JPH11121972A - Reflected radio wave scattering structure - Google Patents

Reflected radio wave scattering structure

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Publication number
JPH11121972A
JPH11121972A JP27700197A JP27700197A JPH11121972A JP H11121972 A JPH11121972 A JP H11121972A JP 27700197 A JP27700197 A JP 27700197A JP 27700197 A JP27700197 A JP 27700197A JP H11121972 A JPH11121972 A JP H11121972A
Authority
JP
Japan
Prior art keywords
radio wave
openings
reflected
conductor
scattering structure
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
Application number
JP27700197A
Other languages
Japanese (ja)
Inventor
Masato Tadokoro
眞人 田所
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.)
Yokohama Rubber Co Ltd
Original Assignee
Yokohama Rubber 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 Yokohama Rubber Co Ltd filed Critical Yokohama Rubber Co Ltd
Priority to JP27700197A priority Critical patent/JPH11121972A/en
Publication of JPH11121972A publication Critical patent/JPH11121972A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To easily inexpensively reduce the amount of reflected radio waves from a turbine wheel which is positioned in an intake duct. SOLUTION: A turbine wheel 2 is disposed in an intake duct 1 of an aircraft. Two conductor meshes 3 and 4 are arranged with a prescribed interval in between in front of the wheel 2 in the duct 1. The meshes 3 and 4 are respectively arranged tilting at prescribed angles from a plane perpendicular to the arriving direction of radio waves. The openings 3a and 4a of the meshes 3 and 4 are formed into square shapes and the sizes of the openings 3a and 4a are set so that the ratio of the circumferential length L1 =4l1 of each of the openings 3a to the peripheral length L2 =4l2 of each of the openings 4a become mutually differing prime numbers, when the ratio is expressed in a natural number. L1 and l2 respectively represent the lengths of one sides of the openings 3a and 4a.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、筒体の内部に配設
された電波反射体、特に、航空機のインテークダクト内
に配設されたダービンホイールの反射電波散乱構造に関
する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a radio wave reflector disposed inside a cylinder, and more particularly, to a reflected radio wave scattering structure of a Durbin wheel disposed in an intake duct of an aircraft.

【0002】[0002]

【従来の技術】図4を参照して、航空機のインテークダ
クトaの内部に配設されたタービンホイールbはレーダ
ー等の電磁波に対して良反射体であるため、非常に大き
な反射波が到来方向に返され、時には好ましくない結果
を招くことになる。そこで、タービンホイールbからの
反射波を低減するために、例えばインテークダクトaの
空気取入口にオージブc(図5参照)や円錐状のカバー
を設けて到来電波の大半を散乱させるか、或いはインテ
ークダクトaのタービンホイールbの前方に位置する部
分を屈曲形成して到来電波の殆どを散乱させる方法(図
6参照)等が提案されている。
2. Description of the Related Art Referring to FIG. 4, a turbine wheel b disposed inside an intake duct a of an aircraft is a good reflector for electromagnetic waves such as radars, so that a very large reflected wave comes in the direction of arrival. And sometimes lead to undesirable results. Therefore, in order to reduce the reflected wave from the turbine wheel b, for example, an orifice c (see FIG. 5) or a conical cover is provided at the air intake of the intake duct a to scatter most of the incoming radio waves, or A method has been proposed in which a portion of the duct a located in front of the turbine wheel b is bent to scatter most of the incoming radio waves (see FIG. 6).

【0003】[0003]

【発明が解決しようとする課題】しかしながら、図5に
示す前者の反射電波散乱構造では、オージブc等がコス
ト的に高くつき、しかも、空気取入口からの空気流入が
妨げられるという不都合がある。また、図6に示す後者
の反射電波散乱構造では、インテークダクトaの屈曲形
成が工作的にコスト高になり、しかも、屈曲形状が他の
機能(例えばエンジン部への空気の平滑な供給)を抑制
することもあって実現困難な場合が多いという不都合が
ある。
However, the former reflected radio wave scattering structure shown in FIG. 5 has disadvantages in that the aug c is expensive in terms of cost and that the air inflow from the air intake is obstructed. Further, in the latter reflected radio wave scattering structure shown in FIG. 6, the bending of the intake duct a is costly in terms of work, and the bent shape has another function (for example, smooth supply of air to the engine unit). There is an inconvenience that it is often difficult to realize due to suppression.

【0004】本発明はかかる不都合を解消するためにな
されたものであり、簡単且つ低コストで電波反射体から
の反射電波を低減することができる反射電波散乱構造を
提供することを目的とする。
SUMMARY OF THE INVENTION The present invention has been made to solve such a problem, and an object of the present invention is to provide a reflected radio wave scattering structure capable of reducing the reflected radio waves from a radio wave reflector at a simple and low cost.

【0005】[0005]

【課題を解決するための手段】かかる目的を達成するた
めに、請求項1に係る反射電波散乱構造は、筒体の内部
に配設された電波反射体の反射電波散乱構造であって、
前記筒体内の前記電波反射体の前方位置に所定の間隔を
存して設けられた複数の導体メッシュを電波の到来方向
に直角な面に対して所定角度傾けて配置し、更に、各導
体メッシュはそれぞれ一定の大きさの開口部を有し、且
つ、各導体メッシュの開口部の周長の比を自然数で表し
たときに互いに異なる素数であることを特徴とする。
In order to achieve the above object, a reflected radio wave scattering structure according to claim 1 is a reflected radio wave scattering structure of a radio wave reflector disposed inside a cylinder,
A plurality of conductor meshes provided at a predetermined interval in front of the radio wave reflector in the cylinder are arranged at a predetermined angle with respect to a plane perpendicular to the direction of arrival of radio waves, and further, each conductor mesh Are characterized in that they have openings of a certain size, and are different prime numbers when the ratio of the perimeters of the openings of the respective conductor meshes is expressed by a natural number.

【0006】請求項2に係る反射電波散乱構造は、請求
項1において、前記互いに異なる素数となる自然数が5
以上であることを特徴とする。
According to a second aspect of the present invention, there is provided the reflected radio wave scattering structure according to the first aspect, wherein the natural numbers having different prime numbers are 5 or more.
It is characterized by the above.

【0007】[0007]

【発明の実施の形態】以下、本発明の実施の形態を図を
参照して説明する。図1は本発明の実施の一形態である
反射電波散乱構造を説明するための説明的断面図、図2
は導体メッシュの部分的平面図、図3は他の導体メッシ
ュの部分的平面図である。なお、この実施の形態では、
筒体として航空機のインテークダクトを、電波反射体と
して該インテークダクトの内部に配設されたタービンホ
イールをそれぞれ例に採る。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is an explanatory cross-sectional view for explaining a reflected radio wave scattering structure according to an embodiment of the present invention.
Is a partial plan view of a conductor mesh, and FIG. 3 is a partial plan view of another conductor mesh. In this embodiment,
As an example, an intake duct of an aircraft is used as a cylinder, and a turbine wheel disposed inside the intake duct is used as a radio wave reflector.

【0008】図1において符号1は航空機のインテーク
ダクト(筒体)であり、該インテークダクト1の内部に
はタービンホイール(電波反射体)2が配設されてい
る。インテークダクト1内のタービンホイール2の前方
位置には、二枚の導体メッシュ3,4が所定の間隔を存
して設けられている。各導体メッシュ3,4は共に電波
の到来方向に直角な面に対して所定角度傾斜し、且つ、
導体メッシュ3と導体メッシュ4とが互いに平行になら
ないように配置されている。
In FIG. 1, reference numeral 1 denotes an intake duct (tubular body) of an aircraft, and a turbine wheel (radio wave reflector) 2 is disposed inside the intake duct 1. Two conductor meshes 3 and 4 are provided at predetermined intervals at a position in front of the turbine wheel 2 in the intake duct 1. Each of the conductor meshes 3, 4 is inclined at a predetermined angle with respect to a plane perpendicular to the arrival direction of the radio wave, and
The conductor mesh 3 and the conductor mesh 4 are arranged so as not to be parallel to each other.

【0009】また、図2及び図3に示すように、各導体
メッシュ3,4の複数の開口部3a,4aはそれぞれ一
定の大きさの正方形状をなしており、一辺の長さを開口
部3a,4aについてそれぞれl1 ,l2 とすると、開
口部3aの周長L1 =4l1と開口部4aの周長L2
4l2 との比が自然数で表したときに互いに異なる素数
となるように設定されている。
As shown in FIGS. 2 and 3, a plurality of openings 3a and 4a of each of the conductor meshes 3 and 4 are formed in a square shape having a fixed size, and the length of one side is defined as the opening. 3a, respectively When l 1, l 2 for 4a, the circumferential length of the opening 3a L 1 = 4l 1 and the circumferential length of the opening 4a L 2 =
When the ratio with 4l 2 is represented by a natural number, the prime numbers are set to be different from each other.

【0010】ここで、一定の開口寸法を有する導体メッ
シュ3,4は一種の周波数選択膜として機能し、おおよ
そその周長Lと波長λがL=nλ(又は周波数f=c/
λ(cは光速))となる関係の波長で共振し、電磁波を
透過する。そして、これ以外の周波数の電波に対しては
全反射する。但し、nは自然数とする。
Here, the conductor meshes 3 and 4 having a fixed opening size function as a kind of frequency selection film, and the circumference L and the wavelength λ are approximately L = nλ (or the frequency f = c /
λ (c is the speed of light)), and resonates at a wavelength having a relationship of λ (c is the speed of light) and transmits electromagnetic waves. Then, radio waves of other frequencies are totally reflected. Here, n is a natural number.

【0011】したがって、インテークダクト1の空気取
入口から進入した到来電波は、導体メッシュ3ではf0
を基底とする逓倍波nf0 (又はλ=4l1 /n)の電
磁波については透過するが、それ以外の波は斜めに全反
射されて到来方向に返ることはない。
Therefore, the arriving radio wave entering from the air intake of the intake duct 1 is f 0 in the conductor mesh 3.
The transmitting the electromagnetic wave of the multiplied wave nf 0 to base (or λ = 4l 1 / n), but waves otherwise never returning to the arrival direction is totally reflected obliquely.

【0012】また、導体メッシュ3を透過した波f0
nf0 (λ=4l2 /n以外の波)については、導体メ
ッシュ4で上記と同様にして斜めに全反射されて到来方
向には返らない。導体メッシュ4は導体メッシュ3と異
なる開口寸法を有しており、しかも、開口部4aの周長
2 と開口部3aの周長L1 との比が自然数で表したと
きに互いに異なる素数であることから、基本的には導体
メッシュ4はf0 を基底とする逓倍波nf0 に対して全
反射する。
Also, the waves f 0 ,
nf 0 (waves other than λ = 4l 2 / n) is totally reflected obliquely by the conductor mesh 4 in the same manner as described above, and does not return in the arrival direction. Conductor mesh 4 has a different opening dimension conductor mesh 3, moreover, at different prime when the ratio of the circumferential length L 1 of the circumferential length L 2 and the opening 3a of the opening 4a is expressed in natural numbers since there is essentially conductor mesh 4 is totally reflected against multiplication waves nf 0 to base the f 0.

【0013】但し、開口部3a,4aの開口寸法の最小
公倍数となる波については導体メッシュ4を透過するた
め、上述した互いに異なる素数となる自然数は5以上で
あることが好ましく、この実施の形態ではL1 :L2
7:5としている。5逓倍以上の逓倍波では透過特性が
大幅に低下するため、両方の導体メッシュ3,4を透過
したとしてもタービンホイール2により反射される波は
かなり減衰されて事実上問題となることはない。
However, since the wave having the least common multiple of the opening dimensions of the openings 3a and 4a is transmitted through the conductor mesh 4, it is preferable that the above-mentioned natural numbers having different prime numbers be 5 or more. Then L 1 : L 2 =
7: 5. Since the transmission characteristics of the multiplied wave of 5 times or more are greatly reduced, the wave reflected by the turbine wheel 2 is considerably attenuated even if it passes through both the conductor meshes 3 and 4, so that there is no practical problem.

【0014】このようにこの実施の形態の反射電波散乱
構造においては、インテークダクト1の形状に係わらず
該インテークダクト1の内部に周波数選択性を有する二
枚の導体メッシュ3,4を配設するだけで、電波反射体
であるタービンホイール2からの反射波を散乱させて到
来方向に返さないようにすることができるので、簡単且
つ低コストで該反射波の低減効果を得ることができる。
As described above, in the reflected radio wave scattering structure of this embodiment, two conductor meshes 3 and 4 having frequency selectivity are disposed inside intake duct 1 regardless of the shape of intake duct 1. With only this, the reflected wave from the turbine wheel 2, which is a radio wave reflector, can be scattered so as not to return to the arrival direction, so that the effect of reducing the reflected wave can be obtained simply and at low cost.

【0015】また、導体メッシュ3の開口部3aの周長
1 と導体メッシュ4の開口部4aの周長L2 との比を
自然数で表したときに互いに5以上の素数にしているの
で、開口部3a,4aの開口寸法の最小公倍数となる波
の透過特性を大幅に低下させてタービンホイール2によ
り反射される波をかなり減衰することができ、この結
果、タービンホイール2からの反射波の低減効果をより
確実なものとすることができる。
Since the ratio of the circumference L 1 of the opening 3a of the conductor mesh 3 to the circumference L 2 of the opening 4a of the conductor mesh 4 is a natural number which is 5 or more when expressed as a natural number, The transmission characteristic of the wave which is the least common multiple of the opening size of the openings 3a and 4a can be significantly reduced, and the wave reflected by the turbine wheel 2 can be considerably attenuated. As a result, the reflected wave of the turbine wheel 2 can be reduced. The reduction effect can be made more reliable.

【0016】更に、インテークダクト1の内部にメッシ
ュ3,4を配設する構造を採用しているため、インテー
クダクト1の空気取入口からの空気の入路がストレート
になって吸入抵抗を小さくすることができる。
Furthermore, since the structure in which the meshes 3 and 4 are disposed inside the intake duct 1 is adopted, the air passage from the air intake of the intake duct 1 is straightened to reduce the suction resistance. be able to.

【0017】なお、導体メッシュ3,4の素材として
は、金属線材、金属板材、金属繊維、炭素繊維、或いは
低比抵抗セラミック繊維等の導体を始めとして、FRP
等の誘電体であっても導電コーティング等の導体化処理
を行えば適用可能である。
The material of the conductor meshes 3 and 4 may be a conductor such as a metal wire, a metal plate, a metal fiber, a carbon fiber, or a ceramic fiber having a low specific resistance.
It is possible to apply a dielectric material such as a conductive material by conducting a conductive coating.

【0018】また、導体メッシュ3,4の形態は網状の
他、平板材にスロットを開けたもの等でもよい。更に、
上記実施の形態では、導体メッシュ3,4の開口部3
a,4aを正方形状としているが、これに限定されず、
例えば開口部3a,4aを長方形やその他の形状にして
もよい。正方形以外の開口形状では素数の共振モードが
異なるため、透過波の周波数は異なる式によって導かれ
るが、本発明では複数の導体メッシュを併設することで
全ての波を散乱させるようにしているので、共振周波数
を求めることは重要ではない。
The shape of the conductor meshes 3 and 4 is not limited to a mesh shape, and may be a plate material having a slot in a plate material. Furthermore,
In the above embodiment, the openings 3 of the conductor meshes 3 and 4 are formed.
Although a and 4a have a square shape, they are not limited to this.
For example, the openings 3a and 4a may be rectangular or other shapes. Since the resonance mode of the prime number is different in an aperture shape other than a square, the frequency of the transmitted wave is derived by a different equation.However, in the present invention, all the waves are scattered by providing a plurality of conductor meshes in parallel, so that Determining the resonance frequency is not important.

【0019】[0019]

【発明の効果】上記の説明から明らかなように、請求項
1の発明によれば、筒体の形状に係わらず該筒体の内部
に周波数選択性を有する二枚の導体メッシュを配設する
だけで、電波反射体からの反射波を散乱させて到来方向
に返さないようにすることができるので、簡単且つ低コ
ストで該反射波の低減効果を得ることができる。
As is apparent from the above description, according to the first aspect of the present invention, two conductor meshes having frequency selectivity are arranged inside the cylindrical body regardless of the shape of the cylindrical body. With only this, the reflected wave from the radio wave reflector can be scattered so as not to return to the arrival direction, so that the effect of reducing the reflected wave can be obtained simply and at low cost.

【0020】請求項2の発明では、請求項1の発明に加
えて、各導体メッシュの開口部の開口寸法の最小公倍数
となる波の透過特性を大幅に低下させて電波反射体より
反射される波をかなり減衰することができるので、電波
反射体からの反射波の低減効果をより確実なものとする
ことができる。
According to the second aspect of the present invention, in addition to the first aspect, the transmission characteristic of a wave which is the least common multiple of the opening size of the opening of each conductor mesh is greatly reduced, and the wave is reflected from the radio wave reflector. Since the wave can be considerably attenuated, the effect of reducing the reflected wave from the radio wave reflector can be further ensured.

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

【図1】本発明の実施の一形態である反射電波散乱構造
を説明するための説明的断面図である。
FIG. 1 is an explanatory cross-sectional view illustrating a reflected radio wave scattering structure according to an embodiment of the present invention.

【図2】導体メッシュの部分的平面図である。FIG. 2 is a partial plan view of a conductor mesh.

【図3】他の導体メッシュの部分的平面図である。FIG. 3 is a partial plan view of another conductor mesh.

【図4】従来例の説明に用いる説明的断面図である。FIG. 4 is an explanatory sectional view used for explaining a conventional example.

【図5】従来の反射電波散乱構造を説明するための説明
的断面図である。
FIG. 5 is an explanatory cross-sectional view for explaining a conventional reflected radio wave scattering structure.

【図6】従来の他の反射電波散乱構造を説明するための
説明的断面図である。
FIG. 6 is an explanatory cross-sectional view for explaining another conventional reflected radio wave scattering structure.

【符号の説明】[Explanation of symbols]

1…インテークダクト(筒体) 2…タービンホイール(電波反射体) 3,4…導体メッシュ 3a,4a…開口部 4l1 ,4l2 …周長1 ... intake duct (tubular body) 2 ... turbine wheel (wave reflector) 3,4 ... conductor mesh 3a, 4a ... opening 4l 1, 4l 2 ... circumference

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 筒体の内部に配設された電波反射体の反
射電波散乱構造であって、前記筒体内の前記電波反射体
の前方位置に所定の間隔を存して設けられた複数の導体
メッシュを電波の到来方向に直角な面に対して所定角度
傾けて配置し、更に、各導体メッシュはそれぞれ一定の
大きさの複数の開口部を有し、且つ、各導体メッシュの
開口部の周長の比を自然数で表したときに互いに異なる
素数であることを特徴とする反射電波散乱構造。
1. A reflected radio wave scattering structure of a radio wave reflector disposed inside a cylinder, wherein a plurality of radio wave reflection structures are provided at predetermined positions in front of the radio wave reflector in the cylinder. The conductor mesh is arranged at a predetermined angle with respect to a plane perpendicular to the arrival direction of the radio wave, and further, each conductor mesh has a plurality of openings each having a fixed size, and the opening of each conductor mesh is formed. A reflected radio wave scattering structure characterized in that when the ratio of the perimeters is represented by a natural number, they are different prime numbers from each other.
【請求項2】 前記互いに異なる素数となる自然数が5
以上であることを特徴とする請求項1記載の反射電波散
乱構造。
2. A natural number which is a different prime number is 5
The reflected radio wave scattering structure according to claim 1, wherein:
JP27700197A 1997-10-09 1997-10-09 Reflected radio wave scattering structure Pending JPH11121972A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP27700197A JPH11121972A (en) 1997-10-09 1997-10-09 Reflected radio wave scattering structure

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP27700197A JPH11121972A (en) 1997-10-09 1997-10-09 Reflected radio wave scattering structure

Publications (1)

Publication Number Publication Date
JPH11121972A true JPH11121972A (en) 1999-04-30

Family

ID=17577389

Family Applications (1)

Application Number Title Priority Date Filing Date
JP27700197A Pending JPH11121972A (en) 1997-10-09 1997-10-09 Reflected radio wave scattering structure

Country Status (1)

Country Link
JP (1) JPH11121972A (en)

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US10830180B2 (en) 2015-06-16 2020-11-10 Ihi Corporation Engine aft section structure
CN112798560A (en) * 2020-12-24 2021-05-14 中国航空工业集团公司西安飞机设计研究所 Cavity inner wall scattering characteristic pre-estimation carrier

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010180756A (en) * 2009-02-04 2010-08-19 Ihi Corp Jet engine
WO2013008346A1 (en) * 2011-07-13 2013-01-17 東急建設株式会社 Partition structure and partition body
JP2013205235A (en) * 2012-03-28 2013-10-07 Mitsubishi Heavy Ind Ltd System and method for evaluating radio wave reflection characteristic
US10830180B2 (en) 2015-06-16 2020-11-10 Ihi Corporation Engine aft section structure
CN112798560A (en) * 2020-12-24 2021-05-14 中国航空工业集团公司西安飞机设计研究所 Cavity inner wall scattering characteristic pre-estimation carrier

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