JP2007067395A - Radio wave absorber, method of fabricating the same, and anechoic chamber - Google Patents

Radio wave absorber, method of fabricating the same, and anechoic chamber Download PDF

Info

Publication number
JP2007067395A
JP2007067395A JP2006215125A JP2006215125A JP2007067395A JP 2007067395 A JP2007067395 A JP 2007067395A JP 2006215125 A JP2006215125 A JP 2006215125A JP 2006215125 A JP2006215125 A JP 2006215125A JP 2007067395 A JP2007067395 A JP 2007067395A
Authority
JP
Japan
Prior art keywords
wave absorber
radio wave
hollow
opening
shape
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.)
Granted
Application number
JP2006215125A
Other languages
Japanese (ja)
Other versions
JP4825074B2 (en
Inventor
Hiroshi Kurihara
弘 栗原
Hisafumi Saito
寿文 齋藤
Yoshinori Kasabo
美紀 笠坊
Toru Sugawara
透 菅原
Takashi Tagami
貴士 田上
Kazuya Matsumura
一也 松村
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.)
TDK Corp
Toray Industries Inc
Original Assignee
TDK Corp
Toray Industries Inc
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 TDK Corp, Toray Industries Inc filed Critical TDK Corp
Priority to JP2006215125A priority Critical patent/JP4825074B2/en
Publication of JP2007067395A publication Critical patent/JP2007067395A/en
Application granted granted Critical
Publication of JP4825074B2 publication Critical patent/JP4825074B2/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
  • Aerials With Secondary Devices (AREA)

Abstract

<P>PROBLEM TO BE SOLVED: To obtain a radio wave absorber which can achieve low cost, a small transportation volume, an excellent radio wave absorbing characteristic from a low frequency to a high frequency with a short length, a small or no difference in the characteristic of a polarization plane, and can be easily fabricated and worked. <P>SOLUTION: In a radio wave absorber 10, four hollow tetrahedrons 20 each of which has one open surface are connected such that a surface 20a opposed to the open surface of the hollow tetrahedron 20 forms a side of a hollow pyramid 22. The radio wave absorber 10 is composed of a radio wave absorbing member shaped like a thin plate. The radio wave absorbing member shaped like a thin plate preferably has a corrugated cardboard structure in which at least one sheet contains a conductive material. <P>COPYRIGHT: (C)2007,JPO&INPIT

Description

本発明は、電波暗室等の用途に好適に使用可能な電波吸収体及びその製造方法、並びに電波暗室に関する。   The present invention relates to an electromagnetic wave absorber that can be suitably used for applications such as an anechoic chamber, a method for manufacturing the same, and an anechoic chamber.

各種電子機器から放射される電磁波ノイズの測定や、外来電磁波ノイズに対する電子機器の耐性評価を行う試験場としてEMC用電波暗室が広く実用化されている。また近年、放射ノイズ測定用のアンテナを校正する場(CALTS = Calibration Test Site)として前記電波暗室を用いる動きがある。   An electromagnetic anechoic chamber for EMC is widely used as a test site for measuring electromagnetic noise radiated from various electronic devices and evaluating the resistance of electronic devices against external electromagnetic noise. In recent years, there has been a movement to use the anechoic chamber as a place (CALTS = Calibration Test Site) for calibrating an antenna for measuring radiation noise.

EMC用電波暗室の天井、壁には電波吸収体が設置され、床面(金属面)以外からの電波反射が極めて小さい空間を実現している。EMC用電波暗室の天井、壁に使用する電波吸収体としては、図20のように磁性損失材料からなる電波吸収材としてのフェライト焼結体1と、導電性材料を含む電波吸収体2とを組み合わせた複合型電波吸収体が現在多く用いられている。   Electromagnetic wave absorbers are installed on the ceiling and walls of the electromagnetic wave anechoic chamber for EMC, and a space where electromagnetic wave reflection from other than the floor (metal surface) is extremely small is realized. As the electromagnetic wave absorber used for the ceiling and wall of the electromagnetic wave anechoic chamber for EMC, a ferrite sintered body 1 as an electromagnetic wave absorber made of a magnetic loss material and an electromagnetic wave absorber 2 containing a conductive material as shown in FIG. Combined composite wave absorbers are currently widely used.

導電性材料を含む電波吸収体としては、発泡ポリスチロールや発泡ポリウレタン等の基材(低誘電率誘電体)にカーボンやグラファイト等の導電性材料を保持させ、ピラミッド形やくさび形としたものが従来からよく用いられている。この電波吸収体の長さは通常0.5〜2m程度であり、大型で高性能な電波暗室ほど長いものが用いられる。このため、電波吸収体の体積がかさばり、輸送コストや施工コストが高いという問題がある。   As a radio wave absorber including a conductive material, a base material (low dielectric constant dielectric) such as foamed polystyrene or foamed polyurethane is used to hold a conductive material such as carbon or graphite, and a pyramid or wedge shape is used. It has been frequently used in the past. The length of this electromagnetic wave absorber is usually about 0.5 to 2 m, and a larger and higher performance anechoic chamber is longer. For this reason, there exists a problem that the volume of a radio wave absorber is bulky and the transportation cost and construction cost are high.

そこで、材料減による低コスト化、輸送体積減、軽量化、施工容易性のために、上記電波吸収体を、導電性材料を含む薄板状の電波吸収材からなる中空構造とし、薄板状態で輸送し、現場で組み立てる電波吸収体が提案されている。   Therefore, in order to reduce costs by reducing material, reduce transport volume, light weight, and ease of construction, the above wave absorber is made into a hollow structure made of a thin plate wave absorber containing a conductive material and transported in a thin plate state. However, radio wave absorbers assembled on site have been proposed.

上記中空構造の電波吸収体としては、図21(A),(B)の中空ピラミッド形や、図22(A),(B),図23(A),(B)の中空くさび形がある。図21、図22及び図23中、1はフェライト焼結体、2はその前面に配置された中空の導電性材料を含む電波吸収体である。図23(A),(B)の中空くさび形は側面(三角形面)が開口面となっている。   The hollow structure wave absorber includes the hollow pyramid shape of FIGS. 21A and 21B and the hollow wedge shape of FIGS. 22A, 22B, 23A, and 23B. . 21, 22, and 23, 1 is a ferrite sintered body, and 2 is a radio wave absorber including a hollow conductive material disposed on the front surface thereof. The side surfaces (triangular surfaces) of the hollow wedge shape shown in FIGS.

下記特許文献1,2は中空の導電性材料を含む電波吸収体の公知技術の例である。
特開平11−87978号公報 特開2000−216584号公報
The following Patent Documents 1 and 2 are examples of known techniques for a radio wave absorber including a hollow conductive material.
JP-A-11-87978 Japanese Patent Laid-Open No. 2000-216584

また、下記特許文献3,4のように、四角筒状の電波吸収体や、電波吸収板を十文字に交差させた電波吸収体も開示されている。
特開平2−97096号公報 特開2001−127483号公報
Further, as in Patent Documents 3 and 4 below, a rectangular tube-shaped radio wave absorber and a radio wave absorber in which a radio wave absorber plate is crossed in a cross shape are also disclosed.
Japanese Patent Laid-Open No. 2-97096 JP 2001-127383 A

ところで、前記くさび形電波吸収体は到来電波の偏波面に対して異方性を有するために、到来電波の偏波面による特性差が生じる。特に薄板状の電波吸収材からなる中空くさび形の場合、偏波面特性差が非常に大きく、電波の偏波面に対してくさび形の稜線が垂直の場合の高周波特性が極めて低いという問題がある。偏波面による特性差の問題を解決するため、壁面取り付け時に、隣り合う電波吸収体のくさび形の稜線が互いに直角となるように配列し、電波の偏波面に対してくさび形の稜線が平行の場合と垂直の場合の平均的な特性となるようにする方法がある。しかし、高周波においては一方の特性(電波の偏波面に対してくさび形の稜線が垂直の場合)が極めて低いため、平均的な特性もやはり低くなってしまう。また、側壁面に上記のごとく配列する場合には、くさび形の稜線が水平となるように配置される電波吸収体が半数存在するが、この配置の場合、長さが長くなるとたわむ等の強度上の問題がある。これらの問題は、コストや製造性、施工性ではより有利な図23(A),(B)の側面開口タイプにおいてより顕著となる。   By the way, since the wedge-shaped wave absorber has anisotropy with respect to the polarization plane of the incoming radio wave, a characteristic difference occurs due to the polarization plane of the incoming radio wave. In particular, in the case of a hollow wedge shape made of a thin plate-shaped electromagnetic wave absorber, there is a problem that the polarization characteristic difference is very large, and the high-frequency characteristic is extremely low when the wedge-shaped ridge line is perpendicular to the polarization plane of the radio wave. In order to solve the problem of characteristic difference due to the polarization plane, the wedge-shaped ridgelines of adjacent radio wave absorbers are arranged at right angles to each other when the wall is mounted, and the wedge-shaped ridgelines are parallel to the plane of polarization of the radio wave. There is a method of achieving an average characteristic in the case of vertical and vertical. However, since one characteristic (when the wedge-shaped ridge line is perpendicular to the plane of polarization of radio waves) is extremely low at high frequencies, the average characteristic is also low. In addition, when arranged on the side wall surface as described above, half of the electromagnetic wave absorbers are arranged so that the wedge-shaped ridge line is horizontal, but in this arrangement, the strength such as bending when the length becomes long There is a problem above. These problems become more conspicuous in the side opening type of FIGS. 23A and 23B, which is more advantageous in terms of cost, manufacturability, and workability.

一方、中空ピラミッド形の場合、偏波面特性差がなく強度的にも強いためよく用いられるが、中空くさび形に比べ30〜100MHzの低周波特性が劣るため、吸収体長さを長くする必要があるという問題があった。   On the other hand, the hollow pyramid type is often used because it has no polarization plane characteristic difference and is strong in strength. However, since the low frequency characteristic of 30 to 100 MHz is inferior to the hollow wedge type, it is necessary to increase the absorber length. There was a problem.

そこで、偏波面特性差がなく、30〜100MHzの低周波特性が良好な電波吸収体として中空の錐状体の先端に開口を設けた形状が本出願人から下記特許文献5として提案されている。
特願2004−161112号
Therefore, the present applicant has proposed a shape in which an opening is provided at the tip of a hollow cone as an electromagnetic wave absorber having no difference in polarization plane characteristics and good low frequency characteristics of 30 to 100 MHz. .
Japanese Patent Application No. 2004-161112

しかし、特許文献5に示した中空の錐状体の先端に開口を設けた形状の電波吸収体の問題点として、高い周波数においては、電波が開口部を通り抜けてフェライト焼結体に到達するが、1GHz以上の高周波ではフェライト焼結体の吸収性能は低いため、反射が大きくなる。従って、高周波特性改善のため底部に電波吸収体を付加する必要があり、薄板状としたメリットが十分活かせない。   However, as a problem of the radio wave absorber having an opening at the tip of the hollow cone shown in Patent Document 5, at a high frequency, the radio wave passes through the opening and reaches the ferrite sintered body. At a high frequency of 1 GHz or higher, the ferrite sintered body has a low absorption performance, so that reflection increases. Accordingly, it is necessary to add a radio wave absorber to the bottom for improving the high frequency characteristics, and the merit of the thin plate cannot be fully utilized.

同様に、特許文献3の四角筒状のものや、特許文献4の電波吸収板を十文字に交差させたものについてもフェライト焼結体が露出しているため高周波特性が良くないという問題がある。高周波特性改善のためには、四角筒の目開きを小さくしたり、十文字の電波吸収板の底部に小型電波吸収体を付加する必要があり、やはり薄板状としたメリットが十分活かせない。   Similarly, the rectangular cylindrical shape disclosed in Patent Document 3 and those obtained by crossing the radio wave absorbing plate disclosed in Patent Document 4 in a cross shape also have a problem that the high frequency characteristics are not good because the ferrite sintered body is exposed. In order to improve the high-frequency characteristics, it is necessary to reduce the opening of the square tube or to add a small wave absorber to the bottom of the crossed wave absorber, and the advantages of the thin plate cannot be fully utilized.

本発明は、かかる問題点に鑑みてなされたもので、低コストで、輸送体積が小さく、短い長さで低周波から高周波まで良好な電波吸収特性が得られ、偏波面特性差が無いか若しくは少なく、軽量で構造強度の強い、製造や施工が容易な電波吸収体及びその製造方法を提供することを目的とする。   The present invention has been made in view of such problems, is low in cost, has a small transport volume, has a short length, has good radio wave absorption characteristics from low to high frequencies, and has no difference in polarization plane characteristics or An object of the present invention is to provide a radio wave absorber that is light in weight, strong in structural strength, easy to manufacture and install, and a manufacturing method thereof.

また、本発明は、上記電波吸収体を用いることで、低コストで施工が容易で電波吸収性能の優れた電波暗室を提供することをもう一つの目的とする。   Another object of the present invention is to provide an anechoic chamber that is inexpensive and easy to construct and has excellent radio wave absorption performance by using the radio wave absorber.

本発明のその他の目的や新規な特徴は後述の実施の形態において明らかにする。   Other objects and novel features of the present invention will be clarified in embodiments described later.

上記目的を達成するために、第1発明に係る電波吸収体は、一面開口の中空四面体の3個以上を、該中空四面体の開口面に対向する面が中空角錐の側面を形成するように連結した形状を有することを特徴としている。   In order to achieve the above object, the radio wave absorber according to the first aspect of the present invention is configured so that three or more hollow tetrahedrons having one opening are formed, and a surface facing the opening surface of the hollow tetrahedron forms a side surface of a hollow pyramid. It has the shape connected with.

第2発明に係る電波吸収体は、一面開口の中空四面体の3個以上を、該中空四面体の開口面が中空角錐の側面を形成するように連結した形状を有することを特徴としている。   The radio wave absorber according to the second invention is characterized in that it has a shape in which three or more hollow tetrahedrons having a single opening are connected so that the opening surfaces of the hollow tetrahedrons form the side surfaces of a hollow pyramid.

第3発明に係る電波吸収体は、第1又は第2発明において、前記中空角錐の外側に形成されたくさび形部分の先端側稜線の長さは、前記中空角錐の底辺の長さの半分よりも短いことを特徴としている。   According to a third aspect of the present invention, in the first or second aspect, the length of the ridge line on the tip side of the wedge-shaped portion formed outside the hollow pyramid is half the length of the bottom of the hollow pyramid. Is also characterized by shortness.

第4発明に係る電波吸収体は、第1、第2又は第3発明において、前記中空四面体が4個連結した形状であることを特徴としている。   A radio wave absorber according to a fourth invention is characterized in that, in the first, second or third invention, the hollow tetrahedron is connected to four pieces.

第5発明に係る電波吸収体は、第1、第2、第3又は第4発明において、薄板状の電波吸収材からなることを特徴としている。   A radio wave absorber according to a fifth invention is characterized in that, in the first, second, third or fourth invention, the radio wave absorber is made of a thin plate-like radio wave absorber.

第6発明に係る電波吸収体は、第5発明において、前記薄板状の電波吸収材は少なくとも1枚のシートが導電性材料を含む段ボール構造であることを特徴としている。   According to a sixth aspect of the present invention, there is provided the radio wave absorber according to the fifth aspect, wherein the thin plate-shaped radio wave absorber has a cardboard structure in which at least one sheet includes a conductive material.

第7発明に係る電波吸収体は、第5又は第6発明において、前記薄板状の電波吸収材の基材が難燃性または不燃性を有することを特徴としている。   The radio wave absorber according to a seventh aspect of the present invention is characterized in that, in the fifth or sixth aspect of the invention, the thin plate-like base material of the radio wave absorber has flame retardancy or incombustibility.

第8発明に係る電波吸収体は、第1、第2、第3、第4、第5、第6又は第7発明において、前記中空角錐の底面にフェライト焼結体が配置されていることを特徴としている。   The radio wave absorber according to an eighth aspect of the present invention is the first, second, third, fourth, fifth, sixth or seventh aspect, wherein a ferrite sintered body is disposed on the bottom surface of the hollow pyramid. It is a feature.

第9発明に係る電波吸収体の製造方法は、薄板状の電波吸収材を2箇所折り曲げて一面開口の中空四面体を3個以上作製し、該中空四面体の開口面に対向する面が中空角錐の側面を形成するように連結することを特徴としている。   According to a ninth aspect of the present invention, there is provided a method of manufacturing a radio wave absorber, wherein two or more thin tetrahedral wave absorbers are folded to produce three or more hollow tetrahedrons having a single-sided opening, and the surface facing the open surface of the hollow tetrahedron is hollow. It is characterized by being connected so as to form a side surface of a pyramid.

第10発明に係る電波吸収体の製造方法は、一面開口の中空四面体の3個以上を、該中空四面体の開口面に対向する三角形面が中空角錐の側面を形成するように連結した形状を有する電波吸収体の製造方法であって、
第1の中空四面体の開口面に対向する三角形面となる第1領域と、前記第1の中空四面体に隣接する第2の中空四面体の開口面に対向する三角形面から立ち上がる逆三角形面となる第2領域とを含む第1の薄板状の電波吸収材と、
前記第1の中空四面体の開口面に対向する三角形面から立ち上がる逆三角形面を含む第2の薄板状の電波吸収材とを用い、
前記第1の薄板状の電波吸収材の第1領域と第2領域の境界位置に、前記第2の薄板状の電波吸収材を接合したものを3個以上連結することを特徴としている。
A method for manufacturing a radio wave absorber according to a tenth aspect of the invention includes a shape in which three or more hollow tetrahedrons having a single open surface are connected such that a triangular surface facing the open surface of the hollow tetrahedron forms a side surface of a hollow pyramid. A method of manufacturing a radio wave absorber having
A first region that is a triangular surface that faces the opening surface of the first hollow tetrahedron, and an inverted triangular surface that rises from the triangular surface that faces the opening surface of the second hollow tetrahedron adjacent to the first hollow tetrahedron. A first thin-plate wave absorber including a second region to be
Using a second thin-plate-shaped wave absorber including an inverted triangular surface rising from a triangular surface facing the opening surface of the first hollow tetrahedron,
Three or more of the first thin-plate wave absorbers joined to the first region and the second region of the first thin-plate wave absorber are connected to each other.

第11発明に係る電波吸収体の製造方法は、薄板状の電波吸収材を2箇所折り曲げて一面開口の中空四面体を3個以上作製し、該中空四面体の開口面が中空角錐の側面を形成するように連結することを特徴としている。   According to an eleventh aspect of the present invention, there is provided a method of manufacturing a radio wave absorber, comprising bending a thin plate-shaped radio wave absorber at two locations to produce three or more hollow tetrahedrons having one opening, and the open surface of the hollow tetrahedron has a side surface of a hollow pyramid. It is characterized by being connected so as to form.

第12発明に係る電波暗室は、室内側側壁面、天井面の少なくとも一面に第1発明から第8発明のいずれかに記載の電波吸収体を配設したことを特徴としている。
また、第13発明に係る薄板状電波吸収材は、三角形面となる部分の境界線に沿って折り曲げる場合に、一面開口の中空四面体となるようにしたことを特徴としている。
第14発明に係る薄板状電波吸収材は、左右対称の台形の上辺又は底辺から、前記上辺又は底辺と等しい長さの底辺を持つ二等辺三角形を切り欠いた形状、又は左右対称の台形の上辺又は底辺に、前記上辺又は底辺と等しい長さの底辺を持つ二等辺三角形を足した五角形状を有している、又は取り出し可能に配置したことを特徴としている。
第15発明に係る薄板状電波吸収材は、二等辺三角形と、当該二等辺三角形の二等辺を共有する2つの三角形とを当該二等辺において折り曲げ可能に連結した形状を有する、又は取り出し可能に配置したことを特徴としている。
なお、第13、14又は15発明の電波吸収材において、嵌め合わせのための切欠又は突起が設けられていてもよい。
第17発明に係る電波吸収材は、一面開口の中空四面体形状であることを特徴としている。
An anechoic chamber according to a twelfth aspect is characterized in that the electromagnetic wave absorber according to any one of the first to eighth aspects is disposed on at least one of the indoor side wall surface and the ceiling surface.
In addition, the thin plate-like electromagnetic wave absorber according to the thirteenth aspect of the invention is characterized in that it is a hollow tetrahedron with one opening when it is bent along the boundary line of the portion that becomes a triangular surface.
The thin plate-shaped electromagnetic wave absorber according to the fourteenth aspect of the invention is a shape obtained by cutting out an isosceles triangle having a base having a length equal to the upper side or the base from the top or bottom of a symmetrical trapezoid, or the upper side of a symmetrical trapezoid Alternatively, the base has a pentagonal shape in which an isosceles triangle having a base equal to the length of the upper side or the base is added to the base, or is arranged so as to be removable.
The thin plate-like electromagnetic wave absorber according to the fifteenth aspect of the present invention has a shape in which an isosceles triangle and two triangles sharing the isosceles of the isosceles triangle are connected so as to be bendable at the isosceles, or arranged so as to be removable It is characterized by that.
In the radio wave absorber of the thirteenth, fourteenth, or fifteenth inventions, notches or protrusions for fitting may be provided.
The radio wave absorber according to the seventeenth aspect of the present invention is characterized by a hollow tetrahedron shape having an opening on one side.

本発明に係る電波吸収体は、一面開口の中空四面体の3個以上を連結した形状であって、薄板状の電波吸収材を折り曲げて形成可能であり、薄板状の電波吸収材として輸送することで輸送体積を小さくできる。また段ボール構造で低コストの電波吸収材を用いることが可能であり、軽量で構造強度を強くでき、製造や電波暗室等に対する施工が容易となる。   The radio wave absorber according to the present invention has a shape in which three or more hollow tetrahedrons having a single opening are connected, and can be formed by bending a thin plate wave absorber, and is transported as a thin plate wave absorber. Thus, the transport volume can be reduced. Moreover, it is possible to use a low-cost radio wave absorber with a cardboard structure, which is lightweight and strong in structural strength, and can be easily manufactured and installed in an anechoic chamber.

本発明に係る電波吸収体の製造方法によれば、薄板状の電波吸収材の折り曲げ加工及び両面接着テープや接着剤等による連結加工によって電波吸収体を組立可能である。組立に際して特殊な用具、部品は不要であり、電波暗室等への施工が容易である。   According to the method for manufacturing a radio wave absorber according to the present invention, the radio wave absorber can be assembled by bending a thin plate-like radio wave absorber and connecting with a double-sided adhesive tape or an adhesive. No special tools or parts are required for assembly, and installation in an anechoic chamber is easy.

また、本発明に係る電波吸収体の外観形状は、角錐の外側にくさび形部分を設けたものに相当し、ピラミッド形に比較して低周波から高周波まで良好な電波吸収特性が得られ、前記くさび形部分は角錐の角(稜線)に沿って3個以上設けられるため偏波面特性差が無いか若しくは少ない特性となる。   Further, the external shape of the radio wave absorber according to the present invention corresponds to that having a wedge-shaped portion outside the pyramid, and good radio wave absorption characteristics from low frequency to high frequency are obtained compared to the pyramid shape, Since three or more wedge-shaped portions are provided along the corners (ridge lines) of the pyramid, there is no or little difference in polarization plane characteristics.

本発明に係る電波暗室によれば、上記電波吸収体を用いることで、低コストで施工が容易であり、電波吸収性能も優れたものとすることが可能である。   According to the anechoic chamber according to the present invention, by using the above-described electromagnetic wave absorber, construction can be easily performed at low cost, and excellent electromagnetic wave absorption performance can be achieved.

以下、本発明を実施するための最良の形態として、電波吸収体及びその製造方法、並びに電波暗室の実施の形態を図面に従って説明する。   Hereinafter, as the best mode for carrying out the present invention, an embodiment of a radio wave absorber, a manufacturing method thereof, and an anechoic chamber will be described with reference to the drawings.

図1乃至図12を用いて本発明に係る電波吸収体及びその製造方法の実施の形態1を説明する。図1は電波吸収体10の外観を示し、図2(A)のように四角形(長方形等)の薄板状電波吸収材11を2箇所折り曲げて、同図(B)のような一面開口の中空四面体20を4個作製し、中空四面体20の開口面に対向する三角形面20aが中空四角錐22の側面を形成するように連結一体化した同図(C)の形状となっている。前記三角形面20aが二等辺三角形を成していれば、前記中空四角錐は正四角錐のピラミッド形となる。前記中空四面体20の三角形面20aに対して折れ曲がって立ち上がった逆三角形面20bは一辺20cにおいて互いに突き合わされ、接合されてくさび形部分21を成すものである。従って、図1、図2(C)の中空四面体20を4個組み合わせた状態では、くさび形部分21は中空四角錐の外側の角(稜線)に沿って4個形成されることになる。   Embodiment 1 of a radio wave absorber and a method for manufacturing the same according to the present invention will be described with reference to FIGS. FIG. 1 shows the external appearance of the radio wave absorber 10, and a rectangular (rectangular, etc.) thin plate-like radio wave absorber 11 is bent at two places as shown in FIG. Four tetrahedrons 20 are produced, and the triangular surface 20 a facing the opening surface of the hollow tetrahedron 20 is connected and integrated so as to form the side surface of the hollow quadrangular pyramid 22. If the triangular surface 20a forms an isosceles triangle, the hollow quadrangular pyramid has a regular quadrangular pyramid shape. The inverted triangular surfaces 20b that are bent and raised with respect to the triangular surface 20a of the hollow tetrahedron 20 are abutted against each other at one side 20c and joined to form a wedge-shaped portion 21. Therefore, in the state where four hollow tetrahedrons 20 in FIGS. 1 and 2C are combined, four wedge-shaped portions 21 are formed along the outer corners (ridge lines) of the hollow quadrangular pyramid.

図1の電波吸収体の製造方法を考えた場合、図2のように4個の中空四面体20を先に作製し、これらを開口面外向きで組み合わせて連結一体化する方法が最も解り易いが、図2(A)の折り曲げ部分が連結部になるため接着代(糊代)が設けにくい。そこで、図3に示すように隣接する中空四面体20同士を連結する連結部材25を用いる方法がある。あるいは、図4(A)に示すように電波吸収材11の一部に切れ目26,27を入れておき、図4(B),(C)のように折り曲げて中空四面体20の作製時に突部28とスリット29を同時に形成し、一方の中空四面体20のスリット29に他方の中空四面体20の突部28を差込み、その部分(差し込まれた突部)を接着代(糊代)とする方法がある。なお、図3及び図4において、図2と同一又は相当部分には同一符号を付してある。   Considering the manufacturing method of the radio wave absorber shown in FIG. 1, it is most easy to understand a method in which four hollow tetrahedrons 20 are first produced as shown in FIG. However, since the bent portion of FIG. 2A becomes a connecting portion, it is difficult to provide an adhesive allowance (glue allowance). Therefore, as shown in FIG. 3, there is a method using a connecting member 25 for connecting adjacent hollow tetrahedrons 20 to each other. Alternatively, as shown in FIG. 4 (A), cuts 26 and 27 are made in a part of the radio wave absorber 11 and bent as shown in FIGS. 4 (B) and 4 (C). The portion 28 and the slit 29 are formed at the same time, and the protrusion 28 of the other hollow tetrahedron 20 is inserted into the slit 29 of one hollow tetrahedron 20, and the portion (inserted protrusion) is bonded to the bonding allowance (glue allowance). There is a way to do it. 3 and 4, the same reference numerals are given to the same or corresponding parts as those in FIG. 2.

また、完成状態において4個の中空四面体20を連結一体化した構造となればよいから、図5及び図6の製造方法も可能である。この場合、第1の中空四面体20−1の開口面に対向する三角形面20a−1となる第1領域13と、第1の中空四面体20−1に隣接する第2の中空四面体20−2の開口面に対向する三角形面から立ち上がる逆三角形面20b−2となる第2領域14と、連結のための接着代(糊代)15とからなる第1の薄板状電波吸収材12を用いるとともに、第1の中空四面体20−1の開口面に対向する三角形面20aから立ち上がる逆三角形面20b−1と連結のための接着代(糊代)17とからなる第2の薄板状電波吸収材16を用いる。   In addition, the manufacturing method shown in FIGS. 5 and 6 is also possible as long as it has a structure in which the four hollow tetrahedrons 20 are connected and integrated in the completed state. In this case, the 1st area | region 13 used as the triangular surface 20a-1 which opposes the opening surface of the 1st hollow tetrahedron 20-1, and the 2nd hollow tetrahedron 20 adjacent to the 1st hollow tetrahedron 20-1. The first thin-plate-shaped electromagnetic wave absorbing material 12 including the second region 14 that becomes the inverted triangular surface 20b-2 rising from the triangular surface facing the opening surface of -2 and the bonding margin (glue margin) 15 for connection is provided. A second thin-plate-shaped radio wave comprising an inverted triangular surface 20 b-1 rising from a triangular surface 20 a facing the opening surface of the first hollow tetrahedron 20-1 and a bonding margin (glue margin) 17 for connection. Absorbent 16 is used.

そして、図6のように、第1の薄板状電波吸収材12の第1領域13と第2領域14の境界位置に、第2の薄板状電波吸収材16を接合したものを4個作製し、それらを連結一体化することで図1の完成状態の電波吸収体10が得られる。各々の薄板状電波吸収材12,16の連結は接着代15,17に接着剤を塗布する、あるいは両面接着テープを貼り付けること等により行うことができる。   Then, as shown in FIG. 6, four pieces in which the second thin plate wave absorber 16 is joined to the boundary position between the first region 13 and the second region 14 of the first thin plate wave absorber 12 are produced. By connecting and integrating them, the completed radio wave absorber 10 of FIG. 1 is obtained. The thin plate wave absorbers 12 and 16 can be connected by applying an adhesive to the bonding margins 15 and 17 or attaching a double-sided adhesive tape.

図5及び図6の製造方法は、連結部に接着代(糊代)が設けられる上、隣接する中空四面体20の一部までを平板の薄板状電波吸収材12で構成しているため、図1の状態に組み立てたときの強度を大きくできる利点がある。   In the manufacturing method of FIGS. 5 and 6, an adhesive allowance (adhesive allowance) is provided at the connecting portion, and up to a part of the adjacent hollow tetrahedron 20 is configured by a flat plate-like electromagnetic wave absorber 12. There is an advantage that the strength when assembled in the state of FIG. 1 can be increased.

図7及び図8は上記実施の形態1で用いることができる薄板状電波吸収材として、段ボール構造の電波吸収材を示す(特開2004−253760号で提案されている)。図7及び図8(A)は両面段ボール構造の電波吸収材30であり、平面シートのライナ31間にコルゲート加工(波形に屈曲加工)したシートである中芯32を介在させて積層一体化したものである。波形に屈曲加工された中芯32の頂部と谷部とは、それぞれ上下のライナ31に接着剤を介して接着されている。ライナ31、中芯32のうちの少なくとも1枚のシートは導電性材料を含んでいる。例えば、ライナ31、中芯32の一方又は両方に導電性材料(カーボン、グラファイト、導電性繊維等)を含むシート、好ましくは炭素繊維の混抄紙等が使用できる。段ボールを構成する混抄紙等の基材として難燃性または不燃性を有する材料を使用することも出来る。   7 and 8 show a corrugated radio wave absorber as a thin plate radio wave absorber that can be used in the first embodiment (proposed in Japanese Patent Application Laid-Open No. 2004-253760). 7 and 8A show a radio wave absorber 30 having a double-sided corrugated cardboard structure, which is laminated and integrated by interposing a core 32 which is a corrugated (bently bent) sheet between liners 31 of a flat sheet. Is. The top portion and the valley portion of the core 32 bent into a corrugated shape are respectively bonded to the upper and lower liners 31 via an adhesive. At least one sheet of the liner 31 and the core 32 includes a conductive material. For example, a sheet containing a conductive material (carbon, graphite, conductive fiber, etc.) in one or both of the liner 31 and the core 32, preferably a carbon fiber mixed paper or the like can be used. A flame retardant or non-flammable material can also be used as a base material such as mixed paper constituting the cardboard.

なお、両面段ボール構造の電波吸収体の他に、図8(B)の1枚のライナ31に、コルゲート加工した中芯32を貼り合わせた片面段ボール構造の電波吸収材、同図(C)の両面段ボールに片面段ボールを接合した複両面段ボール構造の電波吸収材、同図(D)の複両面段ボールに片面段ボールを接合して3段としたトリプルウォール構造の電波吸収材を薄板状電波吸収材として使用することが可能である。   In addition to the radio wave absorber having a double-sided cardboard structure, a single-sided cardboard wave-absorbing material in which a corrugated core 32 is bonded to one liner 31 shown in FIG. Double-sided corrugated wave absorber with single-sided cardboard bonded to double-sided corrugated cardboard, and triple-walled wave absorber with single-sided cardboard bonded to double-sided corrugated cardboard as shown in Figure (D). It can be used as

上記図7や図8(A)〜(D)の薄板状電波吸収材は中空構造であるため、軽量であるとともに、波形の中芯32を内在することで適度の剛性を具備し、電波吸収体に組み立て後においても良好な形態保持性を維持できる。また、平面状のシート状態で保管や運搬ができるため、かさばらず、低コストで輸送することができる。   7 and 8 (A) to (D) have a hollow structure, and thus are light in weight and have a moderate rigidity by including a corrugated core 32, thereby absorbing radio waves. Good form retention can be maintained even after assembly to the body. Moreover, since it can be stored and transported in a flat sheet state, it is not bulky and can be transported at low cost.

図9(A)はフェライト焼結体の前面に配置された四角筒の電波吸収体の開口形状を示し、四角筒の対向する壁面を近づく方向に傾けて開口を閉じる方向に変化させたとき、さらに図9(B)の本発明に係る実施の形態1の電波吸収体形状(2つのくさび形を交差させた形状)としたときに、電波吸収特性における高周波特性が改善されることを以下に説明する。   FIG. 9 (A) shows the opening shape of the rectangular tube radio wave absorber disposed on the front surface of the ferrite sintered body. When the opposing wall surface of the square tube is tilted in the direction of approaching and the opening is changed in the closing direction, Furthermore, when the radio wave absorber shape of the first embodiment according to the present invention shown in FIG. 9B (a shape in which two wedge shapes are crossed), the high frequency characteristics in the radio wave absorption characteristics are improved as follows. explain.

図10は図9(A)のフェライト焼結体の前面に配置された電波吸収体が四角筒形状のときの反射減衰量(dB)の周波数特性(GHz)であり、約1GHz以上で電波吸収特性が低下している。   FIG. 10 shows the frequency characteristics (GHz) of the return loss (dB) when the radio wave absorber disposed on the front surface of the ferrite sintered body of FIG. 9 (A) is a square tube shape, and the radio wave absorption is about 1 GHz or more. The characteristics are degraded.

図11は四角筒形状の対向する一対の壁面(電波吸収材)を閉じて1つのくさび形を形成した場合で、くさび形の先端綾線が到来電波の電界に垂直なときと平行なときの反射減衰量(dB)の周波数特性(GHz)をそれぞれ示す。一対の壁面を閉じて1つのくさび形を形成した場合、くさび形の先端稜線が電界に平行な場合には高周波特性に大きな改善が見られた。しかし、くさび形の先端稜線が電界に垂直な場合には改善効果は小さい。   FIG. 11 shows a case where a pair of opposing rectangular wall surfaces (wave absorbers) are closed to form a single wedge shape, where the wedge-shaped tip traversal line is parallel to when it is perpendicular to the electric field of the incoming radio wave. The frequency characteristics (GHz) of the return loss (dB) are shown respectively. When a pair of wall surfaces were closed to form a single wedge shape, the high-frequency characteristics were greatly improved when the wedge-shaped tip edge line was parallel to the electric field. However, when the wedge-shaped tip edge line is perpendicular to the electric field, the improvement effect is small.

そこで、両偏波に効くように両方向(二対)の壁面を閉じてくさび形としたような形状、つまり図9(B)の本発明の電波吸収体形状(2つのくさび形を交差させた形状)とした。このときの反射減衰量(dB)の周波数特性(GHz)を図12に示す。図10や図11の特性に比べて特に1GHz以上の高周波特性が大幅改善されている。また、形状の対称性から偏波面による特性差は生じないことがわかる。   Therefore, the shape of a wedge shape by closing the walls in both directions (two pairs) so as to be effective for both polarizations, that is, the shape of the electromagnetic wave absorber of the present invention (two wedge shapes in FIG. 9B) is intersected. Shape). FIG. 12 shows the frequency characteristic (GHz) of the return loss (dB) at this time. Compared with the characteristics of FIG. 10 and FIG. 11, the high frequency characteristics of 1 GHz or more are particularly improved. It can also be seen that there is no characteristic difference due to the plane of polarization due to the symmetry of the shape.

この実施の形態によれば、次の通りの効果を得ることができる。   According to this embodiment, the following effects can be obtained.

(1) 電波吸収体10は、一面開口の中空四面体20を4個連結した形状であって、薄板状電波吸収材を折り曲げて形成可能であり、薄板状電波吸収材として輸送することで輸送体積を小さくできる。また段ボール構造で低コストの薄板状電波吸収材30を用いることで、軽量で構造強度を強くでき、製造や電波暗室等に対する施工が容易となる。 (1) The radio wave absorber 10 has a shape in which four hollow tetrahedrons 20 with one opening are connected, can be formed by bending a thin plate wave absorber, and is transported by being transported as a thin plate wave absorber. The volume can be reduced. Further, by using the low-cost thin-plate wave absorber 30 with a cardboard structure, the structure strength is light and the structure strength can be increased, and manufacturing and construction in an anechoic chamber can be facilitated.

(2) 薄板状電波吸収材の折り曲げ加工及び両面接着テープや接着剤等による連結加工によって電波吸収体10を組立可能である。組立に際して特殊な用具、部品は不要であり、電波暗室等への施工が容易である。 (2) The radio wave absorber 10 can be assembled by bending a thin plate wave absorber and connecting with a double-sided adhesive tape or adhesive. No special tools or parts are required for assembly, and installation in an anechoic chamber is easy.

(3) 電波吸収体10の外観形状は、2つのくさび形を交差させて設けたものに相当し、ピラミッド形に比較して低周波から高周波まで良好な電波吸収特性が得られ、前記くさび形は互いに直交するように交差させて設けられるため偏波面特性差が無い特性となる。 (3) The external shape of the radio wave absorber 10 is equivalent to that formed by intersecting two wedge shapes, and can provide better radio wave absorption characteristics from low frequencies to high frequencies than the pyramid shape. Are provided so as to cross each other so as to be orthogonal to each other, so that there is no difference in polarization plane characteristics.

(4) 図9(B)のように電波吸収体10の中空四角錐22の底面にフェライト焼結体が配置された複合型電波吸収体構造とすることで、低周波での電波吸収特性を改善できる。 (4) As shown in FIG. 9B, the composite wave absorber structure in which the ferrite sintered body is disposed on the bottom surface of the hollow quadrangular pyramid 22 of the wave absorber 10 allows the radio wave absorption characteristics at low frequencies to be obtained. Can improve.

図13は本発明に係る電波吸収体の実施の形態2を示す。この場合も、4個の中空四面体20の開口面に対向する三角形面20aで中空四角錐22が形成されるが、その中空四角錐22の外側に形成されたくさび形部分21の先端側稜線21aの長さLが、前述の実施の形態1に比べて短縮されている(図中の点線斜線部が除去されている)。つまり、中空四角錐22の底辺をLとしたとき、
2L<L
となっている。
FIG. 13 shows Embodiment 2 of the radio wave absorber according to the present invention. Also in this case, the hollow quadrangular pyramid 22 is formed by the triangular surface 20 a facing the opening surfaces of the four hollow tetrahedrons 20, and the ridge line on the distal end side of the wedge-shaped portion 21 formed outside the hollow quadrangular pyramid 22 is formed. the length L 1 of 21a has been shortened as compared with the first embodiment described above (dotted hatched portion in the drawing is removed). That is, when the bottom of the hollow quadrangular pyramid 22 was as L 2,
2L 1 <L 2
It has become.

なお、その他の構成は前述した実施の形態1と同様であり、同一又は相当部分に同一符号を付して説明を省略する。   Other configurations are the same as those of the first embodiment described above, and the same or corresponding parts are denoted by the same reference numerals and description thereof is omitted.

この実施の形態2では、くさび形部分21の先端側稜線21aの長さLを調整することで、電波吸収特性の微調整が可能である。 In the second embodiment, by adjusting the length L 1 of the leading-end side ridgeline 21a of the wedge-shaped portion 21, it is possible to finely adjust the radio wave absorption characteristics.

図14乃至図16を用いて本発明に係る電波吸収体及びその製造方法の実施の形態3を説明する。図14は電波吸収体40の外観を示し、図15(A)のように四角形(長方形等)の薄板状電波吸収材11を2箇所折り曲げて、同図(B)のような一面開口の中空四面体20を4個作製し、中空四面体20の開口面が中空四角錐42の側面を形成するように連結一体化した同図(C)の形状となっている。前記開口面が二等辺三角形を成していれば、前記中空四角錐は正四角錐のピラミッド形となる。前記中空四面体20の開口面に対向する面は三角形面20aとなっており、この三角形面20aに対して折れ曲がって立ち上がった逆三角形面20bは一辺20cにおいて互いに突き合わされ、接合されてくさび形部分41を成すものである。従って、図14、図15(C)の中空四面体20を4個組み合わせた状態では、くさび形部分41は中空四角錐42の外側の角(稜線)に沿って形成されることになる。   A third embodiment of the radio wave absorber and the manufacturing method thereof according to the present invention will be described with reference to FIGS. FIG. 14 shows the external appearance of the radio wave absorber 40. A rectangular (rectangular, etc.) thin plate-like radio wave absorber 11 is folded at two locations as shown in FIG. Four tetrahedrons 20 are produced, and the shape of the same figure (C) is obtained by connecting and integrating so that the opening surface of the hollow tetrahedron 20 forms the side surface of the hollow quadrangular pyramid 42. If the opening surface forms an isosceles triangle, the hollow quadrangular pyramid has a regular quadrangular pyramid shape. The surface of the hollow tetrahedron 20 that faces the opening surface is a triangular surface 20a, and the inverted triangular surfaces 20b that are bent and raised with respect to the triangular surface 20a are abutted against each other at one side 20c and joined together to form a wedge-shaped portion. 41. Therefore, in a state where the four hollow tetrahedrons 20 of FIGS. 14 and 15C are combined, the wedge-shaped portion 41 is formed along the outer corner (ridgeline) of the hollow quadrangular pyramid 42.

図16は図14の電波吸収体40を製造するために用いる薄板状電波吸収材50を示し、中空四面体20の開口面に対向する三角形面20aとなる第1領域51と、三角形面20aから立ち上がる2つの逆三角形面20bとなる第2及び第3領域52,53と、連結のための接着代(糊代)54とからなっている。   FIG. 16 shows a thin plate wave absorber 50 used for manufacturing the radio wave absorber 40 of FIG. 14, and includes a first region 51 that becomes a triangular surface 20a facing the opening surface of the hollow tetrahedron 20, and a triangular surface 20a. It consists of second and third regions 52 and 53 that form two inverted triangular surfaces 20b that rise, and an adhesive allowance (glue allowance) 54 for connection.

そして、薄板状電波吸収材50を各領域51,52,53の境界線に沿って折り曲げ加工し、接着代54を利用して中空四面体20を作製し、作製された4個の中空四面体20を、中空四面体20の開口面が中空四角錐22の側面を形成するように接着代54を利用して両面接着テープや接着剤等で連結一体化することで、完成状態の電波吸収体40が得られる。   Then, the thin plate-shaped electromagnetic wave absorber 50 is bent along the boundary lines of the respective regions 51, 52, 53, and the hollow tetrahedron 20 is produced using the bonding margin 54, and the four produced hollow tetrahedrons are produced. 20 is connected and integrated with a double-sided adhesive tape, an adhesive or the like using an adhesive margin 54 so that the opening surface of the hollow tetrahedron 20 forms the side surface of the hollow quadrangular pyramid 22, thereby completing the radio wave absorber in a completed state. 40 is obtained.

この実施の形態3に示す電波吸収体40の外観形状も、2つのくさび形を交差させて設けたものに類似し、前述の実施の形態1とほぼ同様の電波吸収特性が得られる。その他の作用効果も前述の実施の形態1と同様である。   The external shape of the radio wave absorber 40 shown in the third embodiment is also similar to that provided by intersecting two wedge shapes, and substantially the same radio wave absorption characteristics as those in the first embodiment can be obtained. Other functions and effects are the same as those of the first embodiment.

図17は本発明に係る電波吸収体の実施の形態4であって、電波吸収体60は一面開口の中空四面体20の3個を、中空四面体20の開口面に対向する三角形面20aが中空三角錐23の側面を形成するように(開口面が外向きとなるように)連結した形状を有する。   FIG. 17 shows a fourth embodiment of the radio wave absorber according to the present invention, in which the radio wave absorber 60 includes three hollow tetrahedrons 20 having one opening and a triangular surface 20a facing the open surface of the hollow tetrahedron 20. The hollow triangular pyramid 23 has a shape connected so as to form a side surface (so that the opening surface faces outward).

図18は本発明に係る電波吸収体の実施の形態5であって、電波吸収体70は一面開口の中空四面体20の3個を、中空四面体20の開口面が中空三角錐24の側面を形成するように(開口面が内向きとなり、三角形面20aが外側となるように)連結した形状を有する。   FIG. 18 shows a fifth embodiment of the radio wave absorber according to the present invention, in which the radio wave absorber 70 includes three hollow tetrahedrons 20 having a single opening, and the open surface of the hollow tetrahedron 20 is the side of the hollow triangular pyramid 24. So that the opening surface is inward and the triangular surface 20a is outward.

これらの実施の形態4及び5の場合、中空三角錐23,24の外側に形成されたくさび形部分21が3方向を向いており、従来のくさび形の電波吸収体に比較して到来電波の偏波面に起因する偏波面特性差が少ない特性となる。その他の作用効果は前述の実施の形態1と同様である。   In the case of these Embodiments 4 and 5, the wedge-shaped portion 21 formed on the outside of the hollow triangular pyramids 23 and 24 faces three directions, and the incoming radio wave is compared with the conventional wedge-shaped wave absorber. It becomes a characteristic with a small difference in polarization plane characteristics caused by the polarization plane. Other functions and effects are the same as those of the first embodiment.

なお、実施の形態4,5は中空四面体を3個組み合わせた形状であるが、中空四面体を5個以上組み合わせた形状としても良い。つまり、一面開口の中空四面体の5個以上を、該中空四面体の開口面に対向する面が中空角錐の側面を形成するように連結した形状を有する電波吸収体、あるいは一面開口の中空四面体の5個以上を、該中空四面体の開口面が中空角錐の側面を形成するように連結した形状を有する電波吸収体であってもよい。   In addition, although Embodiment 4 and 5 are the shapes which combined three hollow tetrahedrons, it is good also as a shape which combined five or more hollow tetrahedrons. That is, a radio wave absorber having a shape in which five or more hollow tetrahedrons having a single-side opening are connected such that a surface facing the opening surface of the hollow tetrahedron forms a side surface of a hollow pyramid, or a hollow tetrahedron having a single-side opening The electromagnetic wave absorber may have a shape in which five or more of the bodies are connected such that the opening surface of the hollow tetrahedron forms a side surface of a hollow pyramid.

また、実施の形態3〜5の場合においても、図13の実施の形態2と同様に中空角錐の外側に形成されたくさび形部分の先端側稜線の長さを、前記中空角錐の底辺の長さの半分よりも短く設定してもよい。
なお、中空四面体を構成するための薄板状電波吸収材は、図24(A),(B)の形状であってもよい。図24(A)は左右対称の台形の上辺又は底辺から、前記上辺又は底辺と等しい長さの底辺を持つ二等辺三角形を切り欠いた形状である。また、図24(B)は左右対称の台形の上辺又は底辺に、前記上辺又は底辺と等しい長さの底辺を持つ二等辺三角形を足した五角形状である。いずれの形状であっても、三角形面となる部分の境界線に沿って折り曲げたときに、一面開口の中空四面体の電波吸収材を構成することが可能である。
換言すれば、二等辺三角形と、当該二等辺三角形の二等辺を共有する2つの三角形とを当該二等辺において折り曲げ可能に連結した形状を有する、又は取り出し可能に配置した構成である。
なお、それにの電波吸収材において、電波吸収体組立時の嵌め合わせのための切欠又は突起がさらに付加されていてもよい。
Also in the case of the third to fifth embodiments, the length of the ridge line on the front end side of the wedge-shaped portion formed outside the hollow pyramid is set to the length of the bottom of the hollow pyramid as in the second embodiment of FIG. It may be set shorter than half the length.
It should be noted that the thin plate wave absorber for constituting the hollow tetrahedron may have the shape of FIGS. 24 (A) and 24 (B). FIG. 24A shows a shape obtained by cutting out an isosceles triangle having a base having the same length as the top or bottom from the top or bottom of a symmetrical trapezoid. FIG. 24B shows a pentagonal shape in which an isosceles triangle having a base having the same length as the top or bottom is added to the top or bottom of a symmetrical trapezoid. Regardless of the shape, it is possible to constitute a hollow tetrahedron radio wave absorber having a single opening when bent along the boundary line of the triangular surface.
In other words, it is a configuration in which an isosceles triangle and two triangles sharing the isosceles of the isosceles triangle are connected so as to be bendable along the isosceles or are detachably arranged.
In addition, in the radio wave absorber, a notch or a protrusion for fitting at the time of assembling the radio wave absorber may be further added.

図19は本発明の電波暗室を示す実施の形態6であって、前記実施の形態1で述べた電波吸収体10を用いたものである。図19において、電波暗室の内壁面を構成するシールドパネル(導体板が片面又は両面に設けられたパネル)80の室内側の面にフェライト焼結体(フェライトタイル)81が敷設され、その前面に電波吸収体10が相互に隣接して多数配置固定されている。通常、電波暗室の側壁面及び天井面を図19の構成とする。   FIG. 19 shows a sixth embodiment of the anechoic chamber according to the present invention, which uses the radio wave absorber 10 described in the first embodiment. In FIG. 19, a ferrite sintered body (ferrite tile) 81 is laid on the indoor side surface of a shield panel (panel on which one or both surfaces of a conductor plate is provided) 80 constituting the inner wall surface of the anechoic chamber, and on the front surface thereof. A large number of radio wave absorbers 10 are arranged and fixed adjacent to each other. Usually, the side wall surface and the ceiling surface of the anechoic chamber are configured as shown in FIG.

この電波暗室の構成によれば、実施の形態1に示した電波吸収体10を用いることで、施工が容易で、低周波から高周波まで良好な電波吸収特性とすることが可能で、低コストで高い電波暗室性能を実現可能である。   According to the configuration of this anechoic chamber, by using the radio wave absorber 10 shown in the first embodiment, it is easy to construct, and good radio wave absorption characteristics from low frequency to high frequency can be obtained. High anechoic chamber performance can be realized.

なお、図7及び図8の段ボール構造の電波吸収材は実施の形態2〜5に示した電波吸収体にも適用可能であることは自明である。   It is obvious that the radio wave absorber having the corrugated cardboard structure shown in FIGS. 7 and 8 can also be applied to the radio wave absorber shown in the second to fifth embodiments.

また、電波暗室を示す実施の形態6において、実施の形態1に示した電波吸収体を用いたが、他の実施の形態に示した電波吸収体も使用可能であり、一面開口の中空四面体の3個以上を、該中空四面体の開口面に対向する面が中空角錐の側面を形成するように連結した形状を有する電波吸収体、あるいは一面開口の中空四面体の3個以上を、該中空四面体の開口面が中空角錐の側面を形成するように連結した形状を有する電波吸収体を用いることができる。   Further, in the sixth embodiment showing an anechoic chamber, the radio wave absorber shown in the first embodiment is used, but the radio wave absorber shown in other embodiments can also be used, and is a hollow tetrahedron having one opening. A wave absorber having a shape in which the surfaces of the hollow tetrahedron facing the opening surface of the hollow tetrahedron form a side surface of a hollow pyramid, or three or more of the hollow tetrahedron having a single surface opening, A radio wave absorber having a shape in which the opening surfaces of the hollow tetrahedrons are connected so as to form the side surfaces of the hollow pyramid can be used.

以上本発明の実施の形態について説明してきたが、本発明はこれに限定されることなく請求項の記載の範囲内において各種の変形、変更が可能なことは当業者には自明であろう。   Although the embodiments of the present invention have been described above, it will be obvious to those skilled in the art that the present invention is not limited to these embodiments, and various modifications and changes can be made within the scope of the claims.

本発明の実施の形態1であって、電波吸収体を示す斜視図である。It is Embodiment 1 of this invention, Comprising: It is a perspective view which shows an electromagnetic wave absorber. 実施の形態1に示した電波吸収体の構造及び製造方法を示す説明図である。FIG. 3 is an explanatory diagram showing a structure and a manufacturing method of the radio wave absorber shown in the first embodiment. 実施の形態1に示した電波吸収体の製造方法の一例を説明する斜視図である。FIG. 5 is a perspective view for explaining an example of a method for manufacturing the radio wave absorber shown in the first embodiment. 実施の形態1に示した電波吸収体の製造方法のもう一つの例を示す説明図である。FIG. 6 is an explanatory view showing another example of the method for manufacturing the radio wave absorber shown in the first embodiment. 実施の形態1に示した電波吸収体の製造方法の他の例に用いる薄板状電波吸収材の形状を示す平面図である。FIG. 6 is a plan view showing the shape of a thin plate wave absorber used in another example of the method of manufacturing the wave absorber shown in the first embodiment. 図5の薄板状電波吸収材を用いた製造方法を説明する分解斜視図である。It is a disassembled perspective view explaining the manufacturing method using the thin plate-shaped electromagnetic wave absorber of FIG. 実施の形態1に示した電波吸収体に用いることが可能な段ボール構造の電波吸収材を示す斜視図である。3 is a perspective view showing a corrugated cardboard wave absorber that can be used in the radio wave absorber shown in Embodiment 1. FIG. 実施の形態1に示した電波吸収体に用いることが可能な段ボール構造の電波吸収材を示す断面図である。3 is a cross-sectional view showing a corrugated cardboard wave absorber that can be used for the radio wave absorber shown in Embodiment 1. FIG. 電波吸収体の測定試料であって、(A)はフェライト焼結体の前面に四角筒形状の電波吸収体を配置した場合、(B)はフェライト焼結体の前面に実施の形態1に示したくさび形を交差させた形状の電波吸収体を配置した場合をそれぞれ示す斜視図である。A measurement sample of a radio wave absorber, (A) shows a case where a rectangular tube-shaped radio wave absorber is arranged on the front surface of a ferrite sintered body, and (B) shows the first embodiment on the front surface of the ferrite sintered body. It is a perspective view which shows the case where the electromagnetic wave absorber of the shape which crossed the wedge shape is arrange | positioned, respectively. 図9(A)のフェライト焼結体の前面に配置された電波吸収体が四角筒形状のときの反射減衰量の周波数特性図である。FIG. 10 is a frequency characteristic diagram of return loss when the radio wave absorber disposed on the front surface of the ferrite sintered body in FIG. 四角筒形状の電波吸収体の対向する二辺を閉じて1つのくさび形を形成した場合で、くさび形の先端綾線が電界に垂直なときと平行なときの反射減衰量の周波数特性図である。This is a frequency characteristic diagram of the return loss when the two opposite sides of the rectangular tube-shaped wave absorber are closed to form one wedge shape, and when the wedge-shaped tip end cross-lines are parallel to and perpendicular to the electric field. is there. 2つのくさび形を交差させた形状、つまり本発明の実施の形態1の形状の場合の反射減衰量の周波数特性図である。It is a frequency characteristic diagram of the return loss in the case of a shape in which two wedge shapes are crossed, that is, the shape of the first embodiment of the present invention. 本発明の実施の形態2であって、電波吸収体の斜視図である。It is Embodiment 2 of this invention, Comprising: It is a perspective view of a radio wave absorber. 本発明の実施の形態3であって、電波吸収体の斜視図である。It is Embodiment 3 of this invention, Comprising: It is a perspective view of a radio wave absorber. 実施の形態3に示した電波吸収体の構造及び製造方法を示す説明図である。It is explanatory drawing which shows the structure and manufacturing method of the electromagnetic wave absorber shown in Embodiment 3. 実施の形態3に示した電波吸収体の製造方法に用いる薄板状電波吸収材の形状を示す平面図である。6 is a plan view showing the shape of a thin plate wave absorber used in the method of manufacturing a wave absorber shown in Embodiment 3. FIG. 本発明の実施の形態4であって、電波吸収体の斜視図である。It is Embodiment 4 of this invention, Comprising: It is a perspective view of a radio wave absorber. 本発明の実施の形態5であって、電波吸収体の斜視図である。It is Embodiment 5 of this invention, Comprising: It is a perspective view of a radio wave absorber. 本発明の実施の形態6であって、電波暗室の部分断面図である。It is Embodiment 6 of this invention, Comprising: It is a fragmentary sectional view of an anechoic chamber. 複合型電波吸収体の一般的構成を示す側面図である。It is a side view which shows the general structure of a composite type electromagnetic wave absorber. 中空ピラミッド形の複合型電波吸収体であって、(A)は正面図、(B)は側面図である。It is a hollow pyramid type composite wave absorber, wherein (A) is a front view and (B) is a side view. 中空くさび形の複合型電波吸収体であって、(A)は正面図、(B)は側面図である。It is a hollow wedge-shaped composite electromagnetic wave absorber, (A) is a front view, (B) is a side view. 側面開口を有する中空くさび形の複合型電波吸収体であって、(A)は正面図、(B)は側面図である。It is a hollow wedge-shaped composite wave absorber having side openings, where (A) is a front view and (B) is a side view. 本発明で使用できる薄板状電波吸収材であって、(A)は薄板状電波吸収材の1例を示す平面図、(B)は他の例を示す平面図である。FIG. 2A is a plan view showing an example of a thin plate-shaped wave absorber that can be used in the present invention, and FIG.

符号の説明Explanation of symbols

1,81 フェライト焼結体
2,10,40,60,70 電波吸収体
11,12,16,30,50 電波吸収材
20 中空四面体
22,42 中空四角錐
23,24 中空三角錐
25 連結部材
28 突部
29 スリット
31 ライナ
32 中芯
80 シールドパネル
1,81 Ferrite sintered body 2,10,40,60,70 Radio wave absorber 11, 12, 16, 30, 50 Radio wave absorber 20 Hollow tetrahedron 22, 42 Hollow square pyramid 23, 24 Hollow triangular pyramid 25 Connecting member 28 Projection 29 Slit
31 liner 32 center 80 shield panel

Claims (17)

一面開口の中空四面体の3個以上を、該中空四面体の開口面に対向する面が中空角錐の側面を形成するように連結した形状を有することを特徴とする電波吸収体。   A radio wave absorber characterized by having a shape in which three or more hollow tetrahedrons having a single-sided opening are connected such that a surface facing the opening surface of the hollow tetrahedron forms a side surface of a hollow pyramid. 一面開口の中空四面体の3個以上を、該中空四面体の開口面が中空角錐の側面を形成するように連結した形状を有することを特徴とする電波吸収体。   A radio wave absorber characterized by having a shape in which three or more hollow tetrahedrons having one open surface are connected so that the open surface of the hollow tetrahedron forms a side surface of a hollow pyramid. 前記中空角錐の外側に形成されたくさび形部分の先端側稜線の長さは、前記中空角錐の底辺の長さの半分よりも短いことを特徴とする請求項1又は2記載の電波吸収体。   3. The radio wave absorber according to claim 1, wherein a length of a tip side ridge line of a wedge-shaped portion formed outside the hollow pyramid is shorter than a half of a length of a bottom side of the hollow pyramid. 前記中空四面体が4個連結した形状であることを特徴とする請求項1,2又は3記載の電波吸収体。   4. The radio wave absorber according to claim 1, wherein the hollow tetrahedron has a shape in which four hollow tetrahedrons are connected. 薄板状の電波吸収材からなることを特徴とする請求項1,2,3又は4記載の電波吸収体。   The radio wave absorber according to claim 1, 2, 3, or 4, wherein the radio wave absorber is made of a thin plate-like radio wave absorber. 前記薄板状の電波吸収材は少なくとも1枚のシートが導電性材料を含む段ボール構造であることを特徴とする請求項5記載の電波吸収体。   6. The radio wave absorber according to claim 5, wherein the thin plate-like radio wave absorber has a corrugated cardboard structure in which at least one sheet includes a conductive material. 前記薄板状の電波吸収材の基材が難燃性または不燃性を有することを特徴とする請求項5又は6記載の電波吸収体。   The radio wave absorber according to claim 5 or 6, wherein the substrate of the thin plate-like radio wave absorber has flame retardancy or nonflammability. 前記中空角錐の底面にフェライト焼結体が配置されていることを特徴とする請求項1,2,3,4,5,6又は7記載の電波吸収体。   8. The radio wave absorber according to claim 1, wherein a ferrite sintered body is disposed on a bottom surface of the hollow pyramid. 薄板状の電波吸収材を2箇所折り曲げて一面開口の中空四面体を3個以上作製し、該中空四面体の開口面に対向する面が中空角錐の側面を形成するように連結することを特徴とする電波吸収体の製造方法。   Folding two thin plate-shaped wave absorbers to produce three or more hollow tetrahedrons with one opening, and connecting them so that the surface facing the opening of the hollow tetrahedron forms the side surface of a hollow pyramid. A method of manufacturing a radio wave absorber. 一面開口の中空四面体の3個以上を、該中空四面体の開口面に対向する三角形面が中空角錐の側面を形成するように連結した形状を有する電波吸収体の製造方法であって、
第1の中空四面体の開口面に対向する三角形面となる第1領域と、前記第1の中空四面体に隣接する第2の中空四面体の開口面に対向する三角形面から立ち上がる逆三角形面となる第2領域とを含む第1の薄板状の電波吸収材と、
前記第1の中空四面体の開口面に対向する三角形面から立ち上がる逆三角形面を含む第2の薄板状の電波吸収材とを用い、
前記第1の薄板状の電波吸収材の第1領域と第2領域の境界位置に、前記第2の薄板状の電波吸収材を接合したものを3個以上連結することを特徴とする電波吸収体の製造方法。
A method of manufacturing a radio wave absorber having a shape in which three or more hollow tetrahedrons having a single-side opening are connected such that a triangular surface facing the opening surface of the hollow tetrahedron forms a side surface of a hollow pyramid,
A first region that is a triangular surface that faces the opening surface of the first hollow tetrahedron, and an inverted triangular surface that rises from the triangular surface that faces the opening surface of the second hollow tetrahedron adjacent to the first hollow tetrahedron. A first thin-plate wave absorber including a second region to be
Using a second thin-plate-shaped wave absorber including an inverted triangular surface rising from a triangular surface facing the opening surface of the first hollow tetrahedron,
3. Radio wave absorption characterized in that three or more of the first thin plate-like radio wave absorbers joined with the second thin plate-like radio wave absorber are connected to a boundary position between the first region and the second region. Body manufacturing method.
薄板状の電波吸収材を2箇所折り曲げて一面開口の中空四面体を3個以上作製し、該中空四面体の開口面が中空角錐の側面を形成するように連結することを特徴とする電波吸収体の製造方法。   Folding two thin plate-shaped wave absorbers to produce three or more hollow tetrahedrons with one opening, and connecting the hollow tetrahedrons so that the opening faces of the hollow pyramids form the side surfaces of a hollow pyramid Body manufacturing method. 室内側側壁面、天井面の少なくとも一面に請求項1乃至8のいずれか記載の電波吸収体を配設したことを特徴とする電波暗室。   An electromagnetic wave anechoic chamber, wherein the electromagnetic wave absorber according to any one of claims 1 to 8 is disposed on at least one of the indoor side wall surface and the ceiling surface. 三角形面となる部分の境界線に沿って折り曲げる場合に、一面開口の中空四面体となるようにしたことを特徴とする薄板状電波吸収材。   A thin plate-shaped electromagnetic wave absorbing material characterized in that when it is bent along a boundary line of a portion to be a triangular surface, it becomes a hollow tetrahedron having an opening on one surface. 左右対称の台形の上辺又は底辺から、前記上辺又は底辺と等しい長さの底辺を持つ二等辺三角形を切り欠いた形状、又は左右対称の台形の上辺又は底辺に、前記上辺又は底辺と等しい長さの底辺を持つ二等辺三角形を足した五角形状を有している、又は取り出し可能に配置したことを特徴とする薄板状電波吸収材。   A shape in which an isosceles triangle having a base equal in length to the top or bottom is cut out from the top or bottom of a symmetrical trapezoid, or a length equal to the top or bottom in the top or bottom of a symmetrical trapezoid A thin plate-shaped electromagnetic wave absorbing material having a pentagonal shape with an isosceles triangle having a base of or a releasable arrangement. 二等辺三角形と、当該二等辺三角形の二等辺を共有する2つの三角形とを当該二等辺において折り曲げ可能に連結した形状を有する、又は取り出し可能に配置したことを特徴とする電波吸収材。   A radio wave absorber characterized by having an isosceles triangle and two triangles sharing the isosceles of the isosceles triangle and having a shape in which the isosceles are connected so as to be bendable. 請求項13、14又は15の電波吸収材において、嵌め合わせのための切欠又は突起が設けられていることを特徴とする電波吸収材。   16. The radio wave absorber according to claim 13, 14 or 15, wherein a notch or a protrusion for fitting is provided. 一面開口の中空四面体形状であることを特徴とする電波吸収材。   1. A radio wave absorber characterized by having a hollow tetrahedron shape with an opening on one side.
JP2006215125A 2005-08-05 2006-08-07 Radio wave absorber, method for manufacturing the same, and anechoic chamber Active JP4825074B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2006215125A JP4825074B2 (en) 2005-08-05 2006-08-07 Radio wave absorber, method for manufacturing the same, and anechoic chamber

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP2005227717 2005-08-05
JP2005227717 2005-08-05
JP2006215125A JP4825074B2 (en) 2005-08-05 2006-08-07 Radio wave absorber, method for manufacturing the same, and anechoic chamber

Publications (2)

Publication Number Publication Date
JP2007067395A true JP2007067395A (en) 2007-03-15
JP4825074B2 JP4825074B2 (en) 2011-11-30

Family

ID=37929181

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2006215125A Active JP4825074B2 (en) 2005-08-05 2006-08-07 Radio wave absorber, method for manufacturing the same, and anechoic chamber

Country Status (1)

Country Link
JP (1) JP4825074B2 (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009128377A1 (en) * 2008-04-15 2009-10-22 株式会社リケン Composite radio wave absorber
JP2012191182A (en) * 2011-02-22 2012-10-04 Toray Ind Inc Sheet material for radio wave absorber and radio wave absorber
JP2012191181A (en) * 2011-02-22 2012-10-04 Toray Ind Inc Sheet material for radio wave absorber and radio wave absorber
JP2015220411A (en) * 2014-05-20 2015-12-07 Tdk株式会社 Wave absorber and anechoic chamber
WO2023003035A1 (en) * 2021-07-21 2023-01-26 日東電工株式会社 Electromagnetic wave shield

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02161799A (en) * 1988-12-14 1990-06-21 Toppan Printing Co Ltd Electromagnetic wave absorber element
JPH0335597A (en) * 1989-07-03 1991-02-15 Akzo Kashima Ltd Manufacture of radio wave absorber
JPH0339900A (en) * 1989-06-23 1991-02-20 Hughes Aircraft Co Device for distributing filament of missile
JPH06275981A (en) * 1993-03-22 1994-09-30 Tdk Corp Radio wave absorbing structure
JPH1187978A (en) * 1997-09-09 1999-03-30 Nitto Boseki Co Ltd Incombustible radio wave absorber
JP2000216584A (en) * 1999-01-21 2000-08-04 Tdk Corp Electromagnetic-wave absorbing body, members for assembling therewith, and manufacture thereof
JP2001127483A (en) * 1999-10-28 2001-05-11 Riken Corp Electric-wave absorber
JP2004103789A (en) * 2002-09-09 2004-04-02 Tohoku Kako Kk Matching ferrite radio-wave absorber and radio-wave absorbing wall
JP2004253760A (en) * 2002-12-25 2004-09-09 Toray Ind Inc Sheet material for wave absorber, and wave absorber
JP2005109161A (en) * 2003-09-30 2005-04-21 Nisshinbou Engineering Kk Electric wave absorber

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02161799A (en) * 1988-12-14 1990-06-21 Toppan Printing Co Ltd Electromagnetic wave absorber element
JPH0339900A (en) * 1989-06-23 1991-02-20 Hughes Aircraft Co Device for distributing filament of missile
JPH0335597A (en) * 1989-07-03 1991-02-15 Akzo Kashima Ltd Manufacture of radio wave absorber
JPH06275981A (en) * 1993-03-22 1994-09-30 Tdk Corp Radio wave absorbing structure
JPH1187978A (en) * 1997-09-09 1999-03-30 Nitto Boseki Co Ltd Incombustible radio wave absorber
JP2000216584A (en) * 1999-01-21 2000-08-04 Tdk Corp Electromagnetic-wave absorbing body, members for assembling therewith, and manufacture thereof
JP2001127483A (en) * 1999-10-28 2001-05-11 Riken Corp Electric-wave absorber
JP2004103789A (en) * 2002-09-09 2004-04-02 Tohoku Kako Kk Matching ferrite radio-wave absorber and radio-wave absorbing wall
JP2004253760A (en) * 2002-12-25 2004-09-09 Toray Ind Inc Sheet material for wave absorber, and wave absorber
JP2005109161A (en) * 2003-09-30 2005-04-21 Nisshinbou Engineering Kk Electric wave absorber

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009128377A1 (en) * 2008-04-15 2009-10-22 株式会社リケン Composite radio wave absorber
US8466825B2 (en) 2008-04-15 2013-06-18 Kabushiki Kaisha Riken Combined electromagnetic wave absorber
JP5496879B2 (en) * 2008-04-15 2014-05-21 株式会社リケン Composite wave absorber
JP2012191182A (en) * 2011-02-22 2012-10-04 Toray Ind Inc Sheet material for radio wave absorber and radio wave absorber
JP2012191181A (en) * 2011-02-22 2012-10-04 Toray Ind Inc Sheet material for radio wave absorber and radio wave absorber
JP2015220411A (en) * 2014-05-20 2015-12-07 Tdk株式会社 Wave absorber and anechoic chamber
US9819093B2 (en) 2014-05-20 2017-11-14 Tdk Corporation Electromagnetic wave absorber and electromagnetic wave anechoic room
WO2023003035A1 (en) * 2021-07-21 2023-01-26 日東電工株式会社 Electromagnetic wave shield

Also Published As

Publication number Publication date
JP4825074B2 (en) 2011-11-30

Similar Documents

Publication Publication Date Title
US7479917B2 (en) Electromagnetic wave absorber, manufacturing method thereof and electromagnetic wave anechoic room
JP4346360B2 (en) Sheet material for radio wave absorber and radio wave absorber
JP4825074B2 (en) Radio wave absorber, method for manufacturing the same, and anechoic chamber
JP5496879B2 (en) Composite wave absorber
US7471233B2 (en) Electromagnetic wave absorber
KR101456314B1 (en) Triplate line/waveguide converter
JP6103249B2 (en) Radio wave absorber and anechoic chamber
JP2007294903A (en) Shield joint structure and spatial former, and testing method using spatial former
JP2001127483A (en) Electric-wave absorber
JP2006205524A (en) Electric wave absorber
KR20190068321A (en) Available horn antenna in various frequency
CN107994303B (en) Low profile spatial filter
JP4684699B2 (en) Radio wave absorbing sheet material and radio wave absorber using the same
JP2012191183A (en) Sheet material for radio wave absorber and radio wave absorber
JP4617830B2 (en) Radio wave absorber member and radio wave absorber
JP4420253B2 (en) Radio wave absorber and anechoic chamber
CN212896888U (en) Ultra-low frequency resonance sound absorption structure
CN217373728U (en) Opposite-insertion type honeycomb board
JP5953799B2 (en) Sheet material for radio wave absorber and radio wave absorber
JP5953798B2 (en) Sheet material for radio wave absorber and radio wave absorber
JP2004335985A (en) Radio wave absorbing body
JP2014082431A (en) Method of constituting electric circuit radio wave absorber
JP2011086652A (en) Hybrid hollow radiowave absorber, radiowave absorption wall using the same, and anechoic chamber
JP2005026339A (en) Radio wave absorber and its manufacturing method
JPH02192800A (en) Wideband wave absorber

Legal Events

Date Code Title Description
A621 Written request for application examination

Free format text: JAPANESE INTERMEDIATE CODE: A621

Effective date: 20090423

A977 Report on retrieval

Free format text: JAPANESE INTERMEDIATE CODE: A971007

Effective date: 20110325

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20110330

A521 Request for written amendment filed

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20110526

A131 Notification of reasons for refusal

Free format text: JAPANESE INTERMEDIATE CODE: A131

Effective date: 20110615

A521 Request for written amendment filed

Free format text: JAPANESE INTERMEDIATE CODE: A523

Effective date: 20110805

TRDD Decision of grant or rejection written
A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

Effective date: 20110824

A01 Written decision to grant a patent or to grant a registration (utility model)

Free format text: JAPANESE INTERMEDIATE CODE: A01

A61 First payment of annual fees (during grant procedure)

Free format text: JAPANESE INTERMEDIATE CODE: A61

Effective date: 20110909

R150 Certificate of patent or registration of utility model

Ref document number: 4825074

Country of ref document: JP

Free format text: JAPANESE INTERMEDIATE CODE: R150

Free format text: JAPANESE INTERMEDIATE CODE: R150

FPAY Renewal fee payment (event date is renewal date of database)

Free format text: PAYMENT UNTIL: 20140916

Year of fee payment: 3

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250