JP2525151B2 - Telescopic antenna - Google Patents

Telescopic antenna

Info

Publication number
JP2525151B2
JP2525151B2 JP61151528A JP15152886A JP2525151B2 JP 2525151 B2 JP2525151 B2 JP 2525151B2 JP 61151528 A JP61151528 A JP 61151528A JP 15152886 A JP15152886 A JP 15152886A JP 2525151 B2 JP2525151 B2 JP 2525151B2
Authority
JP
Japan
Prior art keywords
antenna
coil
antenna element
different
length
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
JP61151528A
Other languages
Japanese (ja)
Other versions
JPS639204A (en
Inventor
昇三 斎藤
宗二 真島
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 Antenna Co Ltd
Original Assignee
Nippon Antenna Co Ltd
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 Antenna Co Ltd filed Critical Nippon Antenna Co Ltd
Priority to JP61151528A priority Critical patent/JP2525151B2/en
Publication of JPS639204A publication Critical patent/JPS639204A/en
Application granted granted Critical
Publication of JP2525151B2 publication Critical patent/JP2525151B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Details Of Aerials (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は移動可搬式の送受信機器等の伸縮式アンテナ
に係わり、アンテナの外部構成を合成樹脂などの絶縁材
によってテレスコープ状に形成し、その内部にコイル状
アンテナ素子を挿通して伸縮範囲でアンテナの電気長を
変化させて複数の周波数帯の送受信を広帯域に亘って可
能にした伸縮式アンテナの提供にある。
DETAILED DESCRIPTION OF THE INVENTION (Industrial field of application) The present invention relates to a telescopic antenna such as a mobile portable transmitter / receiver device, in which the external configuration of the antenna is formed in a telescope shape by an insulating material such as synthetic resin, Another object of the present invention is to provide a telescopic antenna in which a coiled antenna element is inserted to change the electric length of the antenna within a telescopic range to enable transmission and reception of a plurality of frequency bands over a wide band.

(従来の技術) 移動可搬式のラジオ、テレビ、無線機等の送受信機器
に用いられている伸縮式アンテナとしては金属管による
通常ロッドアンテナが周知、公知のものである。いわゆ
る黄銅などの異径金属管をクロームメッキ等の表面処理
し、各異径管材相互間に金属質弾性部材を介装して伸縮
可能にしたものが一般的であり、単一周波数の送受信時
に伸長させ、使用しない場合は縮小させキャビネットな
どに収納させるものである。
(Prior Art) As a telescopic antenna used in a transmitting / receiving device such as a mobile radio, a television, and a radio, a rod antenna using a metal tube is well known and well known. It is common to use a different diameter metal tube such as so-called brass with a surface treatment such as chrome plating, and to expand and contract by interposing a metallic elastic member between each different diameter tube material when transmitting and receiving a single frequency. When it is not used, it is extended and then reduced and stored in a cabinet or the like.

又、このような構成関係で応用したものに実公昭44−
20097号公報或は実公昭54−19804号公報のようにコイル
状としたアンテナ素子を用いたものがある。前者のもの
は絶縁物の異径管材各々にコイル状導線を埋装し、ロッ
ドアンテナ同様に組付けたもの、後者は絶縁物の異径管
材の内にコイルスプリングによって無線機から突出させ
て使用するいわゆる飛出式アンテナである。このものは
コイルスプリングの弾性力作用によるもので絶縁管材は
単なるスプリングカバーとしたものである。又、本願出
願人はコイル状アンテナを金属細線によって形成し、伸
縮操作に追動できるよう弾発作用の少ないものを用い、
その外部構成を絶縁材で異径管材に形成し、該異径管材
を組付けたとき一連の管材相互間に円周方向における回
動阻止手段を構成し、金属細線によるコイル状アンテナ
素子に機械的にも電気的にも安定した機構を提供してい
る。
In addition, the one applied with such a configuration relationship is
There is one using a coiled antenna element as in 20097 or Japanese Utility Model Publication No. 54-19804. The former one is one in which coil-shaped conductors are embedded in each different diameter pipe material of an insulator and is assembled in the same way as a rod antenna, and the latter is used by being protruded from the wireless device by a coil spring in the different diameter pipe material of an insulator. This is a so-called pop-out type antenna. This is due to the elastic force of the coil spring, and the insulating pipe material is simply a spring cover. In addition, the applicant of the present application forms the coiled antenna with a thin metal wire, and uses one having a small elastic action so as to follow the expansion and contraction operation,
The external structure is formed of a different diameter pipe material with an insulating material, and when the different diameter pipe material is assembled, a rotation preventing means in the circumferential direction is formed between a series of pipe materials, and a coil-shaped antenna element made of a thin metal wire is used as a machine. It provides a stable mechanism both physically and electrically.

(発明が解決しようとする問題点) 上記したコイル状のアンテナ素子を用いたいずれのも
のもロッドアンテナと比べ、短小にまとめ電気長を大き
くした短縮アンテナであるが、所定の単一周波数又は低
いか高いかの何れかである狭帯域に対してのみ送受信を
目的としたもので、コイル状アンテナ素子のコイルピッ
チはいずれも等間隔としたものであり、金属ロッドと同
様に送受信時に伸長させ、使用しない場合は縮小させる
もので、低い周波数から高い周波数までを送受信させる
ことは困難であり、特に近年のFM帯からテレビ帯までの
広帯域を受信する機器などにおいては好ましい受信をな
し得ない。
(Problems to be Solved by the Invention) Any of the antennas using the above-mentioned coiled antenna element is a shortened antenna in which the electrical length is increased in a short size as compared with the rod antenna, but a predetermined single frequency or low It is intended for transmission and reception only for a narrow band that is either high or high, and the coil pitch of the coiled antenna element is set at equal intervals, and it is extended during transmission and reception like a metal rod, If it is not used, it is reduced, and it is difficult to transmit / receive from a low frequency to a high frequency. Especially, it is not possible to achieve preferable reception in a device which receives a wide band from the FM band to the TV band in recent years.

(問題点を解決するための手段) テレスコープ状に伸縮可能として組付けられた複数の
異径管状を合成樹脂などの絶縁材による成形体として夫
々形成し、これら一連の異径管材を樹脂質接合片で摺動
可能にすると共に該異径管材相互間には円周方向に回動
阻止を図る手段を形成して組付け、最上段管材から最下
段管材までの内部空間にコイル状アンテナ素子を挿通し
て両端部を夫々固定して成る伸縮式アンテナにおいて、
前記コイル状アンテナ素子は空間素子長を中間状態に縮
小した場合にコイルピッチが殆んど変化しない疏巻状の
基端側と、コイルピッチが優先的に変化する密巻状の先
端側とによって形成されたことを特徴とする伸縮式アン
テナ。
(Means for solving the problem) A plurality of different-diameter pipes that are telescopically assembled so that they can be expanded and contracted are each formed as a molded body made of an insulating material such as synthetic resin. A coil-shaped antenna element is provided in the internal space from the uppermost pipe member to the lowermost pipe member, which is slidable by a joining piece and has means for preventing rotation in the circumferential direction formed between the different diameter pipe members. In a telescopic antenna that is inserted through and fixed at both ends,
The coiled antenna element has a coiled base end side where the coil pitch hardly changes when the spatial element length is reduced to an intermediate state, and a close coiled tip end side where the coil pitch changes preferentially. A telescopic antenna characterized by being formed.

(作用) 異径管材を合成樹脂などの絶縁材で形成することによ
り形状や軽量化を図るだけでなく、送受信機や取付ける
対象物などにマッチした多様な美観性をもたらした色彩
を採用することも可能であり、又近年の新素材である樹
脂材をもって成形したものは、可撓性に優れ、金属ロッ
ドのように屈曲破損を生じるものと異り、可曲作用によ
り屈曲にも充分耐えるなどの特徴を有するもので、コイ
ル状アンテナ素子を機械的に保護するカバーとしても充
分作用するから該アンテナ素子を金属細線で形成するこ
とも可能となる。即ちアンテナ素子自体には強力な弾圧
力を求めるものでないから異径管材相互間における伸縮
操作に対して実質的にその伸縮を阻害するような抵抗作
用(弾発的作用)を示すことのない金属細線でよい。し
かも、コイル状にした素子の構成を本発明のものは、第
1図に示すように給電点となる導電性保持具7に接続さ
れる基端側を疎巻状に、先端側を密巻状にそれぞれ形成
しその双方において異なった処理をなしたものを異径管
材1、2、3、……による伸縮管内に挿通し密巻端をト
ップ飾り玉9などで固定し、伸縮範囲でコイルのピッチ
変化を行なわしめることにより巻線間静電分布容量(以
下単に分布容量という)が先端側と基端側とが異なった
状態で変化するので、アンテナ電流の分流状態が変り、
実質的なアンテナの電気長が広範囲に変化するので広帯
域特性に優れた伸縮式アンテナとなり得る。
(Function) Not only does the shape and weight be reduced by forming the different-diameter pipe material with an insulating material such as synthetic resin, but also adopts colors that bring about various aesthetics that match the transceiver and the object to be attached. It is also possible, and the one molded with a resin material, which is a new material in recent years, is excellent in flexibility and unlike a metal rod that causes bending damage, it can withstand bending due to a bending effect etc. Since it also has a feature as described above, and it sufficiently acts as a cover for mechanically protecting the coiled antenna element, it is possible to form the antenna element with a thin metal wire. That is, since the antenna element itself does not require a strong elastic force, a metal that does not exhibit a resistance action (elasticity action) that substantially impedes expansion and contraction between pipe members of different diameters. Fine lines are fine. Moreover, in the structure of the coiled element of the present invention, as shown in FIG. 1, the base end side connected to the conductive holder 7 serving as a feeding point is sparsely wound and the tip end side is closely wound. Inserted into the expandable tube with different diameter pipes 1, 2, 3, ... by forming different shapes on both sides, and fixing the close winding end with the top decorative ball 9 etc. By changing the pitch of, the distributed capacitance between windings (hereinafter simply referred to as distributed capacitance) changes with the tip side and the base side different, so the shunt state of the antenna current changes,
Since the substantial electrical length of the antenna varies over a wide range, the antenna can be a telescopic antenna having excellent broadband characteristics.

なお本発明において用いる空間素子長を中間状態に縮
小した場合にコイルピッチが殆んど変化しない疏巻状の
基端側と、コイルピッチが優先的に変化する密巻状の先
端側とによって形成されたコイル状アンテナ素子は、疏
巻状の基端側に焼入れし、あるいはこの疏巻状の基端側
の線材を大径としたものによるコイルとすることの如き
に得られることは当然であるが、焼入などの処理を含め
て同一材質且つ同一径の線材によるコイルであっても一
旦密巻状部分として屈曲成形したものの一半部を疏巻状
に伸ばしてもその密巻部と疏巻部を一体に形成したコイ
ルの長さ方向に圧縮力を作用させたならば、密巻部が優
先的に圧縮変形してコイルピッチがほぼ密着状で、つま
り、管体状導体となるのに対し、疏巻部がコイルピッチ
が殆んど変化しないものとなることは実験的に容易に確
かめられ、本発明ではこのような何れかのコイルを採用
するものである。
In addition, when the spatial element length used in the present invention is reduced to an intermediate state, it is formed by a coiled base end side where the coil pitch hardly changes and a close coiled tip side where the coil pitch changes preferentially. It is natural that the coiled antenna element thus obtained can be obtained by quenching the coiled base end side, or by using a coil having a large diameter wire on the coiled base end side. However, even if it is a coil made of wire material of the same material and the same diameter, including hardening, etc., even if one half of the coil that has been bent and formed as a tightly wound portion is stretched into a leap shape, If a compressive force is applied in the length direction of the coil having the winding portion integrally formed, the close winding portion is preferentially compressed and deformed so that the coil pitch is substantially in close contact, that is, a tubular conductor is formed. On the other hand, the coil pitch of the leap winding part hardly changes. Be made as ascertained readily experimentally, the present invention is intended to employ any such coil.

(実施例) 本発明によるコイル状アンテナ素子(以下アンテナ素
子という)の電気的作用を第9図に示す実施例について
具体的に説明すると、Wはコイル状に巻回してアンテナ
素子を構成する金属細線の長さを示し、Aは異径管材の
伸縮に追動するアンテナ素子のP・T間の空間素子長を
示し、Lは該アンテナ素子の電気長を示し、lは疎・密
それぞれの巻回部分で伸縮追動によって変化する各部分
の電気長を示し、Cはコイルの線間分布容量、Iは電流
分布最大値、Pは高周波電源の給電点をそれぞれ示す。
(Embodiment) The electrical action of the coiled antenna element (hereinafter referred to as an antenna element) according to the present invention will be specifically described with reference to the embodiment shown in FIG. 9. W is a metal that is wound into a coil to form an antenna element. The length of the thin wire is shown, A is the spatial element length between P and T of the antenna element which follows the expansion and contraction of the different diameter pipe material, L is the electrical length of the antenna element, and l is the sparse and dense The electrical length of each part of the winding part which changes due to expansion and contraction is shown. C is the distributed capacitance between the coils, I is the maximum value of the current distribution, and P is the feeding point of the high frequency power source.

アンテナとして作用説明するには第10図に示すように
λ/2の素子長の中央より給電するダブレットアンテナで
行うのが標準的であるが、本発明の第9図に示すものは
ダブレットアンテナの片方を図示したとみなし、λ/4の
素子長を形成したものとして説明する。
To explain the operation as an antenna, it is standard to use a doublet antenna that feeds from the center of the element length of λ / 2 as shown in FIG. 10. However, the doublet antenna shown in FIG. It is assumed that one is shown, and the description will be made assuming that the element length of λ / 4 is formed.

全伸長時 第9図(a)に示すアンテナ素子の空間素子長A1が外
部異径管材によるカバーを最大に伸長させた場合に該カ
バーの両端に固定されたP・T間に疏巻状部分W1と密巻
状部分W2によって形成する。全伸長時の場合ではW2は充
分伸長されることによりコイルの線間分布容量は極めて
小さくC1≒C2≒0の関係を生ずる。即ちアンテナ電流は
殆んどW1、W2部分を流れるので、電気長はl≒W1、l2≒W1
となり、空間素子長A1の電気長はL1(=l1+l2)≒W
(=W1+W2)であるから、共振波長λに対して電気長L
の関係はλ=4L、 によって、 λ1=4L1の関係が成立する。要するにアンテナ素子A1は電気長L1
≒Wで最大となり、最長波長即ち最低周波数に共振する
こととなる。例えば、A1=60cmでW=1mとした場合はλ
1=4m、f1=75MHzに共振することになる。
At full extension When the spatial element length A 1 of the antenna element shown in Fig. 9 (a) is extended to the maximum extent by a cover made of a pipe with a different diameter, a coil-like shape is formed between P and T fixed to both ends of the cover. It is formed by the portion W 1 and the close-wound portion W 2 . In the case of full extension, W 2 is sufficiently extended, so that the distributed capacitance between the coils is extremely small, and the relationship of C 1 ≈C 2 ≈0 occurs. That is, since the antenna current almost flows through the W 1 and W 2 portions, the electrical length is l≈W 1 , l 2 ≈W 1
Therefore, the electrical length of the spatial element length A 1 is L 1 (= l 1 + l 2 ) ≈W
Since (= W 1 + W 2 ), the electrical length L for the resonance wavelength λ
Relationship is λ = 4L, Λ 1 = 4L 1 , The relationship is established. In short, the antenna element A 1 has an electrical length L 1
It becomes maximum when ≈W, and resonates at the longest wavelength, that is, the lowest frequency. For example, if A 1 = 60 cm and W = 1 m, then λ
It will resonate at 1 = 4 m and f 1 = 75 MHz.

中伸長時 第9図(b)に示すアンテナ素子の空間素子長A2は第
2図に示す実施例のように一段縮小したような状態であ
って、空間素子長A2において疏巻状部分W1のピッチは殆
んど変化せずl3≒W1≒l1の状態に保持されるが、密巻状
部分W2のコイルピッチのみが優先的に縮小され、W2の分
布容量はC4>>C2の関係となり、アンテナ電流の大半が
C4側に分流されて、W2には殆んど流れず、その結果W2
分の電気長はl4<<l3となり、従ってアンテナ素子A2
関しての電気的作用は殆んどW1部分のみで行われること
となるのでその電気長L2はl3により決定され、つまりL2
<L1の関係を得る。λ2=4L2からf2>f1となり、f1より高い周波数で共振することに
なる。例えば、A2=30cm、W1=40cmとするならば、λ2
=1.6m、f2=187.5MHzに共振することになる。
At middle extension The spatial element length A 2 of the antenna element shown in FIG. 9 (b) is in a state of being further reduced as in the embodiment shown in FIG. 2 , and the coil-shaped portion at the spatial element length A 2 The pitch of W 1 hardly changes and is maintained in the state of l 3 ≈ W 1 ≈ l 1 , but only the coil pitch of the close-wound portion W 2 is reduced preferentially, and the distributed capacitance of W 2 is Due to the relationship of C 4 >> C 2 , most of the antenna current
Is shunted to C 4 side not flow almost to W 2, the result W electrical length of 2 parts l 4 << l 3, and the thus electric action with respect to the antenna element A 2 is殆Ndo W Since it is done in only one part, its electrical length L 2 is determined by l 3 , that is, L 2
<Get the relationship of L 1 . λ 2 = 4L 2 , Therefore, f 2 > f 1 and resonance occurs at a frequency higher than f 1 . For example, if A 2 = 30 cm and W 1 = 40 cm, then λ 2
= 1.6m, and f 2 = 187.5MHz.

全縮小時 第9図(c)に示すアンテナ素子の空間素子長A3は第
3図に示す実施例のように最下段管材に全て収納させた
ような状態であって、アンテナ素子A3は伸長時、中間伸
長時に疏巻状部分であったW1と密巻状部分W2とがこの収
納された状態において、共に圧縮され、つまり全コイル
Wがほぼ密着状態となり、管体状導体を形成する。すな
わちコイルピッチがほぼ密着されることで電気的には殆
んど短絡されて1本のパイプ状態と見なせるので、その
結果L3≒A3で最短になる。従ってその電気長L3<L2の関
係を得るので、λ3=4L3からf3>f2の関係が得られ、f2より更に高い周波数で共
振することになり得る。例えば、A3=15cmとすればλ3
=60cm、f3=500MHzに共振することになる。
Spatial element length A 3 of the antenna element shown in full reduction at Figure 9 (c) is a state as is housed all the bottom tube member as in the embodiment shown in FIG. 3, the antenna element A 3 is At the time of extension, W 1 and the close-wound portion W 2 which were the coil-wound portion at the time of intermediate extension are compressed together in this housed state, that is, all the coils W are in a close contact state, and the tubular conductor is Form. That is, since the coil pitches are closely contacted with each other, they are electrically short-circuited and can be regarded as a single pipe state. As a result, L 3 ≈A 3 is the shortest. Therefore, we obtain the relation of electric length L 3 <L 2 , so λ 3 = 4L 3 , Therefore, the relationship of f 3 > f 2 is obtained, and the resonance can occur at a frequency higher than f 2 . For example, if A 3 = 15 cm, then λ 3
It resonates at 60 cm and f 3 = 500 MHz.

以上説明したことにより、外部異径管材によって伸縮
追動するアンテナ素子は空間素子長A1>A2>A3の変化率
以上に電気長L1>L2>L3の変化率が大きくなり、従って
小形化にして広帯域の周波数に共振するアンテナが得ら
れ、しかも、アンテナ素子を疏巻状部分と密巻状部分で
形成した本発明のものは第11図に示すように共振周波数
の全帯域に対しても給電点インピーダンスを正常値に保
持し、アンテナの電気的作用が低下せぬように考慮した
ものである。又、原理的には均等のピッチのコイル状と
したアンテナ素子でも順応し得る。
From the above explanation, the antenna element that expands and contracts by the pipe with different diameter has a larger rate of change of electrical length L 1 > L 2 > L 3 than the rate of change of spatial element length A 1 > A 2 > A 3. Therefore, it is possible to obtain an antenna which is miniaturized and resonates in a wide band frequency, and moreover, the antenna element of the present invention in which the antenna element is formed by the coiled portion and the tightly coiled portion has all resonance frequencies as shown in FIG. This is because the impedance of the feeding point is kept at a normal value even for the band so that the electric action of the antenna is not degraded. In principle, a coiled antenna element having a uniform pitch can be adapted.

以上説明したものはλ/4の素子長で行ったが、λ/4以
外にも所望する波長に対しても共振するものである。
What has been described above is performed with an element length of λ / 4, but it is possible to resonate with a desired wavelength other than λ / 4.

上記したような本発明によるものの具体的実施態様を
添付図面に示すものについて説明すると、複数の異径管
材1、2、3、……を用い、これをテレスコープ状に相
互に伸縮可能で、しかも抜け出すことのないように連繋
せしめる機械的構成関係自体は従来から知られている一
般的伸縮アンテナと同じであるが、本発明においては一
連の異径管材1、2、3、……がアンテナ素子として用
いられるものでなく、従って一般的に合成樹脂成形材で
あることにおいて本質を異にしたものであり、別なるコ
イル状アンテナ素子6を用い、このコイル状アンテナ素
子6の一端を上記一連の異径管材1、2、3、……にお
ける最上段管材1の上端飾り玉9と固定し他端を最下段
3に導電性保持具7の段状突部71に挿着し、リング部材
8でそれぞれ固定し、伸縮可能とすると共に導電性保持
具7を介して送受信機器(図示せず)に接続される。
A specific embodiment of the present invention as described above will be described with reference to the accompanying drawings. A plurality of different-diameter pipe materials 1, 2, 3, ... In addition, the mechanical constitutional relation itself that can be connected so as not to come out is the same as that of a general telescopic antenna known from the past, but in the present invention, a series of different diameter pipe materials 1, 2, 3, ... Are antennas. It is not used as an element, and therefore has a different essence in that it is generally a synthetic resin molded material. Another coil-shaped antenna element 6 is used, and one end of this coil-shaped antenna element 6 is connected to the above-mentioned series. Of the different-diameter pipe materials 1, 2, 3, ... Are fixed to the upper end decorative ball 9 of the uppermost pipe material 1 and the other end is inserted into the lowermost step 3 into the stepped projection 71 of the conductive holder 7 to form a ring member. Fix each with 8 It is connected to the transceiver device (not shown) via a conductive retainer 7 with stretchable to.

以上のような構成に挿通されるコイル状アンテナ素子
6は境界部6aより導電性保持具7側の基端側を粗巻状部
61を形成し、先端側に至って密着状部62を形成し、第1
図に示す全伸長時には粗巻61と密着巻62が第9図(a)
で説明した通りの作用をする。第2図は中伸長時を示す
もので、同図は一段縮小したものであるが、伸縮範囲で
中間迄操作したものと同様で、第9図(b)で説明した
通りの作用をする。第3図は全縮小時つまり最下段管材
3に全てを収納した状態を示すもので伸長時に粗巻状部
61であったコイルは密巻状部62と同様に密着状を形成し
両部分61、62が管体状を形成し、第9図(c)で説明し
た通りの作用となる。
In the coil-shaped antenna element 6 which is inserted in the above-described configuration, the base end side closer to the conductive holder 7 than the boundary portion 6a is a rough winding portion.
61 to form a contact-like portion 62 reaching the tip side, and
Coarse winding 61 and contact winding 62 are shown in Fig. 9 (a) during full extension shown in the figure.
It works as described in. FIG. 2 shows a state of middle extension, which is reduced by one step, but it is the same as that operated to the middle in the expansion / contraction range, and operates as described in FIG. 9 (b). FIG. 3 shows a state in which all the parts are retracted, that is, all are accommodated in the lowermost tube material 3.
The coil, which is 61, forms a close contact like the densely wound portion 62, and both portions 61, 62 form a tubular shape, which has the same effect as described in FIG. 9 (c).

前記のように管材1、2、3、……の伸縮に対してコ
イル状アンテナ素子6は金属細線で形成することで伸縮
操作に対して実質的に抵抗作用(いわゆる弾発的作用)
を示すことはない。
As described above, the coiled antenna element 6 is formed of a thin metal wire against expansion and contraction of the tube members 1, 2, 3, ..., Thus, the expansion and contraction operation is substantially resistant (so-called elastic effect).
Is not shown.

更に上記したような異径管材1、2、3、……には円
周方向の回動阻止を図る構造としたもので第4図に示す
ように最下段管材3以外の管材1、2における下端側に
は係合孔10を設け、このような下端部に第5図に示すよ
うな合成樹脂質接合片11を取付ける。最上段管材1以外
の異径管材2、3、……の上端は内側に屈曲させた狭窄
部を形成し、管材内面には軸方向にそって係合条2a又は
3aが形成され、該係合条2a又は3aは前記した接合片11の
両側端縁14、14間に形成された間隙に嵌合される。よっ
て異径管材1、2、3、……を接合片11などで組付けた
ものは伸縮操作に拘わらず円周方向において回動するこ
とがなく、従ってコイル状アンテナ素子6は常に一定し
た関係を維持する。又、異径管材1、2、3、……は多
角状の管材を用い、それに即応した接合片11を用いるこ
とによって係合条2a又は3a……の間隙部なしでも実施で
きる。又接合片11部材は管材同様合成樹脂質たることに
よりして溶着などの手段によってよいことは勿論であ
る。
Further, the different-diameter pipe materials 1, 2, 3, ... As described above have a structure for preventing rotation in the circumferential direction, and as shown in FIG. An engaging hole 10 is provided on the lower end side, and a synthetic resin joining piece 11 as shown in FIG. 5 is attached to such a lower end portion. The upper ends of the different-diameter pipe materials 2, 3, ... Other than the uppermost-stage pipe material 1 form a narrowed portion that is bent inward, and the inner surface of the pipe material has an engagement line 2a or
3a is formed, and the engaging strip 2a or 3a is fitted in the gap formed between the both side edges 14 of the joining piece 11. Therefore, the pipes 1 having different diameters 1, 2, 3, ... Assembled by the joining piece 11 do not rotate in the circumferential direction regardless of the expansion and contraction operation, and therefore the coiled antenna element 6 has a constant relationship. To maintain. Further, the different-diameter pipe materials 1, 2, 3, ... Are made of polygonal pipe materials, and by using the joining piece 11 adapted to them, it is possible to carry out without a gap portion of the engaging strips 2a or 3a. Further, it goes without saying that the joining piece 11 member may be made of a synthetic resin material like the pipe material and may be welded or the like.

保持具7へのコイル状アンテナ素子6の固定は半田づ
けの如きであっても充分である。
The coiled antenna element 6 may be fixed to the holder 7 by soldering or the like.

このようなコイル状アンテナ素子6は必要なアンテナ
線長Lをコイル状とすることにより素子長Aが短縮さ
れ、金属管ロッドアンテナに較べ素子長が相当に短いも
の、例えば50〜60%程度の長さにしても低い共振周波数
から高い共振周波数までの広帯域送受信特性を有するの
でロッドアンテナ以上の優れたものが得られる。
In such a coiled antenna element 6, the element length A is shortened by making the required antenna wire length L into a coil shape, and the element length is considerably shorter than that of the metal tube rod antenna, for example, about 50 to 60%. Even if it has a length, it has a wideband transmission / reception characteristic from a low resonance frequency to a high resonance frequency, so that it is more excellent than a rod antenna.

異径管材1、2、3、……が合成樹脂パイプの如きで
あるからして、適用される送受信機器あるいは取付部体
の色彩と有効に調和したカラーおよび各種の模様等を実
現し、伸縮回数が増大しても金属ロッドアンテナのよう
なめっき剥げなどもなく、軽量でしかも可撓性に優れ、
従来のこの種のアンテナとは機械的電気的いずれもが勝
り、且つ美観性を有するアンテナである。
Since the different-diameter pipe materials 1, 2, 3, ... Are like synthetic resin pipes, they can achieve colors and various patterns that are in harmony with the colors of the applicable transmitter / receiver device or mounting part, and expand and contract. Even if the number of times increases, there is no plating peeling like a metal rod antenna, light weight and excellent flexibility,
The conventional antenna of this type is an antenna that is superior in both mechanical and electrical properties and has an aesthetic appearance.

第11図に示すものは、本発明のアンテナを実施した場
合のものと、従来のロッドアンテナとを同じ長さで実測
した特性の比較を行ったものである。
FIG. 11 shows a comparison between the characteristics when the antenna of the present invention is implemented and the conventional rod antenna, which are actually measured with the same length.

この特性表はFMラジオ受信帯(76〜90MHz)とテレビ
受信帯(90〜108MHz)(170〜222MHz)において本発明
によるものを90MHz近傍に共振周波数を採った伸長時
と、190〜200MHz近傍に共振周波数を採った縮小時の長
さをそれぞれロッドアンテナ(点線で示す)と同じ長さ
で実測したものであり、本発明のものは共振周波数の全
帯域にVSWR、利得共に変化の少ない優れた特性であるに
対してロッドアンテナは変化の大きい特性となり、ロッ
ド長を送受信周波数が変わる度にその都度変えなければ
ならず、更に低い周波数帯に対してはロッド長は長いも
のとならざるを得ない。
This characteristic table shows that according to the present invention in the FM radio reception band (76 to 90 MHz) and the television reception band (90 to 108 MHz) (170 to 222 MHz) when the resonance frequency is extended to around 90 MHz and when it is expanded to around 190 to 200 MHz. The lengths of the resonance antennas at the time of reduction are actually measured with the same length as the rod antenna (shown by the dotted line). The present invention is excellent in that both VSWR and gain are small in the entire resonance frequency band. In contrast to the characteristics, the rod antenna has a large variation, and the rod length must be changed each time the transmission / reception frequency changes, and the rod length must be long for a lower frequency band. Absent.

(発明の効果) 以上説明したように本発明は従来この種の伸縮アンテ
ナについてのイメージを大きく改革した新たな製品を提
供することができる。
(Effects of the Invention) As described above, the present invention can provide a new product in which the image of a conventional telescopic antenna of this type has been greatly reformed.

1)合成樹脂質で成形した管材を用いることで、適用さ
れる取付部(送受信機器或いは車体など)のデザインや
色彩にマッチした色調の選択自在、形状(丸型、角型な
ど)が容易に得られる。
1) By using a pipe material molded from synthetic resin, it is easy to select the color tone that matches the design and color of the mounting part (transmission / reception device or vehicle body) to be applied, and the shape (round shape, square shape, etc.) can get.

2)可撓性や軽量性に優れた特徴を有し、移動可搬型ア
ンテナとして折損事故等も生じにくいものが得られる。
2) It is possible to obtain a mobile and portable antenna that has excellent characteristics of flexibility and light weight and is unlikely to cause breakage accidents.

3)伸縮操作のくりかえしによるめっき剥などのような
表面が変化することもなく長く使用しても表面変化を生
じない。
3) The surface does not change such as plating removal due to repeated expansion and contraction operations, and the surface does not change even after long use.

4)伸縮範囲の選択で実質的に電気長の変化が得られる
もので広帯域に亘って周波数が任意となり得る送受信範
囲が増大する。
4) By selecting the expansion / contraction range, the electrical length can be substantially changed, and the transmission / reception range in which the frequency can be arbitrary over the wide band is increased.

しかも組立ても簡易であり充分低コスト化も得しめる
と共に安定且つ広帯域に亘って優れた特性を有してお
り、工業的にその効果の大きい発明である。
Moreover, the invention is industrially effective because it is easy to assemble, can be manufactured at a sufficiently low cost, and has stable and excellent characteristics over a wide band.

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

図面は本発明の実施態様の1例と電気的作用を示すもの
であって、第1図は本発明による全伸長時の状態を示し
た断面図、第2図は中伸長状態を示した断面図、第3図
は全縮小を示した断面図、第4図〜第8図は異径管材及
び接合片等の構成部材図、第9図は電気的作用説明図、
第10図はインピーダン特性図、第11図はダブレットアン
テナ図、第12図は実測比較特性図である。 図中において1、2、3は合成樹脂製異径管材、6はコ
イル状アンテナ素子、7は導電性保持具、9は飾り玉を
示すものである。
The drawings show an example of an embodiment of the present invention and an electric action. FIG. 1 is a sectional view showing a state at the time of full extension according to the present invention, and FIG. 2 is a sectional view showing an intermediate extension state. Fig. 3, Fig. 3 is a sectional view showing a full reduction, Fig. 4 to Fig. 8 are constituent member diagrams such as pipe members with different diameters and joint pieces, and Fig. 9 is an explanatory view of electrical action.
FIG. 10 is an impedance characteristic diagram, FIG. 11 is a doublet antenna diagram, and FIG. 12 is a measured comparison characteristic diagram. In the figure, reference numerals 1, 2, and 3 denote different diameter pipes made of synthetic resin, 6 a coiled antenna element, 7 a conductive holder, and 9 a decorative ball.

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】テレスコープ状に伸縮可能として組付けら
れた複数の異径管状を合成樹脂などの絶縁材による成形
体として夫々形成し、これら一連の異径管材を樹脂質接
合片で摺動可能にすると共に該異径管材相互間には円周
方向に回動阻止を図る手段を形成して組付け、最上段管
材から最下段管材までの内部空間にコイル状アンテナ素
子を挿通して両端部を夫々固定して成る伸縮式アンテナ
において、前記コイル状アンテナ素子は空間素子長を中
間状態に縮小した場合にコイルピッチが殆んど変化しな
い疏巻状の基端側と、コイルピッチが優先的に変化する
密巻状の先端側とによって形成されたことを特徴とする
伸縮式アンテナ。
1. A plurality of different-diameter pipes, which are telescopically assembled so that they can be expanded and contracted, are each formed as a molded body made of an insulating material such as synthetic resin, and a series of these different-diameter pipe members are slid by resinous joint pieces. A means for preventing rotation in the circumferential direction is formed between the different-diameter pipe members and assembled, and the coil-shaped antenna element is inserted into the internal space from the uppermost pipe member to the lowermost pipe member and both ends are inserted. In the telescopic antenna in which the respective parts are fixed, the coil-shaped antenna element has a coil-shaped base end side in which the coil pitch hardly changes when the spatial element length is reduced to the intermediate state, and the coil pitch has priority. A telescopic antenna, characterized in that it is formed by a closely-wound tip end side that changes with time.
JP61151528A 1986-06-30 1986-06-30 Telescopic antenna Expired - Lifetime JP2525151B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61151528A JP2525151B2 (en) 1986-06-30 1986-06-30 Telescopic antenna

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61151528A JP2525151B2 (en) 1986-06-30 1986-06-30 Telescopic antenna

Publications (2)

Publication Number Publication Date
JPS639204A JPS639204A (en) 1988-01-14
JP2525151B2 true JP2525151B2 (en) 1996-08-14

Family

ID=15520483

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61151528A Expired - Lifetime JP2525151B2 (en) 1986-06-30 1986-06-30 Telescopic antenna

Country Status (1)

Country Link
JP (1) JP2525151B2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4847239U (en) * 1971-10-05 1973-06-21

Also Published As

Publication number Publication date
JPS639204A (en) 1988-01-14

Similar Documents

Publication Publication Date Title
US6031493A (en) Antenna for two frequency bands
JP2795825B2 (en) Antenna device
US4160979A (en) Helical radio antennae
AU731335B2 (en) A dual-frequency antenna
US6232925B1 (en) Antenna device
US3858220A (en) Tunable spiral dipole antenna
JPH10224139A (en) Dual frequency antenna
EP0964474A2 (en) Antenna device
JP2001521358A5 (en)
US6778149B2 (en) Composite antenna apparatus
GB2206243A (en) Dual-frequency helical antenna
US4460896A (en) Antenna with tunable helical resonator
JP2525151B2 (en) Telescopic antenna
US20090115685A1 (en) Dual band helical antenna with wide bandwidth
JPH1051223A (en) Antenna system
US20030117338A1 (en) Structure of helix antenna
JP2003087031A (en) Antenna
US4349825A (en) Antenna assembly for high frequency ranges
JPH08307130A (en) Portable radio equipment and antenna for the portable radio equipment
EP0389705A2 (en) Non-stationary antenna
JP2003087030A (en) Vehicle-mounted antenna
JP4629879B2 (en) Whip antenna and manufacturing method thereof
KR100441922B1 (en) Dual-band antenna and adjusting method of frequency thereon
EP1490926A1 (en) Dual band antenna
JPH09199917A (en) Antenna system