JPH0693568B2 - Series power supply circuit - Google Patents
Series power supply circuitInfo
- Publication number
- JPH0693568B2 JPH0693568B2 JP60231801A JP23180185A JPH0693568B2 JP H0693568 B2 JPH0693568 B2 JP H0693568B2 JP 60231801 A JP60231801 A JP 60231801A JP 23180185 A JP23180185 A JP 23180185A JP H0693568 B2 JPH0693568 B2 JP H0693568B2
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- Prior art keywords
- main line
- coupler
- line
- couplers
- length
- Prior art date
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Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、アレーアンテナ用の給電回路に用いられる
直列給電回路に関するものである。TECHNICAL FIELD The present invention relates to a series feeding circuit used for a feeding circuit for an array antenna.
第5図は例えば「アンテナ工学ハンドブック」(電子通
信学会編、オーム社発行)の第222頁〜第224頁に記載さ
れている従来の直列給電回路を示すブロック図である。
図において、1〜5は結合器、6〜9は各結合器1〜5
を接続している主線路、10は後方端の結合器5に接続さ
れている整合終端、P0は前方端の結合器に接続されてい
る入力端子、P1〜P5は各結合器1〜5における出力端子
であり、各結合器1〜5は、主線路6〜9を介して縦続
接続されている。FIG. 5 is a block diagram showing a conventional series feed circuit described on pages 222 to 224 of, for example, "Antenna Engineering Handbook" (edited by The Institute of Electronics and Communication Engineers, published by Ohmsha).
In the figure, 1-5 are couplers, 6-9 are each couplers 1-5.
, 10 is a matching terminal connected to the coupler 5 at the rear end, P 0 is an input terminal connected to the coupler at the front end, and P 1 to P 5 are each coupler 1 5 to 5, and the couplers 1 to 5 are connected in cascade via the main lines 6 to 9.
次にこの直列給電回路の動作について説明する。Next, the operation of this series feeding circuit will be described.
前方端の結合器1の入力端子P0に入射した波は主線路6
〜9を介して順次結合器1〜5を伝搬する途中必要な量
の電力が各結合器1〜5の出力端子P1〜P5に取り出さ
れ、残った電力は後方端の結合器5から整合終端10に吸
収される。このとき、各出力端子P1〜P5に取り出される
波の位相分布は、主線路6〜9の電気長によって決定さ
れる。The wave incident on the input terminal P 0 of the coupler 1 at the front end is the main line 6
The required amount of electric power is taken out to the output terminals P 1 to P 5 of each of the couplers 1 to 5 while being propagated through the couplers 1 to 5 through 9 to 9, and the remaining electric power is output from the coupler 5 at the rear end. It is absorbed by the matching end 10. At this time, the phase distribution of the waves output to the output terminals P 1 to P 5 is determined by the electrical lengths of the main lines 6 to 9.
いま、各出力端子P1〜P5から等間隔で位相の異なる位相
分布の電力を得ようとすると、主線路6〜9の電気長は
等しく選ぶ必要がある。すなわち主線路6〜9の線路長
を等しい長さL0とすると、出力端子P1〜P5の隣接間位相
差は各出力端子P1〜P5の電力の位相をφ1〜φ5とする
と、次式で表わされる。Now, if it is desired to obtain electric powers of different phase distributions at equal intervals from the output terminals P 1 to P 5 , the electrical lengths of the main lines 6 to 9 must be selected to be equal. I.e. the length L 0 is equal to the line length of the main line 6-9, adjacent phase difference between the output terminals P 1 to P 5 and phi 1 to [phi] 5 power phase of the output terminals P 1 to P 5 Then, it is expressed by the following equation.
但し φ1〜φ5:各端P1〜P5に取り出される波の位相 λg :主線路6〜9の波長 L0 :主線路6〜9の線路長 この式からわかるように隣接端子間位相差は波長λgに
よって変化するので周波数走査アンテナの給電系等に使
用することができる。 However, φ 1 to φ 5 : Phase of the wave extracted at each end P 1 to P 5 λg: Wavelength of the main lines 6 to 9 L 0 : Line length of the main lines 6 to 9 As seen from this equation, the distance between adjacent terminals Since the phase difference changes depending on the wavelength λg, the phase difference can be used for a power feeding system of the frequency scanning antenna.
しかし、従来の直列給電回路では、上述のように等間隔
で隣接位相の異なる位相分布を得るためには主線路6〜
9の長さを等しく取る必要があるので、次式を満足する
管内波長のλgnの周波数で結合器1〜5による反射波が
同相で重畳され、VSWRが著しく劣化する。However, in the conventional series feed circuit, in order to obtain the phase distributions of different adjacent phases at equal intervals as described above, the main line 6 to
Since it is necessary to make the lengths of 9 equal, the reflected waves from the couplers 1 to 5 are superposed in phase at the frequency of the guide wavelength λgn satisfying the following expression, and VSWR is significantly deteriorated.
但し、 n:整数 このときのVSWR特性を第6図に示す。 However, n: integer The VSWR characteristic at this time is shown in FIG.
この図からわかるように、従来の直列給電回路では周期
的にVSWRが著しく劣化するため、この周波数間隔に使用
周波数帯域幅が制限され広帯域に使用することができな
いという問題点があった。又、VSWRの劣化によって、出
力端子P1〜P5に取り出される波の振幅と位相が大きく変
動するという問題点があった。As can be seen from this figure, in the conventional series feed circuit, VSWR is significantly deteriorated periodically, so that there is a problem that the usable frequency band width is limited to this frequency interval and it cannot be used in a wide band. In addition, there is a problem that the amplitude and phase of the waves extracted at the output terminals P 1 to P 5 vary greatly due to the deterioration of VSWR.
この発明は上記のような問題点を解消するためになされ
たもので、広帯域にわたってVSWRが著しく劣化するのを
防ぐとともに、端子P0から入射した波を必要な振幅、位
相分布で複数の出力端子に取り出すことのできる直列給
電回路を得ることを目的とする。The present invention has been made to solve the above problems, and prevents VSWR from significantly deteriorating over a wide band, and also allows a wave incident from the terminal P 0 to have a plurality of output terminals with a required amplitude and phase distribution. The purpose is to obtain a series power supply circuit that can be taken out to the.
本願の第1の発明にかかる直列給電回路は、終端に整合
終端を備え、各結合器を結ぶ各主線路の長さを、L0+2L
d(Ri−0.5)に基づいて、それぞれ異なる長さに設定す
るとともに、各結合器と各出力端子との間に各主線路の
電気長を補正するための各補正線路を設け、これら補正
線路の長さMKは次式、 (L1+M1)−M0=(L2+M2)−M1 =(L3+M3)−M2 ・ ・ ・ =(LK+1+MK+1−MK =L0 (尚、L,Mの添数字が大きくなるに従って入力端側より
遠くなる所の主線路及び補正線路を示している。) に従って設定されて成ることを特徴とする。A series power supply circuit according to a first invention of the present application is provided with a matching termination at the end, and the length of each main line connecting each coupler is L 0 + 2L
Based on d (Ri-0.5), set different lengths and provide each correction line between each coupler and each output terminal to correct the electrical length of each main line. The length M K is calculated by the following equation: (L 1 + M 1 ) −M 0 = (L 2 + M 2 ) −M 1 = (L 3 + M 3 ) −M 2・ ・ ・ = (L K + 1 + M K + 1− M K = L 0 (note that the main line and the correction line that are farther from the input end side as the subscripts of L and M increase) are set.
また本願の第2の発明にかかる直列給電回路は、終端
に、整合終端の代わりに上記式で算出される補正線路を
設けて出力端を接続して成るものである。Further, the series power supply circuit according to the second invention of the present application is configured such that a correction line calculated by the above formula is provided at the terminal end instead of the matching terminal and the output terminal is connected.
この発明における結合器間の異なる長さの主線路は、結
合器から入力端子P0に反射してくる反射波の位相を分散
させ、特定の周波数においてVSWRが著しく劣化するのを
抑制する。The main lines of different lengths between the couplers in the present invention disperse the phase of the reflected wave reflected from the coupler to the input terminal P 0 , and suppress VSWR from significantly deteriorating at a specific frequency.
又、補正線路は主線路の異なった長さによって生じる主
線路の電気長を補正し、各結合器の出力端子から等間隔
で位相の異なる位相分布の電力が得られるように作用す
る。The correction line corrects the electrical length of the main line caused by the different lengths of the main line, and operates so as to obtain the electric power of the phase distribution having different phases at equal intervals from the output terminal of each coupler.
第1図はこの発明の一実施例を示すブロック図であり、
1〜5は結合器、6〜9は主線路、10は整合終端、11〜
15は補正線路、P0は前方端に位置する結合器1の入力端
子、P1〜P5は各結合器1〜5から補正線路11〜15を介し
て接続された出力端子である。FIG. 1 is a block diagram showing an embodiment of the present invention,
1-5 are couplers, 6-9 are main lines, 10 are matching terminations, 11-
Reference numeral 15 is a correction line, P 0 is an input terminal of the coupler 1 located at the front end, and P 1 to P 5 are output terminals connected from the respective couplers 1 to 5 via the correction lines 11 to 15.
ここにおいて各結合器1〜5は主線路6〜9を介して縦
続接続されており、かつ結合器1〜5と出力端子P1〜P5
との間に補正線路11〜15が接続されている。Here, the couplers 1 to 5 are connected in cascade via the main lines 6 to 9, and the couplers 1 to 5 and the output terminals P 1 to P 5 are connected.
Correction lines 11 to 15 are connected between and.
この主線路6〜9の長さL1〜L4はL0を平均値としL0±Ld
の範囲内で異なる長さに選ばれている。The lengths L 1 to L 4 of the main lines 6 to 9 are L 0 ± Ld with L 0 as an average value.
Different lengths are selected within the range.
例えば(0,1)区間の一様乱数をRiとすると、L1〜L4は
次式で表わされる長さとなっている。For example, if Ri is a uniform random number in the (0,1) interval, then L 1 to L 4 have a length represented by the following equation.
Li=L0+2Ld(Ri−0.5) (3) (i=1〜4) 長さLdは第3図のように考えて決定される。即ち、従来
と同様にすべての主線路6〜9が同一長さとし、L0±Ld
で変化させた場合にVSWRのピークとなる周波数が使用周
波数帯域を覆い尽すようにである。この条件から、使用
帯域の下限の周波数の波長をλgとすると、Ldは近似的
に次式で与えられる。Li = L 0 + 2Ld (Ri−0.5) (3) (i = 1 to 4) The length Ld is determined by considering as shown in FIG. That is, as in the conventional case, all main lines 6 to 9 have the same length, and L 0 ± Ld
It seems that the frequency that becomes the peak of VSWR when it is changed by covers the used frequency band. Under this condition, if the wavelength of the lower limit frequency of the used band is λg, Ld is approximately given by the following equation.
又、補正線路11〜15の長さM0〜M4は、隣接出力端子P1〜
P4間で入力端子P0からの線路長の差がL0となるように、
次式で決定される長さとしている。 Further, the lengths M 0 to M 4 of the correction lines 11 to 15 are the same as those of the adjacent output terminals P 1 to
Make sure that the line length difference from the input terminal P 0 between P 4 is L 0 .
The length is determined by the following formula.
(L1+M1)−M0=(L2+M2)−M1 =(L3+M3)−M2 =(L4+M4)−M3 =L0 (5) この直列給電回路では、入力端子P0に入射した波は主線
路6〜9を介して順次結合器1〜5を伝搬する途中で一
部の電力が各出力端子P1〜P5から取り出され、残った電
力は整合終端10に吸収される。 (L 1 + M 1) -M 0 = (L 2 + M 2) -M 1 = (L 3 + M 3) -M 2 = (L 4 + M 4) -M 3 = L 0 (5) In this series feed circuit , The wave incident on the input terminal P 0 is partially propagated through the main lines 6 to 9 through the couplers 1 to 5 so that part of the power is extracted from the output terminals P 1 to P 5 , and the remaining power is It is absorbed by the matching end 10.
出力端子P1〜P5に取り出される電力の波の振幅は、結合
器1〜5の結合量の与え方によって必要な振幅分布とす
ることができる。The amplitude of the power wave extracted at the output terminals P 1 to P 5 can be set to a required amplitude distribution depending on how the coupling amounts of the couplers 1 to 5 are applied.
又、出力端子P1〜P5に取り出される電力の波の位相φ1
〜φ5は、主線路6〜9及び補正線路11〜15の電気長に
よって決定される。この位相分布は、第5式の条件から
従来の直列給電回路と同様に、等間隔で位相の異なる位
相分布となる。このとき出力端子P1〜P5の隣接端子間位
相差は第1式で表わされ、周波数走査アンテナ等に使用
することができる。Also, the phase φ 1 of the wave of electric power taken out at the output terminals P 1 to P 5
˜φ 5 is determined by the electrical lengths of the main lines 6-9 and the correction lines 11-15. From the condition of the fifth expression, this phase distribution is a phase distribution in which the phases are different at equal intervals, as in the conventional series feed circuit. At this time, the phase difference between the adjacent terminals of the output terminals P 1 to P 5 is represented by the first expression and can be used for a frequency scanning antenna or the like.
次に、この直列給電回路のVSWRは、主線路6〜9の長さ
が異なった長さとなっているため、結合器1〜5の反射
がすべて特定の周波数で同相で重畳されることはない。
このため、VSWR特性は第4図のようになり、広帯域な周
波数にわたって著しいVSWRの劣化はなくなる。又、この
ため出力端子P1〜P5に取り出される波の振幅、位相の変
動が小さくなる。Next, in the VSWR of this series power feeding circuit, since the main lines 6 to 9 have different lengths, all the reflections of the couplers 1 to 5 are not superimposed in phase at a specific frequency. .
Therefore, the VSWR characteristics are as shown in FIG. 4, and there is no significant deterioration in VSWR over a wide band of frequencies. Further, for this reason, fluctuations in the amplitude and phase of the waves extracted at the output terminals P 1 to P 5 are reduced.
第2図はこの発明の他の一実施例を示す構成図である。
第1図の実施例では、入力端P0から入射した波のうち結
合器1〜5に接続された出力端子P1〜P5に取り出されず
に残った波の電力が整合終端10に捨てられていたが、第
2図の実施例ではこの電力を出力端子P6に取り出して有
効に利用するようにしている。FIG. 2 is a block diagram showing another embodiment of the present invention.
In the embodiment of FIG. 1, of the waves incident from the input terminal P 0 , the power of the waves remaining without being extracted at the output terminals P 1 to P 5 connected to the couplers 1 to 5 is discarded to the matching termination 10. However, in the embodiment of FIG. 2, this electric power is taken out to the output terminal P 6 and is effectively used.
動作は第1図の直列給電回路と同様であり、出力端子P1
〜P6に取り出される波の振幅は、結合器1〜5の結合量
の選び方によって必要な振幅分布とすることができる。Operation is similar to the series feed circuit of FIG. 1, the output terminal P 1
The amplitudes of the waves extracted to P 6 can be made to have a required amplitude distribution depending on how to select the coupling amount of the couplers 1 to 5.
又、第5式の条件の他に次式の条件を加えることによっ
て、出力端子から取り出される波の位相分布は等間隔で
位相の異なる位相分布となる。Further, by adding the condition of the following formula in addition to the condition of the fifth formula, the phase distribution of the wave extracted from the output terminal becomes a phase distribution having different phases at equal intervals.
L5−M4=L0 (6) 又、VSWR特性は、結合器1〜5が異なる長さの主線路6
〜9を介して縦続接続されているので広帯域な周波数に
わたって著しいVSWRの劣化はない。L 5 −M 4 = L 0 (6) In addition, the VSWR characteristics show that the couplers 1 to 5 have different main line 6 lengths.
Cascaded through ~ 9, there is no significant VSWR degradation over a wide band of frequencies.
なお、上記実施例では結合器の数を5つとしたが、これ
に限定されるものではなく複数以上であればよい。結合
器の数が多い場合ほどこの発明による効果は顕著であ
る。Although the number of couplers is five in the above embodiment, the number of couplers is not limited to five and may be more than one. The larger the number of couplers, the more remarkable the effect of the present invention.
以上のように、この発明によれば各結合器を結ぶ各主線
路の長さを異なる長さとし、かつ上記結合器と出力端子
との間に主線路の電気長を補正する補正線路を設けて構
成したので、広帯域な周波数にわたってVSWRの著しい劣
化はなく、出力波の振幅、位相変動の少ないものが得ら
れるという効果がある。また、第2の発明では、終端に
も補正線路を備えているので、電力を有効に利用でき
る。As described above, according to the present invention, the lengths of the main lines connecting the couplers are different from each other, and the correction line for correcting the electrical length of the main line is provided between the coupler and the output terminal. Since it is configured, VSWR is not significantly deteriorated over a wide band of frequencies, and the output wave amplitude and phase fluctuations are small. Further, in the second invention, the correction line is also provided at the terminal end, so that the electric power can be effectively used.
第1図はこの発明の一実施例による直列給電回路を示す
ブロック図、第2図はこの発明の他の一実施例による直
列給電回路のブロック図、第3図はこの発明の動作原理
を説明するための説明図、第4図はこの発明のVSWR特性
を示す特性図、第5図は従来の直列給電回路を示すブロ
ック図、第6図は従来の直列給電回路のVSWR特性を示す
特性図である。 図において、1〜5は結合器、6〜9は主線路、10は整
合終端、11〜16は補正線路、P0は入力端子、P1〜P6は出
力端子である。 なお、図中、同一符号は同一又は相当部分を示す。FIG. 1 is a block diagram showing a series power feeding circuit according to an embodiment of the present invention, FIG. 2 is a block diagram of a series power feeding circuit according to another embodiment of the present invention, and FIG. 4 is a characteristic diagram showing VSWR characteristics of the present invention, FIG. 5 is a block diagram showing a conventional series feeding circuit, and FIG. 6 is a characteristic diagram showing VSWR characteristics of a conventional series feeding circuit. Is. In the figure, 1 to 5 are couplers, 6 to 9 are main lines, 10 is a matching termination, 11 to 16 are correction lines, P 0 is an input terminal, and P 1 to P 6 are output terminals. In the drawings, the same reference numerals indicate the same or corresponding parts.
フロントページの続き (72)発明者 宮崎 守泰 神奈川県鎌倉市大船5丁目1番1号 三菱 電機株式会社情報電子研究所内 (72)発明者 竹内 紀雄 兵庫県尼崎市塚口本町8丁目1番1号 三 菱電機株式会社通信機製作所内 (56)参考文献 特開 昭51−57150(JP,A)Front page continuation (72) Inventor Moriyasu Miyazaki 5-1-1, Ofuna, Kamakura-shi, Kanagawa Mitsubishi Electric Corporation Information Electronics Laboratory (72) Inventor Norio Takeuchi 8-1-1 Tsukaguchihonmachi, Amagasaki City, Hyogo Prefecture Ryoden Co., Ltd., Communication Equipment Factory (56) Reference JP-A-51-57150 (JP, A)
Claims (2)
て終端に整合終端を備え、始端の結合器の入力端への入
射波を上記主線路を介して各結合器に供給し、順次必要
な電力の電磁波を上記各結合器に接続された出力端子か
ら取り出してアンテナ等の給電系に供給するとともに、
残った電力を上記整合終端に吸収するようにした直列給
電回路において、 上記各結合器を結ぶ各主線路の長さを、L0+2Ld(Ri−
0.5)(尚、L0は主線路の平均長さ、Ld≒1/4・λg、λ
gは使用する周波数の波長、Riは(0,1)区間の一様乱
数である。)に基づいて、それぞれ異なる長さに設定す
るとともに、上記各結合器と各出力端子との間に各主線
路の電気長を補正するための補正線路を設け、これら各
補正線路の長さMKは、次式、 (L1+M1)−M0=(L2+M2)−M1 =(L3+M3)−M2 ・ ・ ・ =(LK+1+MK+1−MK =L0 (尚、L,Mの添数字が大きくなるに従って入力端側より
遠くなる所の主線路及び補正線路を示している。) に従って設定されて成ることを特徴とする直列給電回
路。1. A plurality of couplers are connected in cascade through a main line and a matching termination is provided at the end, and an incident wave to the input end of the coupler at the beginning is supplied to each coupler through the main line. , While sequentially extracting the electromagnetic waves of the required power from the output terminals connected to each of the above-mentioned couplers and supplying them to a power feeding system such as an antenna,
In the series feed circuit configured to absorb the remaining power in the matching termination, the length of each main line connecting the above-mentioned couplers is set to L 0 + 2Ld (Ri-
0.5) (where L 0 is the average length of the main line, Ld ≈ 1/4 · λg, λ
g is the wavelength of the frequency used, and Ri is a uniform random number in the (0,1) interval. ), Set different lengths, and provide a correction line between each coupler and each output terminal to correct the electrical length of each main line. K is calculated by the following equation: (L 1 + M 1 ) −M 0 = (L 2 + M 2 ) −M 1 ═ (L 3 + M 3 ) −M 2・ ・ ・ ・ = (L K + 1 + M K + 1 −M A series feed circuit characterized by being set according to K = L 0 (note that the main line and the correction line are located farther from the input end side as the subscripts of L and M increase).
し、始端の結合器の入力端への入射波を上記主線路を介
して各結合器に供給し、順次必要な電力の電磁波を上記
各結合器に接続された出力端子から取り出してアンテナ
等の給電系に供給する直列給電回路において、 上記各結合器を結ぶ各主線路の長さを、L0+2Ld(Ri−
0.5)(尚、L0は主線路の平均長さ、Ld≒1/4・λg、λ
gは使用する周波数の波長、Riは(0,1)区間の一様乱
数である。)に基づいて、それぞれ異なる長さに設定す
るとともに、上記各結合器と各出力端子との間に各主線
路の電気長を補正するための各補正線路を設け、これら
各補正線路の長さMKは、次式、 (L1+M1)−M0=(L2+M2)−M1 =(L3+M3)−M2 ・ ・ ・ =(LK+1+MK+1)−MK =L0 (尚、L,Mの添数字が大きくなるに従って入力端子側よ
り遠くなる所の主線路及び補正線路を示している。) に従って設定され、 さらに、終端にも上記式で算出される補正線路を設けて
出力端を接続して成ることを特徴とする直列給電回路。2. A plurality of couplers are connected in cascade via a main line, and an incident wave to the input end of the coupler at the starting end is supplied to each coupler via the main line, and electromagnetic waves of necessary power are sequentially supplied. In a series feeding circuit that takes out from the output terminal connected to each coupler and supplies it to a feeding system such as an antenna, the length of each main line connecting each coupler is L 0 + 2Ld (Ri−
0.5) (where L 0 is the average length of the main line, Ld ≈ 1/4 · λg, λ
g is the wavelength of the frequency used, and Ri is a uniform random number in the (0,1) interval. ), Set different lengths, and provide each correction line for correcting the electrical length of each main line between each coupler and each output terminal, and set the length of each correction line. M K is calculated by the following equation: (L 1 + M 1 ) −M 0 = (L 2 + M 2 ) −M 1 = (L 3 + M 3 ) −M 2・ ・ ・ ・ = (L K + 1 + M K + 1 ) -M K = L 0 (Note that the main line and the correction line that are farther from the input terminal side are shown as the subscripts of L and M increase.) A series feeding circuit, characterized in that a calculated correction line is provided and the output ends are connected.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60231801A JPH0693568B2 (en) | 1985-10-17 | 1985-10-17 | Series power supply circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60231801A JPH0693568B2 (en) | 1985-10-17 | 1985-10-17 | Series power supply circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6292503A JPS6292503A (en) | 1987-04-28 |
| JPH0693568B2 true JPH0693568B2 (en) | 1994-11-16 |
Family
ID=16929233
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60231801A Expired - Lifetime JPH0693568B2 (en) | 1985-10-17 | 1985-10-17 | Series power supply circuit |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0693568B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2569792B2 (en) * | 1989-03-17 | 1997-01-08 | 三菱電機株式会社 | Beam forming circuit |
| JP2605628B2 (en) * | 1994-06-15 | 1997-04-30 | 日本電気株式会社 | Spatial diversity delay time difference correction device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5157150A (en) * | 1974-11-14 | 1976-05-19 | Mitsubishi Electric Corp | SHINKOHAKYUDEN AREIANTENA |
-
1985
- 1985-10-17 JP JP60231801A patent/JPH0693568B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6292503A (en) | 1987-04-28 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |