JPS6028441B2 - strip line filter - Google Patents
strip line filterInfo
- Publication number
- JPS6028441B2 JPS6028441B2 JP54122268A JP12226879A JPS6028441B2 JP S6028441 B2 JPS6028441 B2 JP S6028441B2 JP 54122268 A JP54122268 A JP 54122268A JP 12226879 A JP12226879 A JP 12226879A JP S6028441 B2 JPS6028441 B2 JP S6028441B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- dielectric substrate
- electrodes
- surface electrode
- full
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/20—Frequency-selective devices, e.g. filters
- H01P1/201—Filters for transverse electromagnetic waves
- H01P1/205—Comb or interdigital filters; Cascaded coaxial cavities
Description
【発明の詳細な説明】 この発明は、ストリップ線路フィル夕に関する。[Detailed description of the invention] The present invention relates to a strip line filter.
この発明の目的は、従来に比べさらに構造が簡単、取り
あつかいが容易、小形、低価格といった効果が得られる
、ストリップ線路フィル夕を提供することである。An object of the present invention is to provide a strip line filter which has advantages such as simpler structure, easier handling, smaller size, and lower cost than conventional filters.
この発明は、誘電体基板の一方主表面に、第1の全面電
極が設けられ、この全面電極と接続された第2の全面電
極が一つの側表面に設けられるとともに、この第2の全
面電極が、誘電体基板の他方主表面に延在させられる一
方、誘電体基板の他方主表面には、互いに結合し得る間
隔をおきかつ前記第2の全面電極の延在先端辺にそれぞ
れの各一端側が接続された複数の1/唯皮長共振電極が
配置され、そして外部引出用電極が初段および最終段共
振電極に接続されてなるストリップ線路フィルタである
。In the present invention, a first full surface electrode is provided on one main surface of a dielectric substrate, a second full surface electrode connected to this full surface electrode is provided on one side surface, and the second full surface electrode is provided on one side surface. are made to extend on the other main surface of the dielectric substrate, while on the other main surface of the dielectric substrate, one end of each is provided on the other main surface of the dielectric substrate at a distance such that they can be bonded to each other, and on the extending tip side of the second full surface electrode. This is a strip line filter in which a plurality of 1/skin length resonant electrodes whose sides are connected are arranged, and external extraction electrodes are connected to the first and final stage resonant electrodes.
この発明の上述の目的およびその他の目的と特徴は、図
面を参照しておこなう以下の実施例の詳細な説明からよ
り一層明らかとなろう。The above objects and other objects and features of the present invention will become more apparent from the following detailed description of embodiments with reference to the drawings.
図において、1は誘電体基板、2は誘電体基板1の一方
主表面、3は一方主表面2に設けられた全面電極、4は
誘電体基板1の一つの側表面、5は側表面4に設けられ
た全面電極で、全面電極3と一体的に接続されている。In the figure, 1 is a dielectric substrate, 2 is one main surface of the dielectric substrate 1, 3 is an entire surface electrode provided on one main surface 2, 4 is one side surface of the dielectric substrate 1, and 5 is a side surface 4 The entire surface electrode is provided on the surface and is integrally connected to the surface electrode 3.
6は誘電体基板1の他方主表面、7は他方主表面6の一
部へ延在させられた全面電極3の一部分、8は全面電極
3の一部分7の延在先端辺、9a〜9eは延在先端辺8
に一端側が接続された一端開放他端短絡の1/4波長の
共振電極で、各電極間距離によって通過帯城幅が決定さ
れる。10a〜10bは外部引出用電極で入力電極10
aは共振電極9aに接続され、出力電極10bは共振電
極9aに接続されている。6 is the other main surface of the dielectric substrate 1, 7 is a part of the entire surface electrode 3 extending to a part of the other main surface 6, 8 is the extended end side of the part 7 of the entire surface electrode 3, and 9a to 9e are Extended tip side 8
The passband width is determined by the distance between each electrode, with one end open and the other end short-circuited. 10a to 10b are external extraction electrodes, and input electrodes 10
a is connected to the resonant electrode 9a, and the output electrode 10b is connected to the resonant electrode 9a.
共振電極9aにおいて延在端辺8に接続される一端側と
入力電極10aとの間隔Aが大きくなると外部Q(Qe
)が4・さし、値にある。逆に間隔Aが小さくなると外
部Q(Qe)が大きい値になる。また、入力電極10a
の幅Bが狭くなると外部Q(Qe)が大きい値になる。
逆に幅Bが広くなると外部Q(Qe)が小さい値になる
。出力電極1obについても同様である。したがって必
要な外部Q(Qe)値になるよう間隔Aや幅Bを決定す
る。電極3,5,7,9a〜9e,10a,10bは、
Ag,Cu,Au等の電極材料からなるペイントを用い
て印刷手法によって形成されると好ましい。もちろん強
度を向上させるために、印刷後暁付処理してもよい。When the distance A between the input electrode 10a and one end of the resonance electrode 9a connected to the extended end 8 becomes large, the external Q (Qe
) is in the value of 4. Conversely, when the interval A becomes smaller, the external Q (Qe) becomes a larger value. In addition, the input electrode 10a
As the width B becomes narrower, the external Q (Qe) becomes a larger value.
Conversely, as the width B increases, the external Q (Qe) becomes a smaller value. The same applies to the output electrode 1ob. Therefore, the interval A and width B are determined so as to obtain the required external Q (Qe) value. The electrodes 3, 5, 7, 9a to 9e, 10a, 10b are
It is preferable that the electrode is formed by a printing method using paint made of an electrode material such as Ag, Cu, or Au. Of course, in order to improve the strength, it may be subjected to a dazzling treatment after printing.
全面電極3は必ずしも他方主表面6の一部へ延在させる
必要はない。The entire surface electrode 3 does not necessarily need to extend to a part of the other main surface 6.
たとえば、全面電極3を側表面4だけに設け、誘電体基
板1の一辺11に共振電極9a〜9eの一端側が位置す
るようにしてもよいが、生産面からみると、印刷ずれに
よって、たとえば共振電極9a〜9eの長さCや間隔A
などが所定値と異なってしまうことがあるかもしれない
ので、全面電極3を他方主表面6の一部分まで延在させ
た方が実際的である。いいかえると、全面電極3の一部
分7、共振電極9a〜9e、外部引出用電極10a,1
0bを一体的に形成した印刷パターンを用いれば誘電体
基板1への印刷ずれが多少あっても特性に重要な影響を
およぼす前記各寸法に狂いが生じることはない。概略は
以上のとおりであり、次に設計手順について説明する。
まず外部Q(球)を求める。For example, the entire surface electrode 3 may be provided only on the side surface 4, and one end side of the resonance electrodes 9a to 9e may be located on one side 11 of the dielectric substrate 1. However, from a production standpoint, printing misalignment may cause the resonance Length C and interval A of electrodes 9a to 9e
etc. may differ from predetermined values, so it is more practical to extend the entire surface electrode 3 to a part of the other main surface 6. In other words, the part 7 of the entire surface electrode 3, the resonance electrodes 9a to 9e, and the external extraction electrodes 10a, 1
If a printed pattern in which 0b is integrally formed is used, even if there is some misalignment of printing on the dielectric substrate 1, the above-mentioned dimensions, which have an important influence on the characteristics, will not be distorted. The outline is as above, and the design procedure will be explained next.
First, find the external Q (sphere).
Qe=g塾畢生
イニf
ただし△fは帯城幅、&、&はいわゆるgバリュー、W
ま中心周波数である。Qe=gjukukuiyuinii f However, △f is the obijo width, &, & is the so-called g value, W
It is the center frequency.
外部Q(Qe)と間隔Aとの関係は第3図に示すような
傾向をもっている。The relationship between external Q (Qe) and interval A has a tendency as shown in FIG.
したがって第3図により間隔Aを定める。なお幅Bは後
述するようなあらかじめ定められた一定値にしておく。
一方、j段目(実施例ではi=1,2,3,4)の共振
器とj+1段目の共振器との結合係数Kj・i+1を求
める。く」f
Ki.i+1=f。Therefore, the distance A is determined according to FIG. Note that the width B is set to a predetermined constant value as described later.
On the other hand, the coupling coefficient Kj·i+1 between the resonator of the jth stage (i=1, 2, 3, 4 in the embodiment) and the resonator of the j+1st stage is determined. Ki. i+1=f.
ノg.g十1結合係数Ki・i+1と共振器間距離Dx
(実施例ではx=1,2,3,4)との関係は第4図に
示すような頃向をもつている。Nog. g11 coupling coefficient Ki・i+1 and inter-resonator distance Dx
(in the example, x=1, 2, 3, 4) has a direction as shown in FIG.
したがって第4図により間隔■xを定める。共振電極9
a〜9eの長さC,〜C5は、もし他の共振器や入出力
織部の影響を無視すると、300
CI=C2=C3=C4:C5=f。Therefore, the interval x is determined according to FIG. Resonant electrode 9
The lengths C and ~C5 of a~9e are 300 CI=C2=C3=C4:C5=f if we ignore the effects of other resonators and input/output fabrics.
・4ノごreffとなる。ただしご蛇ff‘ま実効ごで
ある。しかし実際には、他の共振器や入出力機部の影響
を受けるので以下のようにして共振電極9a〜9eの長
さC,〜C5を定める。300
C.=C5=(ら十△f。・There will be 4 refs. However, it is not effective. However, in reality, the lengths C and C5 of the resonance electrodes 9a to 9e are determined as follows because they are influenced by other resonators and input/output devices. 300 C. =C5=(ra1△f.
)‐4ノごreff300Cx=(ち十△fX).4ノ
どreff(実施例ではx=2,3,4)入出力端部に
よる周波数変化度合△foと間隔Aとの関係は第5図に
示すような傾向にある。)-4 ref300Cx=(chi1△fX). The relationship between the degree of frequency change Δfo due to the input/output terminals and the interval A tends to be as shown in FIG. 5.
なお、他の共振器の影響もあるが、入出力端部による影
響に比べ実用上無視できる程度のものるある。また、他
の共振器の影響による周波数変化度合△ふと共振器間距
離の平均値DX−季+DXとの関係は、第6図に示すよ
うな額向にある。これらの傾向を参考にして共振電極9
a〜9eの長さC,〜C5を定める。なお共振電極9a
〜9eの幅E、全面電極3の一部分7の幅F、外部引出
用電極10a,1obの長さG,H等は、あらかじめ定
めた一定値にしておく。たとえば中心周波数100のM
HZのものでは、B=0.5側、E=1.6脚、F=1
.仇舷、G=H=4肌である。また、基板の寸法は29
肋×IQ凧×1.5帆、ご=100程度のものを用いた
。第7図と第8図にこのようにして製造したフィル夕の
一特性例を示す。中心周波数foは100■MHZ、0
.&旧帯域幅は18加MHz、反射損失は2の旧、挿入
損失は中心周波数りこて0.7dB、温度特性は、2脚
/℃程度である。以上の実施例からもあきらかなように
、この発明によれば、構造が簡単、取りあつかいが容易
、小形で低価格なストリップ線路フィル夕が提供できる
。Although there are effects from other resonators, they are practically negligible compared to the effects from the input and output terminals. Further, the relationship between the degree of frequency change △ due to the influence of other resonators and the average value of the inter-resonator distance DX-X+DX is as shown in FIG. Based on these trends, the resonant electrode 9
Determine the lengths C and C5 of a to 9e. Note that the resonant electrode 9a
The width E of ~9e, the width F of the part 7 of the entire surface electrode 3, the lengths G and H of the external extraction electrodes 10a and 1ob, etc. are set to predetermined constant values. For example, M with a center frequency of 100
For HZ, B = 0.5 side, E = 1.6 legs, F = 1
.. On the side, G = H = 4 skins. Also, the dimensions of the board are 29
A kite with ribs x IQ x 1.5 sails, approximately 100 pieces, was used. FIGS. 7 and 8 show an example of the characteristics of the filter produced in this manner. The center frequency fo is 100■MHZ, 0
.. & The original bandwidth is 18 MHz, the return loss is 2, the insertion loss is 0.7 dB at the center frequency, and the temperature characteristics are about 2 legs/°C. As is clear from the above embodiments, according to the present invention, it is possible to provide a strip line filter that is simple in structure, easy to handle, small in size, and inexpensive.
第1図は、この発明は一実施例平面図、第2図は、同、
右側面図、第3図は間隔Aと外部Q(扱)との関係を示
す図、第4図は共振器間距離Dxと結合係数Kj・i十
1との関係を示す図、第5図は間隔Aと入出力端部によ
る周波数変化度合△らとの関係を示す図、第6図は共振
器間距離の平均値DX−享十DXと他の共振器の影響に
よる周波数変化度合△&との関係を示す図、第7図は選
択度特性曲線図、第8図は通過帯域特性と反射損失を示
す図である。
1は誘電体基板、3,5は全面電極、9a〜9eは共振
電極、10a,10bは外部引出用電極。
第1図
第2図
第3図
第4図
第5図
第6図
第7図
第8図FIG. 1 is a plan view of one embodiment of the present invention, and FIG. 2 is a plan view of one embodiment of the invention.
The right side view, Fig. 3 is a diagram showing the relationship between the interval A and external Q (handling), Fig. 4 is a diagram showing the relationship between the inter-resonator distance Dx and the coupling coefficient Kj·i11, and Fig. 5 6 is a diagram showing the relationship between the interval A and the degree of frequency change △ etc. due to the input and output ends, and FIG. 7 is a selectivity characteristic curve diagram, and FIG. 8 is a diagram illustrating passband characteristics and reflection loss. 1 is a dielectric substrate, 3 and 5 are full-surface electrodes, 9a to 9e are resonance electrodes, and 10a and 10b are external extraction electrodes. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8
Claims (1)
られ、この全面電極と接続された第2の全面電極が一つ
の側表面に設けられるとともに、この第2の全面電極が
、誘電体基板の他方主表面に延在させられる一方、誘電
体基板の他方主表面には、互いに結合し得る間隔をおき
かつ前記第2の全面電極の延在先端辺にそれぞれの各一
端側が接続された複数の1/4波長共振電極が配置され
、そして外部引出用電極が初段および最終段共振電極に
接続されてなるストリツプ線路フイルタ。1 A first full surface electrode is provided on one main surface of the dielectric substrate, a second full surface electrode connected to this full surface electrode is provided on one side surface, and this second full surface electrode is connected to the dielectric substrate. The electrodes are connected to the other main surface of the dielectric substrate at intervals such that they can be bonded to each other, and are connected at one end to the extending tip side of the second full-surface electrode. A stripline filter in which a plurality of 1/4 wavelength resonant electrodes are arranged, and an external lead-out electrode is connected to the first and final stage resonant electrodes.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP54122268A JPS6028441B2 (en) | 1979-09-22 | 1979-09-22 | strip line filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP54122268A JPS6028441B2 (en) | 1979-09-22 | 1979-09-22 | strip line filter |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5646302A JPS5646302A (en) | 1981-04-27 |
JPS6028441B2 true JPS6028441B2 (en) | 1985-07-04 |
Family
ID=14831747
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP54122268A Expired JPS6028441B2 (en) | 1979-09-22 | 1979-09-22 | strip line filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6028441B2 (en) |
Families Citing this family (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58207701A (en) * | 1982-05-28 | 1983-12-03 | Murata Mfg Co Ltd | Broad band filter |
JPS6025202U (en) * | 1983-07-27 | 1985-02-20 | 株式会社村田製作所 | striped line filter |
JPS60153003U (en) * | 1984-03-19 | 1985-10-12 | 日本電気株式会社 | membrane circuit board |
JPS6224701A (en) * | 1985-07-25 | 1987-02-02 | Nec Corp | Drop-in isolator |
JPS62164301A (en) * | 1986-01-14 | 1987-07-21 | Murata Mfg Co Ltd | Strip line filter |
JPS63127601A (en) * | 1986-11-18 | 1988-05-31 | Murata Mfg Co Ltd | Strip line filter |
JP2667604B2 (en) * | 1991-11-14 | 1997-10-27 | 三菱電機株式会社 | Stripline filter |
-
1979
- 1979-09-22 JP JP54122268A patent/JPS6028441B2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS5646302A (en) | 1981-04-27 |
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