JPH03187626A - Transmission line length determination method for common use device - Google Patents
Transmission line length determination method for common use deviceInfo
- Publication number
- JPH03187626A JPH03187626A JP1327591A JP32759189A JPH03187626A JP H03187626 A JPH03187626 A JP H03187626A JP 1327591 A JP1327591 A JP 1327591A JP 32759189 A JP32759189 A JP 32759189A JP H03187626 A JPH03187626 A JP H03187626A
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- Prior art keywords
- transmission
- filter
- transmission line
- transmission path
- impedance
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- 230000005540 biological transmission Effects 0.000 title claims abstract description 127
- 238000000034 method Methods 0.000 title claims description 46
- 238000003780 insertion Methods 0.000 claims abstract description 49
- 230000037431 insertion Effects 0.000 claims abstract description 49
- 238000004364 calculation method Methods 0.000 claims abstract description 11
- 230000006698 induction Effects 0.000 claims description 7
- 238000001914 filtration Methods 0.000 claims description 4
- 238000005259 measurement Methods 0.000 claims description 4
- 239000000758 substrate Substances 0.000 claims description 3
- 239000000126 substance Substances 0.000 claims 1
- 239000011159 matrix material Substances 0.000 abstract 2
- 230000003252 repetitive effect Effects 0.000 abstract 1
- 238000013461 design Methods 0.000 description 30
- 238000010586 diagram Methods 0.000 description 18
- 238000007796 conventional method Methods 0.000 description 5
- 238000010897 surface acoustic wave method Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 4
- 239000004593 Epoxy Substances 0.000 description 1
- 206010040844 Skin exfoliation Diseases 0.000 description 1
- 230000032683 aging Effects 0.000 description 1
- 238000003491 array Methods 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 230000009977 dual effect Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000006870 function Effects 0.000 description 1
- 230000008571 general function Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 238000002847 impedance measurement Methods 0.000 description 1
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Abstract
Description
【発明の詳細な説明】
(産業上の利用分野〉
本発明は、VHF帯からUHF帯等にかけての周波数を
利用した自動車電話装置等において、送信信号と受信信
号を同一のアンテナ等で送受信するだめの共用器、特に
小型で良好な周波数特性を得るための共用器の伝送路長
決定方法に関するものである。Detailed Description of the Invention (Industrial Field of Application) The present invention provides a method for transmitting and receiving transmission signals and reception signals using the same antenna, etc. in a car telephone device, etc. that uses frequencies from the VHF band to the UHF band, etc. The present invention relates to a duplexer, and particularly to a method for determining the transmission path length of a duplexer to obtain good frequency characteristics with a small size.
(従来の技術)
一般に、共用器は、分波回路、送信フィルタ及び受信フ
ィルタで構成され、送信信号と受信信号を共通の端子で
送受信する機能を有している。(Prior Art) Generally, a duplexer is composed of a branching circuit, a transmission filter, and a reception filter, and has a function of transmitting and receiving a transmission signal and a reception signal through a common terminal.
従来、高性能な共用器を得るために、例えばフィルタの
損失の改善、及び分波回路の抵抗損や分波器の低減等、
種々の提案がなされている。特に、通信装置の小型化に
伴い、小型で高性能な共用器の実現が必要不可欠なもの
となっている。従来の一般的な共用器の一例を第2図に
示す。Conventionally, in order to obtain a high-performance duplexer, it has been necessary to improve filter loss, reduce resistance loss in the duplexer circuit, and reduce the duplexer.
Various proposals have been made. In particular, with the miniaturization of communication devices, it has become essential to realize a compact and high-performance duplexer. An example of a conventional common duplexer is shown in FIG.
第2図は、従来の一般的な共用器の構成図である。FIG. 2 is a block diagram of a conventional common duplexer.
この共用器は、ガラスエポキシ等を用いて製作された基
板1を有し、その基板1上には、共通端子2、入力端子
3及び出力端子4が設けられている。共通端子2には、
分波回路パターン5の一端が接続され、その分波回路パ
ターン5の他端が、送信フィルタ6及び受信フィルタ7
を介して入力端子3及び出力端子4にそれぞれ接続され
ている。This shared device has a substrate 1 made of glass epoxy or the like, and a common terminal 2, an input terminal 3, and an output terminal 4 are provided on the substrate 1. Common terminal 2 has
One end of the branching circuit pattern 5 is connected, and the other end of the branching circuit pattern 5 is connected to the transmission filter 6 and the reception filter 7.
are connected to the input terminal 3 and the output terminal 4 via the respective terminals.
分波回路パターン5は、伝送路長Ltの送信側伝送路5
aと、伝送路長Lrの受信側伝送路5bとで構成されて
いる。The branching circuit pattern 5 is a transmitting side transmission line 5 with a transmission line length Lt.
a, and a receiving side transmission line 5b having a transmission line length Lr.
送信フィルタ6及び受信フィルタ7から共通端子2まで
の送信側及び受信側の伝送路長Lt、Lrは、インピー
ダンス変換効果によって、共通端子2からみたそれぞれ
の送信フィルタ6及び受信フィルタ7のインピーダンス
が相手方の中心周波数において最大になるように設計さ
れている。すなわち、送信周波数Ftにおいて共通端子
2からみた送信フィルタ6のインピーダンスは、この種
の回路で規定された特性インピーダンスZ○にほぼ等し
いが、受信フィルタ7のインピーダンスは最大になる。The transmission path lengths Lt and Lr on the transmitting side and receiving side from the transmitting filter 6 and receiving filter 7 to the common terminal 2 are such that the impedance of each transmitting filter 6 and receiving filter 7 as seen from the common terminal 2 is the same as that of the other side due to the impedance conversion effect. It is designed to have a maximum at the center frequency of . That is, at the transmission frequency Ft, the impedance of the transmission filter 6 viewed from the common terminal 2 is approximately equal to the characteristic impedance Z○ defined for this type of circuit, but the impedance of the reception filter 7 is maximum.
そして、受信周波数Frにおいて受信フィルタ7のイン
ピーダンスは、例えば出力端子4に接続されるインピー
ダンス測定用の測定系の特性インピーダンスZOにほぼ
等しいが、送信フィルタ6のインピーダンスは最大にな
る。実際、相手方の中心周波数FtまたはFrにおいて
送信フィルタ6及び受信フィルタ7のそれぞれのインピ
ーダンスは無限大になることが理想的である。At the reception frequency Fr, the impedance of the reception filter 7 is approximately equal to the characteristic impedance ZO of the measurement system for impedance measurement connected to the output terminal 4, for example, but the impedance of the transmission filter 6 is maximum. In fact, it is ideal that the impedance of each of the transmission filter 6 and the reception filter 7 becomes infinite at the center frequency Ft or Fr of the other party.
というのは、送信フィルタ6及び受信フィルタ7のそれ
ぞれのインピーダンスは大きくなればなるほど、分波損
失が小さくなり、無限大になると、分波損失が完全に無
くなるからである。しかし、各インピーダンスを無限大
にすることは不可能なので、現実的には最大にする努力
が払われている。This is because the greater the impedance of each of the transmission filter 6 and the reception filter 7, the smaller the demultiplexing loss becomes, and when it reaches infinity, the demultiplexing loss completely disappears. However, it is impossible to make each impedance infinitely large, so in reality, efforts are made to maximize each impedance.
この種の共用器では、例えばアンテナ等から受信信号が
共通端子2に入力すると、その受信信号は受信側伝送路
5bを通って受信フィルタ7でろ波され、出力端子4か
ら出力されて受信回路等に送られる。また、送信回路等
からの送信信号が入力端子3に入力すると、その送信信
号は、送信フィルタ6でろ波された後、送信側伝送路5
aを通って共通端子2から出力され、アンテナ等に送ら
れる。In this type of duplexer, when a received signal from an antenna or the like is input to the common terminal 2, the received signal passes through the receiving side transmission path 5b, is filtered by the receiving filter 7, and is outputted from the output terminal 4 to the receiving circuit, etc. sent to. Furthermore, when a transmission signal from a transmission circuit or the like is input to the input terminal 3, the transmission signal is filtered by a transmission filter 6, and then filtered by a transmission line 5 on the transmission side.
a, is output from the common terminal 2, and sent to an antenna or the like.
(発明が解決しようとする課題〉
しかしながら、上記構成の分波器では、次のよな課題が
あった。(Problems to be Solved by the Invention) However, the duplexer having the above configuration has the following problems.
従来の技術では、共通端子2からみた送信側の等価イン
ピーダンスと受信側の等価インピーダンスの各絶対値を
最大になるように、送信側と受信側の伝送路長Lt、L
rを計算して共用器を設計している。この設計法を最大
インピーダンス設計法と呼ぶことにする。このような最
大インピーダンス設計法で設計した共用器の送信側と受
信側の挿入損失を解析してみると、最大インピーダンス
設計法の持つ特性から、送信側と受信側のそれぞれの挿
入損失を最少にすることが不可能であった。In the conventional technology, the transmission path lengths Lt and L on the transmitting side and the receiving side are set so that the respective absolute values of the equivalent impedance on the transmitting side and the equivalent impedance on the receiving side viewed from the common terminal 2 are maximized.
The duplexer is designed by calculating r. This design method will be referred to as the maximum impedance design method. Analyzing the insertion loss on the transmitting side and receiving side of a duplexer designed using such a maximum impedance design method, it is found that due to the characteristics of the maximum impedance design method, the insertion loss on the transmitting side and receiving side can be minimized. It was impossible to do so.
すなわち、送信側と受信側の伝送路長Lt、Lrをうま
く選択できれば、共用器の挿入損失を最少にすることが
できるのであるが、最大インピーダンス設計法を用いて
いるため、最適な伝送路長しt、Lrを決定することが
困難である。挿入損失を最少限に抑えることは、共用密
設計上では重要な課題であるが、従来の最大インピーダ
ンス設計法を用いている限り、それが不可能である。In other words, if the transmission path lengths Lt and Lr on the transmitting and receiving sides are properly selected, the insertion loss of the duplexer can be minimized, but since the maximum impedance design method is used, the optimum transmission path length cannot be determined. It is difficult to determine t and Lr. Minimizing insertion loss is an important issue in shared dense design, but this is not possible using conventional maximum impedance design methods.
本発明は前記従来技術が持っていた課題として、送信側
と受信側の伝送路長を最適に決定して共用器の挿入損失
を最少限に抑えることが困難な点について解決した共用
器の伝送路長決定方法を提供するものである。The present invention solves the problem of the prior art in that it is difficult to optimally determine the transmission path length on the transmitting side and the receiving side to minimize the insertion loss of the duplexer. This provides a path length determination method.
(課題を解決するための手段)
本発明は前記課題を解決するために、一端が共通端子に
接続された伝送路長Ltの送信側伝送路及び伝送路長L
rの受信側伝送路を有する送、受信信号分波用の分波回
路パターンと、前記送信側伝送路の他端に接続された送
信信号ろ波相の送信フィルタと、前記受信側伝送路の他
端に接続された受信信号ろ波相の受信フィルタとが、基
板上に設けられた共用器において、前記送信側及び受信
側の伝送路長を次のように決定したものである。(Means for Solving the Problems) In order to solve the above problems, the present invention provides a transmitting side transmission line with a transmission line length Lt, one end of which is connected to a common terminal, and a transmission line with a transmission line length Lt.
a branching circuit pattern for transmitting and receiving signals having r receiving side transmission lines; a transmitting filter for the transmitting signal filtering phase connected to the other end of the transmitting side transmission line; The reception filter for the reception signal filtering phase connected to the other end is a duplexer provided on the board, and the transmission path lengths on the transmission side and reception side are determined as follows.
すなわち、一定の挿入損失計算式に基づき、送信フィル
タの挿入損失Tt及び受信フィルタの挿入損失Trの絶
対値が常に最少となるように、伝送路長Lt、Lrと、
共通端子からみた送信フィルタ側のインピーダンスZt
及び受信フィルタ側のインピーダンスZrとを、帰納法
によって更新しつつ、伝送路長Lt、Lrが所定精度に
収束するまで反復計算を行って最適な伝送路長を求める
ようにしたものである。That is, based on a certain insertion loss calculation formula, the transmission path lengths Lt and Lr are set so that the absolute values of the transmission filter insertion loss Tt and the reception filter insertion loss Tr are always the minimum.
Impedance Zt on the transmission filter side viewed from the common terminal
and the impedance Zr on the reception filter side are updated by induction, and the optimum transmission path length is determined by performing iterative calculations until the transmission path lengths Lt and Lr converge to a predetermined accuracy.
(作用)
本発明によれば、以上のように共用器における伝送路長
決定方法を構成したので、一定の挿入損失計算方法に基
づき、送信側及び受信側の伝送路長Lt、Lrと送信側
及び受信側のフィルタのインピーダンスZt、Zrとを
更新していき、伝送路長Lt、Lrが所定精度に収束す
るまで反復計算を行うと、送信側と受信側の挿入損失T
tとTrの両方が同時に最小値になる最適な伝送路長が
得られる。従って、前記課題を解決できるのである。(Operation) According to the present invention, since the method for determining the transmission path length in the duplexer is configured as described above, the transmission path lengths Lt and Lr on the transmitting side and the receiving side are determined based on a certain insertion loss calculation method. By updating impedances Zt and Zr of the filters on the receiving side and repeating calculations until the transmission path lengths Lt and Lr converge to a predetermined accuracy, the insertion loss T on the transmitting side and the receiving side is
An optimal transmission path length can be obtained in which both t and Tr are simultaneously at their minimum values. Therefore, the above problem can be solved.
(実施例)
第3図(a>、(b)、(c)は、本発明の実施例を示
す共用器の構成説明図であり、同図(a)は回路図、同
図(b)は送信周波数Ftにおける等価回路図、及び同
図(C)は受信周波数Frにおける等価回路図である。(Example) Figures 3 (a>, (b), and (c) are explanatory diagrams of the configuration of a duplexer showing an example of the present invention, where (a) is a circuit diagram, and (b) is a circuit diagram. is an equivalent circuit diagram at the transmission frequency Ft, and (C) is an equivalent circuit diagram at the reception frequency Fr.
第3図(a)に示すように、この共用器は従来の第2図
と同様に、図示しない基板を有し、その基板上には、共
通端子12、入力端子13及び出力端子14が設けられ
ている。共通端子12には、分波回路パターンエ5の一
端が接続され、その分波回路パターンエ5の他端が送信
フィルタ16及び受信フィルタ17を介して入力端子1
3及び出力端子(4にそれぞれ接続されている。As shown in FIG. 3(a), like the conventional device shown in FIG. 2, this duplexer has a board (not shown), and a common terminal 12, an input terminal 13, and an output terminal 14 are provided on the board. It is being One end of the branching circuit pattern 5 is connected to the common terminal 12, and the other end of the branching circuit pattern 5 is connected to the input terminal 1 via the transmission filter 16 and the reception filter 17.
3 and output terminal (4), respectively.
送信フィルタ16及び受信フィルタ17は、例えば弾性
表面波フィルタ等で構成されている。特に、弾性表面波
フィルタを用いた場合、この弾性表面波フィルタは、小
型でかつ温度や経年変化に対して安定である上、振幅特
性と位相特性をほとんど独立に任意に設計できるという
特徴を有している。The transmission filter 16 and the reception filter 17 are configured with, for example, surface acoustic wave filters. In particular, when a surface acoustic wave filter is used, this surface acoustic wave filter is small and stable against changes in temperature and aging, and has the characteristics that the amplitude characteristics and phase characteristics can be designed almost independently and arbitrarily. are doing.
分波回路パターン■5は、従来と同様に、伝送路長Lt
の送信側伝送路15aと、伝送路長Lrの受信側伝送I
¥815bとで構成されている。入力端子(3及び出力
端子14には、それぞれ終端インピーダンス18.19
が接続されている。一般的に、この終端インピーダンス
18.19は、インピーダンスを測定するための測定系
の特性インピーダンスZOと同じ値である。The branching circuit pattern #5 has a transmission path length Lt as in the conventional case.
A transmitting side transmission line 15a of , and a receiving side transmission I of transmission line length Lr.
It consists of ¥815b. The input terminal (3 and output terminal 14 each have a terminal impedance of 18.19
is connected. Generally, this terminal impedance 18.19 has the same value as the characteristic impedance ZO of the measurement system for measuring impedance.
この第3図(a)の共用器は、従来の共用器と同一の構
成であり、本実施例が従来と異なる点は、送信側及び受
信側の伝送路長Lt、Lrの決定方法である。The duplexer shown in FIG. 3(a) has the same configuration as the conventional duplexer, and the difference between this embodiment and the conventional duplexer is the method of determining the transmission path lengths Lt and Lr on the transmitting side and the receiving side. .
第3図(b)の等価回路において、Ztは共通端子12
からみた受信側の等価インピーダンスZr、16aは送
信側伝送路15aと送信フィルタ16の合成した縦続行
列[T]である。In the equivalent circuit of FIG. 3(b), Zt is the common terminal 12
The equivalent impedance Zr, 16a on the receiving side viewed from the transmission line 16a is a tandem array [T] that is a combination of the transmission line 15a on the transmitting side and the transmission filter 16.
同様に、第3図(c)の等価回路において、20は共通
端子12からみた送信側の等価インピーダンスZt.1
7aは受信側伝送路15bと受信フィルタ17の合成し
た縦続行列[R]である。Similarly, in the equivalent circuit of FIG. 3(c), 20 is the equivalent impedance Zt. on the transmitting side viewed from the common terminal 12. 1
7a is a cascaded row array [R] which is a combination of the receiving side transmission line 15b and the receiving filter 17.
縦続行列[T]と[Rコを式(1)と(2)に示す。(
At、Bt、Ct、Dt>と(Ar、Br、Cr、Dr
)は、それぞれ[Tコと[R]の成分で、複素数である
。The vertical columns [T] and [R are shown in equations (1) and (2). (
At, Bt, Ct, Dt> and (Ar, Br, Cr, Dr
) are components of [T and [R], respectively, and are complex numbers.
縦続行列[T]と[R]から、共用器の送信側と受信側
の挿入損失TtとTrを、求めると、次の式(3)及び
式(4〉のようになる。The insertion losses Tt and Tr on the transmitting side and receiving side of the duplexer are calculated from the cascade arrays [T] and [R] as shown in the following equations (3) and (4).
rt=v+”i
=0.5(A t 十B t/ZO+CtZO+Dt)
+0.5(At+Bt/ZO)/Zr = (3)T
r=0.5(Ar+Br/ZO+CrZO+Dr)+0
.5(Ar+Br/zO)/zt H+ (4)V=
0.5(At+Bt/ZO+CtZO+Dt)・・・・
・・(3−1)
’i=0.5(At+Bt/20)/Zr・・・・・・
(3−2)
但し、zO:測定系の特性インピーダンス挿入損失Tt
とTrの絶対値は、送信側と受信側の伝送路長LtとL
rを変化させることにより、両方とも同時に最小値にす
ることができる。その長さを最適伝送路長、そしてこれ
に基づく設計法を最適設計法と呼ぶことにする。rt=v+”i=0.5(A t 10B t/ZO+CtZO+Dt)
+0.5(At+Bt/ZO)/Zr = (3)T
r=0.5(Ar+Br/ZO+CrZO+Dr)+0
.. 5(Ar+Br/zO)/zt H+ (4)V=
0.5 (At+Bt/ZO+CtZO+Dt)...
...(3-1) 'i=0.5(At+Bt/20)/Zr...
(3-2) However, zO: Characteristic impedance insertion loss Tt of the measurement system
The absolute values of and Tr are the transmission path lengths Lt and L on the sending and receiving sides.
By changing r, both can be minimized at the same time. This length will be called the optimal transmission path length, and the design method based on this will be called the optimal design method.
従来の方法では、受信側の等価インピーダンスZrと送
信側の等価インピーダンスZtの絶対値を最大になるよ
うに送信側と受信側の伝送路長しtとLrを計算して共
用器を設計(最大インピーダンス設計法〉している。こ
れに対して本実施例では、最適設計法を用いて最適伝送
路長を求めるものである。しかし、最適伝送路長の場合
は、−般的な関数式が確立されていないので、従来の最
大インピーダンス設計法と同じように、解析的に求める
ことが困難である。In the conventional method, the duplexer is designed by calculating the transmission path lengths t and Lr on the transmitting and receiving sides so as to maximize the absolute values of the equivalent impedance Zr on the receiving side and the equivalent impedance Zt on the transmitting side (maximum On the other hand, in this example, the optimal transmission path length is determined using the optimal design method.However, in the case of the optimal transmission path length, the general function equation is Since this has not been established, it is difficult to obtain it analytically, similar to the conventional maximum impedance design method.
そこで本実施例では、第1図(a)、(b)に示すよう
な帰納法を用いて、電子計算機等で数値的に最適伝送路
長を計算するようにしている。Therefore, in this embodiment, the optimal transmission path length is calculated numerically by an electronic computer or the like using the induction method shown in FIGS. 1(a) and 1(b).
この帰納法を説明する前に、第4図を参照しつつ、挿入
損失Tt(またはTr)を用いて最大インピーダンス設
計法と最適設計法の違いを幾何学的に説明する。Before explaining this induction method, the difference between the maximum impedance design method and the optimal design method will be explained geometrically using insertion loss Tt (or Tr) with reference to FIG.
第4図は、最大インピーダンス設計法と最適設計法の説
明図であり、横軸に実部r、縦軸に虚部Xがとられてい
る。FIG. 4 is an explanatory diagram of the maximum impedance design method and the optimal design method, with the real part r plotted on the horizontal axis and the imaginary part X plotted on the vertical axis.
送信周波数Ftにおいて、共通端子12からみた受信側
のインピーダンスZrは複素数であり、受信側伝送路長
Lrを変化させると、複素数平面上で第4図に示すよう
な半径RO1中心ω0(rO,xo)の円(Co)を描
く。受信側インピーダンスZrは次式のように表わせる
。At the transmission frequency Ft, the receiving side impedance Zr seen from the common terminal 12 is a complex number, and when the receiving side transmission path length Lr is changed, the radius RO1 center ω0 (rO, xo ) draw a circle (Co). The receiving side impedance Zr can be expressed as follows.
Zr=r+jx
・・・・・・(5〉
アドミタンス1 / Z rもインピーダンスZrと同
じように円(Co)の円周上にあるが、ω0を中心に互
いに対称である。点MはインピーダンスZrが最大にな
るときの位置を示し、そして点MOはその時のアドミタ
ンスL / Z rを示す。半径ROの値と中心ω0の
座標は次のようになる。Zr=r+jx ・・・・・・(5〉 Admittance 1 / Z r is also on the circumference of the circle (Co) like impedance Zr, but they are symmetrical to each other around ω0. Point M is impedance Zr The point MO indicates the admittance L/Z r at that time.The value of the radius RO and the coordinates of the center ω0 are as follows.
RO= I O,5(Z○2/r−r)l −(6
)ωO:
(rOl
xO>
・・・・・・(7〉
ro=0.5(Z02/r+r)
・・・・・・(7−a>
xO=0
・・・・・・(7−b)
式(3〉及び式(3−2>より、Wの軌跡は半径R1,
中心ωl (rl、xi)の円(C1)である。点MO
は、Mlに移動する。半径R1の値と中心ω1の座標は
、次のようになる。RO=IO,5(Z○2/r-r)l-(6
) ωO: (rOl xO>・・・・・・(7> ro=0.5(Z02/r+r) ・・・・・・(7-a> xO=0 ・・・・・・(7-b ) From formula (3> and formula (3-2>), the locus of W has radius R1,
It is a circle (C1) with center ωl (rl, xi). point MO
moves to Ml. The value of radius R1 and the coordinates of center ω1 are as follows.
R1= 0.5(At+Bt/ZO) RO ・・・・・・(8) ωl: 〈rl。R1= 0.5 (At+Bt/ZO) R.O. ・・・・・・(8) ωl: <rl.
xi>
・・・・・・(9)
rl−実部(0,5(At+Bt/ZO)ro)・・・
・・・(9−a)
xi−虚部(0,5(At+Bt/20)rO)・・・
・・・(9−b)
式(3)と円(C1)より、挿入損失Ttの軌跡は半径
R2=R1,中心ω2 (r2.x2)の円(C2)で
ある。そのとき点M1は点M2に移動する。中心ω2の
座標は次のようになる。xi> ......(9) rl-real part (0,5(At+Bt/ZO)ro)...
...(9-a) xi-imaginary part (0,5(At+Bt/20)rO)...
(9-b) From equation (3) and the circle (C1), the locus of the insertion loss Tt is a circle (C2) with radius R2=R1 and center ω2 (r2.x2). At that time, point M1 moves to point M2. The coordinates of the center ω2 are as follows.
ω2:
(r2゜
x2)
・・・・・・(10)
r2=rl+実部(0,5(At+Bt/ZO十CtZ
O+Dt)) −(10−a)x2=x1+虚部(0
,5(At+Bt/ZO十CtZO+Dt)) ・曲−
(1o−b〉以上の説明で明らかなように、挿入損失T
tの絶対値は、第4図に示した複素数平面の座標系の原
点0 (0,O)と、円(C2)の円周上の一点Nとを
結ぶ線分に等しい。受信側伝送路長Lrを変化させると
、点Nは円(C2)の円周上を移動し、当然、挿入損失
Ttの絶対値も変化する。ω2: (r2゜x2) ・・・・・・(10) r2=rl+real part(0,5(At+Bt/ZO×CtZ
O+Dt)) -(10-a)x2=x1+imaginary part(0
,5(At+Bt/ZO1CtZO+Dt)) ・Song-
(1o-b> As is clear from the above explanation, insertion loss T
The absolute value of t is equal to the line segment connecting the origin 0 (0, O) of the coordinate system of the complex plane shown in FIG. 4 and a point N on the circumference of the circle (C2). When the receiving side transmission path length Lr is changed, the point N moves on the circumference of the circle (C2), and naturally the absolute value of the insertion loss Tt also changes.
原点0 (0,O)と(JJ2 (r2.x2>を結ぶ
直線は、円(C2〉と交わり、点Maと点Mbが得られ
る。点Nは、受信側伝送路長Lrの変化によって円(C
2)の円周上を移動し、点Mbと重なると、挿入損失T
tの絶対値が最大になり、点Maと重なると、挿入損失
Ttの絶対値が最小になる。点Nが点Maと重なるよう
にLrを求めるのは、最適設計法の特長で、挿入損失T
tの絶対値が常に最小になるようにする。一方、点Nは
点M2と重なると、最大インピーダンス設計法で設計し
た共用器の送信側挿入損失Ttの絶対値が得られる。The straight line connecting the origin 0 (0, O) and (JJ2 (r2. (C
2), and when it overlaps with point Mb, the insertion loss T
When the absolute value of t becomes maximum and overlaps with point Ma, the absolute value of insertion loss Tt becomes minimum. Obtaining Lr so that point N overlaps with point Ma is a feature of the optimal design method, and the insertion loss T
Make sure that the absolute value of t is always the minimum. On the other hand, when point N overlaps point M2, the absolute value of the transmission side insertion loss Tt of the duplexer designed by the maximum impedance design method is obtained.
点Maは一般的に点M2と異なるため、明らかに最適設
計法で設計した共用器の挿入損失は、最大インピーダン
ス設計法で設計した共用器の挿入損失より小さくなる。Since the point Ma is generally different from the point M2, the insertion loss of the duplexer designed by the optimal design method is clearly smaller than the insertion loss of the duplexer designed by the maximum impedance design method.
従って、最適設計法を用いれば、共用器の挿入損失を最
小値にすることができる。Therefore, by using the optimal design method, the insertion loss of the duplexer can be minimized.
第1図(a>、(b)は、最適伝送路長を計算するため
の帰納法のフローチャートであり、この図を参照しつつ
、電子計算機等を用いた最適伝送路長決定方法について
説明する。Figures 1 (a> and (b) are flowcharts of the induction method for calculating the optimal transmission path length, and with reference to this figure, the method for determining the optimal transmission path length using a computer etc. will be explained. .
ステップ20において、送信側と受信側の伝送路長Lt
とLrの初期値をLtO=OとLr0=Oとする。この
時の縦続行列は[TO] = [T]と[RO] =
[R] 、挿入損失はTtOとTrO1共通端子12か
らみた送信フィルタエ6のインピーダンスと受信フィル
タ17のインピーダンスはZtOとZrOである。In step 20, the transmission path length Lt between the transmitting side and the receiving side
The initial values of and Lr are set to LtO=O and Lr0=O. At this time, the vertical rows are [TO] = [T] and [RO] =
[R], the insertion loss is TtO, and the impedance of the transmission filter 6 and the impedance of the reception filter 17 seen from the common terminal 12 of the TrO1 are ZtO and ZrO.
先ず、ステップZtでは、送信周波数Ftにおいて上述
したような式(1)〜式(10−b)を用いた方法で、
受信側の仮の最適伝送路長Lrlを求め、そのときの送
信側の最小挿入損失をTtlとする。ステップ22では
、最適伝送路長Lrlと縦続行列[RO]で[R1]と
Zrlが得られ、そしてステップ23で、受信周波数F
rにおいて縦続行列[R1]とインピーダンスZtOと
で、送信側の仮の最適伝送路長Ltlと受信側の最小挿
入損失Triを求めることができる。さらにステップ2
4で、最適伝送路長Ltlと縦続行列[TO]で[Tt
lとZt1が得られ、ステップ25で、送信周波数Ft
において縦続行列[T 1 ]とインピーダンスZrl
で受信側の新しい仮の最適伝送路長Lr2と、送信側の
新しい最小挿入損失Tt2を求めることができる。First, in step Zt, the method using equations (1) to (10-b) as described above at the transmission frequency Ft,
A tentative optimal transmission path length Lrl on the receiving side is determined, and the minimum insertion loss on the transmitting side at that time is set as Ttl. In step 22, [R1] and Zrl are obtained from the optimal transmission path length Lrl and the cascade array [RO], and in step 23, the receiving frequency F
At r, the tentative optimum transmission path length Ltl on the transmitting side and the minimum insertion loss Tri on the receiving side can be determined using the cascade array [R1] and the impedance ZtO. Further step 2
4, the optimal transmission path length Ltl and the tandem array [TO] are [Tt
l and Zt1 are obtained, and in step 25, the transmission frequency Ft
, the cascade array [T 1 ] and the impedance Zrl
A new provisional optimal transmission path length Lr2 on the receiving side and a new minimum insertion loss Tt2 on the transmitting side can be obtained using the following equations.
同様に、結合子■を介してステップ26で、最適伝送路
長Lr2と縦続行列[TO]で[R2]とZr2が得ら
れ、ステップ27で、受信周波数Frにおいて縦続行列
[R2]とインピーダンスZtlで送信側の新しい仮の
最適伝送路長Lt2と、受信側の新しい最小挿入損失T
r2を求めることができる。Similarly, [R2] and Zr2 are obtained from the optimum transmission path length Lr2 and the cascade array [TO] via the connector ① at step 26, and at step 27, the cascade array [R2] and the impedance Ztl are obtained at the reception frequency Fr. The new temporary optimal transmission path length Lt2 on the transmitting side and the new minimum insertion loss T on the receiving side are
r2 can be found.
ステップ28では、最適伝送路長のLr2とLr2が送
信側と受信側の最適伝送路長として使用できるかどうか
を判別するために、LtlとLr2の差及びLrlとL
r2の差を求め、これらの差の値が所望の精度N(例え
ば10−6〉より小さいかどうかで決める。条件が満た
されている場合、ステップ2つでLr2とLr2が最適
伝送路長であると決定して計算を終了し、一方条件が満
たされない場合、ステップ30で、Ltl=Lt2、L
r1=Lr2、Zr1=Zr2とし、結合子■を介して
ステップ24に戻り、上述の反復計算を繰り返す。In step 28, in order to determine whether the optimum transmission path lengths Lr2 and Lr2 can be used as the optimum transmission path lengths on the transmitting side and the receiving side,
Find the difference in r2, and decide whether the value of these differences is smaller than the desired accuracy N (for example, 10-6>). If the condition is met, in step 2, Lr2 and Lr2 are determined to be the optimal transmission path length. If it is determined that there is, and the calculation is terminated, but the condition is not satisfied, in step 30, Ltl=Lt2, L
Set r1=Lr2 and Zr1=Zr2, and return to step 24 via connector (2) to repeat the above-mentioned iterative calculation.
このような計算を繰り返すと、送信側と受信側の伝送路
長は、ある値LtnとLrnに収束し、これが求める最
適伝送路長である。このときの挿入損失も最適値Ttn
とTrnになる。When such calculations are repeated, the transmission path lengths on the transmitting side and the receiving side converge to certain values Ltn and Lrn, which are the optimum transmission path lengths to be found. The insertion loss at this time is also the optimum value Ttn
and becomes Trn.
LtnとLrnのような最適伝送路長は、将来的に、一
般的な関数式が確立されれば、解析的に計算できるよう
になるかもしれないが、現在の実用範囲内では、本実施
例の計算精度が最良の方法といえる。Optimum transmission path lengths such as Ltn and Lrn may be calculated analytically in the future if general functional formulas are established, but within the current practical scope, this example The calculation accuracy can be said to be the best method.
次に、第5図(a>、(b)、(c)を参照して、本実
施例の効果を説明する。Next, the effects of this embodiment will be explained with reference to FIGS. 5(a>, (b), and (c)).
第5図(a)〜(c)は、送信フィルタ及び受信フィル
タを弾性表面波フィルタを用いて構成した、従来と本実
施例の共用器の挿入損失特性と反射損失特性図である。FIGS. 5(a) to 5(c) are insertion loss characteristic and reflection loss characteristic diagrams of a conventional duplexer and a duplexer of this embodiment in which the transmitting filter and the receiving filter are configured using surface acoustic wave filters.
そのうち、第5図(a)は、従来の最大インピーダンス
設計法で設計した共用器の挿入損失特性と反射損失特性
を示している。TT−1とTR−↓はそれぞれ送信側と
受信側の挿入損失特性である。TL−1は共通端子12
からみた反射損失特性である。送信側と受信側の伝送路
長は、それぞれ0.2782Xλrと0.2028xλ
tである。Among them, FIG. 5(a) shows the insertion loss characteristics and reflection loss characteristics of a duplexer designed using the conventional maximum impedance design method. TT-1 and TR-↓ are insertion loss characteristics on the transmitting side and receiving side, respectively. TL-1 is common terminal 12
This is the reflection loss characteristic from the perspective of The transmission path lengths on the transmitting side and receiving side are 0.2782Xλr and 0.2028xλ, respectively.
It is t.
第5図(b)は、本実施例の最適設計法で設計した共用
器の挿入損失特性を示している。従来と本実施例との設
計法の効果を確認するために、送信フィルタ16及び受
信フィルタ17を従来と同じ弾性表面波フィルタを用い
て構成した。この場合も、第5図(a>と同様に、TT
−2とTR−2はそれぞれ送信側と受信側の挿入損失特
性で、TL−2は共通端子12からみた反射損失特性で
ある。送信側と受信側の伝送路長はそれぞれ0゜245
2Xλrと0.1872Xλtである。λtとλrは送
信波長と受信波長である。FIG. 5(b) shows the insertion loss characteristics of the duplexer designed by the optimal design method of this embodiment. In order to confirm the effects of the conventional design method and the design method of this embodiment, the transmitting filter 16 and the receiving filter 17 were constructed using the same surface acoustic wave filters as the conventional method. In this case as well, TT
-2 and TR-2 are insertion loss characteristics on the transmitting side and receiving side, respectively, and TL-2 is a return loss characteristic viewed from the common terminal 12. The transmission path length on the sending and receiving sides is 0°245 each.
2Xλr and 0.1872Xλt. λt and λr are the transmission wavelength and reception wavelength.
第5図(C)は、従来と本実施例とを比較しやすくする
ために、第5図(a)と第5図(b)の挿入損失特性を
拡大して同じ座標上で描いたものである。TT−1,T
T−2,TR−1,TR−2は第5図(a>、(b)と
同じものである。TT−1とTT−2そしてTR−1と
TR−2を比較してみると、それぞれの通過帯域の中心
周波数835、OMHzと880、OMHzにおいて、
本実施例の共用器の挿入損失の方が、従来の方法で設計
した共用器の挿入損失よりも少ないことがわかる。従っ
て、本実施例の方法では、従来の方法よりも挿入損失を
小さくでき、それによって共用器の信号減衰量を小さく
することができる。Figure 5(C) is an enlarged version of the insertion loss characteristics in Figures 5(a) and 5(b) drawn on the same coordinates in order to facilitate comparison between the conventional method and this embodiment. It is. TT-1,T
T-2, TR-1, and TR-2 are the same as in Figure 5 (a>, (b). Comparing TT-1 and TT-2 and TR-1 and TR-2, At the center frequencies of each passband, 835, OMHz and 880, OMHz,
It can be seen that the insertion loss of the duplexer of this example is smaller than the insertion loss of the duplexer designed using the conventional method. Therefore, in the method of this embodiment, the insertion loss can be made smaller than in the conventional method, thereby making it possible to reduce the amount of signal attenuation of the duplexer.
(発明の効果)
以上詳細に説明したように、本発明によれば、送信フィ
ルタ及び受信フィルタの挿入損失Tt。(Effects of the Invention) As described above in detail, according to the present invention, the insertion loss Tt of the transmission filter and the reception filter.
Trが同時に最小になるように、共通端子から送信フィ
ルタ及び受信フィルタまでの伝送路長Lt。The transmission path length Lt from the common terminal to the transmission filter and reception filter is set so that Tr is simultaneously minimized.
Lrを帰納法を用いた計算手法で計算し、最適な伝送路
長を求めるようにしたので、送信フィルタ及び受信フィ
ルタの挿入損失を最小限に抑えることが可能となり、そ
れによって小型で良好な周波数特性を持った共用器を提
供することができる。Since Lr is calculated using a calculation method using the induction method to find the optimal transmission path length, it is possible to minimize the insertion loss of the transmitting filter and receiving filter, thereby achieving a small size and a good frequency. It is possible to provide a duplexer with special characteristics.
第工図(a)、(b)は本発明の実施例を示すもので最
適伝送路長を計算するための帰納法のフローチャート、
第2図は従来の共用器の構成国、第3図(a>、(b)
、(c)は本発明の実施例を示す共用器の構成説明図で
あり、同図(a)は回路図、同図(b)は送信周波数F
tにおける等価回路図、及び同図(c)は受信周波数F
rにおける等価回路図、第4図は最大インピーダンス設
計法と最適設計法の説明図、第5図(a)、(b)(c
)は従来と本実施例とを比較するための共用器の挿入損
失特性図であり、同図(a)は最大インピーダンス設計
法で設計した共用器の挿入損失特性図、同図(b)は最
適設計法で設計した共用器の挿入損失特性図、及び同図
(C)は挿入損失の比較図である。
12・・・・・・共通端子、13・・・・・・入力端子
、14・・・・・・出力端子、15・・・・・・分波回
路パターン、15a・・・・・送信側伝送路、15b・
・・・・・受信側伝送路、工6・・・・・・送信フィル
タ、17・・・・・・受信フィルタ。
(a)
小発明の実施例のフローチャート
第1図
(6)
第
図
12;六通瑞子
13:入力端子
14’−出力端子
15:分波回踏パターン
小発明の実施例の共用器
第3図
送信周波数「t、口お(115等価回路<−er)
受信周波数「rにおけう等価回路
(C)
第3図
周波数(閘Hz)
Booo
850.0
周5皮敗 (MHz)“
9ωO
押入損失の比較
(C)
第5図
手続補正書
共用器の伝送路長決定方法
代表者
小
杉
信
光
補正の対象
明細書の「発明の詳細な説明」の欄、及び図面。
(1) 明m書、13頁12行目から14頁7行目の「
第4図は、・・・・・・次のようになる。」を、次の通
り補正する。
「第4図は、最大インピーダンス設計法と最適設計法の
説明図であり、横軸に実部、縦軸に虚部がとられている
。
送信周波数Ftにおいて、共通端子12からみた受信側
のインピーダンスZrは複素数であり、受信側伝送路長
Lrを変化させると、複素数平面上で第4図に示すよう
な半径RO1中心ω0(rO,xo)の円(CO)を描
く。受信側インピーダンスZrは次式のように表わせる
。
Zr=Rr+jXr
・・・・・・(5〉
アドミタンス1/ZrもインピーダンスZrと同じよう
に円(CO)の円周上にあるが、ω0を中心に互いに対
称である。点MはインピーダンスZrが最大になるとき
の位置を示し、そして点MOはその時のアドミタンス1
/Zrを示す。点Mの座標を(r、0)とすれば、点M
Oの座標は(Z02/r、O)である。半径ROの値と
中心ωOの座標は次のようになる。」
(2〉 第4図を別紙の通り補正する。Figures (a) and (b) show an embodiment of the present invention, and are flowcharts of the induction method for calculating the optimal transmission path length;
Figure 2 shows the constituent countries of the conventional shared device, Figure 3 (a>, (b))
, (c) are configuration explanatory diagrams of a duplexer showing an embodiment of the present invention, (a) is a circuit diagram, and (b) is a diagram showing the transmission frequency F.
The equivalent circuit diagram at t and the same figure (c) are the receiving frequency F
Fig. 4 is an explanatory diagram of the maximum impedance design method and optimal design method, Fig. 5 (a), (b) (c
) is an insertion loss characteristic diagram of a duplexer designed for comparison between the conventional and this embodiment, (a) is an insertion loss characteristic diagram of a duplexer designed by the maximum impedance design method, and (b) is The insertion loss characteristic diagram of the duplexer designed by the optimal design method, and the same figure (C) is a comparison diagram of the insertion loss. 12... Common terminal, 13... Input terminal, 14... Output terminal, 15... Branching circuit pattern, 15a... Transmitting side Transmission line, 15b・
. . . Reception side transmission line, Engineering 6 . . . Transmission filter, 17 . . . Reception filter. (a) Flowchart of the embodiment of the small invention Fig. 1 (6) Fig. 12; Rokutsu Mizuko 13: Input terminal 14'-output terminal 15: Branching circuit pattern Duplexer of the embodiment of the small invention Fig. 3 Transmission frequency ``t'' (115 equivalent circuit <-er) Reception frequency ``equivalent circuit at r (C) Figure 3 Frequency (Hz) Boooo 850.0 Round 5 skin loss (MHz) 9ωO Pushing loss Comparison (C) Figure 5 Procedural Amendment Method for Determining Transmission Path Length for Dual Unit Representative Nobumitsu Kosugi The "Detailed Description of the Invention" column of the specification subject to the amendment and the drawings. (1) Book M, page 13, line 12 to page 14, line 7, “
Figure 4 is as follows. ” is corrected as follows. "Figure 4 is an explanatory diagram of the maximum impedance design method and the optimal design method, with the real part on the horizontal axis and the imaginary part on the vertical axis. At the transmission frequency Ft, the receiving side as seen from the common terminal 12 The impedance Zr is a complex number, and when the receiving side transmission path length Lr is changed, a circle (CO) with a radius RO1 and a center ω0 (rO, xo) is drawn on the complex number plane as shown in Fig. 4.The receiving side impedance Zr can be expressed as the following formula: Zr = Rr + j Point M indicates the position where impedance Zr is maximum, and point MO indicates the admittance 1 at that time.
/Zr is shown. If the coordinates of point M are (r, 0), point M
The coordinates of O are (Z02/r, O). The value of the radius RO and the coordinates of the center ωO are as follows. (2) Figure 4 is corrected as shown in the attached sheet.
Claims (1)
送路及び伝送路長Lrの受信側伝送路を有する送、受信
信号分波用の分波回路パターンと、前記送信側伝送路の
他端に接続された送信信号濾波用の送信フィルタと、前
記受信側伝送路の他端に接続された受信信号濾波用の受
信フィルタとが、基板上に設けられた共用器において、 下記の式に基づき、前記送信フィルタの挿入損失Tt及
び前記受信フィルタの挿入損失Trの絶対値が常に最小
となるように、前記伝送路長Lt,Lrと、前記共通端
子からみた前記送信フィルタ側のインピーダンスZt及
び前記受信フィルタ側のインピーダンスZrとを、帰納
法によって更新しつつ、前記伝送路長Lt,Lrが所定
精度に収束するまで反復計算を行って最適伝送路長を求
めることを特徴とする共用器の伝送路長決定方法。 ▲数式、化学式、表等があります▼ 但し、At,Bt,Ct,Dt;受信側伝送路と送信フ
ィルタとの合成した縦続行列[T]の成分で、複素数で
ある。 Ar,Br,Cr,Dr;送信側伝送路と受信フィルタ
との合成した縦続行列[R]の成分で、複素数である。 ZO:測定系の特性インピーダンス[Scope of Claims] A branching circuit pattern for branching transmitting and receiving signals having a transmitting side transmission line having a transmission line length Lt and a receiving side transmission line having a transmission line length Lr, one end of which is connected to a common terminal; A duplexer including a transmission filter for filtering a transmission signal connected to the other end of the transmission line on the transmission side and a reception filter for filtering the reception signal connected to the other end of the transmission line on the reception side, provided on a substrate. In, based on the following formula, the transmission path lengths Lt and Lr and the transmission path length as seen from the common terminal are set such that the absolute values of the insertion loss Tt of the transmission filter and the insertion loss Tr of the reception filter are always minimum. While updating the impedance Zt on the filter side and the impedance Zr on the receiving filter side by induction, iterative calculation is performed until the transmission path lengths Lt and Lr converge to a predetermined accuracy to obtain the optimal transmission path length. A method for determining the transmission path length of a duplexer. ▲There are mathematical formulas, chemical formulas, tables, etc.▼ However, At, Bt, Ct, Dt: These are components of the tandem sequence [T] that is a combination of the receiving side transmission path and the transmitting filter, and are complex numbers. Ar, Br, Cr, Dr: Components of a cascade sequence [R] that is a combination of the transmitting side transmission path and the receiving filter, and are complex numbers. ZO: Characteristic impedance of the measurement system
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1327591A JP3024771B2 (en) | 1989-12-18 | 1989-12-18 | Transmission path length determination method for duplexer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1327591A JP3024771B2 (en) | 1989-12-18 | 1989-12-18 | Transmission path length determination method for duplexer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03187626A true JPH03187626A (en) | 1991-08-15 |
| JP3024771B2 JP3024771B2 (en) | 2000-03-21 |
Family
ID=18200767
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1327591A Expired - Fee Related JP3024771B2 (en) | 1989-12-18 | 1989-12-18 | Transmission path length determination method for duplexer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3024771B2 (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5534829A (en) * | 1993-05-31 | 1996-07-09 | Sanyo Electric Co., Ltd. | Antenna duplexer |
| JPH1075153A (en) * | 1996-08-30 | 1998-03-17 | Oki Electric Ind Co Ltd | Branching filter package |
| JP2000151456A (en) * | 1998-11-05 | 2000-05-30 | Oki Electric Ind Co Ltd | Surface acoustic wave branching device of transmission band split type |
-
1989
- 1989-12-18 JP JP1327591A patent/JP3024771B2/en not_active Expired - Fee Related
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5534829A (en) * | 1993-05-31 | 1996-07-09 | Sanyo Electric Co., Ltd. | Antenna duplexer |
| JPH1075153A (en) * | 1996-08-30 | 1998-03-17 | Oki Electric Ind Co Ltd | Branching filter package |
| JP2000151456A (en) * | 1998-11-05 | 2000-05-30 | Oki Electric Ind Co Ltd | Surface acoustic wave branching device of transmission band split type |
Also Published As
| Publication number | Publication date |
|---|---|
| JP3024771B2 (en) | 2000-03-21 |
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