferable that the changes in each parameter be sinusoidal in order to widen the effective radiation bandwidth of the cable.
発明の実施例
第4図〜第6図は本発明のそれぞれ異なる実施
例の構造説明図であり、らせん導体型漏洩ケーブ
ルの断面を斜めから見たものである。Embodiments of the Invention FIGS. 4 to 6 are structural explanatory diagrams of different embodiments of the present invention, and are oblique views of cross sections of helical conductor type leaky cables.
第4図に示す実施例は、一方の心線を構成する
導体12,13をそれぞれ絶縁体16,17のほ
ぼ中央に埋め込んで、互いにらせんピツチP2で
撚り合せて低損失絶縁材料のテープ或いは糸で作
られた管18内に収容し、この管18の回りに、
絶縁体14,15のほぼ中央に埋め込まれた別の
他方の心線を構成する導体10,11を互いにら
せんピツチP1で撚り合せ、これを管19に収容
したものである。 In the embodiment shown in FIG. 4, conductors 12 and 13 constituting one core wire are buried approximately in the center of insulators 16 and 17, respectively, and are twisted together with a helical pitch P 2 and then covered with a tape or a low-loss insulating material. It is housed in a tube 18 made of thread, and around this tube 18,
Conductors 10 and 11 constituting another core wire embedded approximately in the center of insulators 14 and 15 are twisted together at a helical pitch P 1 and housed in a tube 19.
また、第5図に示す実施例は、絶縁体14で被
覆した導体10と絶縁体15で被覆した導体11
とを互いにらせんピツチP1で撚り合せて管21
に収容し、絶縁体16で被覆した導体12と絶縁
体17で被覆した導体13とを互いにらせんピツ
チP2で撚り合せて管20に収納し、管20,2
1を管22に収納したものである。導体10,1
1が一方の心線を、導体12,13が他方の心線
を構成する。 Further, the embodiment shown in FIG. 5 has a conductor 10 covered with an insulator 14 and a conductor 11 covered with an insulator 15.
Twist them together with a spiral pitch of P 1 to form the tube 21.
The conductor 12 covered with the insulator 16 and the conductor 13 covered with the insulator 17 are twisted together with a spiral pitch P 2 and housed in the tube 20.
1 is housed in a tube 22. Conductor 10,1
1 constitutes one core wire, and conductors 12 and 13 constitute the other core wire.
第6図の実施例は、絶縁体14,15で被覆し
た一方の心線を構成する導体10,11の撚り合
せらせんピツチと絶縁体16,17で被覆した他
方の心線を構成する導体12,13の撚り合せら
せんピツチとを同じP1として管20,21に収
納し、この管20,21を導体10,11と導体
12,13の二対の撚り合せピツチがP2となる
ように撚り合せて管22に収納したものである。 In the embodiment shown in FIG. 6, a twisted spiral pitch of conductors 10 and 11 constituting one core wire covered with insulators 14 and 15 and a conductor 12 constituting the other core wire covered with insulators 16 and 17 are shown. . _ They are twisted together and stored in a tube 22.
第4図〜第6図のケーブルの使用に際しては、
例えば第7図に示すように、導体10,11及び
導体12,13間を結線し、2対の導体間に発振
器Pの出力を接続する。 When using the cables shown in Figures 4 to 6,
For example, as shown in FIG. 7, conductors 10 and 11 and conductors 12 and 13 are connected, and the output of the oscillator P is connected between the two pairs of conductors.
第8図は本発明の別の実施例の外観図であり、
一方の心線を構成する導体30と他方の心線を構
成する導体31を被覆する絶縁体32,33の外
径をピツチP2で変化させ、且つこのような絶縁
体32,33を被覆した導体30,31を互いに
P1で撚り合せたものである。 FIG. 8 is an external view of another embodiment of the present invention,
The outer diameters of the insulators 32, 33 that cover the conductor 30 constituting one core wire and the conductor 31 constituting the other core wire are varied at pitch P2 , and such insulators 32, 33 are coated. conductors 30 and 31 to each other
It is made by twisting P1 .
第9図は本発明の更に別の実施例の外観図であ
り、絶縁体40,41にピツチP1の溝を形成し
てその中に一方の心線を構成する導体42と他方
の心線を構成する導体43を収納し、且つ絶縁体
40,41をP2のピツチで撚り合せたものであ
る。 FIG. 9 is an external view of still another embodiment of the present invention, in which grooves of pitch P 1 are formed in insulators 40 and 41, and a conductor 42 constituting one core wire and a conductor 42 constituting the other core wire are formed in the insulators 40 and 41. The conductor 43 constituting the structure is housed, and the insulators 40 and 41 are twisted together at a pitch of P2 .
発明の効果
以上説明したように、本発明によれば、ケーブ
ルにP1,P2の異なる周期を持たせるように構成
したので、製造の都合上導体のらせんピツチに上
限があつても、その上限以下の二つの異なるピツ
チP1,P2によりケーブルに任意の周期を持たせ
ることが可能となる。従つて、製造が極めて容易
になるものである。また、異なる二つのピツチを
それぞれ独立に所望の放射周波数帯に合わせて設
定すれば、任意の異なる二つの放射周波数帯を得
ることができ、別々の使用者が一つのケーブルを
共用できる効果もある。Effects of the Invention As explained above, according to the present invention, since the cable is configured to have different periods P 1 and P 2 , even if there is an upper limit to the helical pitch of the conductor due to manufacturing reasons, By using two different pitches P 1 and P 2 that are below the upper limit, it is possible to give the cable an arbitrary period. Therefore, manufacturing becomes extremely easy. In addition, by setting two different pitches independently to match the desired radiation frequency band, it is possible to obtain any two different radiation frequency bands, which also has the effect of allowing different users to share one cable. .
第1図〜第3図は従来のらせん導体型漏洩ケー
ブルの説明図、第4図〜第6図、第8図及び第9
図は本発明のそれぞれ異なる実施例の説明図、第
7図は本発明のらせん導体型漏洩ケーブルの使用
方法を示す図である。
10〜13,30,31,42,43は導体、
14〜17,32,33,40,41は絶縁帯で
ある。
Figures 1 to 3 are explanatory diagrams of conventional spiral conductor type leaky cables, Figures 4 to 6, Figures 8 and 9.
The figures are explanatory diagrams of different embodiments of the present invention, and FIG. 7 is a diagram showing how to use the helical conductor type leaky cable of the present invention. 10 to 13, 30, 31, 42, 43 are conductors,
14 to 17, 32, 33, 40, and 41 are insulating bands.
Claims (1)
て使用される2組の心線から成り、各心線はそれ
ぞれ1本ないし2本の導体から成り、ケーブル全
体に二つのそれぞれ異なる周期を持たせたことを
特徴とするらせん導体型漏洩ケーブル。1. In a helical conductor type leaky cable, it consists of two sets of core wires used as a pair, each core wire consists of one or two conductors, and the entire cable has two different periods. Features a spiral conductor type leaky cable.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14744083A JPS6038902A (en) | 1983-08-12 | 1983-08-12 | Spiral conductor type leakage cable |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14744083A JPS6038902A (en) | 1983-08-12 | 1983-08-12 | Spiral conductor type leakage cable |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6038902A JPS6038902A (en) | 1985-02-28 |
JPH0376602B2 true JPH0376602B2 (en) | 1991-12-06 |
Family
ID=15430382
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP14744083A Granted JPS6038902A (en) | 1983-08-12 | 1983-08-12 | Spiral conductor type leakage cable |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6038902A (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE3617899A1 (en) * | 1986-05-29 | 1987-12-17 | Hitachi Cable | INDUCTIVE RF ANTENNA CABLE |
FR2771859B1 (en) * | 1997-11-28 | 1999-12-31 | Telecommunications Sa | RADIANT CABLE |
-
1983
- 1983-08-12 JP JP14744083A patent/JPS6038902A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS6038902A (en) | 1985-02-28 |
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