JPS61149876A - Transmitter for signal for range measurement - Google Patents

Transmitter for signal for range measurement

Info

Publication number
JPS61149876A
JPS61149876A JP59272182A JP27218284A JPS61149876A JP S61149876 A JPS61149876 A JP S61149876A JP 59272182 A JP59272182 A JP 59272182A JP 27218284 A JP27218284 A JP 27218284A JP S61149876 A JPS61149876 A JP S61149876A
Authority
JP
Japan
Prior art keywords
distance
signal
range
projector
light
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
JP59272182A
Other languages
Japanese (ja)
Inventor
Iesato Sato
佐藤 家郷
Hiroshi Kawada
川田 博
Yoshiyuki Eto
江藤 宜幸
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.)
Meisei Electric Co Ltd
Nissan Motor Co Ltd
Original Assignee
Meisei Electric Co Ltd
Nissan Motor Co Ltd
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 Meisei Electric Co Ltd, Nissan Motor Co Ltd filed Critical Meisei Electric Co Ltd
Priority to JP59272182A priority Critical patent/JPS61149876A/en
Publication of JPS61149876A publication Critical patent/JPS61149876A/en
Pending legal-status Critical Current

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  • Radar Systems Or Details Thereof (AREA)
  • Optical Radar Systems And Details Thereof (AREA)

Abstract

PURPOSE:To obtain a small-sized, low-cost range measuring radar which takes a measurement over a wide range from long distance to short distance and is small in power consumption by providing plural signal projectors which differ in projection beam angle according to a distance measurement range. CONSTITUTION:A light emitting element 1 and a lens 2 form the 1st signal projector S1 which has a wide projection beam angle theta1 and a light emitting element 3 and a lens 4 form the 2nd signal projector S2 which has a narrow projection beam angle theta2. Those signal projectors S1 and S2 which have the different projection angles are combined together to form a transmitter TX. Consequently, the projector S1 is made to correspond to a short-range object R1 and the projector S2 is made to correspond to a long-range object R2, so that the power consumption and size are reduced on the whole. A laser light beam, a radio wave, an ultrasonic wave, etc., are applicable as a range measuring medium.

Description

【発明の詳細な説明】 (発明の技術分野) 本発明は、目標物に向けて測距用の信号、例えば光を投
射し、当該信号の目標物での反射信号、例えば反射光を
受信して目標物までの距離を測定するようにした測距レ
ーダーの信号送信装置に関するものである。
Detailed Description of the Invention (Technical Field of the Invention) The present invention projects a ranging signal, such as light, toward a target, and receives a reflected signal, such as reflected light, of the signal at the target. The present invention relates to a signal transmitting device for a distance measuring radar that measures the distance to a target.

(従来技術とその問題点) 従来の測距レーダーでは測距用信号の送信装置は一般に
信号の投射ビーム角について単一の信号投射器で構成さ
れている。
(Prior art and its problems) In conventional ranging radars, the transmitting device for ranging signals is generally comprised of a single signal projector for the signal projection beam angle.

一般に信号投射器から投射された信号が有効に到達する
距離(反射信号の検出可能な最長距離)は信号投射器の
出力電力が大きい程長く、また、その投射ビーム角が狭
い程長い。
Generally, the distance that a signal projected from a signal projector effectively reaches (the longest distance in which a reflected signal can be detected) increases as the output power of the signal projector increases, and also increases as the projection beam angle narrows.

従って、遠距離測定を行おうとする場合には信号投射器
の出力電力を大きくするか、又は投射ビーム角を小さく
する必要がある。
Therefore, when long-distance measurement is desired, it is necessary to increase the output power of the signal projector or to reduce the projection beam angle.

信号投射器の出力電力を大きくすると、機器の価格が高
くな夛、かつ大型化するばかシか、運用する際の消費電
力が多くなシ、また、投射ビーム角を小さくすると特に
近距離に於ける測定可能範囲が狭くなる。従りて例えば
走行車輛の車間距離を測定するための測距レーダーのよ
うに、限られた設置スペースに設備して限られた電力で
運用し、かつ広範囲な測定を必要とする場合には前記従
来の測距゛レーダーでは満足な結果は得られ表い。
Increasing the output power of the signal projector will increase the cost and size of the device, and will also increase the power consumption during operation, while reducing the projection beam angle will increase the cost, especially at short distances. The measurable range becomes narrower. Therefore, for example, when a distance measuring radar for measuring the distance between vehicles is required to be installed in a limited installation space, operated with limited power, and to perform measurements over a wide range, the above-mentioned method is used. Satisfactory results have not been obtained using conventional ranging radars.

(発明の目的) 本発明は上記従来の問題点を解決するために提案するも
ので、遠距離から近距離に至るまで広範囲な測定が可能
であシ、かつ消費電力が少なく小型で低コストの測距レ
ーダーを得ることを目的とする。
(Purpose of the Invention) The present invention is proposed to solve the above-mentioned conventional problems, and is capable of measuring a wide range of distances from long distances to short distances, and is compact and low-cost with low power consumption. The purpose is to obtain a ranging radar.

(発明の概要) 上記目的のため、本発明は測距範囲に応じて投射ビーム
角の異った信号投射器を複数個設けるようにしたもので
ある。
(Summary of the Invention) For the above purpose, the present invention provides a plurality of signal projectors with different projection beam angles depending on the distance measurement range.

(実施例) 図面はいずれも本発明の詳細な説明するためのもので、
第1図は第1実施例の構造図、第2図は第1実施例の投
射ビーム特性を説明する図、第3図は第2実施例の構造
図、第4図は第2実施例の投射ビーム特性を説明する図
である。
(Example) All drawings are for detailed explanation of the present invention.
Fig. 1 is a structural diagram of the first embodiment, Fig. 2 is a diagram explaining the projection beam characteristics of the first embodiment, Fig. 3 is a structural diagram of the second embodiment, and Fig. 4 is a diagram of the second embodiment. FIG. 3 is a diagram illustrating projection beam characteristics.

実施例はいずれも自動車の車間距離計測用測距レーダー
に本発明を実施した例で、測距用信号として光(レーザ
ー光)を使用したものである。
All of the embodiments are examples in which the present invention is applied to a distance measuring radar for measuring the distance between cars, and light (laser light) is used as a distance measuring signal.

まず、第1図及び第2図によって第1実施例を説明する
First, a first embodiment will be explained with reference to FIGS. 1 and 2.

第1図及び第2図に於いて、TXは送信機、Aは道路、
R1及びR3は測距目標物体(例えば先行走行車両、以
下、物体という。)であシ、送信機TXに於いて、S、
及びS、はそれぞれ第1及び第2の投光器(信号投射器
)、1及び3は発光素子、2及び4は投光用レンズ(以
下、レンズという。)である。
In Figures 1 and 2, TX is a transmitter, A is a road,
R1 and R3 are ranging target objects (for example, a preceding vehicle, hereinafter referred to as objects), and in the transmitter TX, S,
and S are first and second projectors (signal projectors), respectively, 1 and 3 are light emitting elements, and 2 and 4 are projecting lenses (hereinafter referred to as lenses).

送信機TXは、発光素子1及びレンズ2でなる近距離用
の第1の投光器S□と、発光素子3及びレンズ4でなる
遠距離用の第2の投光器S、とを有する。
The transmitter TX has a first projector S□ for short distances, which is made up of a light emitting element 1 and a lens 2, and a second projector S, for long distances, which is made up of a light emitting element 3 and a lens 4.

発光素子1,3とレンズ2,4との間の距離及びレンズ
2,4の焦点距離は、第1の投光器S1からの投射光の
投光ビーム角θ、が第2の投光器S、かもの投射光の投
光ビーム角θ雪よシ広くなるように設定しである。
The distance between the light emitting elements 1, 3 and the lenses 2, 4 and the focal length of the lenses 2, 4 are such that the projected beam angle θ of the projected light from the first projector S1 is different from that of the second projector S, The projected beam angle θ of the projected light is set to be wider than the snow.

第2図に示すようにそれぞれの投光器S1  rS、か
らの光の投射方向gは、測距レーダーを搭載した車の走
行方向、すなわち道路人の方向に設定される。尚、投光
器5leS1間の間隔は道路Aの巾息に比べて無視し得
る程短いので、双方の投光器S1  、S!の光の投射
点は同一としてよく、第2図はこれに従って作図しであ
る。
As shown in FIG. 2, the projection direction g of light from each of the projectors S1 to S1 is set in the direction of travel of a vehicle equipped with a distance measuring radar, that is, in the direction of people on the road. Incidentally, since the distance between the floodlights 5leS1 is so short that it can be ignored compared to the width of the road A, both the floodlights S1, S! The projection points of the light may be the same, and FIG. 2 is drawn accordingly.

それぞれの投光器S1*Slからの投射光の投光ビーム
角θ3.θ、は、それぞれの投射光の有効到達距離L1
*A!の最長点に於いて、必要測定中1例えば道路Aの
巾aをカバーするように設定される。
Projection beam angle θ3 of the projection light from each projector S1*Sl. θ, is the effective reach L1 of each projection light
*A! It is set to cover the width a of a road A, for example, during the required measurement at the longest point of the road A.

いま、L H=n L 1とし、第1の投光器Siの投
射光だけで距離t、の範囲をカバーしようとした場合を
考察すると、発光素子1の発光出力は距離t1の範囲を
カバーする場合のn倍を必要とする。
Now, considering the case where L H = n L 1 and an attempt is made to cover the range of distance t with only the projection light of the first projector Si, the light emitting output of light emitting element 1 covers the range of distance t1. It requires n times as much.

すなわち、一般に距離tだけ離れた地点を角度θの投光
角で照射した場合、距離tの地点の被照射面積は、角度
θ、高さLの円錐空間の底面に相当する面積であシ、こ
の面積は角度θが一定であれば距離りの2乗に比例する
。従りて光源の強さが一定であれば当該面積の被照射強
度は距離りの2乗に反比例することとなる。これを関係
式で表わすと次のようになる。
That is, in general, when a point separated by a distance t is irradiated with a projection angle of angle θ, the irradiated area at the point of distance t is an area corresponding to the bottom of a conical space of angle θ and height L, This area is proportional to the square of the distance if the angle θ is constant. Therefore, if the intensity of the light source is constant, the irradiation intensity of the area will be inversely proportional to the square of the distance. This can be expressed as a relational expression as follows.

L=k・−・・・・・・(1) 但し、Lは被照射強度、Xは光源の強度、kは比例定数
(角度θによって決定される定数)である。
L=k (1) where L is the irradiation intensity, X is the intensity of the light source, and k is a proportionality constant (a constant determined by the angle θ).

上記被照射強度りで照射される地点に反射物体があ〕、
これによる反射光が角度θ′で送信機TXと同じ場所に
設置された受信機(図示せず)に帰還したときの強度(
受信機に於ける受光強度)は、上記反射物°体が強度り
の光源であるものとみなせるので、上記と同様に考えれ
ば次の関係式が成シ立つ。
There is a reflective object at the point that is irradiated with the above irradiation intensity],
The intensity (
Since the above-mentioned reflecting object can be regarded as a strong light source (received light intensity at the receiver), the following relational expression holds true if considered in the same way as above.

L′冨に′・−・・・・−(2) 但し、L′は受信機での受光強度、k′は比例定数(角
度θ′によって決定される定数)である。
(2) where L' is the received light intensity at the receiver, and k' is a proportionality constant (a constant determined by the angle θ').

上記(1)及び(2)の関係式から L’=L・□  ・・・(3)   但し、K−に−に
’となる。この(3)式の関係を、距離t1及びり、に
ついて適用すると(但し、物体R3及びR1での反射中
(角度〕は互に同じであるものとする。)、いまの場合
、距離t1 とt、とはrt1=ntIJの関係にあシ
、かつ受信機での受信強度り、/とL2tとは互に等し
くしなければならないので、上記(4)及び(5)式か
ら とな夛、この(6)式から X、=n−X2    ・・・・・・(7)となる。す
なわち、(7)の関係から距離り、の範囲をカバーする
場合に必要な光源の投光出力は、距離t1の範囲をカバ
ーする場合の光源の投光出力のn4倍となる。
From the relational expressions (1) and (2) above, L'=L・□ (3) However, K-to-to'. If we apply the relationship in equation (3) to the distance t1 and t is in the relationship rt1=ntIJ, and since the reception strength at the receiver / and L2t must be equal to each other, from equations (4) and (5) above, From this equation (6), we get: , the light emitting output of the light source when covering the range of distance t1 is n4 times.

次に本発明の実施例について考察する。Next, examples of the present invention will be considered.

第1の投光器S1による距離1X前方の被照射面積と第
2の投光器S、による距離t、前方の被照射面積とは、
それぞれの投光角度θ1及びθ。
The irradiated area at a distance 1X in front of the first projector S1 and the irradiated area in front at a distance t by the second projector S are:
The respective projection angles θ1 and θ.

を異ならしめることによシ同一となるように設定されて
いる。従って、それぞれの投光器S1 。
They are set to be the same by making them different. Thus, each floodlight S1.

S、による投光強度が互に等しければ物体R1゜R3に
達するそれぞれの被照射強度は等しくなる。
If the intensities of the light emitted by the objects R1 and R3 are equal, the intensities of the irradiated light reaching the objects R1 and R3 will be equal.

この関係を前記(1)式と同様にして各距離L’st!
について表わすと、 但し、k、及びに、はそれぞれ角度θ1及びθ冨で決定
される定数である。
Using this relationship as in equation (1) above, each distance L'st!
Expressed for: where k and , are constants determined by the angles θ1 and θ-thickness, respectively.

次に物体R1及びR,によって受信機に帰還した反射光
の強度を、前記(2)式と同様に考えて各距離1.,1
.について表わすと、 ■。
Next, the intensity of the reflected light returned to the receiver by the objects R1 and R is considered in the same manner as in equation (2) above, and the intensity of the reflected light is calculated for each distance 1. ,1
.. Expressed as: ■.

但し、k、′及びに2′はそれぞれ物体R1及びR7で
の反射光の反射中(角度)によって定まる定数であシ、
前記と同様、物体R1及び物体R2での反射光の反射中
(角度)が互に等しいものと考えれば kl−に2′      ・・・・・・αρ距離1..
1.について「t、m nt、Jの関係にあシ、この関
係と上記(8) 、 (9)及び(至)式の関係からま
た、上記(8)式から に=n ・に1    ・・・・・・(ト)の関係が得
られ、とのα1式と上記ぐや及び(6)式の関係から Ll−−L′   ・・・・・・α→ の関係が得られる。このα1式は、距離t1及びLl先
の被照射面積が等しくなるように設定し、光源の投光強
度が同じであれば、距離t、先の物体R2での反射光の
受信強度は距離t、先の物体R1での反射光の受信強度
のr 1/n2Jとなることを示しておル、当該双方の
受信強度が等しくなるようにする場合(すなわち、L、
’!L2’とする場合)には、遠距離用の投光器S、の
投光強度を近距離用の投光器S1の投光強度のn倍とす
ればよいこととなる。
However, k, ' and 2' are constants determined by the angle of reflection of the reflected light on objects R1 and R7, respectively.
As before, assuming that the angles of reflection of the reflected light from objects R1 and R2 are equal, kl- has a distance of 2'...αρ distance 1. ..
1. Regarding the relationship between t, m nt, and J, from this relationship and the relationship between equations (8), (9), and (to) above, from equation (8) above, we get = n ・to 1... ...(g) is obtained, and from the relationship between the α1 equation and the above Guya and equation (6), the relationship Ll--L' .......α→ is obtained.This α1 equation is set so that the irradiated area at distance t1 and Ll ahead are equal, and if the projected light intensity of the light source is the same, the received intensity of the reflected light at distance t and ahead object R2 is equal to distance t and ahead object R2. It is shown that the received intensity of the reflected light at the object R1 is r 1/n2J, and when the received intensities of both are made equal (that is, L,
'! L2'), the light projection intensity of the long-distance projector S may be set to n times the light projection intensity of the short-range projector S1.

以上のことから、本発明の第1実施例に於ける距離1.
の範囲をカバーするに必要な投光出力(投光器S1及び
S、の投光出力の合計)は、距離L1の範囲をカバーす
るに必要な投光出力の(1+n)倍となる。
From the above, it can be seen that the distance 1 in the first embodiment of the present invention.
The light projection output required to cover the range of distance L1 (the sum of the light projection outputs of the projectors S1 and S) is (1+n) times the light projection output necessary to cover the range of distance L1.

従りて、前記投光器が1個の場合と比べて、本発明の第
1実施例では投光出力が(1+n2)/n’倍でよく、
投光器での電力の消費が非常に少くなる0 また、投光器Si 、S、それぞれの投光出力も1個の
投光器を使用した場合に比較して小形でよく、放熱対策
が施し易くて機器の小形化が可能となる。
Therefore, compared to the case where there is only one light projector, in the first embodiment of the present invention, the light projection output may be (1+n2)/n' times,
The power consumption of the projector is extremely low.In addition, the light output of each projector Si and S can be smaller than when using a single projector, making it easier to implement heat dissipation measures and making the equipment smaller. It becomes possible to

自動車に本発明に係る測距レーダーを搭載する場合、自
動車のカーブ走行時を考慮すると、遠方の測定範囲を道
路Aの巾aよシ広く設定するととKよシ曲がろうとする
方向前方の走行車等を捉えることができて好都合である
。以下に説明する第2実施例は上記カーブ走行時を考慮
した実施例で号放射器)、5は発光素子、6は投光用レ
ンズであシ、その他の記号は前記第1図と同じである。
When a vehicle is equipped with the distance measuring radar according to the present invention, if the distance measurement range is set to be wider than the width of the road A, considering when the vehicle is traveling on a curve, it will be possible to set the distance measurement range to be wider than the width of the road A. This is convenient because it allows you to catch cars, etc. The second embodiment described below is an embodiment that takes into consideration the above-mentioned curve traveling, and 5 is a light emitting element, 6 is a light projecting lens, and other symbols are the same as in FIG. 1 above. be.

第2実施例は近距離用に1つの投光器S工を、遠距離用
に2つの投光器S、及びS、をそれぞれ設けたものであ
シ、第1の投光器S1は発光素子1とレンズ2を、第2
の投光器S、は発光素子3とレンズ4を、第3の投光器
S、は発光素子5とレンズ6をそれぞれ有する。
The second embodiment is provided with one floodlight S for short distance use and two floodlights S for long distance use, and the first floodlight S1 includes a light emitting element 1 and a lens 2. , second
The third floodlight S has a light emitting element 3 and a lens 4, and the third floodlight S has a light emitting element 5 and a lens 6, respectively.

第4図に示すように第1の投光器S1からの光の投射方
向gは道路Aの方向に一致させてあシ、第2及び第3の
投光器S、及びS、からの光の投射方向り及びjは道路
Aの方向からそれぞれ角度α1及びα、だけ偏角するよ
うK、また、それぞれの投光ビーム角θ1 、θ、及び
θ、は、θ、〉θ、。
As shown in FIG. 4, the projection direction g of the light from the first floodlight S1 is aligned with the direction of the road A, and the projection direction g of the light from the second and third floodlights S and S is aligned with the direction of the road A. and j are deviated from the direction of road A by angles α1 and α, respectively, and the projected beam angles θ1, θ, and θ are θ,〉θ, respectively.

θ□〉θ、となるようにレンズ2,4.6の焦点距離及
び当該レンズ2,4.6と発光素子1,3゜5との間の
距離が設定しである。
The focal length of the lens 2, 4.6 and the distance between the lens 2, 4.6 and the light emitting element 1, 3°5 are set so that θ□>θ.

第1の投光器S1による測距範囲(投光空間)旬は近距
離t、をカバーする最大中が道路Aの巾aの範囲であシ
、また、第2及び第3の投光器S、及びS、 Kよる測
距範囲(投光空間)d及びeは遠距離t、及びt、をカ
バーし、かつ道路Aから両側にそれぞれ角度β1及びβ
、はみ出した゛範囲である。このはみ出した測距領域が
存在することによりて自動車の斜め前方の物体(先行車
両)を捉えることができ、カーブ走行時に好都合である
The distance measurement range (light projection space) by the first floodlight S1 is a short distance t, and the maximum range is the width a of the road A, and the second and third floodlights S and S , K cover long distances t and t, and have angles β1 and β on both sides from road A, respectively.
, it is outside the range. The existence of this protruding ranging area allows objects diagonally in front of the vehicle (preceding vehicle) to be detected, which is convenient when driving around a curve.

第2実施例に於ける発光素子1,3及び5の発光出力に
ついて述べると、前記第1実施例と同様にt、=HL1
 とし、投光ビーム角θ8.θ、について0.=08、
投光距離1..1.について%%t2== t3、遠距
離用の投光器S、及びS、の距離tt  C=ts  
)における円錐空間(投光空間d。
Regarding the light emitting outputs of the light emitting elements 1, 3 and 5 in the second embodiment, t,=HL1 as in the first embodiment.
and the projected beam angle θ8. 0 for θ. =08,
Projection distance 1. .. 1. For %%t2==t3, the distance of the long-range projector S and S, tt C=ts
) in the conical space (projection space d.

・)の底面の直径は道路Aの道中aに等しいとすれば、
距離t、の範囲を投光器S1だけでカバーする場合の(
1+2 n2)/ n’でよい。
If the diameter of the bottom of ・) is equal to the length a of road A, then
When the range of distance t is covered only by floodlight S1, (
1+2 n2)/n' is sufficient.

すなわち、第2実施例では前述した第1実施例に比べ、
第2の投光器S、と同じ特性の第3の投光器S、が追加
されただけで、その他の条件は前記第1実施例と同じで
あシ、投光器全体の消費電力を考察する場合、前記第1
実施例に於ける消費電力に当該第3の投光器S3の分を
追加するのみでよい。
That is, in the second embodiment, compared to the first embodiment described above,
The other conditions are the same as in the first embodiment except that a third floodlight S having the same characteristics as the second floodlight S is added.When considering the power consumption of the entire floodlight, 1
It is only necessary to add the power consumption of the third light projector S3 to the power consumption in the embodiment.

以上のことから、第2実施例に於いても、前記第1実施
例と同様、電力の消費が少なくなる。
From the above, power consumption is reduced in the second embodiment as well as in the first embodiment.

以上に説明した実施例はいずれも測距媒体として光(レ
ーザー光)を使用したものであるが、測距媒体として例
えば電波、超音波等を使用することもでき、測距媒体の
違いが本発明の要旨を変更するものではない。
Although all of the embodiments described above use light (laser light) as the distance measuring medium, for example, radio waves, ultrasonic waves, etc. can also be used as the distance measuring medium, and the difference in distance measuring medium is the main difference. This does not change the gist of the invention.

また、第2実施例に於いて、遠距離用の投光器S、及び
S、それぞれの投光ビーム角θ、及びθ3、投光方向の
偏角α、及びα1、投光距離t、及びt3は、それぞれ
互に等しくてもよく、また測距範囲等によって互に異な
らしめてもよい。
In addition, in the second embodiment, the long-distance projectors S and S, the respective projection beam angles θ and θ3, the declination angles α and α1 of the projection direction, and the projection distances t and t3 are , may be equal to each other, or may be different depending on the ranging range, etc.

すなわち、これ等の設定の仕方によって種々の測距パタ
ーンを作り出すことができる。
That is, various distance measurement patterns can be created depending on how these settings are made.

(発明の効果) 以上、詳細に説明した↓うに、本発明によれば測距レー
ダーの消費電力を少なくでき、機器の小形化が可能と・
なるため、特に自動車等、使用できる電力が限られてお
シ、かつ設置スペースも限られているようなものに搭載
する測距レーダーに本発明を実施すると極めて有利とな
る。
(Effects of the Invention) As explained in detail above, according to the present invention, the power consumption of the distance measuring radar can be reduced, and the equipment can be made smaller.
Therefore, it is extremely advantageous to apply the present invention to a distance measuring radar installed in an object such as an automobile, which has limited usable electric power and limited installation space.

また、複数の投光器の設定の仕方によって種々の測距/
4’ターンが設定できるので、極めて応用範囲の広い測
距レーダーを提供することができ、本発明は極めて顕著
な効果を奏するものである。
Also, depending on how the multiple projectors are set, various distance measurement/
Since the 4' turn can be set, it is possible to provide a distance measuring radar with an extremely wide range of applications, and the present invention has extremely significant effects.

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

図面はいずれも本発明の詳細な説明するだめのもので、
第1図及び第3図はそれぞれ第1及び第2の実施例の構
造図、第2図及び第4図はそれぞれ第1及び第2の実施
例の投射ビーム特性を説明する図である。 (主な記号) TX・・・送信機      J 、s、 t SI 
”・投光器1.3.5・・・発光素子  2,4.6・
・・投光用レンズ4図  7,7 第2図
The drawings are not meant to provide a detailed explanation of the invention.
1 and 3 are structural diagrams of the first and second embodiments, respectively, and FIGS. 2 and 4 are diagrams for explaining the projection beam characteristics of the first and second embodiments, respectively. (Main symbols) TX...Transmitter J, s, t SI
”・Floodlight 1.3.5...Light emitting element 2,4.6・
...Light projection lens 4 Figure 7, 7 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 目標物に向けて信号を投射し、当該信号の目標物での反
射信号を受信し、信号の投射時から反射信号の受信時ま
での時間を測定することによって目標物までの距離を知
るようにした測距レーダーに於いて、測距範囲に応じて
投射ビーム角の異った信号投射器を複数個設けた測距用
信号の送信装置。
The distance to the target is determined by projecting a signal toward a target, receiving the signal reflected by the target, and measuring the time from the time the signal is projected to the time the reflected signal is received. A distance measurement signal transmitting device for a distance measurement radar equipped with a plurality of signal projectors with different projection beam angles depending on the distance measurement range.
JP59272182A 1984-12-24 1984-12-24 Transmitter for signal for range measurement Pending JPS61149876A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59272182A JPS61149876A (en) 1984-12-24 1984-12-24 Transmitter for signal for range measurement

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59272182A JPS61149876A (en) 1984-12-24 1984-12-24 Transmitter for signal for range measurement

Publications (1)

Publication Number Publication Date
JPS61149876A true JPS61149876A (en) 1986-07-08

Family

ID=17510223

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59272182A Pending JPS61149876A (en) 1984-12-24 1984-12-24 Transmitter for signal for range measurement

Country Status (1)

Country Link
JP (1) JPS61149876A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5623509A (en) * 1994-03-01 1997-04-22 Seiko Epson Corporation Semiconductor laser and light-sensing device using the same
WO2017126294A1 (en) * 2016-01-22 2017-07-27 株式会社デンソー Optical range-finding device
JP2017134052A (en) * 2016-01-22 2017-08-03 株式会社デンソー Optical range finder
CN112470035A (en) * 2018-12-06 2021-03-09 松下知识产权经营株式会社 Distance information acquisition device, distance information acquisition method, and program
WO2023153438A1 (en) * 2022-02-09 2023-08-17 株式会社小糸製作所 Light projector, light receiver, and measurement device

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5863871A (en) * 1981-10-14 1983-04-15 Fujitsu Ten Ltd Car radar

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5863871A (en) * 1981-10-14 1983-04-15 Fujitsu Ten Ltd Car radar

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5623509A (en) * 1994-03-01 1997-04-22 Seiko Epson Corporation Semiconductor laser and light-sensing device using the same
WO2017126294A1 (en) * 2016-01-22 2017-07-27 株式会社デンソー Optical range-finding device
JP2017134052A (en) * 2016-01-22 2017-08-03 株式会社デンソー Optical range finder
CN112470035A (en) * 2018-12-06 2021-03-09 松下知识产权经营株式会社 Distance information acquisition device, distance information acquisition method, and program
WO2023153438A1 (en) * 2022-02-09 2023-08-17 株式会社小糸製作所 Light projector, light receiver, and measurement device

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