JPS6118988B2 - - Google Patents
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- Publication number
- JPS6118988B2 JPS6118988B2 JP9451078A JP9451078A JPS6118988B2 JP S6118988 B2 JPS6118988 B2 JP S6118988B2 JP 9451078 A JP9451078 A JP 9451078A JP 9451078 A JP9451078 A JP 9451078A JP S6118988 B2 JPS6118988 B2 JP S6118988B2
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- JP
- Japan
- Prior art keywords
- speed
- frequency
- wire
- measuring device
- wave
- Prior art date
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- Expired
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- 238000005259 measurement Methods 0.000 claims description 8
- 230000010363 phase shift Effects 0.000 claims description 5
- 230000003321 amplification Effects 0.000 claims description 3
- 238000003199 nucleic acid amplification method Methods 0.000 claims description 3
- 239000000284 extract Substances 0.000 claims description 2
- 230000005540 biological transmission Effects 0.000 description 11
- 238000000034 method Methods 0.000 description 8
- 238000010586 diagram Methods 0.000 description 7
- 238000001514 detection method Methods 0.000 description 5
- 238000010168 coupling process Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 2
- 230000006698 induction Effects 0.000 description 2
- 230000001939 inductive effect Effects 0.000 description 2
- 230000005856 abnormality Effects 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 238000011109 contamination Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 239000000428 dust Substances 0.000 description 1
- 238000010297 mechanical methods and process Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 230000001629 suppression Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
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Description
【発明の詳細な説明】
本発明は一定走行路上を走行するクレーン、台
車、車両、列車などの走行速度を地上固定側(以
下地上局という)にて計測する装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device for measuring the traveling speed of a crane, a bogie, a vehicle, a train, etc. traveling on a fixed traveling path at a fixed ground station (hereinafter referred to as a ground station).
従来は移動体の速度を計測するには光学式、電
磁波方式、超音波方式、電磁結合方式、誘導結合
方式、機械方式に大別される諸方式があつてそれ
ぞれ特徴があり、使用目的に応じてこれらの方式
の1つまたは複数の組合わせが実用されている。
これらのうち特に誘導結合(を用いる)方式は無
接触で塵埃、降雨、降雪、汚損の多い環境でも使
用できるというすぐれた特徴があるので種々の形
式のものが実用されている。さらにこのうち走行
路側(地上局)にて計測するものは走行路上に一
定距離で2つのループコイルを設置し、これに移
動体から特定周波数の信号波を送出結合させ、地
上局ではこの信号を検出して2ループ間の通過所
要時間を計測し速度を演算するものであるが、ル
ープ地点における信号検知は振幅成分で判定する
ため移動体と走行路(ループ)間の間隔の変化や
雑音の混入があると移動体の位置検出誤差の変動
が大きくかつ誤り検出があるなど信頼性に欠ける
という問題があつた。本発明はこのような欠点を
除くために行つたもので、以下実施例によつて詳
細に説明する。 Conventionally, there are various methods for measuring the speed of a moving object, including optical methods, electromagnetic wave methods, ultrasonic methods, electromagnetic coupling methods, inductive coupling methods, and mechanical methods, each with its own characteristics, depending on the purpose of use. One or more combinations of these methods have been put into practice.
Among these, the inductive coupling method in particular has the excellent feature of being non-contact and usable even in environments with a lot of dust, rain, snow, and dirt, so various types are in practical use. Furthermore, among these, to measure on the road side (ground station), two loop coils are installed at a certain distance on the road, and a signal wave of a specific frequency is sent from the mobile object to these and combined, and the ground station receives this signal. The method detects the signal, measures the time required to pass between two loops, and calculates the speed. However, since signal detection at the loop point is determined based on the amplitude component, it is difficult to detect changes in the distance between the moving object and the traveling route (loop) and noise. If there is contamination, there is a problem of a lack of reliability, such as large fluctuations in the position detection error of the moving object and false detections. The present invention was made to eliminate such drawbacks, and will be explained in detail below using Examples.
第1図は本発明による走行速度計測装置の基本
的な構成例図で、移動体走行路に沿つて速度計測
区間に敷設した交差形平行2線式誘導線1とその
一端に結合器4を介して接続した速度計測器6、
誘導線の他端に接続した終端低抗器3、移動体に
載置したアンテナ8と1、2の2周波変調信
号の適当出力の送信機から成立つている。なお実
際の1、2は誘導無線周波帯から選ばれる。 FIG. 1 is a diagram showing an example of the basic configuration of a traveling speed measuring device according to the present invention, in which a cross-shaped parallel two-wire guide wire 1 is laid in a speed measuring section along a traveling path of a moving object, and a coupler 4 is installed at one end of the wire. A speed measuring device 6 connected via
It consists of a terminating resistor 3 connected to the other end of the guide wire, an antenna 8 mounted on a moving body, and transmitters 1 and 2 which output appropriate outputs of two-frequency modulated signals. Note that 1 and 2 are actually selected from the induction radio frequency band.
第2図は本発明の他の実施例の基本的な構成図
で、移動体から地上局へのデータ伝送も同時に行
われるように構成したもので、記号は第1図と共
通である。なお2はこの速度計測区間内には交差
が施されていない平行2線式誘導線で誘導線1と
平行に敷設してある。5は結合器、7はデータ復
調器を含む速度計測器、10は移動体側の2周波
信号送信機で、データ信号でたとえばπ相の位相
偏移変調(PSKという)された周波数1と無変
調の2の各波適当出力をアンテナ8を通じて誘
導線1および2に送出する。この1と2の間
には第1図、第2図の両場合共m1/(m−
1)=2の関係がありmは2以上の整数とす
る。(速度計測区間は走行路に沿つて何個所設け
てもよく誘導線2はすべての個所に共用でき
る。)
第3図は第1図でおよび第2図で7として示し
た速度計測器の回路構成例図で、破線で表わした
部分は第1図の6には含まれない。11,12は
それぞれ入力から2波、1波を分離抽出する
帯域波器(BPF)、13,14は増幅と振幅制
限器(A・L)、15は周波数2逓倍器、16は
位相弁別器(PD)、17は方形波変換器(W)、
18はクロツク(パルス)発生器(C)、19は
クロツクの計数器(カウンタという)、20は速
度情報出力器、21はデータ復調器、Vputは速
度情報出力、Dioはデータ入力、Dputはデータ復
調出力である。 FIG. 2 is a basic configuration diagram of another embodiment of the present invention, which is configured so that data transmission from the mobile unit to the ground station is performed at the same time, and the symbols are the same as those in FIG. 1. Note that 2 is a parallel two-wire guide wire that does not intersect within this speed measurement section and is laid parallel to the guide wire 1. 5 is a coupler, 7 is a speed measuring device including a data demodulator, and 10 is a two-frequency signal transmitter on the moving object side, which uses data signals such as π-phase phase shift keying (PSK) frequency 1 and unmodulated frequency 1 . The appropriate output of each of the two waves is sent to the guide wires 1 and 2 through the antenna 8. Between 1 and 2 , m 1 /(m-
1) = 2 , and m is an integer of 2 or more. (Speed measurement sections may be provided at any number of locations along the running route, and the guide line 2 can be shared by all locations.) Figure 3 shows the circuit of the speed measurement device shown as 7 in Figures 1 and 2. In the configuration example diagram, the portion indicated by a broken line is not included in 6 in FIG. 11 and 12 are bandpass filters (BPF) that separate and extract two waves and one wave from the input, 13 and 14 are amplification and amplitude limiters (A/L), 15 is a frequency doubler, and 16 is a phase discriminator. (PD), 17 is a square wave converter (W),
18 is a clock (pulse) generator (C), 19 is a clock counter (referred to as a counter), 20 is a speed information output device, 21 is a data demodulator, V put is a speed information output, D io is a data input, D put is data demodulation output.
第4図は第1図および第2図の構成における各
部の動作波形図で、これを用いて第1図〜第3図
の動作を次に説明する。まず移動体側から1、
2の2周波の信号が誘導線1および2を介して
地上局に誘導伝送されるが、誘導線1は2つの定
点S1,S2において交差が施されているので、速度
計測器6または7への入力信号波の位相はアンテ
ナ8の位置がS1,S2の位置を通過する度に180゜
異るすなわち位相が反転する。また第2図の誘導
線2による速度計測器7への入力にはこのような
アンテナの位置による位相反転は生じない。 FIG. 4 is an operation waveform diagram of each part in the configurations of FIGS. 1 and 2, and the operations of FIGS. 1 to 3 will be explained using this chart. First , from the moving object side,
2 is guided and transmitted to the ground station via the guide wires 1 and 2, but since the guide wire 1 is crossed at two fixed points S 1 and S 2 , the speed measuring device 6 or The phase of the input signal wave to the antenna 7 differs by 180 degrees each time the antenna 8 passes through the positions S 1 and S 2 , that is, the phase is reversed. Further, such phase inversion due to the position of the antenna does not occur in the input to the speed measuring device 7 through the guide wire 2 shown in FIG.
次に第3図においては誘導線1よりの入力は
BPF11に、誘導線2よりの入力はBPF12にそ
れぞれ入力する第2図の場合を考えるが、第1図
の場合には誘導線1よりの入力はBPF11、BPF
12の双方に入力する。いずれの場合にもBPF1
1は入力から2波成分を、BPF12は入力から
1波成分をそれぞれ選択抽出し第4図b波形お
よびa波形の出力を得るが、これらを次段のA・
L13およびA・L14にてそれぞれ増幅しかつ
一定振幅に制限する。第3図はm=2と仮定した
場合でA・L14の出力の1波は周波数2逓倍
器15で21にされ21=2となつた出力
が位相弁別器PD16の一方の入力に基準位相波
として送られる。これは第4図にc波形で示して
ある。この逓倍器15への入力1波は上記のよ
うにS1,S2の各地点では位相が180゜(π相)変
化したものであるが周波数を2逓倍することによ
つて連続位相波に変えられるからこれを基準位相
波とするわけである。なおmが2以外であつても
2と1の差周波数を取出しm逓倍すれば基準
位相波として用いることができる。 Next, in Figure 3, the input from guide wire 1 is
Consider the case in Figure 2 where the input from guide wire 2 is input to BPF 11 and BPF 12, but in the case of Figure 1, the input from guide wire 1 is input to BPF 11 and BPF 12.
12. BPF1 in both cases
1 receives the 2- wave component from the input, BPF12 receives the 2-wave component from the input.
Each of the first wave components is selectively extracted to obtain the outputs of waveforms b and a in Figure 4, which are used in the next stage A and A.
The signal is amplified at L13 and A/L14 and limited to a constant amplitude. Figure 3 shows the case where m = 2, and one wave of the output of A.L14 is made 2 1 by the frequency doubler 15, and the output that becomes 2 1 = 2 is used as a reference for one input of the phase discriminator PD 16. Sent as a phase wave. This is shown in FIG. 4 as waveform c. As mentioned above, the single wave input to the multiplier 15 has a phase change of 180° (π phase) at each point S 1 and S 2 , but by doubling the frequency, it becomes a continuous phase wave. Since it can be changed, this is used as the reference phase wave. Note that even if m is other than 2,
If the difference frequency between 2 and 1 is extracted and multiplied by m, it can be used as a reference phase wave.
さて位相弁別器PD16の2つの入力はこのc
波形とA・L13よりの2波であつてこの2入
力間の位相弁別が行われ、同相ならたとえば負、
逆相なら正の出力が次段W17に送られる。この
出力は第4図に波形で示してあるがこの極性は逆
であつてもよい。なお第3図のBPF11,12、
A・L13,14等には予測できない固有の位相
回転量を持つているから、PD16の入力には位
相補正回路が設けてあり理想的な判別結果が得ら
れるように補正を行つておくことは言うまでもな
い。PD16よりのd波形は方形波変換器W17
において低域波器に通された後方形波に変換さ
れたe波形をカウンタ19と速度情報出力器20
に出力する。カウンタ19にはクロツク発生器1
8からクロツクパルスが入力していてe波形のH
レベルの間クロツクを計数する。これが第4図の
j波形である。なおこのカウンタ19はe波形の
立上り(L→H)変換点を検知してリセツトされ
その後クロツクを計数するように構成してある。
他方速度情報出力器20ではe波形の立下り(H
→L)変換点を検出してカウンタ19の計数値を
読み込み、あらかじめ設定されたS1とS2間の距離
値を用いてこれらから移動体の速度を演算しKm/
Hなどで表わした速度値Vputを出力する。第4図
のg波形は移動体が第1図において右方向Srに
走行したとき、またh波形は左方向にSlに走行し
たときそれぞれの出力動作を示すものである。 Now, the two inputs of the phase discriminator PD16 are this c
Phase discrimination between these two inputs is performed using the waveform and the two waves from A and L13, and if they are in phase, for example, negative,
If the phase is opposite, a positive output is sent to the next stage W17. Although this output is shown as a waveform in FIG. 4, the polarity may be reversed. In addition, BPF11, 12 in Figure 3,
Since A/L13, 14, etc. have a unique amount of phase rotation that cannot be predicted, it is necessary to install a phase correction circuit at the input of PD16 and perform correction to obtain ideal discrimination results. Needless to say. The d waveform from PD16 is converted to square wave converter W17.
A counter 19 and a speed information output device 20 output the e-waveform converted into a backward waveform passed through a low-frequency wave generator.
Output to. The counter 19 has a clock generator 1.
The clock pulse is input from 8 and the e waveform is H.
Count clocks between levels. This is the j waveform in FIG. The counter 19 is configured to detect the rising edge (L→H) transition point of the e waveform, reset it, and then count the clocks.
On the other hand, the speed information output device 20 detects the falling edge of the e waveform (H
→L) Detect the conversion point, read the count value of the counter 19, calculate the speed of the moving object from these using the distance value set in advance between S 1 and S 2 , and calculate the speed of the moving object from these Km/
A speed value V put expressed as H, etc. is output. The g waveform in FIG. 4 shows the output operation when the moving body moves in the right direction Sr in FIG. 1, and the h waveform shows the output operation when the moving object moves in the left direction in the Sl direction.
第1図の装置と第2図の装置の相違は1波が
無変調であるかデータ信号でPSKされているかに
よつて誘導線を1のみまたは1,2の並列に設け
たことにあるが、第1図の場合1波は無変調と
することは必要条件ではなくたとえば振幅変調を
行つて通話に利用することもできる。また第2図
の場合には無変調の2波のみを移動体側から両
誘導線に送出し、地上局側では誘導線1を2間の
結合がS1,S2の交差にあるため相殺されてゼロす
なわち無誘導となることを利用して誘導線1およ
び2の各出力から別々に2波成分を抽出し、無
交差誘導線2からの2波出力を振幅一定としか
つ基準位相信号波として交差形誘導線1からの
2波出力を一定振幅にしたものとの間の位相差を
弁別し、その後は第3図W17以後の処理を行つ
てS1とS2間の所要時間を計測するようにしても移
動体の速度が得られることは明らかである。 The difference between the device in Fig. 1 and the device in Fig. 2 is that only one guide wire or one or two guide wires are provided in parallel depending on whether one wave is unmodulated or PSKed with a data signal. In the case of FIG. 1, it is not a necessary condition that one wave be unmodulated, but it is also possible to perform amplitude modulation and use it for telephone calls, for example. In addition, in the case of Fig. 2, only two unmodulated waves are sent from the mobile side to both guide lines, and on the ground station side, the coupling between guide line 1 and 2 is at the intersection of S 1 and S 2 , so they are canceled out. Taking advantage of the fact that the output becomes zero, that is, no guidance, two- wave components are extracted separately from each output of the guide wires 1 and 2, and the two- wave output from the non-crossing guide wire 2 is made constant in amplitude and used as a reference phase signal wave. From intersecting guide line 1
Even if the phase difference between the two- wave output with a constant amplitude is discriminated and the processing from W17 onwards in Figure 3 is performed to measure the time required between S 1 and S 2 , the The speed gains are obvious.
以上の説明から明らかなように本発明によれば
移動体の速度を地上側にて計測監視することがで
きるため、移動体側で速度を計測しその計測値を
伝送してくる必要がなく低速から高速まで高精度
の計測が可能である。また交差部すなわち一定地
点の検知には位相検出法を用いているので、移動
体アンテナと誘導線間隔が変動しても振幅制限機
能によつて誤差を最少とすることができ、雑音妨
害に対しても連続信号波による雑音抑圧効果が得
られている。さらに地上局がこの装置を移動体の
走行制御装置よりの速度指令の照合に使用する場
合には速度異状や暴走を直接検知することができ
る。なお移動体側で速度を検出するには従来は車
輪の回転数の計測によつているが、この方法は車
輪外周の摩耗などによる誤差を伴うのに対して本
発明装置ではこのような誤差の発生は皆無であ
る。また本発明においては2=m1/(m−
1)なる関係にある2つの周波数信号を用いてい
るが、この効果について説明すれば次のようであ
る。1波に振幅変調することによつて電話通話
の送受信にも利用できることは前記の通りである
が、m=2としたとき2相(180゜)位相偏移の
データ伝送に使用することもできる。このときは
1を1と0のデータに応じて180゜位相反転さ
せる。また移動体が誘導線の交差位置を通過する
とその前後で誘導線出力には180゜の位相変化が
あるから、これら2つが同時におきれば360゜の
位相変化となり、受信側第3図の2逓倍器15の
出力に2波の位相基準信号を得ることがきる。
さらにm=4として2=41/3とし受信側
で(2−1)を4逓倍すれば周波数2が得
られる。他方1波をデータ伝送に共用して上記
の2相あるいは4相の位相偏移変調によるデータ
伝送を行う場合でも、データによるπ相、あるい
は(π/2)×n相変化と交差位置通過によるπ
相変化があつても、受信側で2×2=4逓倍すれ
ば同じく連続位相の2波が位相基準波として得
られる。このように1波を振幅変調して通話
に、また2相や4相の位相偏移変調を行うデータ
伝送にも併用できることは明かである。 As is clear from the above explanation, according to the present invention, the speed of a moving object can be measured and monitored on the ground side, so there is no need to measure the speed on the moving object side and transmit the measured value. High-precision measurement is possible up to high speeds. In addition, since the phase detection method is used to detect intersections, that is, fixed points, the amplitude limiting function can minimize errors even if the distance between the mobile antenna and the guide wire changes, and it is effective against noise interference. However, the noise suppression effect due to continuous signal waves can be obtained. Furthermore, when a ground station uses this device to verify speed commands from a travel control device of a moving object, it is possible to directly detect speed abnormalities and runaway. Conventionally, speed detection on the moving object side has been based on measuring the number of rotations of the wheels, but this method involves errors due to wear on the outer circumference of the wheels, etc., whereas the device of the present invention eliminates the occurrence of such errors. There are none. Furthermore, in the present invention, 2 = m 1 /(m-
1) Two frequency signals having the following relationship are used, and this effect can be explained as follows. As mentioned above, it can be used for transmitting and receiving telephone calls by amplitude modulating one wave, but when m = 2, it can also be used for data transmission with a two-phase (180°) phase shift. . At this time
The phase of 1 is inverted by 180° according to the data of 1 and 0. Furthermore, when a moving object passes through the crossing point of the guiding wires, there is a 180° phase change in the guiding wire output before and after that point, so if these two occur at the same time, there will be a 360° phase change, and the receiving side 2 in Figure 3. A two- wave phase reference signal can be obtained at the output of the multiplier 15.
Further, by setting m=4, 2 =4 1/3 , and multiplying ( 2 − 1 ) by 4 on the receiving side, frequency 2 can be obtained. On the other hand, even if one wave is shared for data transmission and data transmission is performed by the above-mentioned two-phase or four-phase phase shift keying, data transmission due to π phase or (π/2) × n phase change and cross position passing. π
Even if there is a phase change, if the reception side multiplies the signal by 2×2=4, two waves of continuous phase can be obtained as the phase reference wave. It is clear that amplitude modulation of one wave can be used for telephone calls in this way, and also for data transmission using two-phase or four-phase phase shift keying.
このように本発明の移動体速度の地上計測装置
は運用(伝送)周波数面から見れば他の目的の通
話やデータ伝送に1波を共用するので、2波
のみが速度計測に専用されているともいえる。す
なわち実用上は通話またはデータ伝送に使用され
る1波があれば、速度計測専用の周波数として
は他の1波を割当てればよいことになる。 As described above, from the perspective of operational (transmission) frequency, the ground measuring device for measuring the speed of a mobile object according to the present invention shares one wave for other purposes such as telephone calls and data transmission, so only two waves are dedicated to speed measurement. You can say that. In other words, in practice, if there is one wave used for telephone calls or data transmission, it is sufficient to allocate another wave as a frequency dedicated to speed measurement.
また1と2の周波数関係は2=m1/
(m−1)であつて1と2それぞれの伝送帯
域は運用目的に応じた変調方式の所要帯域、また
は無変調なら最小の帯域の各伝送を行うように選
定した装置を使用すればよく、上記他の目的の装
置を共通の伝送経路を利用できるから全装置に対
して著しい経済効果が得られる。 Also, the frequency relationship between 1 and 2 is 2 = m 1 /
(m-1), and the respective transmission bands 1 and 2 should be the required band of the modulation method according to the operational purpose, or the equipment selected to transmit each of the minimum band if no modulation is used. Since the devices for the other purposes mentioned above can use a common transmission path, significant economical effects can be obtained for all the devices.
第1図および第2図はそれぞれ本発明装置の構
成例図、第3図は速度計測器の回路構成図、第4
図は第1図〜第3図の各部動作波形図である。
1,2……誘導線、3……終端抵抗器、4,5
……結合器、6,7……速度計測器、8……アン
テナ、9,10……送信機、11,12……
BPF、13,14……増幅と振幅制限器(A・
L)、15……周波数2逓倍器、16……位相弁
別器(PD)、17……方形波変換器(W)、18
……クロツク発生器、19……カウンタ、20…
…速度情報出力器、21……データ信号復調器。
1 and 2 are configuration example diagrams of the device of the present invention, FIG. 3 is a circuit configuration diagram of a speed measuring device, and FIG.
The figures are operation waveform diagrams of each part in FIGS. 1 to 3. 1, 2... Induction wire, 3... Terminating resistor, 4, 5
...Coupler, 6,7...Speed measuring device, 8...Antenna, 9,10...Transmitter, 11,12...
BPF, 13, 14...Amplification and amplitude limiter (A/
L), 15... Frequency doubler, 16... Phase discriminator (PD), 17... Square wave converter (W), 18
...Clock generator, 19...Counter, 20...
...Speed information output device, 21...Data signal demodulator.
Claims (1)
し、一定間隔にて2つの交差を行つた交差形平行
2線式誘導線と、その一端に入力側を接続した速
度計測器よりなる地上側設備と、移動体に載置し
上記誘導線と誘導結合するアンテナおよびこのア
ンテナに、2=m1/(m−1)(たゞしm
は2以上の整数)の関係にある1、2の2周
波数を出力する送信機を具備し、上記速度計測器
には誘導線よりの入力から1、2各周波数成
分を別々に分離抽出して増幅した後一定振幅に制
限する回路、これらの回路から得た2と1の
差周波数をm逓倍して2と等しい周波数とした
出力を基準位相波として上記振幅一定の2波と
の位相差を弁別し位相差により高低または正負レ
ベルの方形波を発生する回路、この方形波出力に
よつて一定クロツクパルス計数器のオン−オフを
制御して、移動体が上記交差区間走行中の計数値
を速度情報として取出す回路を含むことを特徴と
する移動体速度の地上計測装置。 2 移動体走行路に沿つた速度計測区間に展張
し、一定間隔にて2つの交差を行つた交差形平行
2線式の第1の誘導線と、これに平行でこの区間
内では無交差の平行2線式の第2の誘導線および
これらの誘導線のそれぞれの一端より、結合器を
通じて信号入力を得る速度計測器よりなる地上側
設備と、移動体に載置し上記誘導線群と誘導結合
する1個以上のアンテナおよび、このアンテナに
2=m1/(m−1)(たゞしmは2以上の
整数)の関係にある周波数2の無変調波のみ、
またはこの2無変調波と無変調またはデイジタ
ル信号にて位相偏移変調を行つた周波数1波の
2周波を送出する送信機を具備し、上記速度計測
器には上記第1誘導線よりの入力から、周波数
2の成分をまた第2誘導線よりの入力から周波数
1を抽出して増幅した後、一定振幅に制限する
回路、これらの回路より得た2と1の差周波
数をm逓倍して、周波数2とした出力を基準位
相波として上記第1誘導線よりの一定振幅2波
との位相差を弁別し、位相差により高低または正
負レベルの方形波を発生する回路、この方形波出
力によつて一定クロツクパルス計数器のオン−オ
フを制御して、移動体が上記交差区間走行中の計
数置を速度情報として取出す回路を含むことを特
徴とする移動体速度の地上計測装置。[Scope of Claims] 1. A cross-type parallel two-wire guide wire extending over a speed measurement section along a moving vehicle travel path and crossing two lines at a constant interval, and a speed sensor connecting an input side to one end of the cross-shaped parallel two-wire guide wire. 2 = m 1 / (m-1) (m
is an integer greater than or equal to 2 ), and the speed measuring device is equipped with a transmitter that outputs two frequencies, 1 and 2 , which are in the relationship of 1 and 2 (integer greater than or equal to 2), and the speed measuring device separately extracts each frequency component of 1 and 2 from the input from the guide wire. A circuit that limits the amplitude to a constant amplitude after amplification, and the output of the difference frequency between 2 and 1 obtained from these circuits is multiplied by m to have a frequency equal to 2 as a reference phase wave, and the phase difference with the above two waves with constant amplitude is A circuit that generates a square wave of high and low or positive and negative levels based on the phase difference.The output of this square wave controls the on-off of a constant clock pulse counter, and the speed of the moving object is determined by the count value while the moving object is traveling in the above-mentioned crossing section. A ground measuring device for measuring the speed of a moving object, characterized in that it includes a circuit for extracting information. 2. The first guide line of the intersecting parallel two-wire system, which is spread out in the speed measurement section along the moving vehicle travel path and intersects at regular intervals, and the first guide line, which is parallel to this and does not cross within this section. ground-side equipment consisting of a parallel two-wire second guide wire and a speed measuring device that receives a signal input from one end of each of these guide wires through a coupler; one or more antennas to couple to and
Only non-modulated waves with frequency 2 in the relationship 2 = m 1 / (m-1) (where m is an integer greater than or equal to 2),
Alternatively, the speed measuring device is equipped with a transmitter that transmits two unmodulated waves and one frequency wave that is unmodulated or phase-shift keyed using a digital signal, and the speed measuring device is provided with an input from the first guiding wire. From, the frequency
The frequency of the second component is also calculated from the input from the second guiding wire.
After extracting and amplifying 1 , a circuit limits the amplitude to a constant amplitude, and the difference frequency between 2 and 1 obtained from these circuits is multiplied by m, and the output with a frequency of 2 is used as a reference phase wave from the first guide line above. A circuit that discriminates the phase difference between two constant amplitude waves of A ground measuring device for the speed of a moving object, characterized in that the device includes a circuit for extracting the counting position while traveling in the crossing section as speed information.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9451078A JPS5522112A (en) | 1978-08-04 | 1978-08-04 | Ground speed meter of moving body |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9451078A JPS5522112A (en) | 1978-08-04 | 1978-08-04 | Ground speed meter of moving body |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5522112A JPS5522112A (en) | 1980-02-16 |
| JPS6118988B2 true JPS6118988B2 (en) | 1986-05-15 |
Family
ID=14112309
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9451078A Granted JPS5522112A (en) | 1978-08-04 | 1978-08-04 | Ground speed meter of moving body |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5522112A (en) |
-
1978
- 1978-08-04 JP JP9451078A patent/JPS5522112A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5522112A (en) | 1980-02-16 |
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