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JPH02140007A - Low pass filter - Google Patents

Low pass filter

Info

Publication number
JPH02140007A
JPH02140007A JP29339888A JP29339888A JPH02140007A JP H02140007 A JPH02140007 A JP H02140007A JP 29339888 A JP29339888 A JP 29339888A JP 29339888 A JP29339888 A JP 29339888A JP H02140007 A JPH02140007 A JP H02140007A
Authority
JP
Japan
Prior art keywords
circuit
stage
coil
final stage
frequency
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
JP29339888A
Other languages
Japanese (ja)
Inventor
Naotake Okamura
尚武 岡村
Teruhisa Tsuru
輝久 鶴
Tetsuo Taniguchi
哲夫 谷口
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing 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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP29339888A priority Critical patent/JPH02140007A/en
Publication of JPH02140007A publication Critical patent/JPH02140007A/en
Pending legal-status Critical Current

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  • Filters And Equalizers (AREA)

Abstract

PURPOSE:To reduce the loss at the cut-off frequency by increasing the anti- resonance point of a circuit including a parallel resonance circuit of the final stage higher than that of the one stage preceding. CONSTITUTION:An inductance of a coil L4' of a parallel resonance circuit A2, of the final stage among inductances of coils L1'-L4' calculated in a way that the inductance is smaller from the 1st stage toward the final stage, and the inductance of the coil L3' of the parallel resonance circuit A3, of one preceding stage is decreased from its calculated value while it is larger than the induct ance of the coil L4'. Thus, the anti-resonance point P4' of the circuit B4' of the final stage is moved toward a high frequency and the antiresonance point P3' of the circuit B2' of one preceding stage is moved toward a low frequency conversely, and the frequency characteristic of each stage is not steep, but even so the entire frequency characteristic of the filter obtained through the synthesis has a steep leading.

Description

【発明の詳細な説明】 主星上皇■里分顆 本発明は、回路中に直列接続された複数の並列共振回路
を含むローパスフィルタに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a low-pass filter including a plurality of parallel resonant circuits connected in series in a circuit.

従j四υL祈 上記のローパスフィルタとして、従来、誘電体基板上に
プリントコイル(L)とコンデンサ(C)を形成して、
第5図に示すような等価回路(4段の並列共振回路へ3
.八2143. A4を含む)となした構成のものがあ
る。この構成の設計は、一般に連立チェビシェフ(Tc
hbyceff )の設計公式を用いて行われており、
誘電体基板を使用してLC回路を形成する場合には、設
計上、1段目(左端)の破線にて示す回路B、中に含ま
れる並列共振回路AIのコイルL、の素子値よりも、そ
れ以降の各段の回路B2゜Bs、 B4中に夫々含まれ
る並列共振回路AX、 Ih。
Conventionally, as the above low-pass filter, a printed coil (L) and a capacitor (C) are formed on a dielectric substrate.
An equivalent circuit as shown in Figure 5 (3 to 4 stages of parallel resonant circuit)
.. 82143. (including A4 size). The design of this configuration is generally a combination of Chebyshev (Tc
This is done using the design formula of hbyceff).
When forming an LC circuit using a dielectric substrate, the element value of the circuit B shown by the broken line in the first stage (left end) and the coil L of the parallel resonant circuit AI included therein should be , parallel resonant circuits AX and Ih included in circuits B2°Bs and B4 of each subsequent stage, respectively.

A4の各コイルLx、 Lz、 L4の素子値が順次小
さ(なるようにする必要がある。
It is necessary to make the element values of each coil Lx, Lz, and L4 of A4 successively smaller.

第6図は、上述のようにして設計したフィルタにおける
最終段の回路B4の周波数特性SAs と、それよりも
1段前の回路B、の周波数特性SA3と、両回路B3お
よびB4の周波数特性SAについてシュミレーションし
て得た結果を示す図である。この図より理解されるよう
に、設計したフィルタは、最終段の回路B、における周
波数特性SA4の反共振点(ボール)B4が、それより
も1段前の回路B3における周波数特性SA、の反共振
点P3よりも低周波側に位置させであると共に、各段の
回路Bl+ B2. B3゜B4のうちで最も低周波側
に位置させである。
Figure 6 shows the frequency characteristics SAs of the final stage circuit B4 in the filter designed as described above, the frequency characteristics SA3 of the circuit B one stage before it, and the frequency characteristics SAs of both circuits B3 and B4. FIG. 2 is a diagram showing the results obtained by simulation. As can be understood from this figure, in the designed filter, the antiresonance point (ball) B4 of the frequency characteristic SA4 in the final stage circuit B is the antiresonance point (ball) B4 of the frequency characteristic SA in the circuit B3, one stage before it. The circuit Bl+B2. is located on the lower frequency side than the resonance point P3. It is located on the lowest frequency side among B3° and B4.

この構成において所望のフィルタ特性を得るためには、
図中D4で示すように最終段の回路B4の波形の立ち上
がりが、その前段の回路B3のそれB3と比べて相当急
峻となることが必要となる。
In order to obtain the desired filter characteristics in this configuration,
As shown by D4 in the figure, it is necessary that the rise of the waveform of the circuit B4 at the final stage is considerably steeper than that of the circuit B3 at the preceding stage.

が”しよ゛と る ところで、誘電体基板を使用した場合、プリントコイル
のQが小さいために、最終段の回路B4の周波数特性S
A4が設計上要請される程急峻に立ち上がらず、カット
オフ周波数域でなだらかとなってしまう。このため、全
段の周波数特性を重畳して得られる総合の周波数特性の
カットオフ周波数域での損失が大きくなるという問題点
があった。
When the dielectric substrate is used, the Q of the printed coil is small, so the frequency characteristic S of the final stage circuit B4 is
A4 does not rise as steeply as required by design, but becomes gradual in the cutoff frequency range. Therefore, there is a problem in that the loss in the cutoff frequency range of the overall frequency characteristic obtained by superimposing the frequency characteristics of all stages becomes large.

本発明はこの問題点を解決するものであり、総合の周波
数特性を設計iJ1りにで・き1、カットオフ周波数域
での損失を小さくできる構成としたローパスフィルタを
桿供することを目的とする。
The present invention is intended to solve this problem, and aims to provide a low-pass filter having a structure in which the overall frequency characteristics can be designed according to the design standard, and the loss in the cutoff frequency region can be reduced. .

課刃奇解次工邊−友−ぬΦ−毛殺 本発明は、誘電体基板のトー下面に導電膜が所定パター
ンで形成されてなる回路を備え、この回路中に直列接続
された複数の並列共振回路を含むローパスフィルタにお
いて、連立チェビシェフの設計公式に基づき並列共振回
路の1段側から最終段側へ順次小さくなる状態に算出さ
れたコイルの素子値のうち、最終段の並列共振回路にお
けるフィルの素子値を算出値よりも大きくし、それより
も1段前の並列共振回路におけるコイルの素子値を、太
きく i、=、た最終段のコイルの素子値よりも大きい
状態で算出値よりも小さくしたことを特徴とする。
The present invention includes a circuit in which a conductive film is formed in a predetermined pattern on the lower surface of a dielectric substrate, and a plurality of circuits connected in series in the circuit. In a low-pass filter that includes a parallel resonant circuit, among the coil element values calculated in a state that decreases sequentially from the first stage side to the final stage side of the parallel resonant circuit based on the simultaneous Chebyshev design formula, the value in the final stage parallel resonant circuit is The element value of the fill is made larger than the calculated value, and the element value of the coil in the parallel resonant circuit one stage before it is made larger than the element value of the final stage coil. It is characterized by being smaller than.

イつ亘−U 発明明番こあっては、直列接続された複数の並列ハ振回
路のうち最終段の並列共振回路のコイルの素子値を算出
値よりも大きくし、それよりも1段前の並列共振回路の
コイル値を算出値よりも小さ(するので、最終段の並列
共振回路を含む回路の反共振点が高周波側へずれ4、一
方、1段前の並列共振回路を含む回路の反共振点が低周
波側へずれろ。従って、第3図に示すように、最終段に
おける周波数特性SA4’の反共振点p%が1段前にお
ける周波数特性SA、  ’の反共振点Pff′よりも
高周波側に位置するように算出値を変更させると、設計
通りの各段重前の周波数特性SAが得られ、この結果力
・yトオフ周波数域での損失が小さくなる。
In this case, the element value of the coil of the last stage parallel resonant circuit of multiple parallel resonant circuits connected in series is made larger than the calculated value, and the element value of the coil of the last stage parallel resonant circuit is made larger than the calculated value, and Since the coil value of the parallel resonant circuit of The anti-resonance point should shift to the lower frequency side. Therefore, as shown in Fig. 3, the anti-resonance point p% of the frequency characteristic SA4' in the final stage is smaller than the anti-resonance point Pff' of the frequency characteristic SA, ' in the previous stage. If the calculated value is changed so that the frequency is also located on the high frequency side, the frequency characteristic SA before each stage loading as designed can be obtained, and as a result, the loss in the force/y-to-off frequency range is reduced.

実、Jt、−狽1 第1図は、本発明に係るローパスフィルタを示す回路図
であり、第2図はこのローパスフィルタの等価回路図で
ある。上記ローパスフィルタは、誘電体基+Fj、10
の上・下面]、Oa、10bに夫々所定のパターンで導
電膜11 (実線)、12(破線)を形成してあり、両
膜11.12が対向しない部分からなるプリントコイル
L、’、 L2’、 t、il、4′と、対向する部分
からなるコンデンサ02C4’、 C4’、 C5’、
 C6’、 C?’、 Ca’、 C9’およびプリン
トコイル14.′の浮遊容量からなるコンデンサC,l
を有する。図中Sは、上側の導電膜11と下側の導電膜
12とを共振器10を貫通して接続するだめの電極であ
る。この回路は、第2図に示すようt、″′複数、例え
ば4つの並列共振回路AA2’、 A3’ 、 A4’
を直列接続すると共に、各並列共振回路A、’、 A2
’+ Aよt、(、、rの両側GこコンデンサC5’、
 Cb’、 C7’、 Ca’、 C=r’が設げられ
た、はt7こ1りをしでおり、各素子の表示は第1図と
対応させて示している。
Actually, Jt, -狽1 Fig. 1 is a circuit diagram showing a low-pass filter according to the present invention, and Fig. 2 is an equivalent circuit diagram of this low-pass filter. The above low-pass filter has a dielectric base +Fj, 10
Conductive films 11 (solid line) and 12 (dashed line) are formed in a predetermined pattern on the upper and lower surfaces], Oa and 10b, respectively, and the printed coils L, ', L2 are made up of portions where both films 11 and 12 do not face each other. ', t, il, 4' and capacitors 02C4', C4', C5', consisting of opposing parts
C6', C? ', Ca', C9' and printed coil 14. A capacitor C, l consisting of a stray capacitance of
has. In the figure, S denotes an electrode that connects the upper conductive film 11 and the lower conductive film 12 through the resonator 10. This circuit consists of a plurality of parallel resonant circuits, for example, four parallel resonant circuits AA2', A3', A4', as shown in FIG.
are connected in series, and each parallel resonant circuit A, ', A2
'+ A, (,, G capacitor C5' on both sides of r,
Cb', C7', Ca', and C=r' are provided for t7, and the display of each element is shown in correspondence with FIG.

かかる回路は、上記連立チエビシェフの設計公式におい
て反共振点の入れ換えを行っている。具体的には、1段
側から最終段へ順次小さくなる状態に公式Gこ基づき算
出された各コイル1.l’、L2L、 l 、 L、 
lの素子値のうち、最終段の並列共振回路A4’のコイ
ル1.4′の素子値を算出値よりも大きくし、それより
も1段前の並列共振回路Aff’のコイルし3′の素子
値を、大きくしたコイルL4′の素子値よりも大きい状
態で算出値よりも小さく設計している。例を示せば、第
5図に示す従来の場合には、各段のコイルL、、 L2
. L、、 I7.の素子値が夫々27.9.2669
.21.3.11.、OnHとなるようにしていたが、
この例ではコイルL+ ’ 、 Lz ’ 、 Lt 
’ 、 Laの素子値を夫々27.9.26.9、■7
.8.14.5nHとなるようにし、最終の2段のコイ
ルLl ’ + L4’  についての素子値を較差が
小さ(なるようにしている。
In this circuit, the anti-resonance points are exchanged in the above-mentioned simultaneous Chiebishev design formula. Specifically, each coil 1. is calculated based on the formula G in a state in which the size becomes smaller from the first stage side to the final stage side. l', L2L, l, L,
Among the element values of l, the element value of coil 1.4' of the final stage parallel resonant circuit A4' is made larger than the calculated value, and the element value of coil 3' of the parallel resonant circuit Aff' one stage before it is made larger than the calculated value. The element value is designed to be smaller than the calculated value while being larger than the element value of the enlarged coil L4'. For example, in the conventional case shown in FIG. 5, each stage of coils L, L2
.. L,, I7. The element value of each is 27.9.2669
.. 21.3.11. , I tried to make it OnH, but
In this example, the coils L+', Lz', Lt
', the element values of La are 27.9, 26.9 and ■7, respectively.
.. 8.14.5 nH, and the element values for the final two stages of coils Ll' + L4' are set so that the difference is small.

なお、コンデンサの容量については、従来では各コンデ
ンサC+、 Cm、 C3,C4,Cs、 Cb、 C
qlCe、 C9を夫々0.39.1.2.2゜3.5
.1.3.3.6.0.5゜2.4.3.0.9 pF
としてあり、この実施例では各コンデンサC+  、C
2、C3、Ca  、Cs  、CbC7’ = CB
 ’ + C9′を夫々0.39.1.2.3.1.3
.3.3.3.6.0.4.8.4.1.1.5 pF
としている。
Regarding the capacitance of the capacitors, conventionally each capacitor C+, Cm, C3, C4, Cs, Cb, C
qlCe, C9 respectively 0.39.1.2.2゜3.5
.. 1.3.3.6.0.5゜2.4.3.0.9 pF
In this example, each capacitor C+, C
2, C3, Ca, Cs, CbC7' = CB
' + C9' respectively 0.39.1.2.3.1.3
.. 3.3.3.6.0.4.8.4.1.1.5 pF
It is said that

作用の欄で説明した第3図は、このように設計した場合
の最終段の回路B、lの周波数特性SA。
FIG. 3, which was explained in the operation section, shows the frequency characteristics SA of the final stage circuits B and I when designed in this way.

と、これより1段前の回路B、lの周波数特性SA3と
、両段重畳の周波数特性SAについてシュミレーション
して得た結果を示す図であるが、最終段の回路B、lの
反共振点p、lが高周波側へ移動し、逆に1段前の回路
B、/の反共振点p、/が低周波側へ移動して、Pa′
>Px’となり、誘電体基板の使用により各周波数特性
SA4’とSA3  ’におけるカントオフ周波数近傍
の周波数特性が緩やかになっていても、合成の周波数特
性SAを設計通りに一致させることができた。
This is a diagram showing the results obtained by simulating the frequency characteristics SA3 of the circuits B and l in the previous stage, and the frequency characteristics SA of the superposition of both stages. p, l move to the high frequency side, and conversely, the anti-resonance point p, / of circuit B, /, one stage before, moves to the low frequency side, and Pa'
>Px', and even though the frequency characteristics near the cant-off frequency in each of the frequency characteristics SA4' and SA3' became gentle due to the use of the dielectric substrate, the synthesized frequency characteristics SA could be matched as designed.

このため、本発明に係るフィルタの出力特性Eは、第4
図に示すように従来のローパスフィルタの出力特性Fと
対比して、カットオフ周波数域での損失を小さくするこ
とができる。
Therefore, the output characteristic E of the filter according to the present invention is the fourth
As shown in the figure, the loss in the cutoff frequency region can be reduced compared to the output characteristic F of the conventional low-pass filter.

発皿皇羞来 以上詳述した如く本発明による場合には、最終段の並列
共振回路を含む回路の反共振点を1段前のそれよりも高
くすることで、誘電体基板の使用により各段の周波数域
が緩やかとなっても、合成して得られるフィルタ全体の
周波数特性を急峻な立上がりをもったものとすることが
でき、カットオフ周波数域での損失の少ない良好なロー
パスフィルタが得られる。
As detailed above, in the case of the present invention, by making the anti-resonance point of the circuit including the final stage parallel resonant circuit higher than that of the previous stage, each Even if the frequency range of the stages becomes gentle, the frequency characteristics of the entire filter obtained by synthesis can be made to have a steep rise, and a good low-pass filter with low loss in the cutoff frequency range can be obtained. It will be done.

【図面の簡単な説明】 第1図は本発明を適用したローパスフィルタの回路図、
第2図はこの回路の等価回路図、第3図は最終段の回路
B4の周波数特性SA、と、これより1段前の回路B3
の周波数特性SA3とを主として示すグラフ、第4図は
本発明のフィルタの出力特性を従来の出力特性と対比し
て示すグラフ、第5図は従来のローパスフィルタの構成
を示す等価回路図、第6図はその回路の設計上の周波数
特性を示すグラフである。 10・・・誘電体基板、11.12・・・導電膜、し。 Lx ’ 、 L3 ’ 、 L4  ・・・コイル、
C+、Cz、C+C4’、 C5’、 Cb’、 C?
’、 CB  、 C9・・・コンデンサ。 第5図 特許出願人 株式会社村田製作所
[Brief Description of the Drawings] Figure 1 is a circuit diagram of a low-pass filter to which the present invention is applied;
Figure 2 is an equivalent circuit diagram of this circuit, and Figure 3 is the frequency characteristics SA of the final stage circuit B4 and the circuit B3 one stage before this.
4 is a graph showing the output characteristics of the filter of the present invention in comparison with the conventional output characteristics. FIG. 5 is an equivalent circuit diagram showing the configuration of the conventional low-pass filter. FIG. 6 is a graph showing the designed frequency characteristics of the circuit. 10... Dielectric substrate, 11.12... Conductive film. Lx', L3', L4...Coil,
C+, Cz, C+C4', C5', Cb', C?
', CB, C9... Capacitor. Figure 5 Patent applicant Murata Manufacturing Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] (1)誘電体基板の上下面に導電膜が所定パターンで形
成されてなる回路を備え、この回路中に直列接続された
複数の並列共振回路を含むローパスフィルタにおいて、 連立チェビシェフの設計公式に基づき並列共振回路の1
段側から最終段側へ順次小さくなる状態に算出されたコ
イルの素子値のうち、最終段の並列共振回路におけるコ
イルの素子値を算出値よりも大きくし、それよりも1段
前の並列共振回路におけるコイルの素子値を、大きくし
た最終段のコイルの素子値よりも大きい状態で算出値よ
りも小さくしたことを特徴とするローパスフィルタ。
(1) A low-pass filter that includes a circuit in which conductive films are formed in a predetermined pattern on the upper and lower surfaces of a dielectric substrate, and that includes multiple parallel resonant circuits connected in series, based on the simultaneous Chebyshev design formula. Parallel resonant circuit 1
Among the element values of the coil calculated in a state that decreases sequentially from the stage side to the final stage side, the element value of the coil in the final stage parallel resonant circuit is made larger than the calculated value, and the parallel resonance of the stage one stage before it is made larger than the calculated value. A low-pass filter characterized in that the element value of a coil in a circuit is made smaller than a calculated value while being larger than the element value of a final stage coil.
JP29339888A 1988-11-18 1988-11-18 Low pass filter Pending JPH02140007A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29339888A JPH02140007A (en) 1988-11-18 1988-11-18 Low pass filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29339888A JPH02140007A (en) 1988-11-18 1988-11-18 Low pass filter

Publications (1)

Publication Number Publication Date
JPH02140007A true JPH02140007A (en) 1990-05-29

Family

ID=17794250

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29339888A Pending JPH02140007A (en) 1988-11-18 1988-11-18 Low pass filter

Country Status (1)

Country Link
JP (1) JPH02140007A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05327400A (en) * 1992-05-25 1993-12-10 Murata Mfg Co Ltd Passing band variable circuit
JPH1051257A (en) * 1996-08-06 1998-02-20 Ngk Spark Plug Co Ltd Lc low-pass filter
US7319850B2 (en) 2001-11-01 2008-01-15 Sharp Kabushiki Kaisha Low noise block downconverter converting received signal to intermediate frequency signal

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05327400A (en) * 1992-05-25 1993-12-10 Murata Mfg Co Ltd Passing band variable circuit
JPH1051257A (en) * 1996-08-06 1998-02-20 Ngk Spark Plug Co Ltd Lc low-pass filter
US7319850B2 (en) 2001-11-01 2008-01-15 Sharp Kabushiki Kaisha Low noise block downconverter converting received signal to intermediate frequency signal

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