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JPS6225283B2 - - Google Patents
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JPS6225283B2 - - Google Patents

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Publication number
JPS6225283B2
JPS6225283B2 JP11390380A JP11390380A JPS6225283B2 JP S6225283 B2 JPS6225283 B2 JP S6225283B2 JP 11390380 A JP11390380 A JP 11390380A JP 11390380 A JP11390380 A JP 11390380A JP S6225283 B2 JPS6225283 B2 JP S6225283B2
Authority
JP
Japan
Prior art keywords
coupling
frequency
parallel
resonator
filter
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.)
Expired
Application number
JP11390380A
Other languages
Japanese (ja)
Other versions
JPS5738001A (en
Inventor
Mitsuo Makimoto
Sadahiko Yamashita
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP11390380A priority Critical patent/JPS5738001A/en
Publication of JPS5738001A publication Critical patent/JPS5738001A/en
Publication of JPS6225283B2 publication Critical patent/JPS6225283B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/201Filters for transverse electromagnetic waves
    • H01P1/203Strip line filters
    • H01P1/20327Electromagnetic interstage coupling
    • H01P1/20354Non-comb or non-interdigital filters
    • H01P1/20363Linear resonators

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Control Of Motors That Do Not Use Commutators (AREA)

Description

【発明の詳細な説明】 本発明は高周波用帯域通過波器に関する。従
来よりマイクロ波集積回路(MIC)に用いられる
帯域通過フイルタは、第1図に示すように両端開
放λg/2共振器を通過域中心周波数において電気長 90゜(π/2)で平行結合させて構成される。第1図 は2段帯域通過波器(以下、BPFという)の例
で11,12は入出力線路、13,14はTEM
線路共振器を示し、θ01,θ23は入出力の結合電
気長、θ12は共振器間の結合長を示す。この結合
長は前述した如く、通過域中心周波数において、
θ01=θ12=θ23=90゜に選ぶ。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high frequency bandpass waver. Conventionally, bandpass filters used in microwave integrated circuits (MICs) have two open-ended λg/2 resonators coupled in parallel with an electrical length of 90° (π/2) at the center frequency of the passband, as shown in Figure 1. It consists of Figure 1 shows an example of a two-stage bandpass filter (hereinafter referred to as BPF), where 11 and 12 are input and output lines, and 13 and 14 are TEM
The line resonator is shown, θ 01 and θ 23 are input and output coupling electrical lengths, and θ 12 is the coupling length between the resonators. As mentioned above, this coupling length is, at the passband center frequency,
Select θ 01 = θ 12 = θ 23 = 90°.

いま周波数を、電磁波の伝搬速度をVg、共
振器の特性アドミタンスをYo、共振器の実際の
長さをl2とし、共振器の開放端より見たアドミタ
ンスをYiとすると、 Yi=jYoton(2πl/Vg) となる。共振条件はYi=Oで与えられるから、
共振周波数は、 2πl/Vg=nπ(n=1,2,3,……) となる。最も低い共振周波数をとすると、こ
れはn=1に対応するから、 2πl/Vg=π となり、を用いて共振条件を書き直すと =n(n=1,2,3,……)となり、
の整数倍にも共振が生ずることになる。い
ま、結合度に周波数特性がないものと仮定するな
らば、第1図に示すフイルタの特性は第2図に示
すように、2,3,4にスプリアス
応答を持つ特性となる。実際には結合度は周波数
特性を持つため、第2図は結合回路が理想的な場
合の応答である。第3図に平行結合回路の部分を
抜き出して示す。結合電気長をθcとすると、そ
の結合度Kの特性は第4図のようになり、 θc=π/2(2m+1) (m=0,1,2,3,……) で最大・θc=kπ(1,2,3,……)の時、
零となる。
Now, let the frequency be the propagation velocity of the electromagnetic wave, Vg be the characteristic admittance of the resonator, Yo be the actual length of the resonator, and let Yi be the admittance seen from the open end of the resonator, then Yi=jYoton(2πl /Vg). Since the resonance condition is given by Yi=O,
The resonance frequency is 2πl/Vg=nπ (n=1, 2, 3,...). If the lowest resonant frequency is 0 , this corresponds to n=1, so 2πl/Vg 0 =π, and if we rewrite the resonance condition using 0 , we get =n 0 (n=1, 2, 3,... ), and
Resonance will also occur at integral multiples of 0 . If we assume that the degree of coupling has no frequency characteristic, the characteristics of the filter shown in FIG. 1 will have spurious responses at 2 0 , 3 0 , and 4 0 as shown in FIG. 2 . In reality, the degree of coupling has frequency characteristics, so FIG. 2 shows the response when the coupling circuit is ideal. FIG. 3 shows an extracted portion of the parallel coupling circuit. If the electrical bond length is θ c , the characteristics of the degree of coupling K are as shown in Figure 4, and the maximum value is θ c = π/2 (2m + 1) (m = 0, 1, 2, 3, ...). When θ c = kπ (1, 2, 3, ...),
It becomes zero.

ところで結合電気長は、周波数に比例して増大
するから、中心周波数で結合電気長を90゜に
選ぶと2,3,4での電気長の180
゜,270゜,360゜となる。したがつてこの場合の
結合度Kの周波数特性は、第5図のようになり、
,4,6で結合がなくなりような
特性を持つことになる。
By the way, the bond electrical length increases in proportion to the frequency, so if you choose the bond electrical length to be 90 degrees at the center frequency of 0 , the electrical length at 20 , 30 , and 40 will be 180 degrees.
゜, 270゜, 360゜. Therefore, the frequency characteristic of the degree of coupling K in this case is as shown in Fig. 5,
It has a characteristic that the bond disappears at 2 0 , 4 0 , and 6 0 .

以上のことにより、通常の両端開放λg/2共振器 を用いた90゜平行結合フイルタ(第1図の例)の
周波数応答は、第6図に示すものとなる。即ち2
,4,6は結合度が零となるため、
スプリアス共振は生じてもレスポンスは小さく、
,5を中心として大きなスプリアス応
答をもつことになる。
As a result of the above, the frequency response of a 90° parallel coupling filter (example shown in FIG. 1) using a normal λg/2 resonator with both ends open is as shown in FIG. 6. That is, 2
0 , 4 0 , 6 0 have zero connectivity, so
Even if spurious resonance occurs, the response is small,
This results in large spurious responses centered around 30 and 50 .

さて従来結合長が90゜に選ばれていた理由の1
つには、結合部の設計が容易であること、また
を中心として結合度の変化が最も少なく、その
変化がを中心として対称特性を示すことが主
たる理由である。ところで第6図に示す従来のフ
イルタが持つ特性は発振器、増幅器の出力フイル
タとして用いるとその出力成分として存在する3
次の高周波成分の抑圧に対しては何らの効果も持
たない。
Now, one of the reasons why the bond length was conventionally chosen to be 90°
The main reason is that the joint design is easy, and
The main reason is that the change in the degree of bonding is the smallest around 0 , and the change exhibits symmetrical characteristics around 0 . By the way, the characteristics of the conventional filter shown in Figure 6 exist as an output component when used as an output filter for an oscillator or amplifier.
It has no effect on the suppression of the next high frequency component.

本発明は、従来のフイルタの持つ3におけ
るスプリアス応答を低減した阻止域の広い高周波
用帯域通過波器を提供せんとするものである。
SUMMARY OF THE INVENTION The present invention aims to provide a high-frequency bandpass filter with a wide stopband and which reduces the spurious response of conventional filters.

本発明はTEM線路共振器として両端開放型の
λg/2共振器を平行結合させて平行結合部を形成し てなる高周波用帯域通過波器において、前記平
行結合部のうち結合電気長が90度および60度のも
のを少なくとも1個ずつ設けることにより、上記
目的を達成するものである。
The present invention provides a high-frequency bandpass waver as a TEM line resonator in which a parallel coupling portion is formed by coupling λg/2 resonators with both ends open in parallel, and a coupling electrical length of the parallel coupling portion is 90 degrees. The above object is achieved by providing at least one angle angle of 60 degrees and one angle of 60 degrees.

もう1つの発明としてはTEM線路共振器とし
て一端開放・他端短絡のλg/4共振器を平行結合さ せて平行結合部を形成してなる高周波用帯域通過
波器において、前記平行結合部のうち結合電気
長が60度のものを少なくとも1個設けることによ
り、上記目的を達成するものである。
Another invention is a high-frequency bandpass waver in which a λg/4 resonator with one end open and the other end short-circuited is coupled in parallel to form a parallel coupling part as a TEM line resonator. The above object is achieved by providing at least one bond having an electrical length of 60 degrees.

以下、図面を参照しながら、本発明の一実施例
について説明する。
An embodiment of the present invention will be described below with reference to the drawings.

第8図は本発明の一実施例を示すものである。
81,82は入出力線路、83〜85はλ/2共振 器、θ01〜θ34は結合部の電気長を示す。いま電
気長と中心周波数においてθ01=θ34=90゜,θ
12=θ23=60゜に選んだ場合を考える。共振器8
3〜85はλg/2型であるのでn(n=1, 2,3)でスプリアス共振を生ずるが、結合長θ
01,θ34部分は結合電気長が90゜であるので2
,4,6で結合が生ぜず、θ12,θ23
の部分は結合電気長が60゜であるので、3
,9で結合を生じない。
FIG. 8 shows an embodiment of the present invention.
81 and 82 are input/output lines, 83 to 85 are λ 0 /2 resonators, and θ 01 to θ 34 are electrical lengths of the coupling portions. Now, at the electrical length and center frequency, θ 01 = θ 34 = 90°, θ
Consider the case where 12 = θ 23 = 60°. Resonator 8
Since 3 to 85 are of the λg/2 type, spurious resonance occurs at n 0 (n = 1, 2, 3), but the coupling length θ
01 , θ 34 part has a bond electrical length of 90°, so 2
No bond occurs at 0 , 4 0 , 6 0 , θ 12 , θ 23
Since the bond electrical length of the part is 60°, 3 0 ,
No bonding occurs at 60 and 90 .

第7図に、結合電気長を中心周波数におい
て、60゜に選んだ場合の結合度Kの周波数特性を
示す。電気長はで60゜であるから、3
おいては180゜となり、この時第4図に示すよう
に結合度Kは零となる。
FIG. 7 shows the frequency characteristics of the degree of coupling K when the electrical coupling length is selected to be 60° at the center frequency of 0 . Since the electrical length is 60° at 0 , it becomes 180° at 30 ° , and at this time, the degree of coupling K becomes zero as shown in Figure 4.

したがつて第8図の構成のフイルタの応答は第
9図に示すように、2,3,4のス
プリアス応答を低減でき広帯域な阻止域が実現可
能となる。
Therefore, as shown in FIG. 9, the response of the filter having the configuration shown in FIG. 8 can reduce the spurious responses of 2 0 , 3 0 , and 4 0 and achieve a wide stop band.

なお、実施例では3段のフイルタを説明した
が、本発明は段数には関係せず、任意の段数のフ
イルタへも適用できるものである。また結合長も
少くとも1つが90°,60゜の部分があればスプリ
アス応答の低減は可能である。
Note that although a three-stage filter has been described in the embodiment, the present invention is not related to the number of stages and can be applied to a filter with any number of stages. Furthermore, if at least one of the bond lengths is 90° and 60°, the spurious response can be reduced.

次に、他の本発明について説明する。 Next, another aspect of the present invention will be explained.

第10図は他の本発明の実施例である。この実
施例は4段のインタデイジタル型フイルタに適用
した場合を示している。101,102は入出力
結合回路部、103〜106が一端開放、他端短
絡のλg/4 共振器、θcは平行結合部の電気長であ る。θcは従来は90゜に選んで設計されるが、本
発明はこれを60゜に選び3のスプリアス応答
を低減した特性を持たせている。
FIG. 10 shows another embodiment of the present invention. This embodiment shows a case where the present invention is applied to a four-stage interdigital type filter. 101 and 102 are input/output coupling circuit parts, 103 to 106 are λg/4 resonators with one end open and the other end short-circuited, and θ c is the electrical length of the parallel coupling part. Conventionally, θ c is selected to be 90° in the design, but in the present invention, it is selected to be 60° to provide a characteristic that reduces spurious response by 30° .

λg/4共振器の開放端よりみたアドミタンスは、 Yi=jYocot(2πl/Vg) となる。(l:共振器長、Vg:電磁波の速度、
Yo:共振器特性アドミタンス)Yi=Oが共振条
件であるから、スプリアス共振は基本共振周波数
として =(2n+1)(n=1,2,3,……) となり、3,5,7……にスプリア
スを生じる。また、結合電気長を90゜に選ぶと、
第5図に示すように、3、5,7
…では結合度は最大となるから、この場合のフイ
ルタの応答は第11図のようになり、の奇数
倍のところにスプリアス応答を生ずる。
The admittance seen from the open end of the λg/4 resonator is Yi=jYocot(2πl/Vg). (l: resonator length, Vg: velocity of electromagnetic wave,
Yo: resonator characteristic admittance) Since Yi= O is the resonance condition, the spurious resonance becomes = (2n + 1) 0 ( n = 1, 2, 3, ...) with the fundamental resonance frequency as 0, and 3 0 , 5 0 ,7 0 . . generates spurious signals. Also, if the bond electrical length is chosen to be 90°,
As shown in Fig. 5, 30 , 50 , 70 ...
..., the degree of coupling is maximum, so the response of the filter in this case is as shown in Figure 11, and spurious responses occur at odd multiples of 0 .

本発明の如くθc=60゜に選ぶと、結合度の周
波数特性は第7図のようになり3で結合が生
じなくなり、フイルタの応答も第12図のように
まで阻止域が拡大する。
When θ c =60° is selected as in the present invention, the frequency characteristic of the degree of coupling becomes as shown in Fig. 7, where no coupling occurs at 30 ° , and the response of the filter also has a stopband up to 50° as shown in Fig. 12. Expanding.

インタデイジタル型フイルタの場合は入出力結
合は、第10図に示すように、磁界結合が多く用
いられるため、本発明は2段以上のフイルタに適
用できる。
In the case of interdigital type filters, magnetic field coupling is often used for input/output coupling as shown in FIG. 10, so the present invention can be applied to filters with two or more stages.

以上述べたように本発明は、TEM線路共振器
として両端開放型のλg/2共振器を平行結合させて 平行結合部を形成してなる高周波用帯域通過波
器において、前記平行結合部のうち結合電気長が
90度および60度のものを少なくとも1個ずつ設け
ることにより、あるいはTEM線路共振器として
一端開放・他端短絡のλg/4共振器を平行結合させ て平行結合部を形成してなる高周波用帯域通過
波器において、前記平行結合部のうち結合電気長
が60度のものを少なくとも1個設けることによ
り、3におけるスプリアス応答を低減たもの
であり、阻止域が拡大され、発振器、増幅器の出
力フイルタとしての利用価値がきわめて高いもの
である。
As described above, the present invention provides a high-frequency bandpass waver in which a parallel coupling portion is formed by coupling λg/2 resonators with both ends open in parallel as a TEM line resonator. The bond electrical length is
A high-frequency band formed by providing at least one 90-degree and one 60-degree resonator, or by parallel coupling λg/4 resonators with one end open and the other end short-circuited as a TEM line resonator to form a parallel coupling part. By providing at least one of the parallel coupling parts with a coupling electrical length of 60 degrees in the pass wave device, the spurious response at 30 ° C is reduced, the stopband is expanded, and the output of the oscillator and amplifier is It has extremely high utility value as a filter.

【図面の簡単な説明】 第1図はλg/2共振器を用いた従来のフイルタの 構成図、第2図は結合度が周波数をもたない場合
の第1図のフイルタ周波数応答を示す図、第3図
は平行結合部の説明図、第4図は結合度と結合電
気長の関係を示す図、第5図は中心周波数
おいて結合電気長を90゜に選んだ場合の結合度K
の周波数特性を示す図、第6図は結合長を90゜と
した時の第1図のフイルタの周波数応答を示す
図、第7図は結合長を60゜に選んだ場合の平行結
合部の結合度周波数特性を示す図、第8図は本発
明の一実施例における高周波用帯域通過波器の
構成図、第9図は第8図の構成の周波数応答を示
す図、第10図は本発明の他の実施例の構成図、
第11図は従来のインタデイジタルフイルタの応
答を示す図、第12図は本発明のフイルタの周波
数応答を示す図である。 81,82……入出力線路、83〜85……
λg/2共振器、θ01〜θ34……結合部の電気長、1 01,102……入出力結合回路部、103〜1
06……λg/4共振器、θc……平行結合部の電気 長。
[Brief Description of the Drawings] Figure 1 is a diagram showing the configuration of a conventional filter using a λg/2 resonator, and Figure 2 is a diagram showing the frequency response of the filter in Figure 1 when the degree of coupling has no frequency. , Fig. 3 is an explanatory diagram of the parallel coupling part, Fig. 4 is a diagram showing the relationship between the degree of coupling and the electrical length of the coupling, and Fig. 5 is the degree of coupling K when the electrical coupling length is chosen to be 90° at the center frequency 0 .
Figure 6 shows the frequency response of the filter in Figure 1 when the coupling length is 90°, and Figure 7 shows the frequency response of the filter in parallel coupling when the coupling length is 60°. Figure 8 is a diagram showing the frequency characteristics of the coupling degree, Figure 8 is a diagram showing the configuration of a high frequency bandpass waver according to an embodiment of the present invention, Figure 9 is a diagram showing the frequency response of the configuration shown in Figure 8, and Figure 10 is a diagram showing the frequency response of the configuration shown in Figure 8. A configuration diagram of another embodiment of the invention,
FIG. 11 is a diagram showing the response of a conventional interdigital filter, and FIG. 12 is a diagram showing the frequency response of the filter of the present invention. 81, 82...Input/output lines, 83-85...
λg/2 resonator, θ 01 to θ 34 ... Electrical length of coupling section, 1 01, 102 ... Input/output coupling circuit section, 103 to 1
06...λg/4 resonator, θc ...electrical length of parallel coupling part.

Claims (1)

【特許請求の範囲】 1 TEM線路共振器として両端開放型のλg/2共振 器を互いに平行結合させて平行結合部を形成して
なる高周波用帯域通過波器において、前記平行
結合部のうち結合電気長が90度および60度のもの
を少なくとも1個ずつ有する高周波用帯域通過
波器。 2 TEM線路共振器として一端開放・他端短絡
のλg/4共振器を互いに平行結合させて平行結合部 を形成してなる高周波用帯域通過波器におい
て、前記平行結合部のうち結合電気長が60度のも
のを少なくとも1個有する高周波用帯域通過波
器。
[Scope of Claims] 1. In a high-frequency bandpass waver formed by coupling λg/2 resonators with both ends open in parallel to each other as a TEM line resonator to form a parallel coupling part, the coupling part of the parallel coupling part A high-frequency bandpass transducer having at least one electrical length of 90 degrees and 60 degrees. 2. In a high-frequency bandpass resonator in which λg/4 resonators with one end open and the other end short-circuited are coupled in parallel to each other to form a parallel coupling part as a TEM line resonator, the coupling electrical length of the parallel coupling part is High-frequency bandpass waver with at least one 60-degree angle.
JP11390380A 1980-08-18 1980-08-18 Band-pass filter for high frequency Granted JPS5738001A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11390380A JPS5738001A (en) 1980-08-18 1980-08-18 Band-pass filter for high frequency

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11390380A JPS5738001A (en) 1980-08-18 1980-08-18 Band-pass filter for high frequency

Publications (2)

Publication Number Publication Date
JPS5738001A JPS5738001A (en) 1982-03-02
JPS6225283B2 true JPS6225283B2 (en) 1987-06-02

Family

ID=14624045

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11390380A Granted JPS5738001A (en) 1980-08-18 1980-08-18 Band-pass filter for high frequency

Country Status (1)

Country Link
JP (1) JPS5738001A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0649231U (en) * 1992-12-15 1994-07-05 トヨタ車体株式会社 Air spoiler mounting structure

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5187459A (en) * 1991-11-18 1993-02-16 Raytheon Company Compact coupled line filter circuit
US5442330A (en) * 1993-12-27 1995-08-15 Motorola, Inc. Coupled line filter with improved out-of-band rejection
CN102522617A (en) * 2011-12-28 2012-06-27 上海大学 Stepped impedance resonator (SIR) coaxial-cavity band-pass filter

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0649231U (en) * 1992-12-15 1994-07-05 トヨタ車体株式会社 Air spoiler mounting structure

Also Published As

Publication number Publication date
JPS5738001A (en) 1982-03-02

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