TWI616646B - Laser based distance measurement device - Google Patents
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Abstract
一種雷射測距裝置,係包括測距體、彈性體、弧形反射體、參考球體,其中,測距體係具有凸管於該測距體之底部,彈性體係對應地設置於該凸管中,弧形反射體係設置於該彈性體下方,而參考球體係頂靠於該弧形反射體。弧形反射體係用以反射雷射光束,參考球體作為該弧形反射體運動方向的導引,使該測距體產生平行光軸方向與垂直光軸方向之位移時,令量測結果保持正確。 A laser ranging device includes a distance measuring body, an elastic body, an arc reflecting body and a reference sphere, wherein the distance measuring system has a convex tube at the bottom of the distance measuring body, and the elastic system is correspondingly disposed in the convex tube The arc reflecting system is disposed under the elastic body, and the reference ball system is abutted against the arc reflecting body. The arc reflection system is used to reflect the laser beam, and the reference sphere is used as a guide for the movement direction of the arc reflector, so that the distance measurement body maintains the displacement of the parallel optical axis direction and the vertical optical axis direction, so that the measurement result remains correct. .
Description
本案係一種雷射測距裝置,尤指一種搭配弧形反射體與參考球體之雷射測距裝置。 The present invention relates to a laser ranging device, and more particularly to a laser ranging device matched with a curved reflector and a reference sphere.
高精密雷射測距裝置係大幅應用於各類產業,例如精密機械業、工具機業、航太業、船舶業、汽車業以及營建業等。對於精密機械業三維尺寸量測來說,目前量測精度最佳的是自動追蹤雷射測距儀,例如德國的LaserTRACER。 High-precision laser range finder is widely used in various industries, such as precision machinery, machine tool industry, aerospace industry, shipbuilding industry, automobile industry and construction industry. For the three-dimensional measurement of precision machinery industry, the best measurement accuracy is automatic tracking laser range finder, such as LaserTRACER in Germany.
LaserTRACER之重要元件係包括參考球體,此參考球體一般係為鏡面鋼球,具體言之,雷射測距裝置之雷射光束在經過分光、反射等過程後的光束品質,與參考球體之鏡面品質具有密切關聯性,然而,運作過程中,容易令參考球體之球面產生瑕疵,而此瑕疵會影響光束品質,進而降低測距之精度。由於參考球體為鋼製,在溫度變化較大的場合下,參考球體因溫度所產生的尺寸熱膨脹變化,也會降低測距之精度。 The important components of LaserTRACER include the reference sphere, which is generally a mirrored steel ball. Specifically, the beam quality of the laser beam of the laser ranging device after the process of splitting and reflection, and the mirror quality of the reference sphere. It is closely related. However, during operation, it is easy to cause the spherical surface of the reference sphere to produce flaws, which will affect the beam quality and thus reduce the accuracy of the ranging. Since the reference sphere is made of steel, in the case where the temperature changes greatly, the reference thermal expansion of the sphere due to the temperature changes, which also reduces the accuracy of the distance measurement.
再者,參考球體與搭配之凸透鏡間的距離會因為轉動軸承跳動誤差的關係,隨著運作過程改變,而此距離變化會使雷射光束焦點無法精準地落在參考球體之球心,進而 影響反射效果,降低量測精度。 Furthermore, the distance between the reference sphere and the matching convex lens may change due to the running error of the rotating bearing, and the change of the distance may cause the focus of the laser beam to not accurately fall on the center of the reference sphere. Affects the reflection effect and reduces the measurement accuracy.
習知技術中,復有將角耦反射鏡透過治具與參考球體連接之技術,然而,由於與參考球體之接觸方式係平面接觸,故在運作過程中,角耦反射鏡的平行位移和角度旋轉會導致量測誤差。 In the prior art, there is a technique of connecting the angular coupling mirror through the jig and the reference sphere. However, since the contact with the reference sphere is in planar contact, the parallel displacement and angle of the angular coupling mirror during operation are Rotation can cause measurement errors.
因此,如何解決前述設計上的瑕疵,實已成業界亟欲解決的課題。 Therefore, how to solve the flaws in the aforementioned design has become an issue that the industry is eager to solve.
為了克服習知技術之種種瑕疵,本案係提供了一種雷射測距裝置 In order to overcome the various flaws of the prior art, the present invention provides a laser ranging device.
該雷射測距裝置係包括測距體、弧形反射體、參考球體以及彈性體,其中,測距體係具有凸管於該測距體底部;彈性體係對應地設置於該凸管中;弧形反射體係設置於該彈性體下方;參考球體係頂靠於該弧形反射體,弧形反射體內部的反射面係用以反射雷射光束,參考球體係作為該弧形反射體運動方向的導引,使該測距體產生平行光軸方向與垂直光軸方向之位移時,令量測結果保持正確。 The laser ranging device includes a distance measuring body, a curved reflector body, a reference sphere body and an elastic body, wherein the distance measuring system has a convex tube at the bottom of the distance measuring body; the elastic system is correspondingly disposed in the convex tube; the arc The reflective system is disposed under the elastic body; the reference ball system is abutted against the curved reflector, and the reflective surface inside the curved reflector is used to reflect the laser beam, and the reference ball system is used as the moving direction of the curved reflector. The guiding result is such that the measuring body produces a displacement in the direction of the parallel optical axis and the direction of the vertical optical axis, so that the measurement result remains correct.
相較於習知技術,由於本案之弧型反射體得使雷射光束無須直接藉由參考球體進行反射,亦即參考球體之瑕疵或作動皆不會影響量測品質,又因本案之參考球體材質可使用低熱膨脹材質製造,進而得以改善量測誤差。 Compared with the prior art, since the arc-shaped reflector of the present case does not need to directly reflect the laser beam by the reference sphere, that is, the reference sphere does not affect the measurement quality, and the reference sphere of the present case The material can be made from a low thermal expansion material to improve measurement error.
11‧‧‧弧形反射體 11‧‧‧Arc reflector
110‧‧‧反射面 110‧‧‧reflecting surface
12‧‧‧參考球體 12‧‧‧Reference sphere
13‧‧‧彈性體 13‧‧‧ Elastomers
14‧‧‧測距體 14‧‧‧ verning body
15‧‧‧目標反射鏡 15‧‧‧Target mirror
16‧‧‧凸管 16‧‧‧Concave tube
17‧‧‧線性位移拘束元件 17‧‧‧ Linear Displacement Constraints
L1、L2、L3、L4‧‧‧距離 L1, L2, L3, L4‧‧‧ distance
△L、δL、δb‧‧‧位移 △L, δ L , δ b ‧‧‧ displacement
Rb、Rc‧‧‧半徑 Radius of R b , R c ‧‧‧
第1圖係為本案之雷射測距裝置之一結構示意圖;第2圖係為本案之測距體產生平行量測光軸方向位移 之作動示意圖;第3圖係為本案之測距體產生垂直量測光軸方向位移之作動示意圖;第4圖係為第3圖之模型化計算圖;第5圖係為本案之測距體之橫向位移與光程差之XY散布圖;以及第6圖係為本案之線性位移拘束元件套設於弧形反射體之結構示意圖。 The first picture is a schematic diagram of one of the laser ranging devices of the present case; the second picture is the displacement of the parallel measuring optical axis in the measuring body of the present case. Schematic diagram of the operation; Figure 3 is a schematic diagram of the displacement of the measuring body in the vertical direction of the measuring body in the direction of the measuring body; Figure 4 is the model calculation drawing of Figure 3; Figure 5 is the measuring body of the case The XY scatter diagram of the lateral displacement and the optical path difference; and the sixth figure is a schematic structural view of the linear displacement restraining element of the present invention disposed on the curved reflector.
以下藉由特定之具體實施例加以說明本揭露之實施方式,而熟悉此技術之人士可由本說明書所揭示之內容輕易地瞭解本揭露之其他優點和功效,亦可藉由其他不同的具體實施例加以施行或應用。 The embodiments of the present disclosure are described in the following specific embodiments, and those skilled in the art can easily understand other advantages and functions of the disclosure by the contents disclosed in the present specification, and can also use other different embodiments. Implement or apply.
請參閱第1圖,第1圖係為本案之雷射測距裝置之一結構示意圖。 Please refer to FIG. 1 , which is a schematic structural view of one of the laser ranging devices of the present invention.
如圖所示,本案之雷射測距裝置,包括弧形反射體11、參考球體12、彈性體13、測距體14,其中,該測距體14可具備雷射光源、偏振片、極化分光鏡、1/4 λ玻片、分光鏡、位移感測器、擴束鏡、雷射干涉儀感測器等光學元件。 As shown in the figure, the laser ranging device of the present invention comprises a curved reflector 11, a reference sphere 12, an elastic body 13, and a distance measuring body 14, wherein the distance measuring body 14 can be provided with a laser light source, a polarizing plate and a pole. Optical components such as a beam splitter, a 1/4 λ slide, a beam splitter, a displacement sensor, a beam expander, and a laser interferometer sensor.
於本實施例中,測距體14係具有凸管16於該測距體14之底部,彈性體13係對應地設置於該凸管16中,弧形反射體11係設置於該彈性體13下方,參考球體12係頂靠於該弧形反射體11,其中,該弧形反射體11內部的反射 面110係用以反射雷射光束,該參考球體12作為該弧形反射體11運動方向的導引,使該測距體14產生平行光軸方向與垂直光軸方向之位移時,令量測結果保持正確。 In the present embodiment, the distance measuring body 14 has a convex tube 16 at the bottom of the distance measuring body 14, and the elastic body 13 is correspondingly disposed in the convex tube 16, and the curved reflector 11 is disposed on the elastic body 13. Below, the reference sphere 12 is placed against the arc reflector 11 , wherein the reflection inside the arc reflector 11 The surface 110 is used to reflect the laser beam, and the reference sphere 12 serves as a guide for the direction of movement of the arc reflector 11 so that the distance measuring body 14 generates a displacement between the parallel optical axis direction and the vertical optical axis direction, and the measurement is performed. The result remains correct.
於一實施例中,該參考球體12係可為金屬或非金屬材質所製成者,例如,所述之金屬之材質係可為不銹鋼、鋁、鐵或铟鋼等鏡面可反射雷射光之材質,而所述之非金屬之材質係可為陶瓷、玻璃、紅寶石、碳纖維或玻璃陶瓷。 In one embodiment, the reference sphere 12 can be made of a metal or a non-metal material. For example, the metal material can be a mirror-reflective laser light material such as stainless steel, aluminum, iron or indium steel. The non-metallic material may be ceramic, glass, ruby, carbon fiber or glass ceramic.
於一實施例中,該弧形反射體11係可內建有反射面110,例如可為內球面反射鏡。依據不同之應用情境,弧形反射體11亦可內建有其它型態的反射單元,例如平面反射鏡、貓眼反射鏡、角耦反射鏡,或是聚焦透鏡及凹面鏡之整合模組,而為了配合內建之反射單元,弧形反射體11上半部之結構亦可不同於圖式之半圓形。 In an embodiment, the curved reflector 11 can have a reflective surface 110 built therein, for example, an inner spherical mirror. Depending on the application scenario, the curved reflector 11 may also have other types of reflective units, such as a planar mirror, a cat's eye mirror, a corner-coupled mirror, or an integrated module of a focusing lens and a concave mirror, and With the built-in reflection unit, the structure of the upper half of the arc reflector 11 can also be different from the semicircle of the figure.
於一實施例中,該彈性體13係可為壓縮彈簧、板形彈簧、盤型彈簧、彈片彈簧、皿型彈簧、橡膠彈簧或O型環(o-ring),並對應地設置於凸管16中,而凸管16係位於測距體14之底部。具體言之,彈性體13施力於該弧形反射體11之施力方向,係可平行於雷射光束之光軸方向。 In an embodiment, the elastic body 13 can be a compression spring, a plate spring, a disc spring, a spring spring, a dish spring, a rubber spring or an O-ring, and is correspondingly disposed on the convex tube. 16 and the convex tube 16 is located at the bottom of the distance measuring body 14. Specifically, the elastic body 13 applies a force to the direction of the force of the arc reflector 11 to be parallel to the optical axis direction of the laser beam.
實際實施時,該測距體14係可為積分型雷射干涉儀、都卜勒測距儀,或絕對測距型式之雷射測距儀。該彈性體13一端頂靠於該測距體14,另一端施力於該弧形反射體11,且施力方向平行於雷射光軸之方向,以令該弧形反射體11之底部弧面能持續地接觸該參考球體12之球面。 In actual implementation, the distance measuring body 14 can be an integral laser interferometer, a Doppler range finder, or an absolute ranging type laser range finder. One end of the elastic body 13 abuts against the distance measuring body 14 , and the other end applies a force to the curved reflector 11 , and the direction of the force is parallel to the direction of the laser optical axis, so that the bottom surface of the curved reflector 11 is curved. The spherical surface of the reference sphere 12 can be continuously contacted.
請參閱第2圖,第2圖係為本案之測距體產生平行量 測光軸方向位移之作動示意圖。 Please refer to Figure 2, which is the parallel amount of the measuring body in this case. Schematic diagram of the displacement of the metering axis direction.
如圖所示,L1為該弧形反射體11與該參考球體12之交點到該測距體14底部之距離,L2為目標反射鏡15到該測距體14底部之距離,L為該目標反射鏡15到該弧型反射體11與該參考球體12交點的總距離(即L1+L2)。當測距體14產生平行量測光軸方向之位移△L,L1’=L1+△L,L2’=L2-△L,該目標反射鏡15到該弧型反射體11與該參考球體12交點的原始總距離為L1’+L2’,仍等於L,因此不會產生光程差。 As shown, L1 is the distance from the intersection of the arc reflector 11 and the reference sphere 12 to the bottom of the distance measuring body 14, L2 is the distance from the target mirror 15 to the bottom of the distance measuring body 14, and L is the target. The total distance (i.e., L1 + L2) of the mirror 15 to the intersection of the arc-shaped reflector 11 and the reference sphere 12. When the distance measuring body 14 generates the displacement ΔL in the direction of the parallel measuring optical axis, L1'=L1+ΔL, L2'=L2-ΔL, the target mirror 15 reaches the intersection of the curved reflecting body 11 and the reference spherical body 12. The original total distance is L1'+L2', which is still equal to L, so there is no optical path difference.
請一併參閱第3圖至第5圖,第3圖係為本案之測距體產生垂直量測光軸方向位移之作動示意圖,第4圖係為第3圖之模型化計算圖,第5圖係為本案之測距體之橫向位移與光程差之XY散布圖,其中X軸為測距體14橫向位移,Y軸為光程差,單位為微米。 Please refer to Fig. 3 to Fig. 5 together. Fig. 3 is a schematic diagram of the displacement of the measuring body in the direction of the vertical measuring optical axis in the case, and Fig. 4 is the model calculation drawing of Fig. 3, the fifth The figure is an XY scatter diagram of the lateral displacement and optical path difference of the ranging body of the present case, wherein the X axis is the lateral displacement of the distance measuring body 14, and the Y axis is the optical path difference, and the unit is micrometer.
如第3圖所示,其中,L3為該弧形反射體11與該參考球體12交點到該測距體14底部之距離,L4為該測距體14產生垂直量測光軸方向位移後該弧形反射體11與該參考球體12交點到該測距體14底部之距離,是以,δL=L4-L3。 As shown in FIG. 3, where L3 is the distance from the arc-shaped reflector 11 and the reference sphere 12 to the bottom of the distance measuring body 14, L4 is the displacement of the distance measuring body 14 in the direction of the vertical measuring optical axis. The distance between the curved reflector 11 and the reference sphere 12 to the bottom of the distance measuring body 14 is δ L = L4 - L3.
透過如第4圖進行分析,得到一方程式:
其中,Rb為該參考球體12之半徑;Rc為該弧形反射體11之半徑;以及δb為該測距體14之橫向位移。 Where R b is the radius of the reference sphere 12; R c is the radius of the arc reflector 11; and δ b is the lateral displacement of the distance measuring body 14.
如第5圖所示,當該測距體14之橫向位移δb在正負5微米時,所造成之光程差遠小於10nm。轉軸之跳動誤差一般都可控制在正負5微米,因此該測距體14所產生垂直量測光軸方向位移之光程差對量測結果幾乎不會影響。 As shown in Fig. 5, when the lateral displacement δ b of the distance measuring body 14 is at plus or minus 5 μm, the resulting optical path difference is much smaller than 10 nm. The runout error of the rotating shaft can generally be controlled at plus or minus 5 micrometers. Therefore, the optical path difference of the displacement of the vertical measuring optical axis generated by the measuring body 14 has little influence on the measurement result.
請參閱第6圖,第6圖係為本案之線性位移拘束元件17套設於弧形反射體11之結構示意圖。如圖所示,線性位移拘束元件17係搭配凸管16套設住該弧形反射體11,以限制、維持該弧形反射體11之活動範圍,進而減少量測誤差。於一實施例中,線性位移拘束元件17係可為保持片、空心圓環、線性滑軌或直線軸承。而線性位移拘束元件17之設置方向,係可垂直於雷射光束之光軸方向。 Please refer to FIG. 6 , which is a schematic structural view of the linear displacement restraining element 17 of the present invention which is sleeved on the curved reflector 11 . As shown, the linear displacement restraining element 17 is fitted with the convex tube 16 to cover the arc reflector 11 to limit and maintain the range of motion of the arc reflector 11, thereby reducing measurement errors. In one embodiment, the linear displacement restraining element 17 can be a retaining plate, a hollow ring, a linear slide or a linear bearing. The linear displacement restraining element 17 is disposed perpendicular to the optical axis of the laser beam.
綜上所述,本案之弧型反射體得使雷射光束無須直接藉由參考球體進行反射,是故參考球體之球面瑕疵不會影響量測品質,且參考球體得藉由多種材質構成,如使用低膨脹係數材質製造,可大幅減少尺寸熱膨脹所造成的量測誤差;再者,由於本案之弧型反射體與參考球體能始終保持著弧面對弧面之接觸關係,故弧形反射體之中心至參考球體之中心的距離,不會因為設備作動而改變,進而得以避免因光程差所造成之量測誤差。 In summary, the arc-shaped reflector of the present case does not need to directly reflect the laser beam by the reference sphere, so the spherical surface of the reference sphere does not affect the measurement quality, and the reference sphere can be composed of various materials, such as Made of low expansion coefficient material, it can greatly reduce the measurement error caused by dimensional thermal expansion. Moreover, since the arc-shaped reflector and the reference sphere in this case can always maintain the contact relationship of the arc facing the arc surface, the arc reflector The distance from the center to the center of the reference sphere is not changed by the operation of the device, and the measurement error caused by the optical path difference can be avoided.
上述實施形態僅為例示性說明本揭露之技術原理、特點及其功效,並非用以限制本揭露之可實施範疇,任何熟習此技術之人士均可在不違背本揭露之精神與範疇下,對上述實施形態進行修飾與改變。然任何運用本揭露所教示內容而完成之等效修飾及改變,均仍應為下述之申請專利 範圍所涵蓋。而本揭露之權利保護範圍,應如下述之申請專利範圍所列。 The above-mentioned embodiments are merely illustrative of the technical principles, features, and functions of the present disclosure, and are not intended to limit the scope of the disclosure. Any person skilled in the art can do without departing from the spirit and scope of the disclosure. The above embodiments are modified and changed. However, any equivalent modifications and changes made using the teachings of this disclosure should still be the following patent application. Covered by the scope. The scope of protection of the present disclosure should be as set forth in the following patent application.
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TW106106421A TWI616646B (en) | 2017-02-24 | 2017-02-24 | Laser based distance measurement device |
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Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
TWI329190B (en) * | 2007-05-25 | 2010-08-21 | Asia Optical Co Inc | Ranging system and method and apparatus of sampling signal for the same |
CN202563088U (en) * | 2012-05-02 | 2012-11-28 | 杭州钢冶科技有限公司 | Laser range finder |
TWI400429B (en) * | 2009-09-09 | 2013-07-01 | Asia Optical Co Inc | Optical system for monocular laser rangefinder |
CN103608642B (en) * | 2011-03-14 | 2016-02-24 | 法罗技术股份有限公司 | By the automatic measurement of laser tracker to dimension data |
CN103857984B (en) * | 2012-01-25 | 2016-08-24 | 法罗技术股份有限公司 | For environment being carried out the device of optical scanning and measurement |
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Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
TWI329190B (en) * | 2007-05-25 | 2010-08-21 | Asia Optical Co Inc | Ranging system and method and apparatus of sampling signal for the same |
TWI400429B (en) * | 2009-09-09 | 2013-07-01 | Asia Optical Co Inc | Optical system for monocular laser rangefinder |
CN103608642B (en) * | 2011-03-14 | 2016-02-24 | 法罗技术股份有限公司 | By the automatic measurement of laser tracker to dimension data |
CN103857984B (en) * | 2012-01-25 | 2016-08-24 | 法罗技术股份有限公司 | For environment being carried out the device of optical scanning and measurement |
CN202563088U (en) * | 2012-05-02 | 2012-11-28 | 杭州钢冶科技有限公司 | Laser range finder |
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