JPH06334382A - Wave absorber - Google Patents
Wave absorberInfo
- Publication number
- JPH06334382A JPH06334382A JP5185594A JP5185594A JPH06334382A JP H06334382 A JPH06334382 A JP H06334382A JP 5185594 A JP5185594 A JP 5185594A JP 5185594 A JP5185594 A JP 5185594A JP H06334382 A JPH06334382 A JP H06334382A
- Authority
- JP
- Japan
- Prior art keywords
- absorber
- radio wave
- wave absorber
- area
- blowing
- 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.)
- Withdrawn
Links
Landscapes
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、電波暗室の内壁面等に
用いられる電波吸収体に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electromagnetic wave absorber used for an inner wall surface of an anechoic chamber.
【0002】[0002]
【従来の技術】EMC(Electro Magnetic Compatibili
ty)評価用の設備として電波暗室が広く用いられてお
り、一般に、電波暗室内の壁面や天井、床等には複数の
円錐状、三角錐状、四角錐状の電波吸収体が配置されて
いる。このような電波吸収体は、カーボンブラックを含
有する発泡ポリスチレンやカーボンブラックを含有する
ポリウレタンフォームなどから構成されている。2. Description of the Related Art EMC (Electro Magnetic Compatibili
ty) An anechoic chamber is widely used as a facility for evaluation, and in general, a plurality of cone-shaped, triangular-pyramidal, or quadrangular-pyramidal electromagnetic wave absorbers are placed on the walls, ceiling, or floor of the anechoic chamber. There is. Such a radio wave absorber is made of expanded polystyrene containing carbon black, polyurethane foam containing carbon black, or the like.
【0003】四角錐状(スラミッド型)吸収体01の第
1例を図5に示す。電波吸収体が円錐、三角錐、四角錐
等の形状となっているのは、電波の進行aに合わせて電
波吸収体の断面積を漸増させるためである。すなわち、
電波吸収体表面部(電波の到来方向)の断面積が小さけ
れば、そこでの等価的な導電率及び誘電率が小さくなっ
て表面部での入射電波の反射が抑制されて電波は吸収体
内部に進入しやすくなり、吸収体内部に進入した電波は
吸収体断面積の漸増とともに等価的に導電率及び誘電率
が大きくなる吸収体を含んだ空間によって効率よく熱エ
ネルギーに変換されて吸収される。FIG. 5 shows a first example of a quadrangular pyramid (sramid type) absorber 01. The reason why the radio wave absorber is in the shape of a cone, a triangular pyramid, a quadrangular pyramid, or the like is to gradually increase the cross-sectional area of the radio wave absorber in accordance with the progress a of the radio wave. That is,
If the cross-sectional area of the surface of the radio wave absorber (direction of arrival of radio waves) is small, the equivalent electric conductivity and permittivity there will be small, and the reflection of incident radio waves on the surface will be suppressed, so that the radio waves will enter Radio waves that enter the absorber easily enter the absorber and are efficiently converted into thermal energy and absorbed by the space containing the absorber whose conductivity and dielectric constant are equivalently increased as the absorber cross section gradually increases.
【0004】第2例の吸収体02を図7および図8に示
す。波型の電波吸収材02aの谷d部に嵌合するくさび
型の電波透明材03を複数挿入し、図8のように錐体型
凹みを形成したものである。これにより、電波吸収材0
2aの形状が保持されている。また、上記とほぼ同様に
作用し電波が吸収される。A second example of the absorber 02 is shown in FIGS. 7 and 8. A plurality of wedge-shaped radio wave transparent materials 03 that fit into the valleys d of the wave-shaped radio wave absorber 02a are inserted to form cone-shaped recesses as shown in FIG. As a result, the radio wave absorber 0
The shape of 2a is retained. In addition, the function is almost the same as above, and the radio wave is absorbed.
【0005】[0005]
【発明が解決しようとする課題】上記従来の第1例の電
波吸収体の性能は錐体の高さに大きく依存しており、一
般にその高さは吸収すべき電波の波長の1/2〜1/3
以上が必要とされている。例えば、周波数50MHz
(波長6m)の電波を吸収するための図5のピラミッド
高さは2m〜3mにもなり、壁面に取り付けた場合に図
6に示すように自重によって先端が垂れ下がって錐体が
変形してしまい、所期の電波吸収性能が得られないとい
う問題点があった。The performance of the radio wave absorber of the above-mentioned first example largely depends on the height of the cone, and the height is generally 1/2 to the wavelength of the radio wave to be absorbed. 1/3
More is needed. For example, frequency 50MHz
The height of the pyramid in FIG. 5 for absorbing the radio wave of (wavelength 6 m) becomes 2 to 3 m, and when it is attached to the wall surface, the tip hangs down due to its own weight and the cone is deformed as shown in FIG. However, there is a problem that the desired electromagnetic wave absorption performance cannot be obtained.
【0006】また第2例の電波吸収体02は、くさび型
の電波透明材03が電波を吸収しないので吸収性能が余
りよくなかった。また多数の透明材03を挿入し、接着
しなければならないので製作工数がかかるという問題点
があった。Further, the radio wave absorber 02 of the second example is not so good in absorption performance because the wedge-shaped radio wave transparent material 03 does not absorb radio waves. Further, since many transparent materials 03 have to be inserted and adhered, there is a problem that the number of manufacturing steps is increased.
【0007】[0007]
【課題を解決するための手段】本発明は上記課題を解決
するため次の手段を講ずる。The present invention takes the following means in order to solve the above problems.
【0008】すなわち、カーボンブラック含浸の発泡プ
ラスチックス製の電波吸収体において、その表面に軸が
ほぼ垂直に配列された複数の錐体型凹みを設けた。That is, in a radio wave absorber made of foamed plastics impregnated with carbon black, a plurality of cone-shaped recesses whose axes are arranged substantially vertically are provided on the surface thereof.
【0009】[0009]
【作用】上記手段において、電波が電波吸収体の面にほ
ぼ垂直に進行してくる。錐体型凹みにより電波吸収体表
面部の断面積は十分小さくなって、そこでの入射電波の
反射は抑制される。また、吸収体内部の進入した電波は
進入深さとともに等価的に導電率及び誘電率が漸増する
吸収体を含んだ空間内で、効率良く熱エネルギーに変換
される。このとき、電波吸収体はその表面に形成する錐
体型凹みによって定まる構造を有しており(例えば、凹
面が正四角錐状のときは格子構造、凹面が正六角錐状の
ときはハニエム構造)、吸収体が自重によって垂れ下
り、錐体型凹み形状が変形して所期の吸収性能が得られ
ないという従来からの問題点は発生しない。In the above means, the radio wave propagates almost perpendicularly to the surface of the radio wave absorber. The cone-shaped recess sufficiently reduces the cross-sectional area of the surface of the radio wave absorber and suppresses the reflection of incident radio waves there. In addition, the radio waves that have entered the absorber are efficiently converted into thermal energy in the space containing the absorber whose conductivity and dielectric constant are equivalently increased with the penetration depth. At this time, the radio wave absorber has a structure defined by a cone-shaped recess formed on the surface (for example, a lattice structure when the concave surface is a regular quadrangular pyramid, a Haniem structure when the concave surface is a regular hexagonal pyramid), The conventional problem that the body hangs down by its own weight and the shape of the cone-shaped recess is deformed and the desired absorption performance cannot be obtained does not occur.
【0010】また、電波吸収体部に進入した電波に対す
る吸収体断面積の増大は、従来例の電波吸収体02より
も大きくなるため、電波吸収性能が向上する。Further, since the increase in the cross-sectional area of the absorber with respect to the radio wave entering the radio wave absorber portion is larger than that of the radio wave absorber 02 of the conventional example, the radio wave absorbing performance is improved.
【0011】[0011]
【実施例】(1) 本発明の第1実施例を図1により説
明する。表面bに、軸を垂直にし、かつ各底辺を隣接し
て四角錐体型凹み2を有する電波吸収体1が形成され
る。電波吸収体1はカーボンブラックを含浸したポリウ
レタン、発泡スチロール、プラスチック等の発泡体、す
なわち発泡プラスチック製である。Embodiments (1) A first embodiment of the present invention will be described with reference to FIG. An electromagnetic wave absorber 1 having a quadrangular pyramid-shaped recess 2 is formed on the surface b with its axis perpendicular to each other and adjacent to each base. The radio wave absorber 1 is made of foamed material such as polyurethane impregnated with carbon black, styrofoam, and plastic, that is, foamed plastic.
【0012】以上において、電波が表面bにほぼ垂直に
進入aする。吸収体1の表面の面積は3で示した格子状
部の面積であり、隣りあった四角錐体型凹み2を互いに
接しあうように設けることにより、十分小さな値とする
ことができる。十分小さな表面積を有する吸収体1に入
射した電波は四角錐体型凹み2の斜面によって複数回の
反射を繰返しながら吸収体内部に進入し、熱エネルギー
に変換(吸収)されてゆく。ここで、四角錐体型凹み2
の形状は、吸収対象とする電波の波長、電波吸収体の製
造、取り付け作業の難易度等を考慮して決定することが
できる。In the above, the radio wave enters the surface b almost vertically. The area of the surface of the absorber 1 is the area of the lattice-shaped portion indicated by 3, and it can be made a sufficiently small value by providing the adjacent quadrangular pyramidal recesses 2 so as to be in contact with each other. The radio wave that has entered the absorber 1 having a sufficiently small surface area enters the absorber while being repeatedly reflected multiple times by the slope of the quadrangular pyramid-shaped recess 2 and is converted (absorbed) into thermal energy. Here, the quadrangular pyramid-shaped recess 2
The shape of can be determined in consideration of the wavelength of the radio wave to be absorbed, the difficulty of manufacturing and mounting the radio wave absorber, and the like.
【0013】側壁として電波吸収体1の裏面cを電波暗
室内壁面に設置したときの吸収体1表面は格子状となっ
ており、自重によりダレて変形し、吸収体の性能が悪く
なるという問題は発生しない。When the back surface c of the electromagnetic wave absorber 1 is installed as a side wall on the wall surface of the anechoic chamber, the surface of the absorber 1 has a lattice shape and is deformed by its own weight to deteriorate the performance of the absorber. Does not occur.
【0014】また一体成形が容易にでき、コストダウン
が図れる。Further, integral molding can be easily carried out and the cost can be reduced.
【0015】本実施例(図1)で、開口幅L1 =8イン
チ、深さL2 =20インチ、底部厚さL3 =4インチと
した場合と、第1の従来例(図5)で、吸収体01の幅
L1′=L1 、高さL2 ′=L2 、底部厚さL3 ′=L
3 とした場合の電波性能の実測結果は、前者が−48d
Bであり、後者が−32dBであった。この結果より本
実施例が極めて優れていることが判る。 (2) 本発明の第2実施例を図2に示す。前記の四角
錐体型凹みを三角錐体型凹み4としたものである。 (3) 本発明の第3実施例を図3に示す。第1実施例
の四角錐体型凹みを正六角錐体型凹み5としたものであ
る。 (4) 本発明の第4実施例を図4に示す。第1実施例
の四角錐体型凹みを円錐体型凹み6としたものである。In this embodiment (FIG. 1), the opening width L 1 = 8 inches, the depth L 2 = 20 inches, and the bottom portion thickness L 3 = 4 inches, and the first conventional example (FIG. 5). Then, the width L 1 ′ = L 1 , the height L 2 ′ = L 2 , and the bottom thickness L 3 ′ = L of the absorbent body 01.
The actual measurement result of the radio performance when the value is 3 is -48d for the former.
B, and the latter was -32 dB. From this result, it can be seen that this example is extremely excellent. (2) A second embodiment of the present invention is shown in FIG. The above-mentioned quadrangular pyramid-shaped recess is made into a triangular-pyramidal recess 4. (3) A third embodiment of the present invention is shown in FIG. The quadrangular pyramidal recess of the first embodiment is replaced by a regular hexagonal pyramid recess 5. (4) FIG. 4 shows a fourth embodiment of the present invention. The quadrangular pyramidal recess of the first embodiment is replaced with a conical recess 6.
【0016】なお、錐体型凹みの形状は前記以外のもの
でもよい。またこれらの組合せでもよい。The shape of the conical recess may be other than the above. Also, a combination of these may be used.
【0017】[0017]
【発明の効果】以上に説明したように、本発明によれ
ば、複数の錐体型凹みを設けたため、電波吸収性能が高
い。また、壁面に設置した場合、自重によって垂れ下
り、形状が変形するということがないため、吸収体本来
の性能を損なうことなく使用することができる。さらに
一体成形が容易にできる。As described above, according to the present invention, since a plurality of cone-shaped recesses are provided, the electromagnetic wave absorption performance is high. Further, when it is installed on the wall surface, it does not hang down due to its own weight and its shape is not deformed, so that it can be used without impairing the original performance of the absorber. Further, integral molding can be easily performed.
【図1】本発明の第1実施例に係る電波吸収体の斜視図
である。FIG. 1 is a perspective view of a radio wave absorber according to a first embodiment of the present invention.
【図2】本発明の第2実施例に係る電波吸収体の表面形
状図である。FIG. 2 is a surface shape diagram of a radio wave absorber according to a second embodiment of the present invention.
【図3】本発明の第3実施例に係る電波吸収体の表面形
状図である。FIG. 3 is a surface shape diagram of a radio wave absorber according to a third embodiment of the present invention.
【図4】本発明の第4実施例に係る電波吸収体の表面形
状図である。FIG. 4 is a surface shape diagram of a radio wave absorber according to a fourth embodiment of the present invention.
【図5】従来例の第1例の電波吸収体の斜視図である。FIG. 5 is a perspective view of a radio wave absorber of a first example of a conventional example.
【図6】同従来例の作用説明図である。FIG. 6 is a diagram for explaining the operation of the conventional example.
【図7】従来例の第2例の電波吸収体の分解斜視図であ
る。FIG. 7 is an exploded perspective view of a radio wave absorber of a second example of the related art.
【図8】同従来例の電波吸収体の斜視図である。FIG. 8 is a perspective view of a radio wave absorber of the conventional example.
1 電波吸収体 2 四角錐体型凹み 1 Radio wave absorber 2 Square pyramid-shaped recess
───────────────────────────────────────────────────── フロントページの続き (72)発明者 平田 誠裕 広島市西区観音新町四丁目6番22号 三菱 重工業株式会社広島製作所内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Masahiro Hirata 4-22 Kannon Shinmachi, Nishi-ku, Hiroshima City Mitsubishi Heavy Industries Ltd. Hiroshima Works
Claims (1)
クス製の電波吸収体において、その表面に軸がほぼ垂直
に配列された複数の錐体型凹みを有することを特徴とす
る電波吸収体。1. A radio wave absorber made of foamed plastics impregnated with carbon black, characterized in that it has a plurality of cone-shaped recesses whose axes are arranged substantially perpendicularly to the surface thereof.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5185594A JPH06334382A (en) | 1993-03-23 | 1994-03-23 | Wave absorber |
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6383993 | 1993-03-23 | ||
JP5-63839 | 1993-03-23 | ||
JP5185594A JPH06334382A (en) | 1993-03-23 | 1994-03-23 | Wave absorber |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH06334382A true JPH06334382A (en) | 1994-12-02 |
Family
ID=26392437
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5185594A Withdrawn JPH06334382A (en) | 1993-03-23 | 1994-03-23 | Wave absorber |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH06334382A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0980758A2 (en) | 1998-08-19 | 2000-02-23 | Canon Kabushiki Kaisha | Printing head, head cartridge having printing head, printing apparatus using printing head, and printing head substrate |
WO2019077808A1 (en) | 2017-10-19 | 2019-04-25 | 関西ペイント株式会社 | Milliwave band radio wave absorption sheet and milliwave radio wave absorption method |
-
1994
- 1994-03-23 JP JP5185594A patent/JPH06334382A/en not_active Withdrawn
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0980758A2 (en) | 1998-08-19 | 2000-02-23 | Canon Kabushiki Kaisha | Printing head, head cartridge having printing head, printing apparatus using printing head, and printing head substrate |
WO2019077808A1 (en) | 2017-10-19 | 2019-04-25 | 関西ペイント株式会社 | Milliwave band radio wave absorption sheet and milliwave radio wave absorption method |
US11509061B2 (en) | 2017-10-19 | 2022-11-22 | Kansai Paint Co., Ltd. | Milliwave band radio wave absorption sheet and milliwave radio wave absorption method |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
A300 | Withdrawal of application because of no request for examination |
Free format text: JAPANESE INTERMEDIATE CODE: A300 Effective date: 20010605 |