JPH01125003A - Reflector for yagi antenna - Google Patents
Reflector for yagi antennaInfo
- Publication number
- JPH01125003A JPH01125003A JP15677587A JP15677587A JPH01125003A JP H01125003 A JPH01125003 A JP H01125003A JP 15677587 A JP15677587 A JP 15677587A JP 15677587 A JP15677587 A JP 15677587A JP H01125003 A JPH01125003 A JP H01125003A
- Authority
- JP
- Japan
- Prior art keywords
- reflector
- elements
- short
- long
- stage
- 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.)
- Pending
Links
- 238000010586 diagram Methods 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 230000001360 synchronised effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
[発明の技術分野]
本発明は八木式アンテナの前方後方比(F/B )を大
きくとって、後方からの妨害波を防止することができる
八木式アンテナの反射器に関する。[Detailed Description of the Invention] [Technical Field of the Invention] The present invention provides a reflector for a Yagi antenna that has a large front-to-back ratio (F/B) and can prevent interference waves from the rear. Regarding.
[従来技術とその欠点]
テレビ放送の1視聴解消のために、多くのサテており、
チャンネル不足という問題がおきつつある。そこで周波
数を効率的に使用するテレビ同期放送の使用が検討され
ている。しかしテレビ同期放送を行なう場合における、
電波の干渉によるゴーストの発生という問題も大きな問
題となる。この問題を解決する一つの方法は、受信アン
テナを高性能化することである。[Prior art and its disadvantages] In order to eliminate the single viewing of TV broadcasts, many satays are used.
There is a growing problem of lack of channels. Therefore, the use of television synchronized broadcasting, which uses frequencies efficiently, is being considered. However, in the case of TV synchronized broadcasting,
Another major problem is the generation of ghosts due to radio wave interference. One way to solve this problem is to improve the performance of the receiving antenna.
[発明の目的]
本発明は上記の点に鑑みてなされたもので、その目的は
、アンテナの前方後方比(F/B)を改善することがで
きる八木式アンテナの反射器を提供することにある。[Object of the Invention] The present invention has been made in view of the above points, and its purpose is to provide a reflector for a Yagi antenna that can improve the front/back ratio (F/B) of the antenna. be.
[発明の要点]
八木式アンテナの反射器において、反射器を2段に構成
し、1段目は短い素子を2列とその上下に中央を開放し
た長い素子を各1列づつ並べ、2段目は前記反射素子の
長い素子と短い素子の位置を入替え1段目の後方の位置
に配置するようにして、アンテナの前方後方比(F/8
)を改善するようにしている。[Key Points of the Invention] In the reflector of the Yagi antenna, the reflector is configured in two stages, with two rows of short elements arranged in the first stage and one row each of long elements with the center open above and below it. The eyes are placed at the rear of the first stage by swapping the positions of the long and short reflective elements, and the antenna's front-to-back ratio (F/8
).
[発明の実施例]
以下口面を参照して本発明の一実施例に係わる八木式ア
ンテナの反射器について説明する。第1因はアンテナ全
体の形状を示しているもので、図面を貫くように20素
子の導波素子D1〜D2G、給電素子P1反射素子R1
〜R8が配設されている。導波素子D1〜020の半径
は0.3CIであり、導波素子D1の右方には給電素子
Pが一本配置されている。[Embodiments of the Invention] A reflector for a Yagi antenna according to an embodiment of the present invention will be described below with reference to the mouth side. The first factor shows the shape of the entire antenna, which includes 20 waveguide elements D1 to D2G, a feeding element P1, a reflecting element R1, and a feeding element P1.
~R8 are arranged. The radius of the waveguide elements D1 to 020 is 0.3 CI, and one feeding element P is arranged on the right side of the waveguide element D1.
ここで、 −反射素子R
1〜R4により反射器Aが構成され、ぢ
−′ 反射素子R4P〜
R8により反射器←Bが構成される。Here, - reflective element R
1 to R4 constitute a reflector A, and reflecting elements R4P to R8 constitute a reflector←B.
第2図(A)は1段目の反射器Aで、短い素子R2、R
3を2列とその上下に中央を開放して長い素子R1、R
4を各1列ずつ並べたものである。Figure 2 (A) shows the first stage reflector A, with short elements R2, R
3 with two rows and the center open above and below it, long elements R1, R
4 are arranged in one column each.
素子の長さはLl 4L2であり、長い素子R1゜R4
は使用周波数の約1波長、短い素子は約半波長である。The length of the element is Ll 4L2, and the long element R1°R4
is about one wavelength of the operating frequency, and the short element is about half a wavelength.
また、1段目の反射素子の間隔は中心から短い素子まで
6.2C−であり、中心から長い素子まで16.0cm
である。Also, the spacing between the first stage reflective elements is 6.2C- from the center to the shortest element, and 16.0cm from the center to the longest element.
It is.
また、第2図(A)は2段目の反射器Bであり、1段目
の反射器Aの右方9.OC−のところに配置される。そ
して、長い素子Re、R7を2列とし、その上下に短い
反射素子R5,R8を各1列ずつ並べたものである。す
なわち、反射器Aと反射器Bとは長い素子と短い素子の
位置を入替えたものである。反射素子の長さはL4〜L
3で、長い素子は使用周波数の約1波長、短い素子は使
用周波数の約半波長であり、反射素子の間隔は中心より
4.5と10.3C−である。Moreover, FIG. 2(A) shows the second stage reflector B, and the right part 9 of the first stage reflector A. It is located at OC-. The long elements Re and R7 are arranged in two rows, and the short reflective elements R5 and R8 are arranged one row each above and below. That is, reflector A and reflector B have long elements and short elements interchanged in position. The length of the reflective element is L4~L
3, the long element is about one wavelength of the operating frequency, the short element is about half a wavelength of the operating frequency, and the spacing between the reflective elements is 4.5 and 10.3 C- from the center.
次に、第2図(A)及び(B)に示した各反射器A、
B・、を第1図に示した様に、第1段若しくは第2段に
配列したときの周波数対F/Bのグラフを第3図及び第
4図に示しておく。ここで、周波数は給電素子の長さを
基準にKL(K−2π/λ)で表わし縦軸は120度〜
240度の方向の電界と最大放射電界強度(0方向)と
の比をデシベルで表わしである。ここで、指向性は左右
対称なため、120〜180度を2度おきにプロットし
てあり、この線群の最も小さい値を結んだものがF/B
を表わしている。Next, each reflector A shown in FIGS. 2(A) and (B),
FIGS. 3 and 4 show graphs of frequency versus F/B when F/B is arranged in the first or second stage as shown in FIG. 1. Here, the frequency is expressed as KL (K-2π/λ) based on the length of the feeding element, and the vertical axis is from 120 degrees to
The ratio between the electric field in the 240 degree direction and the maximum radiated electric field strength (0 direction) is expressed in decibels. Here, since the directivity is symmetrical, 120 to 180 degrees are plotted every 2 degrees, and the line connecting the smallest value of this line group is F/B.
It represents.
また、長い反射素子R1,R4と短い反射素子R2,R
3とを組合わせることにより、第3図に見られるような
急峻なピークを得ることができる。In addition, long reflective elements R1, R4 and short reflective elements R2, R
3, a steep peak as shown in FIG. 3 can be obtained.
また、反射器が一段でもF/Bが24d 8以上のF/
Bを得ることができるが、帯域はK L −1,65〜
1.80とノ狭い範囲しか満足していない。Also, even if the reflector is one stage, the F/B is 24d or more.
B can be obtained, but the band is K L −1,65 ~
It is only satisfied within a narrow range of 1.80.
また、KLが小さな場合にF/Bの大きなところが、1
20度方向であり、F/Bの小さなところが180度方
向で、殆んどF/Bは180度方向で決まっている。し
かし、K L −1,6付近からサイドロブが大きくな
ってきて複雑な指向性となる。ここで、反射素子の長さ
を給電素子の4倍程度に延してもF/Bは改善されない
。このように、反射素子1段の場合のF/B特性は24
dB以上となることは少なく、なったとしても狭い範囲
であった。Also, when KL is small, the area where F/B is large is 1
The direction is 20 degrees, and the point where F/B is small is the direction of 180 degrees, and most F/B is determined in the direction of 180 degrees. However, the side lobe becomes large from around K L -1,6, resulting in complicated directivity. Here, even if the length of the reflective element is extended to about four times the length of the feeding element, F/B is not improved. In this way, the F/B characteristic in the case of one stage of reflective elements is 24
It rarely exceeded dB, and even if it did, it was within a narrow range.
そこで、反射器A、Bを第2図(A)、(B)のように
取付け、長さの違う反射器A、Bを立体的に配置するこ
とによって、180度F/Bに2つのピークができ、高
いF/Bを広い周波数範囲で得ることができる( K
L −1,55〜2.20) 、従って、UHFテレビ
に用いる場合にはLM帯域用(470〜660M1b)
及びMH帯域用(518〜770MTo)とに利用でき
るものである。この反射器の場合、反射器A、Bの素子
の長さがそれでれ第4図に示した寸法の場合が帯域が最
も広い例である。第4図に示すように、F/Bが30
[d B ]以上の帯域がかなり広くなりている( K
L−’1.75〜1.95)。Therefore, by installing reflectors A and B as shown in Figure 2 (A) and (B) and arranging reflectors A and B with different lengths three-dimensionally, two peaks can be obtained at 180 degrees F/B. , and high F/B can be obtained over a wide frequency range (K
L -1,55~2.20), therefore, when used for UHF TV, it is for LM band (470~660M1b)
and for the MH band (518 to 770 MTo). In the case of this reflector, when the lengths of the elements of reflectors A and B are as shown in FIG. 4, the band is the widest. As shown in Figure 4, F/B is 30
The band above [dB] is quite wide (K
L-'1.75-1.95).
このように、反射器を2段構造とすることにより、例え
ばUHFテレビ帯域を広帯域に良好なF/Bを得ること
ができる。この反射器はVHFテレビあ〜るいは通信用
アンテナにも利用できるものである。また、導波器の本
数が少なくなっても、F/Bの影響は少ない。By forming the reflector in a two-stage structure in this manner, it is possible to obtain a good F/B over a wide range of UHF television bands, for example. This reflector can also be used for VHF television or communication antennas. Furthermore, even if the number of waveguides is reduced, the influence of F/B is small.
[考案の効果]
以上詳述したように本発明によれば、F/Bを良好とす
ることによりテレビ放送の混信を解消するとができるの
で、周波数の有効利用が計れ、高画質テレビ受信アンテ
ナとして優れている八木式アンテナの反射器を提供する
ことができる。[Effects of the invention] As detailed above, according to the present invention, it is possible to eliminate interference in television broadcasting by improving the F/B, so that frequencies can be used effectively, and it can be used as a high-definition television receiving antenna. An excellent Yagi antenna reflector can be provided.
第1図は本発明の一実施例に係わる八木式アンテナの反
射器の構成図、第2図は第1段及び第2段の反射器の構
成を示す平面図、第3図は反射器を1段とした場合の周
波数対KL特性を示すグラフ、第4図反射器を2段とし
た場合の周波数対にし特性をI示すグラフである。
P・・・給電素子、D1〜D20・・・導波素子、R1
−R8・・・反射素子。
出願人代理人 弁理士 鈴江武彦
にL
第3図
にL
第4図Figure 1 is a configuration diagram of a reflector of a Yagi antenna according to an embodiment of the present invention, Figure 2 is a plan view showing the configuration of the first and second stage reflectors, and Figure 3 is a diagram showing the configuration of the reflector. FIG. 4 is a graph showing the frequency vs. KL characteristic when the reflector is in one stage, and FIG. 4 is a graph showing the frequency vs. KL characteristic when the reflector is in two stages. P... Feeding element, D1-D20... Waveguide element, R1
-R8...Reflection element. Applicant's agent Patent attorney Takehiko Suzue L Figure 3 L Figure 4
Claims (1)
し、1段目は短い素子を2列とその上下に中央を開放し
た長い素子を各1列づつ並べ、2段目は前記反射素子の
長い素子と短い素子の位置を入替え1段目の後方の位置
に配置するようにした八木式アンテナの反射器。In the Yagi antenna reflector, the reflector is configured in two stages, the first stage has two rows of short elements, the top and bottom of which are arranged one row each of long elements with the center open, and the second stage has the above-mentioned reflecting elements. A reflector for a Yagi antenna in which the positions of the long and short elements are switched and placed behind the first stage.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15677587A JPH01125003A (en) | 1987-06-24 | 1987-06-24 | Reflector for yagi antenna |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15677587A JPH01125003A (en) | 1987-06-24 | 1987-06-24 | Reflector for yagi antenna |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01125003A true JPH01125003A (en) | 1989-05-17 |
Family
ID=15635043
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP15677587A Pending JPH01125003A (en) | 1987-06-24 | 1987-06-24 | Reflector for yagi antenna |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01125003A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5442221A (en) * | 1992-05-27 | 1995-08-15 | Schlumberger Industries, S.A. | Hall effect sensor |
-
1987
- 1987-06-24 JP JP15677587A patent/JPH01125003A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5442221A (en) * | 1992-05-27 | 1995-08-15 | Schlumberger Industries, S.A. | Hall effect sensor |
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