JP2000081457A - Electric wave absorber measuring jig and measuring method thereof - Google Patents

Electric wave absorber measuring jig and measuring method thereof

Info

Publication number
JP2000081457A
JP2000081457A JP28861798A JP28861798A JP2000081457A JP 2000081457 A JP2000081457 A JP 2000081457A JP 28861798 A JP28861798 A JP 28861798A JP 28861798 A JP28861798 A JP 28861798A JP 2000081457 A JP2000081457 A JP 2000081457A
Authority
JP
Japan
Prior art keywords
conductor
outer conductor
radio wave
short
wave absorber
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
JP28861798A
Other languages
Japanese (ja)
Inventor
Manabu Omori
学 大森
Yukio Terai
幸雄 寺井
Minoru Kaneda
實 金田
Yasuo Mogi
靖夫 茂木
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.)
KYORITSU DENSHI KOGYO KK
KYORITSU ELECTRICAL WORKS
Tokyo Metropolitan Government
Original Assignee
KYORITSU DENSHI KOGYO KK
KYORITSU ELECTRICAL WORKS
Tokyo Metropolitan Government
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 KYORITSU DENSHI KOGYO KK, KYORITSU ELECTRICAL WORKS, Tokyo Metropolitan Government filed Critical KYORITSU DENSHI KOGYO KK
Priority to JP28861798A priority Critical patent/JP2000081457A/en
Publication of JP2000081457A publication Critical patent/JP2000081457A/en
Pending legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To enhance the easiness of sample loading and measuring accuracy. SOLUTION: This measuring jig comprises: an outer conductor 12, having a cross section in the form of a rectangle that is 400 mm×600 mm and having a cylindrical part 12b taking the form of a rectangle that is also 400 mm×600 mm and integrated with the open end of a hone-antenna-shaped part 12a gradually spreading from a coaxial connector 16 while keeping that ratio as does a hone antenna; a short-circuit board 14 in which a metallic thin inner conductor 13 electrically insulated from the outer conductor 12 is placed in a position dividing the insides of both the hone-antenna-shaped part 12a and the cylindrical part 12b of the outer conductor 12 into two equal parts, and which causes an electric short circuit on the end faces of the outer conductor 12 and the inner conductor 13 in order to load and evaluate a sample; a closing door 15 equipped with a spring mechanism, for installing and removing the sample and for completing contact with the outer conductor 12; and an N-type coaxial connector 16 for applying a TEM wave between the outer conductor 12 and the inner conductor 13.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は,外部導体がホーンアン
テナ状の端面寸法が400mm×600mmでやはり端
面形状が同様の筒形状部を一体化し,外部導体内部の短
辺を端面幅が400mmの薄板状の内部導体で2等分さ
れかつ,それぞれの端面部分が金属製の短絡板で短絡さ
れた構造並びに外部導体が角錐状端面寸法が300mm
でやはり端面形状が同様の筒形状部を一体化し,内部
導体も外部導体と相似形で端面寸法が100mmでか
つ,それぞれの端面部分が金属製の短絡板で短絡された
角形の同軸構造であり,更に外部導体及び内部導体のホ
ーンアンテナ状部または角錐状部と筒形状部との比率が
8:2から9:1までの割合で,外部導体のホーンアン
テナ状部または角錐状部か筒形状部のどちらかに測定試
料の着脱機能を果たす外部導体とのコンタクト面を有し
た開閉扉を取付けた構造の電波吸収体測定ジグに関する
ものと,周波数領域での反射減衰量特性の下限周波数が
一定値になるように時間領域でのゲート時間処理の幅を
可変調整する電波吸収体の測定法に関するものである。
BACKGROUND OF THE INVENTION The present invention relates to a horn antenna having an outer conductor having an end face dimension of 400 mm.times.600 mm and a cylindrical portion having the same end face shape, and a short side inside the outer conductor having an end face width of 400 mm. A structure in which a thin plate-shaped inner conductor is divided into two equal parts, and each end face is short-circuited by a metal short-circuit plate.
Again edge shapes with 2 integrated similar cylindrical portion, the inner conductor is also an outer conductor and an end surface dimensions and a 100 mm 2 in similar shape, square each of the end face portion is short-circuited by the metallic short circuit plate of coaxial structure In addition, the ratio of the horn antenna-like portion or pyramid-like portion of the outer conductor and the inner conductor to the cylindrical portion is from 8: 2 to 9: 1. For a radio wave absorber measurement jig with a structure with an open / close door that has a contact surface with an external conductor that performs the function of attaching and detaching the measurement sample to either of the cylindrical parts, and the lower limit frequency of the return loss characteristic in the frequency domain The present invention relates to a method for measuring a radio wave absorber that variably adjusts a width of a gate time process in a time domain so that a constant value is obtained.

【0002】[0002]

【従来の技術】従来の電波吸収体測定ジグには,同軸管
を利用した測定ジグや断面形状が矩形の外部導体内部を
平板状のストリップ導体を外部導体の一面に平行に設け
た測定ジグ(実願平01−082800)あるいは断面
が四角のホーン型の本体にやはり断面が四角の筒形部を
一体にした外部導体を本体部分及び筒形部両方にわたり
内部を2等分する仕切板を設けた測定ジグ(特開平8−
285907)など使われている。
2. Description of the Related Art Conventional radio wave absorber measurement jigs include a measurement jig utilizing a coaxial tube and a measurement jig in which a flat strip conductor is provided in parallel with one surface of an external conductor having a rectangular cross section. Or a horn-shaped main body having a square cross section, and a partition plate for dividing an inner conductor into two equal parts over both the main body part and the cylindrical part by providing an external conductor having a square cylindrical part. Measuring jig (Japanese Unexamined Patent Publication
285907).

【0003】 また電波吸収体の測定では,時間領域で
のゲート時間処理法により周波数領域での反射減衰特性
に補正を加える手法が存在する。
In the measurement of a radio wave absorber, there is a method of correcting a return loss characteristic in a frequency domain by a gate time processing method in a time domain.

【0004】 しかしこれら測定ジグでは,試料である
電波吸収体を着脱する際に測定器であるネットワークア
ナライザからの高周波信号を印加するコネクタ部分の反
対面に位置する外部導体と内部導体とを短絡する短絡板
を外部導体および内部導体より一度切離し,この短絡板
の面上に試料を装着させた後,外部導体と内部導体とを
再度短絡させてから測定を行っていた。しかし,高周波
測定において短絡板を移動させることは,僅かな接触抵
抗の変化が測定に影響を与えると共に,この短絡板移動
式の測定ジグでは試料の着脱もやや困難であった。
However, in these measurement jigs, when the radio wave absorber as the sample is attached or detached, the external conductor and the internal conductor located on the opposite surface of the connector portion to which a high frequency signal from the network analyzer as the measuring device is applied are short-circuited. The short-circuit plate was once separated from the outer conductor and the inner conductor, and after mounting the sample on the surface of the short-circuit plate, the outer conductor and the inner conductor were short-circuited again before measurement. However, moving the short-circuiting plate in the high-frequency measurement has a slight change in contact resistance affecting the measurement, and it is somewhat difficult to attach and detach the sample using the short-circuiting plate-movable measurement jig.

【0005】 また従来の時間領域でのゲート時間処理
法では,ジグの短絡板面に試料である電波吸収体を装荷
させたことにより新たに発生するジグ内部での複雑な反
射波を抑制できる優れた効果がある。しかしながら,周
波数領域に移し反射減衰量特性に補正を加えると,特に
下限周波での減衰特性に大きな誤差が生じていた。
[0005] Further, the conventional gate time processing method in the time domain is excellent in that a complicated reflected wave newly generated inside the jig can be suppressed by loading a radio wave absorber as a sample on the short-circuit plate surface of the jig. Has an effect. However, when the reflection attenuation characteristic is shifted to the frequency domain and corrected, a large error occurs particularly in the attenuation characteristic at the lower limit frequency.

【0006】[0006]

【発明が解決しようとする課題】本発明では,従来の測
定ジグの欠点である試料を装荷する短絡板の移動による
測定誤差の解消と試料着脱の困難さ並びにゲート時間処
理法での補正誤差の低減が課題であり,電波吸収体の吸
収特性を正確に捉えるための測定ジグとその測定法の提
供を目的にする。
SUMMARY OF THE INVENTION In the present invention, the disadvantages of the conventional measuring jig are the elimination of the measurement error due to the movement of the short-circuit plate for loading the sample, the difficulty in attaching and detaching the sample, and the correction error in the gate time processing method. The purpose is to provide a measuring jig and a measuring method for accurately capturing the absorption characteristics of the radio wave absorber.

【0007】[0007]

【課題を解決するための手段】上記の目的を達成するた
めに,本発明に係わる電波吸収体測定ジグの断面寸法
は,100mm×100mmの試料寸法を基準に決め
た。また、ジグの高さ寸法は測定精度の観点から決め
た。
In order to achieve the above object, the cross-sectional dimension of the radio wave absorber measuring jig according to the present invention is determined based on a sample size of 100 mm × 100 mm. The height of the jig was determined from the viewpoint of measurement accuracy.

【0008】 同軸コネクタからおおよそ15度の角度
でホーンアンテナ状の広がりをなした断面寸法が400
mm×600mmの長方形の開口端面に断面形状が同等
な筒形状の部分を一体化させた外部導体内部を短辺方向
に2等分する位置に外部導体とは接触しないように保持
された外部導体と相似形で端面幅が400mmの薄い平
板状の内部導体を設け,外部導体の長方形な端面と内部
導体の平板状の端面を金属製の短絡板で短絡した構造で
24枚の試料を装荷できるジグと,
[0008] The cross-sectional dimension of a horn antenna-like spread at an angle of about 15 degrees from the coaxial connector is 400.
An external conductor held in such a manner that it does not come into contact with the external conductor at a position where the inside of the external conductor is divided into two equal parts in the short side direction in which a cylindrical part having the same cross-sectional shape is integrated with the rectangular opening end surface of mm × 600 mm. A thin plate-shaped inner conductor with a 400 mm end face width similar to that of the above is provided, and a rectangular end face of the outer conductor and a flat end face of the inner conductor are short-circuited by a metal short-circuit plate, so that 24 samples can be loaded. Jig and

【0009】 同軸コネクタからおおよそ15度の角度
で角錐状の広がりをした断面寸法が300mmの正方
形の開口端面に断面形状が同等な筒形状の部分を一体化
させた外部導体内部を外部導体とは接触しない等位置に
保持された外部導体と相似形で端面の断面寸法が100
mmの内部導体を設け,外部導体の正方形な端面と内
部導体のやはり正方形な端面を金属製の短絡板で短絡し
た構造で8枚の試料を装荷できるジグである。
The inside of the outer conductor, in which a cylindrical portion having the same cross-sectional shape is integrated with the opening end face of a square having a cross-sectional size of 300 mm 2 and having a pyramid shape extending at an angle of about 15 degrees from the coaxial connector, is referred to as an external conductor. Is similar to the outer conductor held at the same position where it does not touch and has a cross-sectional dimension of 100
The inner conductor of mm 2 provided, which is also jig square end face can loaded with eight samples structure shorted by metallic short circuit plate of the outer conductor of the square end face and the inner conductor.

【0010】 そしてこれら測定ジグの高さ寸法は10
00mmとしたが,時間領域でのゲート処理法による反
射波の抑制を考慮して,測定ジグのホーンアンテナ状部
と筒形状部あるいは角錐状部と筒形状部との比率を8:
2から9:1までの範囲に選んだ。
The height of these measuring jigs is 10
However, in consideration of the suppression of the reflected wave by the gate processing method in the time domain, the ratio of the horn antenna part and the cylindrical part or the pyramid part and the cylindrical part of the measurement jig is set to 8:
Selected from 2 to 9: 1.

【0011】 さらに、これら測定ジグの外部導体の適
当な位置に外部導体と確実な接触が得られるスプリング
性のあるコンタクト面を有する開閉扉を取付ける手段を
講じた。
Further, a means is provided for attaching an opening / closing door having a spring-like contact surface capable of obtaining reliable contact with the outer conductor at an appropriate position of the outer conductor of the measuring jig.

【0012】 電波吸収特性の測定では,周波数領域で
の反射減衰量特性の下限周波数が一定値になるように時
間領域でのゲート時間処理の幅を可変調整する手段を新
たに開発した。このゲート時間可変調整法が可能になっ
たのは,測定ジグのホーンアンテナ状あるいは角錐状部
と筒形状部との比率を8:2から9:1までの範囲内に
選んだ結果である。
In the measurement of the radio wave absorption characteristic, a means for variably adjusting the width of the gate time processing in the time domain so that the lower limit frequency of the return loss characteristic in the frequency domain becomes a constant value has been newly developed. The gate time variable adjustment method became possible as a result of selecting the ratio of the horn antenna-like or pyramid-like portion to the cylindrical portion of the measurement jig within the range of 8: 2 to 9: 1.

【0013】[0013]

【作用】試料である電波吸収体は前記測定ジグの外部導
体に取付けられた着脱用開閉扉を介して短絡板上に装荷
すると共に,外部導体と内部導体間にTEM波電磁界を
印加するための同軸コネクタに同軸ケーブルを介してネ
ットワークアナライザを接続すると試料からの反射波を
捉えることができ,電波吸収体の周波数に対する吸収特
性を評価できる。
The electromagnetic wave absorber, which is a sample, is loaded on the short-circuit plate via the detachable opening / closing door attached to the outer conductor of the measuring jig, and a TEM electromagnetic field is applied between the outer conductor and the inner conductor. When a network analyzer is connected to the coaxial connector of the above via a coaxial cable, the reflected wave from the sample can be captured, and the absorption characteristics of the radio wave absorber with respect to frequency can be evaluated.

【0014】 このとき,測定ジグのホーンアンテナ状
あるいは角錐状部と筒形状部との比率を8:2から9:
1までの範囲内に選ぶと,試料を測定ジグに装荷したこ
とにより測定ジグ内部での反射波の影響が低減可能にな
る。この結果ゲート時間処理の幅が可変可能になり、試
料からの反射波の影響を抑制した電波吸収特性がえら
れ、従来法よりも再現性よく、しかも高精度な測定が実
施できるようになった。
At this time, the ratio of the horn antenna-shaped or pyramid-shaped portion to the cylindrical portion of the measuring jig is changed from 8: 2 to 9:
When it is selected within the range of 1, the influence of the reflected wave inside the measuring jig can be reduced by loading the sample on the measuring jig. As a result, the width of the gate time processing can be changed, the radio wave absorption characteristics with the effect of the reflected wave from the sample suppressed can be obtained, and the measurement can be performed with higher reproducibility and higher accuracy than the conventional method. .

【0015】[0015]

【実施例】以下添付図面を参照して,本発明を具体化し
た実施例につき説明する。なお、この実施例は、本発明
を具体化した2つの例であって、本発明の技術的範囲を
限定するものではない。図1、図2は本発明の第1の実
施例に使用するホーンアンテナ型電波吸収体測定ジグ1
1の構造を示している。ホーンアンテナ型電波吸収体測
定ジグ11は断面が400mm×600mmの長方形
で,ホーンアンテナと同様に徐々にこの比率を保持した
まま同軸コネクタ16から広るホーンアンテナ状部12
aの開口端にやはり400mm×600mmの長方形の
筒形状部12bを一体化させた外部導体12と,この外
部導体12のホーンアシテナ状部12a及び筒形状部1
2bの両方にわたって内部を2等分する位置に,外部導
体12とは電気的に絶縁された金属製の薄い内部導体1
3を配置しかつ,試料を装荷し評価するために,外部導
体12と内部導体13の端面で電気的に短絡する短絡板
14と、試料を着脱し外部導体12との接触を完全とす
るためのスプリング機構付きの開閉扉15と,外部導体
12と内部導体13の間にTEM波を印加するためのN
型の同軸コネクタ16からなる。
Embodiments of the present invention will be described below with reference to the accompanying drawings. This embodiment is only two examples that embody the present invention, and does not limit the technical scope of the present invention. 1 and 2 show a horn antenna type radio wave absorber measuring jig 1 used in a first embodiment of the present invention.
1 shows the structure of FIG. The horn antenna type radio wave absorber measuring jig 11 is a rectangle having a cross section of 400 mm × 600 mm, and the horn antenna-like portion 12 which spreads from the coaxial connector 16 while maintaining this ratio gradually like the horn antenna.
a external conductor 12 having a rectangular cylindrical portion 12b of 400 mm × 600 mm integrated with the open end of the outer conductor 12, a horn attenuator-like portion 12a and a cylindrical portion 1
2b, a thin inner conductor 1 made of metal that is electrically insulated from the outer conductor 12
In order to dispose the sample 3 and load and evaluate the sample, a short-circuit plate 14 for electrically short-circuiting the end surfaces of the outer conductor 12 and the inner conductor 13, and to attach and detach the sample to complete the contact with the outer conductor 12. The opening and closing door 15 with a spring mechanism, and N for applying a TEM wave between the outer conductor 12 and the inner conductor 13
Type coaxial connector 16.

【0016】 ホーンアンテナ型電波吸収体測定ジグ1
1を用いて試料7の電波吸収特性を測定するには,試料
7を装荷しない短絡状態とし,2つの開閉扉15を外部
導体11に接触するよう確実に締め,同軸コネクタ16
には測定器であるネッワークアナライザを接続する。ネ
ッワークアナライザは,短絡板14からの完全反射波を
短絡校正する。このとき,外部導体11のホーンアンテ
ナ状部12a及び筒形状部12bの比率が8:2から
9:1の範囲に選ぶと,金属箱と同様である電波吸収体
測定ジグ11内での反射が少ない利点を生ずる。そして
100mm角の試料7を図2(A)のように短絡板14
上に装荷する。この装荷状態は図2(B)のようにな
り、24枚の試料7が2つの開閉扉15を介して短絡板
14上に隙間なく配列される。このとき,内部導体13
の長辺方向の寸法を400mmとしたことで,外部導体
11からはそれぞれ100mmのギヤップが開き、試料
7間の隙間が少なくできる効果が発揮された。
Horn antenna type radio wave absorber measurement jig 1
In order to measure the radio wave absorption characteristics of the sample 7 using the sample 1, the sample 7 is short-circuited without being loaded, the two doors 15 are securely fastened so as to contact the outer conductor 11, and the coaxial connector 16 is connected.
Is connected to a network analyzer as a measuring instrument. The network analyzer short-circuit-calibrates the completely reflected wave from the short-circuit plate 14. At this time, if the ratio of the horn antenna-like portion 12a and the cylindrical shape portion 12b of the outer conductor 11 is selected in the range of 8: 2 to 9: 1, the reflection in the radio wave absorber measurement jig 11, which is similar to the metal box, is obtained. Produces fewer advantages. Then, as shown in FIG.
Load on top. This loading state is as shown in FIG. 2B, and the 24 samples 7 are arranged on the short-circuit plate 14 via the two opening / closing doors 15 without any gap. At this time, the inner conductor 13
By setting the dimension in the long side direction to 400 mm, a gap of 100 mm was opened from each of the external conductors 11, and the effect of reducing the gap between the samples 7 was exhibited.

【0017】 図3、図4は本発明の第2の実施例に使
用する角型電波吸収体測定ジグ21の構造を示してい
る。角型電波吸収体測定ジグ21は断面が300mm×
300mmの正方形で,角錐状部22aの開口端にやは
り300mm×300mmの正方形の筒形部22bを一
体化させた外部導体22と、この外部導体22の角錐状
部22a及び正方形な筒形部22bの両方にわたって、
外部導体22とは電気的に絶縁され、外部導体22と相
似形で端面が100mm×100mmの内部導体23を
外部導体22と等位置に配置しかつ,試料を装荷し評価
するために,外部導体22と内部導体23の端面で電気
的に短絡する短絡板24と、試料を着脱し外部導体22
との接触を完全とするためのスプリング機構付きの開閉
扉25と,外部導体22と内部導体23の間にTEM波
を印加するためのN型同軸コネクタ26からなる。
FIGS. 3 and 4 show the structure of a square wave absorber measuring jig 21 used in the second embodiment of the present invention. Square wave absorber measuring jig 21 has a cross section of 300 mm x
An external conductor 22 having a square shape of 300 mm and also having a square cylindrical portion 22 b of 300 mm × 300 mm integrated with the open end of the pyramid-shaped portion 22 a, a pyramid-shaped portion 22 a of the external conductor 22 and a square cylindrical portion 22 b Over both,
The inner conductor 23 is electrically insulated from the outer conductor 22, has a shape similar to that of the outer conductor 22, and has an end surface of 100 mm × 100 mm at the same position as the outer conductor 22. A short-circuit plate 24 electrically short-circuited at the end faces of the inner conductor 22 and the inner conductor 23;
An opening / closing door 25 having a spring mechanism for making complete contact with the N-type coaxial connector 26 for applying a TEM wave between the outer conductor 22 and the inner conductor 23.

【0018】 角型電波吸収体測定ジグ21を用いて試
料7の電波吸収特性を測定するには,試料7を装荷しな
い短絡状態とし,2つの開閉扉25を外部導体22に接
触するよう確実に締め,同軸コネクタ26には測定器で
あるネッワークアナライザを接続する。ネッワークアナ
ライザは,短絡板24からの完全反射波を短絡校正す
る。このとき,外部導体21の角錐状部22a及び筒状
部22bの比率が8:2から9:1の範囲に選ぶと,金
属箱と同様である電波吸収体測定ジグ21内での反射が
少ない利点を生ずる。そして100mm角の試料7を図
4(A)のように短絡板24上に装荷する。この装荷状
態は図4(B)のようになり、8枚の試料7が2つの開
閉扉25を介して短絡板24上に隙間なく配列される。
In order to measure the radio wave absorption characteristics of the sample 7 using the square radio wave absorber measurement jig 21, the sample 7 is not loaded and a short circuit state is set, and the two doors 25 are securely contacted with the external conductor 22. Then, a network analyzer as a measuring instrument is connected to the coaxial connector 26. The network analyzer short-circuit-calibrates the completely reflected wave from the short-circuit plate 24. At this time, if the ratio between the pyramid-shaped portion 22a and the cylindrical portion 22b of the outer conductor 21 is selected in the range of 8: 2 to 9: 1, the reflection in the radio wave absorber measuring jig 21 which is similar to the metal box is small. Produce benefits. Then, the sample 7 of 100 mm square is loaded on the short-circuit plate 24 as shown in FIG. This loading state is as shown in FIG. 4B, and eight samples 7 are arranged on the short-circuit plate 24 via the two doors 25 without any gap.

【0019】 電波吸収特性は,実施例1の場合は、試
料7を24枚隙間なく短絡面14上に配列装荷した状態
で,図5のように反射減衰量特性を図5(A)の周波数
領域と図5(B)の時間領域を同時に測定する手段で測
る。
In the case of the first embodiment, in the case of the first embodiment, the return loss characteristics are shown in FIG. 5 with the 24 samples 7 arranged and loaded on the short-circuit surface 14 without any gap. The region and the time region of FIG. 5B are measured simultaneously.

【0020】 測定は図5(A)の周波数領域で、ゲー
ト時間処理を施さない状態での下限周波数fを−20
dBにセット後ゲート処理する。そして図5(B)の時
間領域へ移り、ゲート時間幅を可変調整することに伴っ
て、図5(A)の周波数領域でfが−20dBのレベ
ルに一致するようゲート時間幅を可変する。測定はf
が−20dBと一致したとき完了する。
In the measurement, the lower limit frequency f L in a state where the gate time processing is not performed is −20 in the frequency domain of FIG.
Gate processing after setting to dB. Then, the processing shifts to the time domain of FIG. 5B, and the gate time width is variably adjusted, so that the gate time width is varied so that f L coincides with the level of −20 dB in the frequency domain of FIG. 5A. . Measurement is f L
Is completed when the value is equal to -20 dB.

【0021】 この可変ゲート時間処理法により電波吸
収体測定ジグ11あるいは21内部の反射波の影響をほ
ぼ抑制でき,試料7の電波吸収特性のみを再現性よく高
精度に評価できるようになった。
By the variable gate time processing method, the influence of the reflected wave inside the radio wave absorber measurement jig 11 or 21 can be substantially suppressed, and only the radio wave absorption characteristic of the sample 7 can be evaluated with high reproducibility and high accuracy.

【0022】[0022]

【発明の効果】本発明に係わる電波吸収体測定ジグ11
あるいは21及びその測定法は、上記のような試料着脱
の容易な構造や反射波抑制手法としたことで、電波吸収
体の着脱が容易となりかつ、測定ジグ内部での反射波を
抑制することができた。そのため試料7の電波吸収特性
を高精度で再現よく測定できるようになった。
The radio wave absorber measuring jig 11 according to the present invention.
Alternatively, 21 and its measurement method employ the above-described structure for easily attaching and detaching the sample and the method of suppressing reflected waves, thereby making it easy to attach and detach the radio wave absorber and suppressing reflected waves inside the measurement jig. did it. Therefore, the radio wave absorption characteristics of the sample 7 can be measured with high accuracy and good reproducibility.

【0023】 また,上記電波吸収体測定ジグ11ある
いは21の12aと12bの比及び22aと22bの比
を8:2から9:1の範囲に選ぶことで、可変ゲート時
間処理法が可能となり、試料7の電波吸収特性を高精度
に測定できる効果が生じた。
Further, by selecting the ratio of 12a and 12b and the ratio of 22a and 22b of the radio wave absorber measuring jig 11 or 21 in the range of 8: 2 to 9: 1, a variable gate time processing method becomes possible. The effect that the radio wave absorption characteristics of the sample 7 can be measured with high accuracy has been produced.

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

【図1】 本発明の第1実施例によるホーンアンテナ形
電波吸収体測定ジグの斜視図である。
FIG. 1 is a perspective view of a horn antenna type radio wave absorber measuring jig according to a first embodiment of the present invention.

【図2】 (A)はホーンアンテナ形電波吸収体測定ジ
グの縦断面図、(B)はこれの横断面図である。
2A is a longitudinal sectional view of a horn antenna type radio wave absorber measuring jig, and FIG. 2B is a transverse sectional view thereof.

【図3】 本発明の第2実施例による角形電波吸収体測
定ジグの斜視図である。
FIG. 3 is a perspective view of a square wave absorber measuring jig according to a second embodiment of the present invention.

【図4】 (A)は角形電波吸収体測定ジグの縦断面
図、(B)はこれの横断面図である。
FIG. 4A is a longitudinal sectional view of a rectangular wave absorber measuring jig, and FIG. 4B is a transverse sectional view thereof.

【図5】 可変ゲート処理時間法での測定方法で、
(A)が周波数領域での反射減衰量特性、(B)が時間
領域での反射電圧特性である。
FIG. 5 shows a measurement method using a variable gate processing time method.
(A) is a return loss characteristic in a frequency domain, and (B) is a reflection voltage characteristic in a time domain.

【符号の説明】[Explanation of symbols]

11‥‥‥‥‥‥ホーンアンテナ形電波吸収体測定ジグ 21‥‥‥‥‥‥角形電波吸収体測定ジグ 12、22‥‥‥外部導体 12a‥‥‥‥‥ホーンアンテナ状部 22a‥‥‥‥‥角錐状部 12b、22b‥筒形状部 13、23‥‥‥内部導体 14、24‥‥‥短絡板 15、25‥‥‥開閉扉 16、26‥‥‥同軸コネクタ 11 ‥‥‥‥‥‥ Horn antenna type radio wave absorber measurement jig 21 ‥‥‥‥‥‥ Square radio wave absorber measurement jig 12, 22 ‥‥‥ Outer conductor 12 a ‥‥‥‥‥ Horn antenna-like portion 22 a ‥‥‥ {Pyramidal part 12b, 22b} Cylindrical part 13, 23} Inner conductor 14, 24} Short circuit board 15, 25} Opening door 16, 26} Coaxial connector

───────────────────────────────────────────────────── フロントページの続き (72)発明者 茂木 靖夫 東京都府中市浅間町4丁目14番1号 協立 電子工業株式会社内 ────────────────────────────────────────────────── ─── Continued on the front page (72) Inventor Yasuo Mogi 4-4-1-1, Asama-cho, Fuchu-shi, Tokyo Inside Kyoritsu Electronics Industry Co., Ltd.

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 同軸コネクタからホーンアンテナ状の
広がりをなした断面の短辺と長辺の寸法がそれぞれ40
0mmと600mmの長方形部の開口端面部分に断面形
状が該部分と同等な筒形状部を一体化させた外部導体
と,該外部導体のホーンアンテナ状部および長方形の断
面をなした筒形状部の両方にわたり外部導体内部の短辺
を2等分する位置に外部導体の長辺面の平面形状と相似
で前記外部導体とは接触しないように保持しかつ筒形状
長辺面と同形の幅が400mmの薄板状の内部導体と,
該外部導体の長方形断面の端面部分と該内部導体の薄板
状断面の端面部分を金属製の短絡板で短絡した構造が特
徴な電波吸収体測定ジグ。
The dimensions of a short side and a long side of a cross section of a horn antenna-shaped spread from a coaxial connector are each 40.
An outer conductor in which a tubular portion having a sectional shape equivalent to that of the opening portion of the rectangular portion of 0 mm and 600 mm is integrated, a horn antenna-shaped portion of the outer conductor, and a tubular portion having a rectangular cross section. It is similar to the plane shape of the long side surface of the outer conductor at a position where the short side inside the outer conductor is divided into two equal parts, and is held so as not to contact with the outer conductor, and has the same width as the cylindrical long side surface of 400 mm. A thin inner conductor of
A radio wave absorber measurement jig characterized by a structure in which an end portion of a rectangular cross section of the outer conductor and an end surface portion of a thin plate cross section of the inner conductor are short-circuited by a metal short-circuit plate.
【請求項2】 同軸コネクタから角錐状の広がりをな
した断面寸法が300mmの正方形部に断面形状が該
部分と同様の筒形状部を一体化させた外部導体と,該外
部導体の角錐状部および筒形状部と相似形で筒形状部の
寸法が100mmの内部導体と,該外部導体の正方形
断面の端面部分と該内部導体のやはり正方形断面の端面
部分を金属製の短絡板で短絡した角形の同軸構造が特徴
な電波吸収体測定ジグ。
2. An external conductor in which a cylindrical portion having a cross-sectional shape similar to that of a square portion having a cross-sectional size of 300 mm 2 and having a pyramidal shape extending from the coaxial connector is integrated, and a pyramidal shape of the external conductor. The inner conductor having a shape similar to that of the cylindrical portion and the cylindrical portion and having a cylindrical shape of 100 mm 2 , and a square cross-sectional end surface portion of the external conductor and a square cross-sectional end surface portion of the internal conductor also short-circuited by a metal short-circuit plate. A radio wave absorber measurement jig that features a rectangular coaxial structure.
【請求項3】 請求項1の外部導体及び内部導体のホ
ーンアンテナ状部と筒形状部あるいは請求項2の外部導
体及び内部導体の角錐状部と筒形状部との比率が8:2
から9:1までの割合にある構造が特徴の電波吸収体測
定ジグ。
3. The ratio of the horn antenna-shaped portion and the cylindrical portion of the outer conductor and the inner conductor of claim 1 or the pyramid-shaped portion and the cylindrical portion of the outer conductor and the inner conductor of claim 2 is 8: 2.
A radio wave absorber measurement jig characterized by a structure ranging from 1 to 9: 1.
【請求項4】 請求項1あるいは請求項2の外部導体
のホーンアンテナ状部または角錐状部か筒形状部のどち
らかに測定試料の着脱機能を果たす外部導体とのコンタ
クト面を有する開閉扉を取付ける構造が特徴な電波吸収
体測定ジグ。
4. An open / close door having a contact surface with an external conductor, which functions to attach and detach a measurement sample, to one of a horn antenna-shaped portion, a pyramid-shaped portion, and a cylindrical portion of the external conductor according to claim 1 or 2. A radio wave absorber measurement jig that features a mounting structure.
【請求項5】 電波吸収特性を示す周波数領域での反
射減衰特性の下限周波数が一定の値になるように時間領
域でのゲート時間処理の幅を可変調整することが特徴な
電波吸収体の測定法。
5. A measurement of a radio wave absorber characterized by variably adjusting a width of a gate time processing in a time domain so that a lower limit frequency of a reflection attenuation characteristic in a frequency domain showing a radio wave absorption characteristic becomes a constant value. Law.
JP28861798A 1998-09-04 1998-09-04 Electric wave absorber measuring jig and measuring method thereof Pending JP2000081457A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28861798A JP2000081457A (en) 1998-09-04 1998-09-04 Electric wave absorber measuring jig and measuring method thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28861798A JP2000081457A (en) 1998-09-04 1998-09-04 Electric wave absorber measuring jig and measuring method thereof

Publications (1)

Publication Number Publication Date
JP2000081457A true JP2000081457A (en) 2000-03-21

Family

ID=17732525

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28861798A Pending JP2000081457A (en) 1998-09-04 1998-09-04 Electric wave absorber measuring jig and measuring method thereof

Country Status (1)

Country Link
JP (1) JP2000081457A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20200137258A (en) * 2019-05-29 2020-12-09 국방과학연구소 Surface contact type device of measuring electromagnetic radiation absorbance and method of measuring electromagnetic radiation absorbance of object using the same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20200137258A (en) * 2019-05-29 2020-12-09 국방과학연구소 Surface contact type device of measuring electromagnetic radiation absorbance and method of measuring electromagnetic radiation absorbance of object using the same
KR102219340B1 (en) * 2019-05-29 2021-02-23 국방과학연구소 Surface contact type device of measuring electromagnetic radiation absorbance and method of measuring electromagnetic radiation absorbance of object using the same

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