JPH0695605B2 - Antenna mirror structure - Google Patents
Antenna mirror structureInfo
- Publication number
- JPH0695605B2 JPH0695605B2 JP2394788A JP2394788A JPH0695605B2 JP H0695605 B2 JPH0695605 B2 JP H0695605B2 JP 2394788 A JP2394788 A JP 2394788A JP 2394788 A JP2394788 A JP 2394788A JP H0695605 B2 JPH0695605 B2 JP H0695605B2
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- JP
- Japan
- Prior art keywords
- mirror
- split
- shells
- shell
- mirror surface
- 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.)
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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、高精度が要求され、かつ厳しい熱環境下で使
用されるパラボラアンテナの鏡面(反射鏡)に関し、例
えば、人工衛星搭載用の大形アンテナなどの鏡面に適用
されるものである。TECHNICAL FIELD The present invention relates to a mirror surface (reflecting mirror) of a parabolic antenna that is required to have high accuracy and that is used in a severe thermal environment. It is applied to mirror surfaces such as large antennas.
<従来の技術> 人工衛星に搭載されるアンテナの従来のものの鏡面は、
第6図及びその一部の縦断面である第7図に示すよう
に、一枚の鏡面殻1で形成されている。つまり、鏡面2
は、一枚の鏡面殻1で得られ、それを支柱3を介して骨
組構造体4に支持した構成となっているのである。<Prior Art> The mirror surface of the conventional antenna mounted on the satellite is
As shown in FIG. 6 and FIG. 7 which is a longitudinal cross section of a part thereof, it is formed of one mirror shell 1. That is, mirror surface 2
Is obtained by a single mirror-like shell 1 and is supported by the frame structure 4 through the columns 3.
ところで、このような構造の鏡面2にあっては、第9図
に示すように、太陽光(図中矢印で示す)の方向によ
り、鏡面2上に人工衛星の他の構造物等5(例えば、タ
ワー)の影(図中斜線で示す部分)が部分的にできた場
合には、鏡面2における日照部と日陰部とで著しい温度
差が生じ、鏡面殻材料の膨張あるいは収縮により、日照
部と日陰部とで曲率が不連続に変化しようとする。By the way, in the mirror surface 2 having such a structure, as shown in FIG. 9, depending on the direction of sunlight (indicated by an arrow in the figure), another structure 5 of the artificial satellite or the like (for example, 5 , A tower) is partially formed (shaded portion in the figure), a remarkable temperature difference occurs between the sunlit portion and the shaded portion on the mirror surface 2, and the sunlit portion is expanded or contracted due to expansion or contraction of the mirror surface shell material. And the shade part tries to change discontinuously.
このため、日照部と日陰部との間に大きな面外の歪が生
じ、鏡面としての性能を劣化させることとなっていた。Therefore, a large out-of-plane distortion occurs between the sunlit part and the shaded part, which deteriorates the performance as a mirror surface.
<発明が解決しようとする課題> 上記のような問題を解決するために、第8図に示すよう
に、鏡面殻1をいくつか(ここでは三つ)に分割し、か
つ各分割鏡面殻1a,1b,1c間に隙間を設けたものが考えら
れている。<Problems to be Solved by the Invention> In order to solve the above problems, as shown in FIG. 8, the mirror shell 1 is divided into several (here, three), and each split mirror shell 1a , 1b and 1c are considered to have a gap between them.
この鏡面では、部分的な影による温度偏差によって生じ
た変形を、各分割鏡面殻1a,1b,1cの面内方向の変形とし
て、前記隙間で吸収するのである。On this mirror surface, the deformation caused by the temperature deviation due to the partial shadow is absorbed in the gap as the deformation in the in-plane direction of each of the split mirror shells 1a, 1b, 1c.
隙間は、鏡面殻1が最高温度(宇宙空間においては約10
0℃)のときに、分割鏡面殻1a,1b,1cが膨張して零とな
るように調整しなければならず、そのため、鏡面殻1が
最低温度(約−200℃)となったときには、分割鏡面殻1
a,1b,1cが収縮して大きな隙間となってしまう。As for the gap, the mirror shell 1 has the highest temperature (about 10
(0 ° C), the split mirror shells 1a, 1b, 1c must be adjusted so that they expand and become zero. Therefore, when the mirror shell 1 reaches the minimum temperature (about -200 ° C), Split mirror shell 1
a, 1b, 1c contract and become a large gap.
通常、鏡面殻1は、線膨張係数の小さい炭素繊維強化プ
ラスチック(CFRP)の表皮でアルミハニカムコアをサン
ドイッチにし、軽量で高剛性の構造とするが、このとき
の鏡面殻1の線膨張係数は、5×10-6/℃程度となる。
一方、鏡面殻1を支える骨組構造体4は、炭素繊維の配
向等の関係で線膨張係数は鏡面殻1のそれより一桁小さ
くなったり、ときには、負の値になったりする。したが
って、例えば、開口径5メートルといった大形鏡面殻1
を、第8図に示すように三分割した場合、各分割鏡面殻
1a,1b,1cの隙間は最大時で4ミリメートル程度となり、
利得低下を招く。更に、部分的に影ができる場合には、
日照下の鏡面殻部と日陰の鏡面殻部とでは曲率が異なる
ように変形するので、エッジ部においては、第10図に示
すように段差6が生じてしまう。このような段差は、サ
イドローブ特性を大きく劣化させてしまう。したがっ
て、従来の如く、鏡面を分割しただけでは、熱変形によ
る鏡面の性能低下を充分に解決することはできなかった
のである。Normally, the mirror shell 1 has a lightweight and high-rigidity structure by sandwiching an aluminum honeycomb core with a skin of carbon fiber reinforced plastic (CFRP) having a small linear expansion coefficient. At this time, the coefficient of linear expansion of the mirror shell 1 is It will be about 5 × 10 -6 / ° C.
On the other hand, the skeleton structure 4 supporting the mirror shell 1 has a linear expansion coefficient smaller than that of the mirror shell 1 by an order of magnitude or sometimes a negative value due to the orientation of the carbon fibers. Therefore, for example, a large mirror shell 1 with an opening diameter of 5 meters
Is divided into three parts as shown in FIG.
The maximum gap between 1a, 1b and 1c is about 4mm,
This leads to a decrease in gain. Furthermore, if there is a partial shadow,
Since the mirror surface shell portion under sunshine and the mirror surface shell portion in the shade are deformed so as to have different curvatures, a step 6 is formed at the edge portion as shown in FIG. Such a step greatly deteriorates the side lobe characteristic. Therefore, as in the prior art, merely by dividing the mirror surface, it was not possible to sufficiently solve the performance deterioration of the mirror surface due to thermal deformation.
<課題を解決するための手段> 上記課題を解決するため、本発明では、反射鏡アンテナ
の反射面を形成する鏡面殻を複数に分割すると共に、各
分割鏡面殻の境界が接する外縁に沿って、隣り合う分割
鏡面殻同士の境界部分における面内方向への相異なる動
きを許容しながら、隣り合う分割鏡面殻同士の境界部分
における面外方向への相異なる動きおよび、隣り合う分
割鏡面殻の境界を隔てて曲面の接線が不連続になるよう
な変形を阻止する嵌合構造を形成し、かつ該嵌合部では
一方の分割鏡面殻の一部に他方の分割鏡面殻の反射面の
一部が重なる構造とし、分割鏡面殻が形成する反射面が
その境界において該分割鏡面殻の面内方向への相異なる
動きによって間隙が生じた場合に該嵌合部の反射面側の
面が該間隙部分における反射面となるアンテナ鏡面構造
としたのである。<Means for Solving the Problems> In order to solve the above problems, in the present invention, the mirror shell that forms the reflecting surface of the reflector antenna is divided into a plurality of pieces, and along the outer edge where the boundary of each divided mirror shell contacts. , While allowing different movements in the in-plane direction at the boundary between adjacent split mirror shells, different movements in the out-of-plane direction at the boundary between adjacent split mirror shells, and between adjacent split mirror shells. A fitting structure is formed to prevent deformation such that the tangent of the curved surface becomes discontinuous across the boundary, and at the fitting portion, a part of one of the split mirror surface shells is provided with one of the reflecting surfaces of the other split mirror surface shell. When the reflecting surface formed by the split specular shells has a gap at the boundary due to different movements of the split specular shells in the in-plane direction, the reflecting surface of the fitting portion is Anne which becomes the reflective surface in the gap The Tena mirror surface structure was adopted.
<作用> 上記構成のアンテナ鏡面構造においては、分割された各
分割鏡面殻間に温度差による収縮、膨張があったとして
も、面内方向の相対的な動きについては嵌合構造部は拘
束せず、嵌合のかみ合わせ部の摺動によって吸収する。
また、このように隣り合う分割鏡面殻が面内方向に相異
なる動きをして反射面を形成する部分が離れてしまって
も、嵌合部が、この間隙部分における反射面となる。更
に、分割鏡面殻の面外方向への相対的な動きおよび、隣
り合う鏡面殻が形成する反射面がその境界において不連
続な曲面となることは嵌合構造の嵌合によって拘束され
るので、各分割鏡面間の段差となることなく連続した曲
面を保つことができる。<Operation> In the antenna mirror surface structure having the above configuration, even if there is contraction or expansion due to a temperature difference between the divided split mirror surface shells, the fitting structure portion is restrained from the relative movement in the in-plane direction. Instead, it is absorbed by sliding the mating engagement part.
In addition, even if the adjacent split mirror shells move differently in the in-plane direction and the portions forming the reflecting surface are separated from each other, the fitting portion serves as the reflecting surface in the gap portion. Furthermore, the relative movement of the split mirror shells in the out-of-plane direction and the fact that the reflecting surfaces formed by the adjacent mirror shells are discontinuous curved surfaces at their boundaries are constrained by the fitting of the fitting structure, It is possible to maintain a continuous curved surface without forming a step between the split mirror surfaces.
<実施例> 第1図(a)(b)には本発明の一実施例に係るアンテ
ナ鏡面構造における各分割鏡面殻の部分拡大斜視を示し
てあり、第2図,第3図には二つの分割鏡面殻の異なる
嵌合状態を示してある。<Embodiment> FIGS. 1 (a) and 1 (b) show partially enlarged perspective views of respective divided mirror shells in an antenna mirror structure according to an embodiment of the present invention, and FIG. 2 and FIG. The different mating states of the two split mirror shells are shown.
第1図ないし第3図には、第8図に示したように、鏡面
2を三分割する三つの分割鏡面殻のうちの二つ(分割鏡
面殻1a,1b)を示す。各分割鏡面殻は、前述の如く、あ
る程度の曲げ剛性を持たせるために、CFRP製の表皮7を
アルミハニカムコア8の両面に設けたサンドイッチ構造
となっており、その全体の肉厚は5〜10ミリメートル程
度である。1 to 3 show two of the three divided mirror shells (the divided mirror shells 1a and 1b) that divide the mirror surface 2 into three, as shown in FIG. As described above, each of the split mirror shells has a sandwich structure in which CFRP skins 7 are provided on both sides of the aluminum honeycomb core 8 in order to have a certain degree of bending rigidity, and the overall wall thickness is 5 to 5. It is about 10 mm.
各分割鏡面殻1a,1bの合せ面は、例えば、図に示すよう
に直線状となっており、また分割された鏡面はそれらを
合わせた状態で一つの曲面を形成するようにその合わせ
面で同一の曲率を持っている。これらの合せ面間に両者
の嵌合構造9が構成されている。この嵌合構造9は、一
方の分割鏡面殻1aの合せ部に設けられた横断面形状が凹
状の嵌合部材10と、もう一方の分割鏡面殻1bの合せ部に
設けられ、前記嵌合部材10と嵌合する横断面形状が凸状
の嵌合部材11とからなっている。嵌合部材10と11は、嵌
合状態で面内方向(鏡面2の表面に平行な方向)に自由
に摺動し得、かつ面外方向(鏡面2の表面に直交する方
向)のずれや合わせ面での曲率が不連続になろうとする
変形を抑制し合う。第8図に示したように三分割とし、
開口径5メートル程度の鏡面ならば、面内方向の最大変
位量は3〜4ミリメートル程度であるから、嵌合部材10
の凹部10aの深さあるいは嵌合部材11の凸部11aの高さは
10ミリメートル程度あれば充分である。嵌合部材10の上
面10bは鏡面2の一部ともなり得るので、金属あるいはC
FRPで製作される。The mating surface of each split mirror surface shell 1a, 1b is, for example, linear as shown in the figure, and the split mirror surface is a mating surface so as to form one curved surface in the state where they are put together. They have the same curvature. A fitting structure 9 is formed between these mating surfaces. The fitting structure 9 is provided at the fitting portion of the split mirror surface shell 1a on one side and has a concave cross-sectional shape, and on the fitting portion of the split mirror surface shell 1b on the other side, The fitting member 11 has a convex cross section and is fitted with the fitting member 11. The fitting members 10 and 11 can freely slide in the in-plane direction (direction parallel to the surface of the mirror surface 2) in the fitted state, and can be displaced in the out-of-plane direction (direction orthogonal to the surface of the mirror surface 2). It suppresses the deformation that the curvatures on the mating surfaces tend to become discontinuous. As shown in FIG. 8, it is divided into three,
With a mirror surface having an opening diameter of about 5 meters, the maximum displacement in the in-plane direction is about 3 to 4 mm.
The depth of the concave portion 10a or the height of the convex portion 11a of the fitting member 11 is
About 10 mm is enough. Since the upper surface 10b of the fitting member 10 can also be a part of the mirror surface 2, metal or C
Manufactured by FRP.
この実施例では、嵌合構造として、単一的な凹凸状の組
合せによるものをあげているが、嵌合構造としてはこれ
に限らず、要は、面内方向に摺動可能で、面外方向に互
いに拘束するものであればいかなるものでもよい。In this embodiment, the fitting structure is a combination of a single concavo-convex shape, but the fitting structure is not limited to this, and the point is that it can slide in the in-plane direction and Any one may be used as long as it constrains each other in the direction.
上記アンテナ鏡面構造を備えたパラボラアンテナにおい
ては、最高温度下では、各分割鏡面殻1a,1b,1cが膨張
し、第2図に示すように、嵌合部材10,11同士は緊密に
嵌合した状態となる。In the parabolic antenna having the above antenna mirror surface structure, the split mirror shells 1a, 1b, 1c expand at the highest temperature, and the fitting members 10, 11 are closely fitted to each other as shown in FIG. It will be in the state of doing.
また、最低温度下では、各分割鏡面殻1a,1b,1cが収縮
し、第3図に示すように、嵌合部材10,11は嵌合状態を
保ったまま面内方向にずれた状態となる。このとき、表
皮7間には隙間cができ、嵌合部材10の表面10bが鏡面
の一部となる。各分割鏡面殻1a,1b,1cの表面(鏡面)と
嵌合部材10の表面10bとの間には表皮7の厚さに相当す
る分の段差hができるが、この段差hは0.1ミリメート
ル程度にすることができるので、例えば波長が数ミリ以
上の電波を用いる場合においては鏡面2の性能にはほと
んど影響しない。Further, at the lowest temperature, the split mirror shells 1a, 1b, 1c contract, and as shown in FIG. 3, the fitting members 10, 11 are displaced in the in-plane direction while maintaining the fitted state. Become. At this time, a gap c is formed between the skins 7, and the surface 10b of the fitting member 10 becomes a part of the mirror surface. A step h corresponding to the thickness of the skin 7 is formed between the surface (mirror surface) of each split mirror shell 1a, 1b, 1c and the surface 10b of the fitting member 10. The step h is about 0.1 mm. Therefore, when using a radio wave having a wavelength of several millimeters or more, the performance of the mirror surface 2 is hardly affected.
更に、第9図に示したように、鏡面2に部分的に影がで
き、例えば、隣り合う分割鏡面殻の一方が太陽光を受け
て高温となり、他方が影になって低温となって、第10図
に示したように逆方向の変位が生じるような状況におい
ても、変位は各分割鏡面殻1a,1b,1cの膨張、収縮により
相殺され、また、面外方向へのずれ(曲率が異なる変
形)も嵌合部材10,11の嵌合により拘束され、結果とし
て各分割鏡面殻1a,1b,1cはなだらかにつながる状態を保
つ。Furthermore, as shown in FIG. 9, a shadow is partially formed on the mirror surface 2, for example, one of the adjacent split mirror shells receives sunlight and becomes hot, and the other becomes shadow and becomes cold, Even in the situation where displacement occurs in the opposite direction as shown in FIG. 10, the displacement is canceled by the expansion and contraction of each split mirror surface shell 1a, 1b, 1c, and the displacement in the out-of-plane direction (curvature is (Different deformations) are also restrained by the fitting of the fitting members 10 and 11, and as a result, the split mirror shells 1a, 1b and 1c are kept in a smoothly connected state.
第4図,第5図には、鏡面2に第9図に示すように、影
が生じた場合の鏡面2の変形状態を示す。鏡面殻1を三
分割したもので、第4図に示すものが本発明に係るも
の、つまり、各分割鏡面殻1a,1b,1c間に嵌合構造を設け
たものであり、第5図に示すものが従来のもの、つま
り、各分割鏡面殻1a,1b,1cがそれぞれ完全に独立したも
のである。図中の縞は等高線を表わし、縞番号が変位
0の線であり、より若い縞番号が下側への変位、上の
縞番号が上側への変位を示す。4 and 5 show a deformed state of the mirror surface 2 when a shadow is produced on the mirror surface 2 as shown in FIG. The mirror shell 1 is divided into three parts, and the one shown in FIG. 4 relates to the present invention, that is, the fitting structure is provided between the divided mirror shells 1a, 1b, 1c, and FIG. What is shown is a conventional one, that is, each of the split mirror shells 1a, 1b, 1c is completely independent. The stripes in the figure represent contour lines, and the stripe number is a line with a displacement of 0. The younger stripe number indicates the downward displacement, and the upper stripe number indicates the upward displacement.
第4図に示す本発明のものでは、等高線の数が少なく、
縞番号もほとんどで、変形量が小さいことがわかる。
また、各分割鏡面殻1a,1b,1c間で等高線はなめらかにつ
ながっている。In the present invention shown in FIG. 4, the number of contour lines is small,
It can be seen that the amount of deformation is small with almost all stripe numbers.
Further, contour lines are smoothly connected between the divided mirror shells 1a, 1b, 1c.
これに対し、第5図に示す従来のものでは、等高線が密
であり、2倍以上の変形量となっており、また、隣り合
う分割鏡面殻でも、縁部で縞番号が食い違っていること
から、大きな段差ができていることがわかる。更に、図
では示されていないが、各分割鏡面殻間にも大きな隙間
が生じる。On the other hand, in the conventional one shown in FIG. 5, the contour lines are dense and the deformation amount is more than twice, and the stripe numbers are different at the edges even between the adjacent split mirror shells. From this, it can be seen that there is a large step. Further, although not shown in the figure, a large gap also occurs between each split mirror shell.
なお、本発明に係る構造のものでは、例えば、開口径5
メートル、三分割のものに適用した場合、重量増加は、
1.5kg程度ですむ。これに対し、従来のもので、本発明
に係るものと同様の精度を得るためには、支柱3を大幅
に増やし、鏡面殻1の厚みを大幅に増すなどの対策が必
要となり、そのときには大幅な重量増加(同様のものの
場合で、5kg以上)を招いてしまう。In the structure according to the present invention, for example, the opening diameter is 5
When applied to meters and three-part ones, the weight increase is
It only takes about 1.5kg. On the other hand, in order to obtain the same accuracy as the one according to the present invention, it is necessary to take measures such as significantly increasing the number of columns 3 and significantly increasing the thickness of the mirror-like shell 1, and at that time, Will increase the weight (in the case of similar things, more than 5kg).
<発明の効果> 本発明に係るアンテナ鏡面構造によれば、分割鏡面殻間
に嵌合構造を設けたので、鏡面の温度変化による鏡面殻
の膨張収縮による変形は嵌合構造を形成する嵌合部材間
の摺動により吸収され、また、面外方向への変形も嵌合
部材同士の拘束により抑制され、常になめらかな鏡面が
得られ、性能低下を来たすことがなくなる。また、本構
造を採用することによる重量増加はわずかであり、この
面でも有利である。<Effects of the Invention> According to the antenna mirror surface structure of the present invention, since the fitting structure is provided between the split mirror surface shells, the deformation due to the expansion and contraction of the mirror surface shell due to the temperature change of the mirror surface forms the fitting structure. It is absorbed by the sliding between the members, and the deformation in the out-of-plane direction is also suppressed by the restraint of the fitting members, so that a smooth mirror surface is always obtained and the performance is not deteriorated. Further, the weight increase due to the adoption of this structure is slight, which is also advantageous in this respect.
第1図(a)(b)は本発明の一実施例に係るアンテナ
鏡面を構成する分割鏡面殻の拡大部分斜視図、第2図,
第3図は一実施例の状態を異にする部分斜視図、第4図
は一実施例に係るアンテナ鏡面の変形状態を等高線で示
す説明図、第5図は従来のものにおける第4図と同様の
説明図、第6図はパラボラアンテナ鏡面の斜視図、第7
図はその断面図、第8図は鏡面を三分割したものの斜視
図、第9図,第10図はアンテナ鏡面に影ができた様子、
温度差により変形が生じた様子の説明図である。 図面中、1は鏡面殻、1a,1b,1cは分割鏡面殻、2は鏡
面、3は支柱、4は骨組構造体、7は表皮、8はアルミ
ハニカムコア、9は嵌合構造、10,11は嵌合部材、10aは
凹部、11aは凸部である。1 (a) and 1 (b) are enlarged partial perspective views of a split mirror surface shell constituting an antenna mirror surface according to an embodiment of the present invention, FIG.
FIG. 3 is a partial perspective view showing a different state of the embodiment, FIG. 4 is an explanatory view showing the deformed state of the antenna mirror surface according to the embodiment with contour lines, and FIG. The same explanatory view, FIG. 6 is a perspective view of the parabolic antenna mirror surface, FIG.
The figure is its cross-sectional view, Figure 8 is a perspective view of the mirror surface divided into three parts, and Figures 9 and 10 show the shadow of the antenna mirror surface.
It is an explanatory view of a state in which deformation occurs due to a temperature difference. In the drawing, 1 is a mirror surface shell, 1a, 1b, 1c are split mirror surface shells, 2 is a mirror surface, 3 is a pillar, 4 is a skeleton structure, 7 is a skin, 8 is an aluminum honeycomb core, 9 is a fitting structure, 10, Reference numeral 11 is a fitting member, 10a is a concave portion, and 11a is a convex portion.
Claims (1)
は複数に分割され、更に各分割鏡面殻の境界が接する外
縁に沿って、隣り合う分割鏡面殻同士の境界部分におけ
る面内方向への相異なる動きを許容しながら、隣り合う
分割鏡面殻同士の境界部分における面外方向への相異な
る動きおよび、隣り合う分割鏡面殻の境界を隔てて曲面
の接線が不連続になるような変形を阻止する嵌合構造を
形成し、かつ該嵌合部では一方の分割鏡面殻の一部に他
方の分割鏡面殻の反射面の一部が重なる構造を持ち、分
割鏡面殻が形成する反射面がその境界において該分割鏡
面殻の面内方向への相異なる動きによって間隙が生じた
場合に該嵌合部の反射面側の面が該間隙部分における反
射面となることを特徴とするアンテナ鏡面構造。1. A mirror shell forming a reflecting surface of a reflector antenna is divided into a plurality of pieces, and further along an outer edge where the boundaries of the respective split mirror shells are in contact with each other, in an in-plane direction at a boundary portion between adjacent split mirror shells. While allowing different movements of the two split specular shells, different movements in the out-of-plane direction at the boundary between the adjacent split specular shells and the deformation so that the tangent of the curved surface becomes discontinuous across the boundary of the adjacent split specular shells And a reflecting structure formed by the split mirror surface shell, which has a structure in which a part of the split mirror surface shell of one of the split mirror surfaces overlaps with a part of the reflecting surface of the other split mirror surface shell. An antenna mirror surface characterized in that when a gap is generated at the boundary by different movements of the split mirror shell in the in-plane direction, the surface of the fitting portion on the reflection surface side becomes the reflection surface in the gap portion. Construction.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2394788A JPH0695605B2 (en) | 1988-02-05 | 1988-02-05 | Antenna mirror structure |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2394788A JPH0695605B2 (en) | 1988-02-05 | 1988-02-05 | Antenna mirror structure |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01200803A JPH01200803A (en) | 1989-08-14 |
| JPH0695605B2 true JPH0695605B2 (en) | 1994-11-24 |
Family
ID=12124741
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2394788A Expired - Fee Related JPH0695605B2 (en) | 1988-02-05 | 1988-02-05 | Antenna mirror structure |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0695605B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100723605B1 (en) * | 2006-02-14 | 2007-06-04 | (주)하이게인안테나 | Polarized Conversion Tracking Radar Antenna |
-
1988
- 1988-02-05 JP JP2394788A patent/JPH0695605B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH01200803A (en) | 1989-08-14 |
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