JPH02131032A - Transmission method for densely coupled signal - Google Patents
Transmission method for densely coupled signalInfo
- Publication number
- JPH02131032A JPH02131032A JP63284369A JP28436988A JPH02131032A JP H02131032 A JPH02131032 A JP H02131032A JP 63284369 A JP63284369 A JP 63284369A JP 28436988 A JP28436988 A JP 28436988A JP H02131032 A JPH02131032 A JP H02131032A
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- Prior art keywords
- signal
- cable
- electromagnetic field
- antenna
- conductors
- Prior art date
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Links
- 238000000034 method Methods 0.000 title claims description 14
- 230000005540 biological transmission Effects 0.000 title abstract description 11
- 239000004020 conductor Substances 0.000 claims abstract description 37
- 230000008054 signal transmission Effects 0.000 claims description 18
- 230000005672 electromagnetic field Effects 0.000 abstract description 21
- 230000005684 electric field Effects 0.000 abstract description 4
- 238000009413 insulation Methods 0.000 abstract 2
- 230000002238 attenuated effect Effects 0.000 abstract 1
- 230000008878 coupling Effects 0.000 abstract 1
- 238000010168 coupling process Methods 0.000 abstract 1
- 238000005859 coupling reaction Methods 0.000 abstract 1
- 230000008030 elimination Effects 0.000 abstract 1
- 238000003379 elimination reaction Methods 0.000 abstract 1
- 230000036039 immunity Effects 0.000 abstract 1
- 230000000644 propagated effect Effects 0.000 abstract 1
- 230000000694 effects Effects 0.000 description 3
- 102220111832 rs368482949 Human genes 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 239000012212 insulator Substances 0.000 description 2
- 238000012544 monitoring process Methods 0.000 description 2
- 238000009795 derivation Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000001131 transforming effect Effects 0.000 description 1
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は信号伝送方法に関し、より詳細には、トロリ
ー導体に沿って配設される信号ケーブルと、この信号ケ
ーブルと対向するアンテナ間で、移動機器への情報の伝
送および移動機器からの情報の伝送を非接触に行う密結
合信号伝送方法に関する。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a signal transmission method, and more specifically, between a signal cable arranged along a trolley conductor and an antenna facing the signal cable, The present invention relates to a tightly coupled signal transmission method for transmitting information to and from a mobile device in a non-contact manner.
[従来の技術]
組み立て工程における部品の自動搬送、製品の工程間自
動搬送あるいは劣悪な環境下の無人監視等に供される、
線上を移動する自動機器への電力の供給の多くはトロリ
ー導体の摺動により行われている。そしてまた、その移
動機器への制御情報の伝送および移動機器からの監視情
報等の伝送は、トロリー導体に沿って配設される単線、
平行導体あるいは漏洩同軸ケーブル等の開放伝送線路と
、この開放伝送線路と対向するアンテナ間の密結合信号
伝送装置により行われている。[Prior art] Used for automatic transportation of parts in assembly processes, automatic transportation of products between processes, unmanned monitoring in poor environments, etc.
Much of the power supply to automatic equipment moving on lines is accomplished by sliding trolley conductors. Furthermore, the transmission of control information to the mobile equipment and the transmission of monitoring information from the mobile equipment are carried out using a single wire disposed along the trolley conductor.
This is performed using a tightly coupled signal transmission device between an open transmission line such as a parallel conductor or a leaky coaxial cable, and an antenna facing the open transmission line.
以下、第5図を参照して従来の密結合信号伝送装置を説
明する。同図において、長尺状の配線レール本体20に
は互いに平行する3本の講部2 22.22’が形成さ
れたハンガー21が固定され、この溝部22には、電気
機器本体27に対して電力を供給するための2本のトロ
リー導体23が絶縁体24を介して固定されている。ま
た、いま一つの溝部22′には大径部に漏洩同軸ケーブ
ル等で形成される信号漏洩線41が埋設され、小径部に
吊線43が埋設される瓢箪形のシース42が固定されて
いる。Hereinafter, a conventional tightly coupled signal transmission device will be explained with reference to FIG. In the figure, a hanger 21 in which three parallel rails 22, 22' are formed is fixed to a long wiring rail main body 20, and a hanger 21 in which three parallel rails 22, 22' are formed is fixed to the long wiring rail main body 20. Two trolley conductors 23 for supplying power are fixed via an insulator 24. Further, in the other groove 22', a signal leakage line 41 formed of a leaky coaxial cable or the like is buried in the large diameter part, and a gourd-shaped sheath 42 in which a hanging wire 43 is buried in the small diameter part is fixed.
さらに、トロリー導体23には、電気機器の本体27に
設けられたバネ26によって外方に突出する付勢力が与
えられたブラシ25が電気接触されていて、信号漏洩線
41と対向する位置には、所定距離を保って支持部材3
1を介してループアンテナ30が設けられている。Furthermore, the trolley conductor 23 is electrically contacted with a brush 25 which is biased to protrude outward by a spring 26 provided on the main body 27 of the electrical equipment, and is located at a position facing the signal leakage line 41. , the support member 3 while maintaining a predetermined distance.
A loop antenna 30 is provided via 1.
したがって、電気機器本体27への電力供給が2本のブ
ラシ25を介して2本のトロリー導体23によってなさ
れ、信号漏洩線41に供給される信号がループアンテナ
30を介して電気機器本体27へ、また電気機器本体2
7からの信号がループアンテナ30を介して信号漏洩線
41に供給されることによって信号伝送がなされるもの
である。Therefore, power is supplied to the electrical equipment main body 27 by the two trolley conductors 23 via the two brushes 25, and the signal supplied to the signal leakage line 41 is transmitted to the electrical equipment main body 27 via the loop antenna 30. Also, the electrical equipment body 2
Signal transmission is performed by supplying the signal from 7 to the signal leakage line 41 via the loop antenna 30.
ところが、この種の装置が設置される環境は本来的に雑
音レベルが高いことと、トロリー導体を摺動する際の雑
音のため、従来の装置では移動する電気機器との安定な
信号伝送が行えないという問題があった。この問題は電
磁界強度を高くすることにより解決されるのであるが、
電波法上の規定である微弱無線局(アンテナから3mの
離隔地点で500μV/m=54dBμV/m以下の電
界強度)の規定を満たすこともまた困難であった。However, due to the inherently high noise level of the environment in which this type of equipment is installed and the noise generated when the trolley conductor slides, conventional equipment cannot perform stable signal transmission with moving electrical equipment. The problem was that there was no. This problem can be solved by increasing the electromagnetic field strength, but
It was also difficult to meet the regulations of the Radio Law for weak radio stations (field strength of 500 μV/m = 54 dBμV/m or less at a point 3 meters away from the antenna).
[発明が解決しようとする課題]
この発明は、このような点に鑑みなされたものであって
、外部雑音に強く、電波法上の規定を満たしながら伝送
距離において充分に高い電磁界強度を有し、さらに電気
機器の移動によって受信電界強度が変化しない密結合信
号伝送方法を提供することにある。[Problems to be Solved by the Invention] The present invention has been devised in view of the above-mentioned points. Another object of the present invention is to provide a tightly coupled signal transmission method in which the received electric field strength does not change due to movement of electrical equipment.
[問題点を解決するための手段および作用]この発明の
密結合信号伝送方法は、移動する電気機器に対して摺動
方式で電力を供給する配線レールに沿って信号ケーブル
が配設され、該信号ケーブルに対して非接触状態で電気
的に結合するアンテナを介して前記電気機器に対して情
報信号を送信もしくは同電気機器からの情報信号を受信
する信号伝送方法において、前記信号ケーブルは絶縁導
体2本を対撚りしてなり、該絶縁導体間を信号が伝搬す
る際に形成されるTEMモードに前記アンテナを結合さ
せるようにしたことを特徴とするものである。[Means and effects for solving the problem] In the tightly coupled signal transmission method of the present invention, a signal cable is arranged along a wiring rail that supplies power to moving electrical equipment in a sliding manner. In a signal transmission method, the signal cable is an insulated conductor, and the signal cable is an insulated conductor. It is characterized in that it is made by twisting two wires in pairs, and the antenna is coupled to a TEM mode that is formed when a signal propagates between the insulated conductors.
上記のように対撚型の信号ケーブルを用いることにより
、ケーブル周囲に形成される電磁界は相殺、微弱化され
、外部空間への電磁界発生を抑止できる。また、アンテ
ナとしてループアンテナ2個を前記絶縁導体の撚りピッ
チの(2n+1)/4倍の間隔にて配置したものを使用
することにより、信号ケーブルの長さ方向の電磁界強度
を一定にできる。By using the twisted pair signal cable as described above, the electromagnetic field formed around the cable is canceled out and weakened, and generation of the electromagnetic field into the external space can be suppressed. Furthermore, by using two loop antennas arranged at an interval of (2n+1)/4 times the twisting pitch of the insulated conductors, the electromagnetic field strength in the length direction of the signal cable can be made constant.
[実 施 例] 以下、この発明の一実施例を説明する。[Example] An embodiment of this invention will be described below.
初めに、第1図を参照して実施例の構造を説明する。同
図において、長尺状の配線レール本体20には互いに平
行する3本の溝部22,22゜22′が形成されたハン
ガー21が固定され、このハンガー21の溝部22には
、電気機器本体27に対して電力を供給するための2本
のトロリー導体23が絶縁体24を介して固定されてい
る。また、いま一つの溝部22”には平行導体を一定の
ピッチで撚り合わせた対撚りケーブル11を埋設した瓢
箪形のシース42が固定されている。First, the structure of the embodiment will be explained with reference to FIG. In the figure, a hanger 21 in which three mutually parallel grooves 22, 22° 22' are formed is fixed to a long wiring rail main body 20, and an electrical equipment main body 27 is provided in the grooves 22 of the hanger 21. Two trolley conductors 23 for supplying power to are fixed via an insulator 24. Further, a gourd-shaped sheath 42 in which a twisted pair cable 11 made of parallel conductors twisted at a constant pitch is embedded is fixed in the other groove 22''.
さらに、トロリー導体23には、電気機器本体27に設
けられたバネ26によって外方に突出する付勢力が与え
られたブラシ25が電気接触されていて、対撚りケーブ
ル11の対向位置には、所定距離を保って支持部材31
を介して一対のループアンテナ32.32’が設けられ
ている。Furthermore, the trolley conductor 23 is electrically contacted with a brush 25 which is given an outward protruding force by a spring 26 provided on the electrical equipment main body 27, and is placed in a predetermined position opposite to the twisted pair cable 11. Support member 31 while keeping a distance
A pair of loop antennas 32, 32' are provided via the antenna.
したがって、電気機器本体27への電力供給は一対のブ
ラシ25を介して一対のトロリー導体23によってなさ
れ、対撚りケーブル11に供給される信号がアンテナ3
2.32“を介して電気機器本体27へ、また電気機器
本体27からの信号がアンテナ32.32’を介して対
撚りケーブル11に供給されることによって信号伝送が
なされるようになっている。Therefore, power is supplied to the electrical equipment body 27 by the pair of trolley conductors 23 via the pair of brushes 25, and the signal supplied to the twisted pair cable 11 is transmitted to the antenna 3.
2.32'' to the electrical equipment main body 27, and signals from the electrical equipment main body 27 are supplied to the twisted pair cable 11 via the antenna 32.32', thereby performing signal transmission. .
続いて、第2図及至第4図を参照して実施例をさらに詳
細に説明する。Next, the embodiment will be described in further detail with reference to FIGS. 2 to 4.
第2図は平行導体14.14”がその軸に直角な方向に
発生ずる電界Eおよび磁界H1すなわちTEM波(tr
ansverse
electromagnetic wave)を説明
している。ここで、平行導体14.14’の開口面に垂
直な方向、すなわちループアンテナ32の方向を基準(
θ=0)にすると、平行導体14.14’の単位線分が
その周囲に発生する磁界強度ΔH3□は、
ΔH3゜−A(r)・B(q)・CO8θ・・・(1)
ただし、平行導体14.14’の単位線分かの距離をA
(r)、平行導体14.14’の単位線分のヘルツ双極
能率をB (q)とする。Figure 2 shows the electric field E and magnetic field H1, that is, the TEM wave (tr
anverse electromagnetic wave). Here, the direction perpendicular to the aperture plane of the parallel conductors 14, 14', that is, the direction of the loop antenna 32 is used as a reference (
When θ=0), the magnetic field strength ΔH3□ generated around the unit line segment of the parallel conductor 14.14' is ΔH3゜-A(r)・B(q)・CO8θ...(1)
However, the distance of the unit line segment of parallel conductor 14.14' is A
(r), and the Hertzian dipole efficiency of the unit line segment of the parallel conductor 14, 14' is B (q).
で与えられ、この式より、平行導体を一定のピッチで撚
り合わせるときは、電磁界が軸方向に正弦状に変化する
ことが予想される。From this equation, it is predicted that when parallel conductors are twisted at a constant pitch, the electromagnetic field changes sinusoidally in the axial direction.
次に、第3図を参照して対撚りケーブル11の周囲に形
成される電磁界を説明する。同図において、対撚りケー
ブル11の平行導体14.14’は一定のピッチPで撚
り合わされており、図示するように平行導体14.14
’の開口面がループアンテナ32と対面する位置を起点
としてループアンテナ32の軸方向の偏位をZ、撚りピ
ッチをPとすると、平行導体14.14’の開口面がア
ンテナ32となす角度αは、
α=2πZ/P・・・・・・・・・・・・(2)である
。そこで、ループアンテナ32の距離における平行導体
14.14’の全線分からの磁界強度は(1)式を利用
して、
H32= f A (r) ・B (Q)・cos
(θ+2πZ/P)dθ・・・・(3)となる。ここで
、cos (θ+2 yr Z / P )cos θ
−c o s (2πZ/P) −s i
n (2’rZ/P )・sinθなる数学公式によ
り(3)式を変形すると、
H32=J’ A (r) ・B (q) ・COSθ
−c o s (2πZ/P)dθ
、FA(r) ・B (q)−sinθ−s i n
(2πZ/P)dθ−−−(4)が得られる。式中の関
数B (q)は信号に比例する量であるので今は一定と
考えることができ、また関数A (r)はθに対し対称
であるので、上記(4)式の右辺の第2項はOになる。Next, the electromagnetic field formed around the twisted pair cable 11 will be explained with reference to FIG. In the figure, the parallel conductors 14.14' of the twisted pair cable 11 are twisted at a constant pitch P, and as shown in the figure, the parallel conductors 14.14'
If the axial deviation of the loop antenna 32 is Z and the twisting pitch is P, starting from the position where the aperture of the parallel conductor 14.14' faces the loop antenna 32, then the angle α between the aperture of the parallel conductor 14 and 14' and the antenna 32 is is α=2πZ/P (2). Therefore, using equation (1), the magnetic field strength from all segments of the parallel conductor 14, 14' at the distance of the loop antenna 32 is calculated as follows: H32= f A (r) ・B (Q) ・cos
(θ+2πZ/P)dθ (3). Here, cos (θ+2 yr Z / P) cos θ
-c o s (2πZ/P) -s i
Transforming equation (3) using the mathematical formula n (2'rZ/P)・sinθ, H32=J' A (r) ・B (q) ・COSθ
-cos (2πZ/P)dθ, FA(r) ・B (q)-sinθ-sin
(2πZ/P)dθ---(4) is obtained. Since the function B (q) in the equation is a quantity proportional to the signal, it can be considered constant for now, and since the function A (r) is symmetrical with respect to θ, the right-hand side of the above equation (4) The second term becomes O.
したがって、Cを定数とし、
H32−J’A (r) ・ B (q)
・ cos θ−cos (2πZ/P)dθ
=C−cos (2π・Z/P)
が導かれ、対撚りケーブルの周囲に形成される電磁界が
軸方向に正弦状に変化することが理解される。Therefore, with C as a constant, H32-J'A (r) ・B (q)
・ cos θ−cos (2πZ/P) dθ = C−cos (2π・Z/P) is derived, and it is understood that the electromagnetic field formed around the twisted pair cable changes sinusoidally in the axial direction. Ru.
さて、このように電磁界が軸方向に正弦状に変化すると
、撚りピッチPより充分に遠方の電磁界はP/2隔たっ
た線分からの互いに逆位相の電磁界により相殺され、急
速に電磁界強度が減衰することになる。この電磁界特性
を従来例の電磁界特性と共に第4図に示す。Now, when the electromagnetic field changes sinusoidally in the axial direction in this way, the electromagnetic field sufficiently far away from the twist pitch P is canceled out by the electromagnetic fields with mutually opposite phases from line segments separated by P/2, and the electromagnetic field rapidly changes. The intensity will be reduced. This electromagnetic field characteristic is shown in FIG. 4 together with the electromagnetic field characteristic of the conventional example.
以上の説明により、対撚りケーブルが伝送距離にて充分
な強度の、かつ遠方にて急速に減衰する電磁界を形成す
ること、また同様な理由により、遠方から到来する雑音
が対撚りケーブルの全線分にて相殺され、雑音除去能力
の高い伝送系が形成され得ること、さらに平行導体14
.14″の撚り合わせにより、アース系との容量アンバ
ランスがなく安定な伝送系が形成され得ることが容易に
理解される。From the above explanation, it is clear that the twisted pair cable forms an electromagnetic field that is sufficiently strong over the transmission distance and rapidly attenuates at a distance, and for the same reason, the noise coming from a long distance is transmitted over the entire length of the twisted pair cable. In addition, the parallel conductor 14
.. It is easily understood that by twisting the strands of 14", a stable transmission system can be formed without a capacitance imbalance with the ground system.
しかしながら、軸方向の移動に対し電磁界が正弦状に変
化することは、ループアンテナの位置によっては信号の
伝送が行われないことを意味しており、この方法を直ち
に信号伝送に供することはできない。そこで、この発明
は対撚りケーブル11の撚りピッチの(2n + 1
) / 4倍(n0.1,2. ・・ )の間隔にて
ループアンテナ32.32’を2個配置することによっ
て、この問題を解決せんとするものである。なお、nの
値は撚りピッチあるいはループアンテナ32゜32“相
互の干渉を考慮して任意に決定することができる。However, the fact that the electromagnetic field changes sinusoidally with respect to movement in the axial direction means that signal transmission may not occur depending on the position of the loop antenna, and this method cannot be used immediately for signal transmission. . Therefore, the present invention has been developed so that the twist pitch of the twisted pair cable 11 is (2n + 1
) / 4 times (n0.1, 2. . . ) by arranging two loop antennas 32, 32' at an interval of n0.1, 2, . . . to solve this problem. Note that the value of n can be arbitrarily determined in consideration of the twisting pitch or the mutual interference of the loop antennas.
さらに説明を続ける。上記(5)式の導出と同様にして
、ループアンテナ32′の磁界強度H32・を求めると
、
H32= =C−c o s (2πZ/P+π/2)
C−s i n (2πZ/P) ・・・(6)となる
。この磁界を検出するループアンテナ32°の出力は移
相器15によりπ/2あるいはπ/2移相され、他方の
ループアンテナ32の出力と混合され、端子Tに出力さ
れている。したがって、端子Tに生ずる受信電圧■は次
式で表される。Let's continue the explanation. Similarly to the derivation of equation (5) above, the magnetic field strength H32 of the loop antenna 32' is determined as follows: H32= =C-cos (2πZ/P+π/2)
C-s in (2πZ/P) (6). The output of the loop antenna 32° that detects this magnetic field is phase-shifted by π/2 or π/2 by the phase shifter 15, mixed with the output of the other loop antenna 32, and output to the terminal T. Therefore, the received voltage ■ generated at the terminal T is expressed by the following equation.
V=C(cos (2rZ/P)
± j −sin (2’rZ/P) )
・ ・ 17)この(7)式は、Zの変化によ
り、すなわちループアンテナ32.32’の移動に伴っ
て、受信電圧■の位相が変化するもののその振幅は一定
であることを表している。これにより、この発明は安定
な信号伝送が可能であるばかりか、位相の変化の検出に
より電気機器の位置の判定をも行うことができるのであ
る。V=C(cos (2rZ/P) ± j -sin (2'rZ/P))
. . . 17) Equation (7) expresses that although the phase of the received voltage ■ changes as Z changes, that is, as the loop antenna 32, 32' moves, the amplitude remains constant. As a result, the present invention not only enables stable signal transmission, but also allows the position of electrical equipment to be determined by detecting changes in phase.
なお、上記のように一方のループアンテナより得られる
信号を移相し加算する方法に代え、双方のループアンテ
ナより得られる信号を検波手段等により絶対値を生成し
、加算することによっても同様目的を達成することが可
能である。すなわち、
VOcICO52πZ/P
+1sin2πZ/Pl ・・・・(8)は比較的一
定の振幅を有しており、簡素な構成により電気機器本体
27の位置に係わらない安定な信号伝送を行うことが可
能である。In addition, instead of the method of phase-shifting and adding the signals obtained from one loop antenna as described above, the same purpose can also be achieved by generating the absolute value of the signals obtained from both loop antennas using a detection means etc. and adding them. It is possible to achieve this. That is, VOcICO52πZ/P +1sin2πZ/Pl (8) has a relatively constant amplitude, and with a simple configuration it is possible to perform stable signal transmission regardless of the position of the electrical equipment main body 27. be.
[発明の効果]
以上述べたようにこの発明によれば、
(1)伝送距離において充分な電界強度が得られ、遠方
では急速に減衰する電磁界特性が得られる。[Effects of the Invention] As described above, according to the present invention, (1) Sufficient electric field strength can be obtained over a transmission distance, and electromagnetic field characteristics can be obtained that rapidly attenuate at a long distance.
(2)対撚りケーブルとアース系との容量アンバランス
かないため安定な信号伝送が可能である。(2) Stable signal transmission is possible because there is no capacity imbalance between the twisted pair cable and the ground system.
(3)近接するトロリー導体からの誘導電圧、その他の
外部雑音が相殺される。(3) Induced voltages from adjacent trolley conductors and other external noises are canceled out.
(4)受信信号の位相変化より電気機器の移動距離を知
ることができる。(4) The moving distance of the electrical equipment can be determined from the phase change of the received signal.
という顕著な効果を奏する密結合伝送方法を提供するこ
とができる。It is possible to provide a tightly coupled transmission method that achieves this remarkable effect.
第1図はこの発明の一実施例の構造を説明する断面図、
第2図は平行導体が形成するTEM波を説明する図、
第3図は対撚りケーブルとループアンテナとの幾何学的
関係を説明する図、
第4図は電磁界特性図、
第5図は従来例の構造を説明する断面図である。
11 ・
14、 14’
15 ・
23 ・
27 ・
32、 32’Figure 1 is a cross-sectional view explaining the structure of an embodiment of the present invention, Figure 2 is a diagram explaining TEM waves formed by parallel conductors, and Figure 3 is the geometric relationship between the twisted pair cable and the loop antenna. FIG. 4 is an electromagnetic field characteristic diagram, and FIG. 5 is a cross-sectional view explaining the structure of a conventional example. 11 ・ 14, 14' 15 ・ 23 ・ 27 ・ 32, 32'
Claims (2)
する配線レールに沿って信号ケーブルが配設され、該信
号ケーブルに対して非接触状態で電気的に結合するアン
テナを介して前記電気機器に対して情報信号を送信もし
くは同電気機器からの情報信号を受信する信号伝送方法
において、前記信号ケーブルは絶縁導体2本を対撚りし
てなり、該絶縁導体間を信号が伝搬する際に形成される
TEMモードに前記アンテナを結合させることを特徴と
する密結合信号伝送方法。(1) A signal cable is arranged along a wiring rail that supplies power to moving electrical equipment in a sliding manner, and the signal cable is connected to the signal cable through an antenna that is electrically coupled to the signal cable in a non-contact state. In a signal transmission method for transmitting an information signal to or receiving an information signal from an electrical device, the signal cable is made up of two insulated conductors twisted in pairs, and when the signal propagates between the insulated conductors, A tightly coupled signal transmission method, characterized in that the antenna is coupled to a TEM mode formed in a TEM mode.
導体の撚りピッチの(2n+1)/4倍の間隔にて配置
してなる請求項1記載の密結合信号伝送方法。(2) The tightly coupled signal transmission method according to claim 1, wherein the antenna comprises two loop antennas arranged at an interval of (2n+1)/4 times the twisting pitch of the insulated conductor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63284369A JPH0734553B2 (en) | 1988-11-10 | 1988-11-10 | Mobile electrical equipment signal transmission method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63284369A JPH0734553B2 (en) | 1988-11-10 | 1988-11-10 | Mobile electrical equipment signal transmission method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH02131032A true JPH02131032A (en) | 1990-05-18 |
JPH0734553B2 JPH0734553B2 (en) | 1995-04-12 |
Family
ID=17677690
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63284369A Expired - Lifetime JPH0734553B2 (en) | 1988-11-10 | 1988-11-10 | Mobile electrical equipment signal transmission method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0734553B2 (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0439752U (en) * | 1990-07-31 | 1992-04-03 | ||
JP2008085890A (en) * | 2006-09-28 | 2008-04-10 | Sumitomo Electric System Solutions Co Ltd | Radio transmission system and mobile station therefor |
WO2014049932A1 (en) * | 2012-09-26 | 2014-04-03 | 株式会社デンソー | Communication system |
DE202009018979U1 (en) | 2008-10-01 | 2015-02-09 | Borgwarner Inc. | Wastegate with variable flow |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS4850626A (en) * | 1971-10-25 | 1973-07-17 | ||
JPS52137915A (en) * | 1976-05-14 | 1977-11-17 | Sumitomo Electric Ind Ltd | Data transmission system |
JPS56150113U (en) * | 1980-04-09 | 1981-11-11 |
-
1988
- 1988-11-10 JP JP63284369A patent/JPH0734553B2/en not_active Expired - Lifetime
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS4850626A (en) * | 1971-10-25 | 1973-07-17 | ||
JPS52137915A (en) * | 1976-05-14 | 1977-11-17 | Sumitomo Electric Ind Ltd | Data transmission system |
JPS56150113U (en) * | 1980-04-09 | 1981-11-11 |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0439752U (en) * | 1990-07-31 | 1992-04-03 | ||
JP2008085890A (en) * | 2006-09-28 | 2008-04-10 | Sumitomo Electric System Solutions Co Ltd | Radio transmission system and mobile station therefor |
DE202009018979U1 (en) | 2008-10-01 | 2015-02-09 | Borgwarner Inc. | Wastegate with variable flow |
WO2014049932A1 (en) * | 2012-09-26 | 2014-04-03 | 株式会社デンソー | Communication system |
JP2014068220A (en) * | 2012-09-26 | 2014-04-17 | Nippon Soken Inc | Communication system |
US9762294B2 (en) | 2012-09-26 | 2017-09-12 | Denso Corporation | Communication system |
Also Published As
Publication number | Publication date |
---|---|
JPH0734553B2 (en) | 1995-04-12 |
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