JPS58142271A - Transmission laser beam measurement of laser radar - Google Patents
Transmission laser beam measurement of laser radarInfo
- Publication number
- JPS58142271A JPS58142271A JP2460482A JP2460482A JPS58142271A JP S58142271 A JPS58142271 A JP S58142271A JP 2460482 A JP2460482 A JP 2460482A JP 2460482 A JP2460482 A JP 2460482A JP S58142271 A JPS58142271 A JP S58142271A
- Authority
- JP
- Japan
- Prior art keywords
- laser beam
- diameter
- target
- laser
- measured
- 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.)
- Granted
Links
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
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
- G01S7/497—Means for monitoring or calibrating
-
- 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
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/48—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
- G01S7/483—Details of pulse systems
- G01S7/484—Transmitters
Abstract
Description
【発明の詳細な説明】
本発明はレーザレーダ装置の送信レーザビームの測定方
法に関するものであり、更に詳しくは人工衛星レーザレ
ーダ装置などパルスレーザを使用するレーザレーダ装置
の送信レーザビームの簡易な”m定方性に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring a transmitted laser beam of a laser radar device, and more specifically, a method for measuring a transmitted laser beam of a laser radar device using a pulsed laser such as a satellite laser radar device. Regarding m-orthotropy.
人工衛星レーザ測距装置などのレーザレーダ装置では、
送信レーずビームの径や拡がシ角などを測定し較正する
手段がシステムを運用−保守する上で必要とされる・し
かし、レーダレーダ装置の送信レーザビームは大−口径
でかつその拡がり角が狭小という特徴を有している・こ
れは1次の様な理由による。即ち、レーザレー・ダ装置
の送信レーザビームは送信望遠鏡あるいはコリメータと
称する光学系を1通して射出するのが晋通である。この
目的はレーザ発振器から出力されるビームの拡がp角を
適切に設定し、制御するためであシ、一般に送信レーザ
ビーム径Fi該光学系にょシレーザ発振器から出力され
るビーム径に比らべて、数倍から数十倍に拡大変換され
る。1+、送信レーザビームの拡がフ角は、一般にレー
ザ発振器から出力されるビームよりも狭小にすることを
目的としている。そこで、レーずレーダ装置から射出さ
れる送信レーザビームは、大口径でかつ狭小の拡がり角
を有するものとなシ、そのため送信レーザビームの径測
定−及び拡がシ角測定は容易ではなく、簡単で精度の良
いレーザレーダ装置の送信レーザビームの測定方法の開
発が望まれてい友。In laser radar devices such as satellite laser ranging devices,
A means to measure and calibrate the diameter and divergence angle of the transmitted laser beam is required for system operation and maintenance.However, the transmitted laser beam of radar radar equipment has a large diameter and its divergence angle. It has the characteristic of being narrow. This is due to the following reasons. That is, the transmitting laser beam of a laser radar device is normally emitted through an optical system called a transmitting telescope or a collimator. The purpose of this is to appropriately set and control the p-angle of the beam output from the laser oscillator. Generally, the transmitted laser beam diameter Fi is compared to the beam diameter output from the laser oscillator. The image is enlarged several times to several tens of times. 1+, the spread angle of the transmitted laser beam is generally intended to be narrower than the beam output from the laser oscillator. Therefore, the transmitted laser beam emitted from the laser radar device has a large diameter and a narrow divergence angle, and therefore it is not easy to measure the diameter and divergence angle of the transmitted laser beam. Therefore, it is desired to develop a method for measuring the transmitted laser beam of a laser radar device with high precision.
従来の送信レーザビームの測定手段としては、送信レー
ザビームのビーム軸に垂直な断面の電力強変分布を測定
し、この測定値から送信レーザビームの径を求めるもの
が知られている@しかし、この様な従来の手段はビーム
軸に直角にピンホール、スリット、ナイフェツジ等を移
動走査し、このときの通過電力の変化を測定するもので
あるため、大口径の送信レーザビームをカバーできる大
型の移動走査機構や通過ビームの電力測定に用いる大口
径の集光光学系などが必要であるという欠点があった。As a conventional method for measuring a transmitted laser beam, it is known to measure the strongly variable power distribution in a cross section perpendicular to the beam axis of the transmitted laser beam, and calculate the diameter of the transmitted laser beam from this measurement value. These conventional methods move and scan pinholes, slits, knives, etc. at right angles to the beam axis and measure changes in the passing power at this time. The drawback is that it requires a moving scanning mechanism and a large-diameter condensing optical system used to measure the power of the passing beam.
また、送信レーザビームの拡が9角が狭小であるため、
拡が1角を正確に求めるためには十分に遠方でビーム径
を測定する必要があり、上記大型の装置を運搬して測定
する必要があp1多大の時間と労力を要するという欠点
があり九。In addition, since the spread of the transmitted laser beam is narrow at 9 angles,
In order to accurately determine the angle of divergence, it is necessary to measure the beam diameter from a sufficiently far distance, and the large device described above must be transported and measured, which requires a great deal of time and effort. .
本発明はかかる従来技術の欠点に鑑みなされ九・もので
、人工衛星レーザ測距装置などレーザレーダ装置の送信
レーザビームのビーム径及び拡がり角を簡単かつ正確に
測定できるレーザレーダ装置の送信レーザビーム測定方
法を提供することを目的としている〇
本発明のレーザレーダ装置の送信レーザビーム測定方法
は、レーザレーダ装置の本来・有する機能を利用し、ピ
ンホール、スリット、ナイフェツジ等に代わシ、被測定
レーザビームのビーム軸に斜め角度で細長い形状の反射
標的を配置し、この反射標的からの反射光の拡がりを遠
隔検知し、この反射光の拡が9値と被測定レーザビーム
のパルス幅と反射標的の被測定レーザビームに対する上
記斜め角度の値から被測定レーザビームのビーム径を求
めることを特徴としている。尚、この発明の方法は人工
衛星レーザ測距装置に使用きれるようなパルス幅の短い
パルスレーザに通用すると効果が大であるとい5411
1がある。The present invention has been made in view of the drawbacks of the prior art, and provides a transmitting laser beam of a laser radar device that can easily and accurately measure the beam diameter and divergence angle of a transmitting laser beam of a laser radar device such as an artificial satellite laser ranging device. The purpose of the present invention is to provide a measurement method for a transmitted laser beam of a laser radar device, which utilizes the original functions of the laser radar device and uses the measurement target instead of a pinhole, slit, knife, etc. An elongated reflective target is placed at an oblique angle to the beam axis of the laser beam, and the spread of the reflected light from this reflective target is remotely detected. The present invention is characterized in that the beam diameter of the laser beam to be measured is determined from the value of the oblique angle of the target with respect to the laser beam to be measured. It should be noted that the method of the present invention is highly effective when applied to pulsed lasers with short pulse widths that can be used in satellite laser ranging devices.5411
There is 1.
以下添付の図面に示す実施例;により、更に詳細に本発
明について説明する。添付の図面において、lOは被測
定レーザビーム13を出力するレーザレー・ダ装置であ
る0また、114レ一ザ発振器であシ、12II′iレ
ーザ送信光学系であり、13はレーザ送信光学系12か
ら射出されるパルス幅でのレーザビ−ムである。14は
レーザレーダ装置10から距離ρだけ隔てた場所に、被
測定レーザビーム13に対して角glの傾斜をもって設
置された細長い形状の標的である。15は標的14から
の反射光であり、16はレーザレーダ装置10の受信光
学系で1)、17は検知器である。更に、1gはオシロ
スコープであp、検知器17の出力で反射光15をトレ
ースするものであるO
この系にンいて、距離ρにおける被測定レーザビーム1
3の径をdとし、また被測定レーザビーム13と標的1
4が父わるビーム軸方向長さをLとし、)τの条件を満
足するものとするO但し、Cは光速である0
この場合、オシロスコープ18上で観測される反射光1
5の波形の広がシtは、訃よそ次の11)式で費わされ
る0
t−y+τ ・・・・・・・・・・・・・・・・・・
・・・・・・・・・(11tた、送信レーザビーム13
の径dは次の(2)式で表わされる。The present invention will be explained in more detail with reference to embodiments shown in the accompanying drawings. In the accompanying drawings, 10 is a laser radar device that outputs a laser beam 13 to be measured, 114 is a laser oscillator, 12 is a laser transmission optical system, and 13 is a laser transmission optical system 12. A laser beam with a pulse width emitted from Reference numeral 14 denotes an elongated target installed at a distance ρ from the laser radar device 10 and inclined at an angle gl with respect to the laser beam 13 to be measured. 15 is reflected light from the target 14, 16 is a receiving optical system 1) of the laser radar device 10, and 17 is a detector. Furthermore, 1g is an oscilloscope p, which traces the reflected light 15 with the output of the detector 17.
3 is the diameter of d, and the laser beam to be measured 13 and the target 1 are
4 is the length in the axial direction of the beam, and the condition of ) τ is satisfied. However, C is the speed of light. In this case, the reflected light 1 observed on the oscilloscope 18
The spread of the waveform of No. 5, t, is 0 t-y+τ ・・・・・・・・・・・・・・・・・・
・・・・・・・・・(11t, transmission laser beam 13
The diameter d is expressed by the following equation (2).
d峻A*tan# ・・・・・・・・・・・・・・・
・・・・・・・・・・・・(21第(1)式と第(2)
式から送信レーザビーム13の径dは次の(3)式で求
められる。dshunA*tan# ・・・・・・・・・・・・・・・
・・・・・・・・・・・・(21 Equation (1) and Equation (2)
From the formula, the diameter d of the transmitted laser beam 13 can be determined by the following formula (3).
d−2(i−τ)・を龍θ・・・・・・・・・・・・・
・・・・・+3)以上の説明から明らかな様に、送信レ
ーザビーム13のパルス幅τと標的14の設置角度θが
わかれば、反射波15の拡がり幅tをオシロスコープ1
8で測定することにより、距離ρにおける送信レーザビ
ーム13の径dが容易に求められる0以上の説明から明
らかな様に本発明の方法によれば、簡単な形状の標的を
被測定レーザビーム上に配置するだけで被測定レーザビ
ームのビーム径を容易に測定することが可能になる@ま
た、被測定レーザビームの拡がり角の測定は、真なる距
離の2ケ所以上に標的を配置して、それぞれの位置にお
ける被測定レーザビームのビーム径を測定することによ
p、精度良く求めることがで暑る@この場合、標的が簡
単な形状・構造で良いため複数個の設置も大変容易であ
るという効果を有する。d-2(i-τ)・is dragon θ・・・・・・・・・・・・
...+3) As is clear from the above explanation, if the pulse width τ of the transmitted laser beam 13 and the installation angle θ of the target 14 are known, the spread width t of the reflected wave 15 can be calculated using the oscilloscope 1.
By measuring at 8, the diameter d of the transmitted laser beam 13 at the distance ρ can be easily determined. The beam diameter of the laser beam to be measured can be easily measured by simply placing the target at two or more locations at the true distance. By measuring the beam diameter of the laser beam to be measured at each position, it is possible to obtain it with high precision.In this case, the target can be of simple shape and structure, so it is very easy to install multiple targets. It has this effect.
添付の図面は本発明のレーザレーダ装置の送信レーザビ
ーム測定方法の一実施例を示す図である・lO・・・レ
ーザレーダ装置、 11・・・レーザ発振器、12・・
・レーザ送信光学系、13・・・被測定レーザビーム、
14・・・標的、15・・・反射光、16・・・受信光
学系、17・・・検知器、18・・・オシロスコープ。
代理人 弁理士 秋 本 正 実The attached drawings are diagrams showing an embodiment of a method for measuring a transmitted laser beam of a laser radar device according to the present invention. 1O... Laser radar device, 11... Laser oscillator, 12...
- Laser transmission optical system, 13... Laser beam to be measured,
14...Target, 15...Reflected light, 16...Reception optical system, 17...Detector, 18...Oscilloscope. Agent Patent Attorney Masami Akimoto
Claims (1)
斜め角度に配置され九11IIl定レーザビームのビー
ム径より小さい幅の細長い形状の反射標的を配設し、皺
反射標的からの被測定レーザビームの反射光の拡がりを
遠隔検知し、該反射光の拡が910値と被測定レーザビ
ームのパルス幅と反射標的の被測定レーザビームに対す
る上記斜め角度値から被測定レーザビームのビーム径を
求めることを特徴とするレーザレーダ装置の送信レーザ
ビーム測定方法。Column 511 A reflective target in an elongated shape, which is arranged at an oblique angle with respect to the laser beam and has a width smaller than the beam diameter of the 911III constant laser beam, is arranged on the 511 constant laser beam, and the laser beam to be measured from the wrinkled reflective target is remotely detecting the spread of the reflected light, and determining the beam diameter of the laser beam to be measured from the 910 value of the spread of the reflected light, the pulse width of the laser beam to be measured, and the oblique angle value of the reflection target with respect to the laser beam to be measured. A method for measuring a transmitted laser beam of a laser radar device, characterized by:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2460482A JPS58142271A (en) | 1982-02-19 | 1982-02-19 | Transmission laser beam measurement of laser radar |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2460482A JPS58142271A (en) | 1982-02-19 | 1982-02-19 | Transmission laser beam measurement of laser radar |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS58142271A true JPS58142271A (en) | 1983-08-24 |
JPH0126514B2 JPH0126514B2 (en) | 1989-05-24 |
Family
ID=12142748
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2460482A Granted JPS58142271A (en) | 1982-02-19 | 1982-02-19 | Transmission laser beam measurement of laser radar |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58142271A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0446691A (en) * | 1990-06-14 | 1992-02-17 | Mitsubishi Heavy Ind Ltd | Method for measuring divergent angle of yag laser beam |
JP2017032459A (en) * | 2015-08-04 | 2017-02-09 | 日本電気株式会社 | Target designation laser observation system |
-
1982
- 1982-02-19 JP JP2460482A patent/JPS58142271A/en active Granted
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0446691A (en) * | 1990-06-14 | 1992-02-17 | Mitsubishi Heavy Ind Ltd | Method for measuring divergent angle of yag laser beam |
JP2017032459A (en) * | 2015-08-04 | 2017-02-09 | 日本電気株式会社 | Target designation laser observation system |
Also Published As
Publication number | Publication date |
---|---|
JPH0126514B2 (en) | 1989-05-24 |
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