JPS5871405A - Distance measuring device - Google Patents

Distance measuring device

Info

Publication number
JPS5871405A
JPS5871405A JP56170593A JP17059381A JPS5871405A JP S5871405 A JPS5871405 A JP S5871405A JP 56170593 A JP56170593 A JP 56170593A JP 17059381 A JP17059381 A JP 17059381A JP S5871405 A JPS5871405 A JP S5871405A
Authority
JP
Japan
Prior art keywords
measured
signal
electromagnetic wave
distance
phase difference
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.)
Pending
Application number
JP56170593A
Other languages
Japanese (ja)
Inventor
Kiyoshi Iizuka
飯塚 清志
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Canon Inc
Original Assignee
Canon Inc
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Canon Inc filed Critical Canon Inc
Priority to JP56170593A priority Critical patent/JPS5871405A/en
Publication of JPS5871405A publication Critical patent/JPS5871405A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO 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
    • G01S17/00Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
    • G01S17/02Systems using the reflection of electromagnetic waves other than radio waves
    • G01S17/06Systems determining position data of a target
    • G01S17/08Systems determining position data of a target for measuring distance only
    • G01S17/32Systems determining position data of a target for measuring distance only using transmission of continuous waves, whether amplitude-, frequency-, or phase-modulated, or unmodulated

Abstract

PURPOSE:To measure a plurality of the distances highly accurately, by modulating electromagnetic waves whose wavelengths are 0.5mum or more and 5mum or less, by frequencies of 100kHz or more and 5MHz or less, and comparing the phase delays corresponding to the time length during which the electromagnetic waves go to and return from the object to be measured with a reference signal. CONSTITUTION:The electromagnetic waves, whose wavelengths are 0.5mum or more and 5mum or less, are generated by light emitting diode 2, and modulated by frequencies of 100kHz or more and 5MHz or less from an oscillator 1. Reference luminous flux 4a and reflected luminous flux 4c are received by light receiving elements 6 and 7. The phase is delayed in correspondence with the time length during which the electromagnetic waves go to and return from the object to be measured. The phase delays corresponding to the distances 2m, 5m, and 8m are imparted to reference signal generating means 101-10n. The outputs from phase difference detectors 111-11n become the voltages corresponding to the phase differences between the reference signal and the measured signal. When both distances are agreed, the outputs become zero. This fact is detected by zero detectors 12, and converted by a signal converting means 13 as a distance signal, and displayed by a display 14. Therefore the distances of 2m, 5m, and 8m can be measured accurately.

Description

【発明の詳細な説明】 本発明は電磁波を利用する測距装置に関する。[Detailed description of the invention] The present invention relates to a distance measuring device that uses electromagnetic waves.

この種の測距装置紘電磁波発生装置から出力された電磁
波と、この電磁波が被測定物で反射した反射電磁波との
位相差によって測距を行うものである。従来、#l距性
能および精度を向上させるために、電磁波を変調する周
波−として10〜100−以上の高周波を用いているが
、このような高周波では電磁波発生手段および電−波受
信手段が大形となり、信号処理回路も複雑化4価となる
欠点があった。
This type of distance measuring device measures distance based on the phase difference between the electromagnetic wave output from the electromagnetic wave generating device and the reflected electromagnetic wave that is reflected by the electromagnetic wave from the object to be measured. Conventionally, in order to improve distance performance and accuracy, high frequencies of 10 to 100 or more have been used to modulate electromagnetic waves, but at such high frequencies, electromagnetic wave generating means and radio wave receiving means are very difficult to use. However, there was a drawback that the signal processing circuit became complex and quadrivalent.

そこで、出願人は試作、研究を重ねた結果、*用台的例
えばカメラにおける焦点距離、車両における車間距離等
を測定する場合には、数100KHz〜数馳程度の比較
的低い変−周波数でも十分使用に耐え得る本のであシ、
ま九、低4波とすることによシ′電磁波発生手段等の小
形化および信号処理回路の簡略化低廉化を図ることがで
きることを見出した。この場合、変調周波数は1001
0h以下では位相差が少なく検出積度が愚くなシ使用で
きない0ま九e S hlklz以上になると汎用集積
回路(IC)の動作限界周波数をこえるため、特別な集
積回路が必要となって高価となる。電磁波の波長は0.
5踊以下で発光するものが発光ダイオード(Ia )な
どKあるが市販までに至っていない。従って。
As a result of prototyping and research, the applicant has found that a relatively low variable frequency of several hundred KHz to several tens of kilohertz is sufficient when measuring, for example, the focal length of a camera or the inter-vehicle distance of a vehicle. A book that can withstand use,
Furthermore, it has been found that by using four low waves, it is possible to downsize the electromagnetic wave generating means and the like, and to simplify and reduce the cost of the signal processing circuit. In this case, the modulation frequency is 1001
Below 0h, the phase difference is too small and the detection integration is unusable, making it unusable.If it is above 0h, the operating limit frequency of a general-purpose integrated circuit (IC) is exceeded, and a special integrated circuit is required, which is expensive. becomes. The wavelength of electromagnetic waves is 0.
There are light emitting diodes (Ia) and other devices that emit light with less than 5 digits, but they have not reached the point where they are commercially available. Therefore.

高価である。また、5an以上では発光手段が大型とな
ることがわかった6 本発明は上記に鑑みて提案されたもので、迅速且つ高a
度に複数の距離ゾーンの測距を行うことができる測距装
置を簡単な構成で安価に得ることを目的とする。
It's expensive. In addition, it was found that the light emitting means becomes large when it is 5 an or more.6 The present invention was proposed in view of the above, and it can be used quickly and with high a
To provide a distance measuring device capable of measuring distances in a plurality of distance zones at once with a simple configuration and at low cost.

以下1本発明の実施例を図面について説明する。An embodiment of the present invention will be described below with reference to the drawings.

第1図はその第1実施例を示すブロック図にして。FIG. 1 is a block diagram showing the first embodiment.

1は周波数100KHz以上5MHz以下で発振する電
輯波変調手段としての発振器、2は0.5丸以上5p以
下の成長の電磁波を発生する%磁波発生中段としての発
光ダイオード、3は発光ダイオード2の前面近傍に配置
した光分割器にして1発光ダイオード2からの光4を基
準光束4aと照射光束4bとに分割する。この照射光束
4bは被測定物5を照射する。6は上記基準光束4aを
受光する受光、素子、7は被側定−物5からの反射光束
4cを受光する受光素子、8・9は受光索子6・7の出
力を増幅する交流増幅器、101〜10nは遅延素子よ
りなる基準信号発生手段にして、交流増幅器8の出力に
所望の位相遅れを与えて複数の被測定物距離に対応した
基準信号を発生する。111〜11nは上記交流増幅器
9の出力と上記基準信号発生手段101〜1 inの出
力との位相差を検出する位相差検出手段、121〜12
nは各位相差検出手段111〜11mの出力が零である
ことを検出する零検出器13は零検出器121〜12n
の出力(1または0)を距離信号に変化する信号変換手
段、14は表示器である。
1 is an oscillator as a radio wave modulation means that oscillates at a frequency of 100 KHz or more and 5 MHz or less; 2 is a light emitting diode as a middle stage of % magnetic wave generation that generates an electromagnetic wave with a growth of 0.5 circles or more and 5 p or less; 3 is a light emitting diode 2; A light splitter placed near the front side splits the light 4 from one light emitting diode 2 into a reference light beam 4a and an irradiation light beam 4b. The object to be measured 5 is irradiated with this irradiation light beam 4b. Reference numeral 6 denotes a light receiving element for receiving the reference light beam 4a, 7 a light receiving element for receiving the reflected light beam 4c from the fixed object 5, 8 and 9 AC amplifiers for amplifying the outputs of the light receiving elements 6 and 7; Reference numerals 101 to 10n are reference signal generating means made up of delay elements, which give a desired phase delay to the output of the AC amplifier 8 to generate reference signals corresponding to a plurality of distances to objects to be measured. 111 to 11n are phase difference detection means 121 to 12 for detecting a phase difference between the output of the AC amplifier 9 and the output of the reference signal generation means 101 to 1 inch;
n is a zero detector 13 that detects that the output of each phase difference detection means 111 to 11m is zero; and zero detector 121 to 12n.
14 is a signal converting means for converting the output (1 or 0) into a distance signal.

上記位相差検出手段10としては例えばRCA社。The phase difference detection means 10 is manufactured by RCA, for example.

CD4046A”で指定される7エイズ・ロックド・ル
ープ(Phase * Locked @ Loop 
)中の位相差検出回路部を用いる事も可能である。
7 AIDS Locked Loop (Phase * Locked @ Loop specified by “CD4046A”)
It is also possible to use the phase difference detection circuit section in ).

また9発光ダイオード2は半導体レーザ等の可視域から
赤外域に至る光波の発生手段を有し、この光波を100
馳から数MHzに至る周波数で変調可能な素子または装
置であってもよい。交流増幅器8・9は前記変調周波数
付近のみを通過させるバンドパスフィルターを含む構成
であってもよい。
In addition, the 9 light emitting diodes 2 have means for generating light waves ranging from the visible range to the infrared range, such as a semiconductor laser, and the light waves are generated at 100
It may be an element or device that can be modulated at frequencies ranging from a few MHz to several MHz. The AC amplifiers 8 and 9 may include bandpass filters that pass only frequencies near the modulation frequency.

ところで、電磁波が速度Cで被測定物5までの距離りを
往復するのに要する時間ΔtはΔt=2L/C で表わす事が出来る0また電磁波を周波数fで変調した
とき、前記Δtの時間による周波数fの位相遅れRは t?屹t x f x 560  =2L X t x
 560/C(”)で表わすことが出来る0 そこで、今、被測定物5までの距離を、2m。
By the way, the time Δt required for the electromagnetic wave to travel the distance to the object to be measured 5 at the speed C can be expressed as Δt=2L/C 0 Also, when the electromagnetic wave is modulated at the frequency f, the time Δt is determined by the time Δt mentioned above. Is the phase delay R of frequency f t? t x f x 560 = 2L x t x
It can be expressed as 560/C ('').0 So, now, the distance to the object to be measured 5 is 2 m.

5ms 8mとし、電磁波を光波すなわち速[C−5X
 10’ rrim@a *光11 O変1i111 
Fi!tl t& 数f −50010hとすると、Δ
Pはそれぞれ、2.4°、6.0°、9.6°となる。
5ms 8m, and electromagnetic waves are light waves, that is, speed [C-5X
10' rrim@a *light 11 Ohen 1i111
Fi! If tl t& number f -50010h, Δ
P is 2.4°, 6.0°, and 9.6°, respectively.

基準信号発生手段101は500KHzの周波数を2.
4°、同102は500 KHzの周波数を6.0.同
10mは500mの周波数を9.6位相遅れを与える橡
に選択すると0位相差検出器111〜11mの出力は前
記基準信号発生手段101〜10nによって1位相遅れ
を与えられた基準信号と、前被測定物5からの反射光束
4 c’を電気信号に復調された測定信号との位相差に
対応した電圧となる。
The reference signal generating means 101 generates a frequency of 500 KHz by 2.
4°, the same 102 has a frequency of 500 KHz at 6.0. When the frequency of 500 m is selected to give a 9.6 phase delay, the outputs of the zero phase difference detectors 111 to 11m are the same as the reference signal given one phase delay by the reference signal generating means 101 to 10n. The voltage corresponds to the phase difference between the reflected light beam 4c' from the object to be measured 5 and the measurement signal demodulated into an electrical signal.

第2図は位相差検出手段111〜11nが、たとえば、
前記7エイス・筒ラクト・ループ中の位相差検出回路部
で構成されている場合の基準信号入力の位相に対する創
定偏号入力の位相差を横軸に位相差検出器111の出力
は、測定信号と基準信号Il1発生手段101によって
2.4の位相差れを与えられた基準信号との位相差が零
すなわち被測定物5までの距離が2. mの時、零とな
る。位相差検知器111の出力と接続した零検出器12
1はた改ば入力零0時出力1″、入力が零以外の時出力
゛0゛なる構成゛にすると、被測定物5tでの距離が2
mの時出力1とな少他の条件では0となる。同様にして
、被測定物までの距離が5mの時は零検出器122、の
出力のみ°1″となり8mの時は零検出器123の出力
のみ12となる。
FIG. 2 shows that the phase difference detection means 111 to 11n, for example,
The output of the phase difference detector 111 is measured with the horizontal axis representing the phase difference of the created polarization input with respect to the phase of the reference signal input in the case of the phase difference detection circuit section in the 7-eighth tube tract loop. The phase difference between the signal and the reference signal to which the reference signal Il1 generating means 101 gives a phase difference of 2.4 is zero, that is, the distance to the object to be measured 5 is 2.4. When m, it becomes zero. Zero detector 12 connected to the output of phase difference detector 111
1. If we change the configuration so that when the input is zero, the output is 1'', and when the input is other than zero, the output is ``0'', the distance at the object to be measured 5t will be 2.
When m, the output is 1, and under some other conditions, it becomes 0. Similarly, when the distance to the object to be measured is 5 m, only the output of the zero detector 122 is 1'', and when the distance is 8 m, only the output of the zero detector 123 is 12.

上記零検出器121〜12nの出力°丁または0″は信
号変換中R15によって、距離信号に変換され、鍼示器
14により被測定物5までの距離を表示する。この場合
衆示器14の代りにカメラ用レンズの駆動回路を設け、
この駆動回路を上記信号変換手段11からの出力で制御
して自動的に焦点調節を行なうようにすることもできる
The output of the zero detectors 121 to 12n is converted into a distance signal by R15 during signal conversion, and the distance to the object to be measured 5 is displayed by the acupuncture indicator 14. Instead, a camera lens drive circuit is installed.
It is also possible to control this drive circuit with the output from the signal conversion means 11 to automatically adjust the focus.

上記第1図例においては測距ゾーンを3点としたが、必
賛に応じて測距ゾーンは増減することは十分回前であり
、所望の距離に応じた位相遅れをそれぞれに与えればよ
い0また。?に単信号発生手段101〜10nの位相遅
れ量の差が所殖の距離変化賞に対応し位相差検出子@1
11@11にの出力の最小値を求める構成であって奄よ
い0また。上記の基準信号発生手段101〜10nおよ
び位相差検出手段111〜11nの構成によっては最大
値を求めることにより測距を行なうようにすることもで
きる。
In the example in Figure 1 above, the distance measurement zone is set to 3 points, but the distance measurement zone can be increased or decreased depending on the need, and it is sufficient to give each one a phase delay according to the desired distance. 0 again. ? The difference in the amount of phase delay of the single signal generating means 101 to 10n corresponds to the distance change value obtained by the phase difference detector @1.
11@11 is configured to find the minimum value of the output, and it is easy to get 0. Depending on the configuration of the reference signal generating means 101 to 10n and the phase difference detecting means 111 to 11n, distance measurement may be performed by determining the maximum value.

第3図は本発明装置の他の実施例を示すもので。FIG. 3 shows another embodiment of the device of the present invention.

第1図におゆる光分割riI5.基準光束4aを受光受
光素子6.この受光菓子の出力を増幅する交流増幅器8
を省略し9代りに発振器1からの周波数fの電気信1号
社基準信号発生手段151〜15nによって1発光素子
2.受光素子7および増幅#!に9等による物体距離に
依存しない位相遅れ麓と、所望の被測定物距離によって
生じる周波数fの位相遅れ量を加味して、被測定物距離
に対応した位相遅れを与えられ、基準信号として位相差
検出手段111・〜11nに供給されるOこの位相差検
出手段から以後の作用は前記m1図と同じであるから説
明は省略する◇ 本発明は上記の如く、波長が0.5,91以上5縄以下
の電磁波を該電磁波jよりも十分低い周波数100KH
z以上51&Iz以下で変調を行い、この変調を受1け
走電磁波が被測定物間を往復する時間に対応して生ずる
位相遅れによって測距するものであるから、迅速且つ高
楕[K複数の距離ゾーンの測距を行なうことができる測
距ii&を簡単な構成によって女価に、得ることが出き
る幼果がめる0例えば本発tjliilj距装置をカメ
ラに通用することによυ、非常に短時間に精度の高い測
距を行なうことがで色るもので、得られた距離信号でス
トロボ発光量の制御、撮影レンズの絞り値制御等を行な
って、ストロボ撮影の際に被写体距離に応じた蝦適繕光
での撮影が可能である0ま九9本発明−距装置を車輌の
車間距離測定用に用いれば、安全車間距離を短時間で測
定することができて安全性が向上する。
FIG. 1 shows the light splitting riI5. The reference light beam 4a is received by a light receiving element 6. AC amplifier 8 that amplifies the output of this light-receiving confectionery
9 is omitted, and instead of the electric signal of frequency f from the oscillator 1, the 1 light emitting element 2. Photodetector 7 and amplification #! 9, etc., and the phase delay amount of frequency f caused by the desired distance to the object to be measured, a phase lag corresponding to the distance to the object to be measured is given, and the position is used as a reference signal. O supplied to the phase difference detection means 111 to 11n, the subsequent operations from this phase difference detection means are the same as those in the m1 diagram above, so the explanation will be omitted. Electromagnetic waves of 5 ropes or less with a frequency of 100KH, which is sufficiently lower than the electromagnetic wave j.
Modulation is performed above z and below 51 For example, by applying the distance measuring device developed in this invention to a camera, it is possible to obtain a distance measuring device that can perform distance measurement with a simple configuration, and to obtain a very short distance. It is important to be able to perform highly accurate distance measurement on time, and the obtained distance signal is used to control the amount of flash light emitted, the aperture value of the photographic lens, etc., and adjust the distance according to the subject distance during flash photography. If the distance device of the present invention, which is capable of photographing with a blinding light, is used for measuring the distance between vehicles, the safe distance between vehicles can be measured in a short time, improving safety.

【図面の簡単な説明】[Brief explanation of drawings]

i@1図は本発明の第1の実施例を示すブロック図、第
2図は位相差対出力電圧の関係図、第3図は本発明の第
2実施例を示すブロック図でめる01は・発振!、2は
発光ダイオード、5は光分割器、5は被測定物、6・7
は受光素子、8・9は交流増幅器、101〜10n・1
51〜15nは基準信号発生手段、111〜11nは位
相差検出手段。 121〜12njL零検出益、16は信号変換手段。 14は表示器。
i@1 Figure 1 is a block diagram showing the first embodiment of the present invention, Figure 2 is a diagram showing the relationship between phase difference and output voltage, and Figure 3 is a block diagram showing the second embodiment of the present invention.01 Ha-oscillation! , 2 is a light emitting diode, 5 is a light splitter, 5 is an object to be measured, 6 and 7
is a light receiving element, 8 and 9 are AC amplifiers, and 101 to 10n・1
51 to 15n are reference signal generating means, and 111 to 11n are phase difference detection means. 121-12njL zero detection gain, 16 signal conversion means. 14 is a display.

Claims (1)

【特許請求の範囲】[Claims] (1)波長が0.5踊以上5勤以下の電磁波を発生する
電磁波発生手段と、この電磁波発生手段を制御して上記
電磁波を周波数100KHz以上5 MHz以下で変調
する電a波変調手段と、上紀電憾波の被測定物からの反
射電磁波を電気信号に複調する復調手段と、上記被#j
定物に依存しない上記電磁波又は上記電悼波変調手段の
出力に漬いて上記被測定物までの種々の距離に対応した
基準信号を発生する複数の基準信号発生手段と、?:、
れ等基準信号に対する上に2電気信号の位相差を検出す
る複数の位相差検出手段と、これ等位相差検出手段の出
力が零であることを各別に検出する11!数の零検出手
段と。 これ等零検出手段からの位相慶匍号を距離信号に変換す
る信号変換手段とを備えたことを特徴とする#J距装置
(1) an electromagnetic wave generating means for generating an electromagnetic wave with a wavelength of 0.5 kHz or more and 5 MHz or less, and an electromagnetic wave modulating means that controls the electromagnetic wave generating means to modulate the electromagnetic wave at a frequency of 100 KHz or more and 5 MHz or less; a demodulating means for demodulating the electromagnetic wave reflected from the object to be measured of the Joki electric wave into an electrical signal;
a plurality of reference signal generating means for generating reference signals corresponding to various distances to the object to be measured by immersing in the output of the electromagnetic wave or the electromagnetic wave modulating means that does not depend on a fixed object; :,
A plurality of phase difference detection means for detecting the phase difference between the two electrical signals with respect to the reference signal, and 11 for individually detecting that the output of these phase difference detection means is zero! Number zero detection means. #J distance device 0 characterized by comprising signal conversion means for converting the phase signal from the zero detection means into a distance signal.
JP56170593A 1981-10-24 1981-10-24 Distance measuring device Pending JPS5871405A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56170593A JPS5871405A (en) 1981-10-24 1981-10-24 Distance measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56170593A JPS5871405A (en) 1981-10-24 1981-10-24 Distance measuring device

Publications (1)

Publication Number Publication Date
JPS5871405A true JPS5871405A (en) 1983-04-28

Family

ID=15907707

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56170593A Pending JPS5871405A (en) 1981-10-24 1981-10-24 Distance measuring device

Country Status (1)

Country Link
JP (1) JPS5871405A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114415080A (en) * 2022-01-24 2022-04-29 中国科学技术大学 Diamond NV color center magnetometer and method for measuring magnetic field

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114415080A (en) * 2022-01-24 2022-04-29 中国科学技术大学 Diamond NV color center magnetometer and method for measuring magnetic field
CN114415080B (en) * 2022-01-24 2023-06-02 中国科学技术大学 Diamond NV color center magnetometer and method for measuring magnetic field

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