JPS62247601A - Fixed resistance attenuator - Google Patents

Fixed resistance attenuator

Info

Publication number
JPS62247601A
JPS62247601A JP8137186A JP8137186A JPS62247601A JP S62247601 A JPS62247601 A JP S62247601A JP 8137186 A JP8137186 A JP 8137186A JP 8137186 A JP8137186 A JP 8137186A JP S62247601 A JPS62247601 A JP S62247601A
Authority
JP
Japan
Prior art keywords
transmission line
frequency
lines
resistors
fixed resistance
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
JP8137186A
Other languages
Japanese (ja)
Other versions
JPH0261165B2 (en
Inventor
Haruki Nishida
西田 治樹
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.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP8137186A priority Critical patent/JPS62247601A/en
Publication of JPS62247601A publication Critical patent/JPS62247601A/en
Publication of JPH0261165B2 publication Critical patent/JPH0261165B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Non-Reversible Transmitting Devices (AREA)

Abstract

PURPOSE:To obtain a fixed resistance attenuator having comparatively satisfactory frequency characteristics by inserting a transmission line having a characteristic impedance lower than that of other two transmission lines and the electrical length of 1/4 wavelength compared with the using frequency in series between said two transmission lines via resistors. CONSTITUTION:A transmission line 31 having an impedance lower than those of both transmission lines 30 and 32 is inserted between these two lines 30 and 32. These lines 30-32 are connected with each other by the 1st and 2nd resistors 33 and 34. In this case, the electrical length of the 2nd transmission line 31 is set at 1/4 using frequency so that the impedances are equal to pure resistance in terms of both resisters 33 and 34. For instance, the impedances of both lines 30 and 32 are set at 50OMEGA together with the resistance values of resistors 33 and 34 set at 25OMEGA and the impedance of the line 31 set at 43.3OMEGA respectively. Under such conditions, a 4-6GHz using frequency band is secured with 5dB insertion loss and 20dB reflection loss respectively.

Description

【発明の詳細な説明】 〔概要〕 固定抵抗減衰器において、第1の伝送線路と第2の伝送
線路及び第2の伝送線路と第3の伝送線路とをそれぞれ
第1及び第2の抵抗器を介して接続し、第2の伝送線路
は第1及び第2の抵抗器を見たインピーダンスが所定の
周波数で純抵抗と見える位置の間隔がλg/4(λgは
短縮波長)となる様な電気長を有すると共に、特性イン
ピーダンスを第1及び第3の伝送線路のそれよりも低く
することにより、低価格で比較的良好な周波数特性が得
られる様にしたものである。
[Detailed Description of the Invention] [Summary] In a fixed resistance attenuator, a first transmission line and a second transmission line, and a second transmission line and a third transmission line are connected to the first and second resistors, respectively. and the second transmission line is connected so that the distance between the positions where the impedance of the first and second resistors appears to be pure resistance at a predetermined frequency is λg/4 (λg is the shortened wavelength). By having a long electrical length and a characteristic impedance lower than that of the first and third transmission lines, relatively good frequency characteristics can be obtained at a low cost.

〔産業上の利用分野〕[Industrial application field]

本発明は固定抵抗減衰器、特にマイクロ波帯で使用され
る固定抵抗減衰器の改良に関するものである。
The present invention relates to improvements in fixed resistance attenuators, particularly fixed resistance attenuators used in the microwave band.

固定抵抗減衰器は、例えばマイクロ波回路の殆ど全ての
回路に使用されているが、低価格でしかも比較的良好な
周波数特性を持つことが必要である。
Fixed resistance attenuators are used in almost all microwave circuits, for example, and are required to be inexpensive and have relatively good frequency characteristics.

〔従来の技術〕[Conventional technology]

第3図は従来例の構成図、第4図は別の従来例の構成図
、第5図は更に別の従来例の構成図を示す。以下、第3
図〜第5図により固定抵抗減衰器の従来例の構成等を説
明する。
FIG. 3 is a block diagram of a conventional example, FIG. 4 is a block diagram of another conventional example, and FIG. 5 is a block diagram of still another conventional example. Below, the third
The structure of a conventional example of a fixed resistance attenuator will be explained with reference to FIGS.

第3図(alは平面図、第3図(b)は第3図(a)の
A−A“断面図を示すが、第3図に示す様に接地導体5
の上に固定されたアルミナ基板4の上に形成された抵抗
膜2でストリップ線路1が切断され、この抵抗膜の両端
は接地金具3.3“を介して接地される。この様な構成
の固定抵抗減衰器は直流から例えば10GHz程度まで
使用可能であり、測定器等にも用られるが■アルミナ基
板を使用する ■抵抗膜を所定の値に調整しなければな
らないので高価であり接地金具が必要となる。
FIG. 3 (al is a plan view, and FIG. 3(b) is a cross-sectional view taken along line A-A in FIG. 3(a). As shown in FIG. 3, the ground conductor 5
The strip line 1 is cut by a resistive film 2 formed on an alumina substrate 4 fixed thereon, and both ends of this resistive film are grounded via grounding fittings 3.3''. Fixed resistance attenuators can be used from DC to about 10 GHz, and are also used in measuring instruments, etc. However, they use an alumina substrate, are expensive because the resistive film must be adjusted to a specified value, and require no grounding fittings. It becomes necessary.

第4図はπ形の固定抵抗減衰器で第4図(alはアルミ
ナ基板上に薄膜抵抗器6,7.8で形成し、この抵抗器
7.8の一端はλg/4オーブンスタブ9.10に接続
される。この様な構成のものは抵抗器の一端が短絡と見
なされる帯域においては減衰量、特性インピーダンス等
について問題なく使用可能である。尚、1はストリップ
線路である。
FIG. 4 shows a π-type fixed resistance attenuator (Al is formed of thin film resistors 6, 7.8 on an alumina substrate, and one end of this resistor 7.8 is connected to a λg/4 oven stub 9. 10. Such a configuration can be used without problems regarding attenuation, characteristic impedance, etc. in a band where one end of the resistor is considered to be short-circuited. Note that 1 is a strip line.

第4図(b)はフローグラス基板又はエポキシ基板(ア
ルミナ基板よりも低価格)等の上に形成されたストリッ
プ線路11.12にチップ抵抗器13.14゜15を接
続したもので、第4図(a)と同じくπ型の固定抵抗減
衰器である。尚、チップ抵抗器13.15の一端がスル
ーホール16.16“を介して接地されるが、チップ抵
抗器は低価格で、又半田付は作業で接続が可能なことか
ら数100MHz〜2 GHz程度まで使用可能である
Figure 4(b) shows a chip resistor 13.14°15 connected to a strip line 11.12 formed on a flow glass substrate or an epoxy substrate (lower price than an alumina substrate). It is a π-type fixed resistance attenuator like the one in Figure (a). Note that one end of the chip resistor 13.15 is grounded through the through hole 16.16'', but since chip resistors are inexpensive and can be connected by soldering, it is possible to connect at several 100 MHz to 2 GHz. It can be used to some extent.

第5図(a)、第5図(b)は第4図(a)、第4図(
blのπ型の固定抵抗減衰器の代りにT型で構成したも
ので、16.17.18は薄膜抵抗器、19はλg/4
オープンスタブ、20〜22はストリップ線路、23〜
25はチップ抵抗器で使用可能な周波数範囲は上記と同
じである。第5図(C)は第5図(blのスルーホール
16゜柔gグを介しての接地でなく、λg /4オーブ
ンスタブにより高周波的に接地する。しかし、使用周波
数が4 GHz以上になると、抵抗器の寸法により抵抗
膜の外に虚数部が現れて減衰量、特性インピーダンスが
所望の値より劣化する。
Figure 5(a) and Figure 5(b) are shown in Figure 4(a) and Figure 4(
Instead of the π-type fixed resistance attenuator in bl, it is configured with a T-type, and 16, 17, and 18 are thin film resistors, and 19 is a λg/4
Open stub, 20~22 is strip line, 23~
25 is a chip resistor, and the usable frequency range is the same as above. Figure 5 (C) shows that the grounding is not done through the 16° flexible through hole in Figure 5 (bl), but is grounded at a high frequency using a λg/4 oven stub. However, if the operating frequency is 4 GHz or higher, Depending on the dimensions of the resistor, an imaginary part appears outside the resistive film, causing the attenuation amount and characteristic impedance to deteriorate from desired values.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

上記で説明した様に、周波数特性が良好な固定抵抗減衰
器は高価で、低価格のものは周波数特性が悪く、低価格
で、比較的周波数特性の良好な固定抵抗減衰器を得るこ
とが困難であると云う問題点がある。
As explained above, fixed resistance attenuators with good frequency characteristics are expensive, low-priced ones have poor frequency characteristics, and it is difficult to obtain fixed resistance attenuators with relatively good frequency characteristics at a low price. There is a problem with this.

〔問題点を解決する為の手段〕[Means for solving problems]

上記の問題点は第1図に示す如く、第1の伝送線路30
と第2の伝送線路31及び該2の伝送線路と第3の伝送
線路32とを、第1の抵抗器33及び第2の抵抗器34
を介して接続し、該第2の伝送線路31は、該第1及び
第2の抵抗器を見たインピーダンスが所定の周波数で純
抵抗と見える位置の間隔がλg/4となる様な電気長を
有すると共に、該第1及び第3の伝送線路30.32の
特性インピーダンスより低く設定された特性インピーダ
ンスを持つ本発明の固定抵抗減衰器により解決される。
The above problem is caused by the first transmission line 30 as shown in FIG.
and the second transmission line 31, the second transmission line and the third transmission line 32, and the first resistor 33 and the second resistor 34.
The second transmission line 31 has an electrical length such that the distance between the positions where the impedance of the first and second resistors appears to be pure resistance at a predetermined frequency is λg/4. This problem is solved by the fixed resistance attenuator of the present invention having a characteristic impedance set lower than the characteristic impedance of the first and third transmission lines 30, 32.

〔作用〕[Effect]

本発明は第2の伝送線路の電気長を抵抗器33及び34
を見たインピーダンスが所要の周波数で純抵抗と見える
位置の間隔がλg/4となる様にし、抵抗器33の抵抗
値RI+第2の伝送線路のインピーダンスZ+、抵抗器
34の抵抗値R2+  と負荷インピーダンスZLとで
電圧分配を行う事により減衰特性を得る様にした。
In the present invention, the electrical length of the second transmission line is determined by resistors 33 and 34.
The distance between the positions where the impedance seen as a pure resistance at the required frequency is λg/4, and the resistance value RI of the resistor 33 + the impedance Z+ of the second transmission line, the resistance value R2+ of the resistor 34, and the load. Attenuation characteristics were obtained by performing voltage distribution with impedance ZL.

即ち1周波数が高くなるにつれて抵抗器の寸法による純
抵抗と見える位相のずれ(電気長のずれ)が大きくなり
周波数特性が劣化するが、抵抗器33、34の純抵抗と
見える位置をλg離れに配置することで解決できる。但
し、抵抗器33.34の寸法が合わせてλg/4以上の
周波数にでは上記の構成ができないので、以下の周波数
に限る。
In other words, as the frequency increases, the phase difference (deviation in electrical length) that appears to be pure resistance due to the dimensions of the resistor increases, deteriorating the frequency characteristics. This can be solved by placing it. However, since the above configuration cannot be achieved when the dimensions of the resistors 33 and 34 are combined at a frequency of λg/4 or more, the frequency is limited to the following.

これにより、低価格、簡単な構成で比較的周波数特性の
良好な固定抵抗減衰器が得られる。
As a result, a fixed resistance attenuator with relatively good frequency characteristics can be obtained at a low cost and with a simple configuration.

〔実施例〕〔Example〕

損失の計算値と実測値を示す。 Calculated and measured loss values are shown.

先ず、第1図に示す本発明の実施例の等価回路を求める
と、第2図(alに示す様になる。
First, when an equivalent circuit of the embodiment of the present invention shown in FIG. 1 is obtained, it becomes as shown in FIG. 2 (al).

ここで、R,、R2は抵抗器33.34の抵抗値、z、
は第2の伝送線路のインピーダンス、 Z、、Z、は負
荷。
Here, R,, R2 are the resistance values of the resistors 33 and 34, z,
is the impedance of the second transmission line, and Z, , Z, is the load.

信号源インピーダンスをそれぞれ示す。The signal source impedance is shown respectively.

第2図(alに示す回路の特性は公知の様にF行列を用
いることにより容易に求めることができる。
The characteristics of the circuit shown in FIG. 2 (al) can be easily determined by using the F matrix as is well known.

であり、 中心周波数では で求められる。and At the center frequency is required.

但し、計算値は抵抗器のみとして計算しているが、実際
にはチップ抵抗器の寸法による位相ずれ及びλgの周波
数特性により虚数部が入ってくるので、中心周波数から
離れるに従って特性も、変化する。
However, although the calculated value is calculated using only the resistor, in reality, an imaginary part is included due to the phase shift due to the dimensions of the chip resistor and the frequency characteristics of λg, so the characteristics will change as you move away from the center frequency. .

例えば、R,=R,=25Ω、第2の伝送線路のインピ
ーダンス43.3Ω、信号源インピーダンスZsと負値
が得られ、5 GHzでλg/4になる様な間隔にしで
あるので反射損失は非常に大きくなって反射される電力
は小さく(即ち、通過する電力が大きく)なるが、周波
数がこれよりもずれると虚数部が生じて反射損失が劣化
する。叉、挿入損失は4〜を実測すると実線の様な値が
得られ、約4〜6GH2程度で反射損先約20dB以上
、挿入損先約5dBが得られ、前記の第5図fc)の4
 GHz程度よりも高い6 GHz程度でも十分に使用
可能であり、抵抗器とし 〜ノ てチップ抵抗器を、誘電体基板としてフローグラス基板
を用いるので低価格である。
For example, negative values are obtained for R, = R, = 25 Ω, the impedance of the second transmission line is 43.3 Ω, and the signal source impedance Zs, and the spacing is λg/4 at 5 GHz, so the reflection loss is If the frequency becomes very large, the reflected power will be small (that is, the transmitted power will be large), but if the frequency deviates beyond this value, an imaginary part will occur and the reflection loss will deteriorate. Furthermore, when the insertion loss is actually measured from 4 to 4, a value like the solid line is obtained, and at about 4 to 6 GH2, a reflection loss of about 20 dB or more and an insertion loss of about 5 dB are obtained, which is 4 in Figure 5 fc) above.
It is sufficiently usable even at a frequency of about 6 GHz, which is higher than about GHz, and is inexpensive because a chip resistor is used as the resistor and a flow glass substrate is used as the dielectric substrate.

〔発明の効果〕〔Effect of the invention〕

上記で詳細に説明した様に本発明によれば、チップ抵抗
器と例えばフローグラス基板を用いて低価格で比較的周
波数特性の良好な固定抵抗減衰器が得られると云う効果
がある。
As explained in detail above, the present invention has the advantage that a fixed resistance attenuator with relatively good frequency characteristics can be obtained at a low cost by using a chip resistor and, for example, a flow glass substrate.

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

第1図は本発明の実施例の構成図、 第2図は第1図の減衰特性図、 第3図は従来例の構成図、 第4図は別の従来例の構成図、 第5図は更に別の従来例の構成図を示す。 図において、 30は第1の伝送線路、 31は第2の伝送線路、 32は第3の伝送線路、 33は第1の抵抗器、 34は第2の抵抗器を示す。 不会旧月0逮3枳靴例aTIt戸ぐじ〕%−tD 不 2 ■ (C) 史(−男i]の屹未例0)末牡1堕 早 5 口 FIG. 1 is a configuration diagram of an embodiment of the present invention, Figure 2 is the attenuation characteristic diagram of Figure 1, Figure 3 is a configuration diagram of the conventional example. FIG. 4 is a configuration diagram of another conventional example, FIG. 5 shows a configuration diagram of yet another conventional example. In the figure, 30 is a first transmission line; 31 is a second transmission line; 32 is the third transmission line, 33 is the first resistor; 34 indicates a second resistor. Non-meeting old month 0 arrest 3 shoes example aTIt doorguji]%-tD Un 2 ■ (C) History (-man i)'s unheard 0) Sueo 1 fall 5 mouths early

Claims (1)

【特許請求の範囲】  第1の伝送線路(30)と第2の伝送線路(31)及
び該2の伝送線路と第3の伝送線路(32)とを、第1
の抵抗器(33)及び第2の抵抗器(34)を介して接
続し、 該第2の伝送線路(31)は、該第1及び第2の抵抗器
を見たインピーダンスが所定の周波数で純抵抗と見える
位置の間隔がλg/4となる様な電気長を有すると共に
、該第1及び第3の伝送線路(30、32)の特性イン
ピーダンスより低く設定された特性インピーダンスを持
つことを特徴とする固定抵抗減衰器。
[Claims] The first transmission line (30) and the second transmission line (31), and the two transmission lines and the third transmission line (32) are connected to the first transmission line (30) and the second transmission line (31).
is connected through a resistor (33) and a second resistor (34), and the second transmission line (31) has an impedance looking at the first and second resistors at a predetermined frequency. It is characterized by having an electrical length such that the distance between the positions that appear to be pure resistance is λg/4, and having a characteristic impedance set lower than the characteristic impedance of the first and third transmission lines (30, 32). Fixed resistance attenuator.
JP8137186A 1986-04-09 1986-04-09 Fixed resistance attenuator Granted JPS62247601A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8137186A JPS62247601A (en) 1986-04-09 1986-04-09 Fixed resistance attenuator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8137186A JPS62247601A (en) 1986-04-09 1986-04-09 Fixed resistance attenuator

Publications (2)

Publication Number Publication Date
JPS62247601A true JPS62247601A (en) 1987-10-28
JPH0261165B2 JPH0261165B2 (en) 1990-12-19

Family

ID=13744449

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8137186A Granted JPS62247601A (en) 1986-04-09 1986-04-09 Fixed resistance attenuator

Country Status (1)

Country Link
JP (1) JPS62247601A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003289205A (en) * 2003-03-27 2003-10-10 Murata Mfg Co Ltd Dielectric line attenuator, terminator and radio apparatus
RU2743940C1 (en) * 2020-05-26 2021-03-01 Федеральное Государственное Бюджетное Образовательное Учреждение Высшего Образования «Новосибирский Государственный Технический Университет» Fixed attenuator

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2003289205A (en) * 2003-03-27 2003-10-10 Murata Mfg Co Ltd Dielectric line attenuator, terminator and radio apparatus
RU2743940C1 (en) * 2020-05-26 2021-03-01 Федеральное Государственное Бюджетное Образовательное Учреждение Высшего Образования «Новосибирский Государственный Технический Университет» Fixed attenuator

Also Published As

Publication number Publication date
JPH0261165B2 (en) 1990-12-19

Similar Documents

Publication Publication Date Title
CN114421113B (en) Low-loss high-isolation one-to-eight power divider
US5235296A (en) Directional coupler using a microstrip line
CN114464973A (en) Reconfigurable filter attenuator based on continuously adjustable center frequency
GB2170358A (en) Microwave power divider
JPH06152206A (en) Reflectionless termination
CN112448113A (en) Butterfly-shaped microstrip filtering power divider
JPS62247601A (en) Fixed resistance attenuator
US6657518B1 (en) Notch filter circuit apparatus
NO970558L (en) Wilkinson split device that can be bypassed
JPS5930323B2 (en) Reflection-free termination for strip line
JPS62247602A (en) Fixed resistance attenuator
JPH08279704A (en) Resistance element for termination
CN119766181B (en) An attenuator chip
US4799032A (en) Directional coupler
Linner et al. Theory and design of broad-band nongrounded matched loads for planar circuits (short paper)
JPS60160201A (en) Attenuator
JP3131342B2 (en) High frequency detection circuit
JP3807032B2 (en) Phase shifter
JPS6058605B2 (en) π type resistor attenuator
KR19990031577A (en) Wilkenson Power Splitter
CN220400879U (en) Broadband microstrip directional coupler
JPH04127701A (en) Microstrip line attenuator
JPS60173901A (en) Diode line switching device
JPS6149843B2 (en)
JPH0555813A (en) Micro strip line terminator