JPS5925444B2 - Time occupancy measurement method - Google Patents
Time occupancy measurement methodInfo
- Publication number
- JPS5925444B2 JPS5925444B2 JP51138156A JP13815676A JPS5925444B2 JP S5925444 B2 JPS5925444 B2 JP S5925444B2 JP 51138156 A JP51138156 A JP 51138156A JP 13815676 A JP13815676 A JP 13815676A JP S5925444 B2 JPS5925444 B2 JP S5925444B2
- Authority
- JP
- Japan
- Prior art keywords
- time
- moving target
- time occupancy
- output
- measurement method
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 238000000691 measurement method Methods 0.000 title description 4
- 238000000034 method Methods 0.000 claims description 4
- 238000005259 measurement Methods 0.000 description 6
- 238000007796 conventional method Methods 0.000 description 3
- 238000001514 detection method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- 230000002123 temporal effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
Landscapes
- Engineering & Computer Science (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Computer Networks & Wireless Communication (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Length-Measuring Devices Using Wave Or Particle Radiation (AREA)
- Radar Systems Or Details Thereof (AREA)
Description
【発明の詳細な説明】
本発明は移動物標の時間オキユパンシイを測定方式に関
するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring time occupancy of a moving target.
従来道路を走行する車輛10等の移動物標の時間オキユ
パンシイを測定するには第1図のように超音波あるいは
マイクロ波センサ11によるビームを道路12に投射し
反射波があるレベル以上の強さで受信される期間を時間
オキユパンシイとして出力していた。Conventionally, to measure the temporal occupancy of a moving target such as a vehicle 10 traveling on a road, a beam from an ultrasonic or microwave sensor 11 is projected onto the road 12 as shown in Fig. 1, and the intensity of the reflected wave is above a certain level. The period received by the server was output as a time interval.
この方法はビームの大きさAすなわち感知領域の大きさ
分l’だけ車長lに加えられたものを速度りで徐した値
Ti時間が時間オキユパンシイとして出力されるが、物
標の反射の大小、感度設定のバラツキ、アンテナの指向
性の大小等によつて実効的な感知領域長l’が変化し出
力値Tlに影響を与える。In this method, the beam size A, that is, the sensing area size l', is added to the vehicle length l, and the value Ti, which is divided by the speed, is output as time occupancy. , the effective sensing region length l' changes due to variations in sensitivity settings, the magnitude of antenna directivity, etc., which affects the output value Tl.
すなわち11’
T、=−+−
本発明はこれらの欠点を除去し、できるだけ物標の移動
方向に厚みの少ない感知領域を形成し、物標の反射の大
小、感知領域の大小による影響の少ない時間オキユパン
シイ測定方式を提供するものである。That is, 11'T, = - + - The present invention eliminates these drawbacks, forms a sensing area as thin as possible in the direction of movement of the target object, and is less affected by the size of the reflection of the target object and the size of the sensing area. This provides a time occupancy measurement method.
以下にその実施例について説明する。Examples thereof will be described below.
第2図は測定状態を示すもので、センサ11より超音波
あるいはマイクロ波ビームを道路12に投射する。Aは
ビームの大きさであり、Bは感知領域を示している。放
射したマイクロ波ビームの受信波をホモターン検波して
ドップラ信号を得る。FIG. 2 shows a measurement state in which an ultrasonic or microwave beam is projected onto a road 12 from a sensor 11. A is the beam size and B indicates the sensing area. The received wave of the emitted microwave beam is subjected to homoturn detection to obtain a Doppler signal.
これらドップラ波は一波ごとに移動物標の速度方向の正
負弁別を行うことができる。These Doppler waves can discriminate whether the direction of velocity of the moving target is positive or negative for each wave.
例えばマイクロ波レーダにおいては受信波を分岐して二
つの検波器に同位相で供給し、一方送信出力の一部を二
つの検波器にπ/2位相を変えて供給して検波させると
二つの検波器のドップラ信号の位相差は移動物標の速度
方向の正負によつて逆転する。第2図のようにセンサ1
1を設定した例について第3図において説明するとaの
ようなドップラ信号にしきい値Dを設けて感知領域の大
きさをきめて感知領域内を物標10が移動する間、発生
する従来の考え方による時間オキユパイン信号をbとす
る。これは移動物標10の先端が感知領域Bに進入した
時点から移動物標10の後端が感知領域10を脱出する
時点まで続く信号である。次に信号bの継続時間中ドツ
プラ信号の正負方向弁別を行つたとする。例えば接近状
態を”ビ、遠去伏態を“0゛とするとcのように移動物
標10の先端がセンサ11の直下をすぎるまでは方向弁
別出力ば1”であり、直下をすぎた時点から移動物標1
0の後端が直下をすぎるまでは61―“0゛゜混在する
状態となる。これはセンサ11の直下通過前の移動物標
10の部分の反射と、センサ11の直下通過後の移動物
標10の部分の反射との大小関係がいろいろに変わるた
めである。移動物標10の後端がセンサ11の直下を通
過し終ると方向弁別出力ばO゛となる。上に述べた方向
弁別出力をdのようなTIl−Tn+1,tn+1〜T
n+2,tn+2〜Tn+3,・・・・・の単位時間T
Oごとにその間に方向弁別出力の反転があつたか否かを
調べ、あれば″1−なければ″0゛とするような信号を
作ると1単位時間おくれ考慮した場合eのようになる。For example, in a microwave radar, the received wave is branched and supplied to two detectors with the same phase, while a portion of the transmitted output is supplied to the two detectors with a π/2 phase difference and detected. The phase difference between the Doppler signals of the detector is reversed depending on whether the velocity direction of the moving target is positive or negative. Sensor 1 as shown in Figure 2
An example of setting 1 will be explained with reference to FIG. 3.The conventional idea is that a threshold value D is set for the Doppler signal as shown in a to determine the size of the sensing area, and that the threshold value D is generated while the target object 10 moves within the sensing area. Let b be the time occupine signal. This is a signal that continues from the time when the leading end of the moving target 10 enters the sensing area B until the time when the rear end of the moving target 10 exits the sensing area 10. Next, assume that the Doppler signal is discriminated in the positive and negative directions during the duration of signal b. For example, if the approaching state is "bi" and the far away state is "0", the direction discrimination output is "1" until the tip of the moving target 10 passes directly below the sensor 11 as shown in c, and at the time it passes directly below. Target moving from 1
Until the rear end of 0 passes directly below, 61-"0゛° is mixed. This is due to the reflection of the moving target 10 before passing directly below the sensor 11 and the reflection of the moving target 10 after passing directly below the sensor 11 This is because the magnitude relationship with the reflection of the portion 10 changes in various ways.When the rear end of the moving target 10 finishes passing directly under the sensor 11, the direction discrimination output becomes O゛.The above-mentioned direction discrimination output TIl-Tn+1, tn+1~T like d
Unit time T of n+2, tn+2 to Tn+3,...
It is checked whether or not there has been a reversal of the direction discrimination output during each O period, and if a signal is created that indicates "1" if there is, and "0" if not, the result will be as shown in e when one unit time delay is taken into account.
これを時間オキユパンシイ出力とすることができる。時
間オキユパンシイeの精度はT。そのものであるので、
この場合の感知領域Bの長さ15は、21−VXTO
となる。This can be made into a time occupancy output. The accuracy of time accuracy is T. Because it is that
The length 15 of the sensing region B in this case is 21-VXTO.
TOの大きさは物標10がセンサ11の直下を通過する
とき方向弁別出力が”1−またば01のどちらか一方に
最も長く拘束される可能性を実験的に調べて、それより
も少し大きくしておけば良い。このようにして信号eの
出力時間T2は
そして実際にはl′〉11となるため、従来の方式に較
べて、センサ11のビームの大きさや、移動物標10の
反射の大小に殆んど関係のない、きわめて薄い感知領域
Bを移動物標の進行方向に直交するように形成すること
ができる。The size of TO is determined by experimentally investigating the possibility that the direction discrimination output will be constrained to either "1" or "01" for the longest time when the target object 10 passes directly under the sensor 11. In this way, the output time T2 of the signal e is actually l'>11, so compared to the conventional method, the size of the beam of the sensor 11 and the size of the moving target 10 are It is possible to form an extremely thin sensing region B, which has almost no relation to the magnitude of reflection, so as to be orthogonal to the traveling direction of the moving target.
その結果従来の方式に較べ物標10の長さに対する時間
オキユパンシイの比例関係は大巾に改善され、測定確度
も向上する。As a result, compared to the conventional method, the proportional relationship of time occupancy to the length of the target object 10 is greatly improved, and measurement accuracy is also improved.
動物物標10の長さの測定においても従来の方式におい
てとした場合に較べ
l=v(T2−TO)
となりl′/vの実測における変動分よりT。When measuring the length of the animal target 10, compared to the conventional method, l=v(T2-TO), and T is calculated from the variation in the actual measurement of l'/v.
の値は小さいので本方式によつて確度の高い測定ができ
る。上記実施例より明らかなように本発明によれば移動
方向に厚みの少ない感知領域を設けたことにより移動物
標による時間オキユパンシイを正確に測定することがで
きる。Since the value of is small, highly accurate measurements can be made using this method. As is clear from the above embodiments, according to the present invention, time occupancy caused by a moving target can be accurately measured by providing a sensing region with a small thickness in the moving direction.
第1図は従来の時間オキユパンシイ測定方式における測
定領域の側面図、第2図は本発明による時間オキユパン
シイ測定方式における測定領域の側面図、第3図はその
動作波形図である。
10・・・・・・移動物標、11・・・・・・センサ。FIG. 1 is a side view of a measurement region in a conventional time occupancy measurement method, FIG. 2 is a side view of a measurement region in a time occupancy measurement method according to the present invention, and FIG. 3 is an operation waveform diagram thereof. 10...Moving target, 11...Sensor.
Claims (1)
を有するレーダによつて移動物標の存在を検知する間、
一定単位時間ごとにその時間内に方向弁別回路出力に正
負の反転が存在したか否かを検出し、反転の存在する単
位時間の継続する時間を時間オキユパンシイ出力とする
ことを特徴とする時間オキユパンシイ測定方法。1. While the presence of a moving target is detected by a radar that has a function of distinguishing between positive and negative directions of a moving target using a Doppler signal,
Time occupancy characterized by detecting whether or not there is a positive/negative reversal in the output of the direction discrimination circuit every fixed unit time, and setting the continuous time of the unit time in which the reversal exists as the time occupancy output. Measuring method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51138156A JPS5925444B2 (en) | 1976-11-16 | 1976-11-16 | Time occupancy measurement method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51138156A JPS5925444B2 (en) | 1976-11-16 | 1976-11-16 | Time occupancy measurement method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5362578A JPS5362578A (en) | 1978-06-05 |
| JPS5925444B2 true JPS5925444B2 (en) | 1984-06-18 |
Family
ID=15215318
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP51138156A Expired JPS5925444B2 (en) | 1976-11-16 | 1976-11-16 | Time occupancy measurement method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5925444B2 (en) |
-
1976
- 1976-11-16 JP JP51138156A patent/JPS5925444B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5362578A (en) | 1978-06-05 |
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