TWI252907B - Laser beam span module capable of simultaneously generating two mutually perpendicular optical indicating surfaces - Google Patents
Laser beam span module capable of simultaneously generating two mutually perpendicular optical indicating surfaces Download PDFInfo
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1252907 厂 光學指 )中曾 設有一 的垂直 學偏轉 成。從 兩片旋 射光垂 為水平 雷射指 射儀之 的施工中,需要一個或 基準。而在工程的現場,這 可見的,通常,最常用的基 較小的尺寸、很高的亮度、 準線和基準面的工具。 生一個光學水平面,或以外 作為垂直度量基準,這是不 一種結構輕巧、功耗低、構 學平面和垂直光學面的雷射 示面的 描述過 帶有空 光學偏 器可以 雷射模 轉的平 直的掃 面。 向儀」 應用裝 五、發明說明(1) 【本發明所屬 在建築、 參考面用以作 些基準參考面 準是水平面或 半導體雷 低廉的價格, 目前的雷 加機構輔助操 方便的。 本發明的 造簡易之同時 儀。 在創作人 及其應用」( 光學平面發生 馬達,一固定 生細光束的雷 度的鍍膜光學 光,通過轉軸 連續反射而掃 轉軸垂直地心 在創作人 8 8 2 0 2 5 5 6 )及 之技術領域】 室内裝修等工程 為測量、測定的 應該是確定的、 垂直面。 射器由於其具有 是常用於指示基 射掃描器僅能產 作,形成垂直面 主要目的是提供 可以產生水平光 前一專利「產生 案號:8 9 1 2 3 9 0 1 器;該發生器中 在該馬達轉軸上 射模組。垂直光 平面平行平板組 的通孔,部分為 描出與入射之雷 時,掃描平面即 另一專利「自動 全角位激光雷 組 雷射掃描模組 一種能線產生 心轴轉的驅動 轉器和一能產 是由兩互成4 5 組來的筆直 面平行平板所 描面。當這旋 (案號: 置」(美國申In 1252907, the factory optical index has a vertical deflection. One or the reference is required for the construction of a horizontal laser detector from two pieces of rotatory light. At the engineering site, this is visible, usually, the most commonly used tools with smaller dimensions, very high brightness, alignment and datum. Produce an optical level, or as a vertical metric, which is not a lightweight, low power, textured plane and vertical optical surface. The description of the laser surface with an optical optics can be lasered. Straight sweeping. Application to the instrument 5. Description of the invention (1) [The invention is used in construction and reference surfaces for reference. The reference plane is the price of water level or semiconductor mine. The current Reggae mechanism is convenient for operation. The invention is simple and easy to manufacture. In the creator and its application" (optical plane generating motor, a coated optical light with a fixed beam of light, through the continuous reflection of the rotating shaft and sweeping the axis perpendicular to the center of the heart in the creator 8 8 2 0 2 5 5 6) Technical field: Engineering such as interior decoration should be a defined, vertical surface for measurement and measurement. Since the ejector is commonly used to indicate that the base-radiation scanner can only be produced, the main purpose of forming a vertical plane is to provide a horizontal light that can be generated by the former patent "Generation Case Number: 8 9 1 2 3 9 0 1; The module is fired on the motor shaft. The vertical light plane is parallel to the through hole of the flat plate group, and part of the scanning and the incident lightning, the scanning plane is another patent "automatic full-angle laser laser group laser scanning module" The drive shaft that produces the mandrel rotation and the energy production are drawn by the straight parallel plates of the two groups of 45. When this is the case (the case number: set) (US application
第6頁 1252907Page 6 1252907
五、發明說明(2) 月案號;· 10/310894)曾描述過另一種能線產生弁風 路斗-· 义二, 〜予十面 益,匕包括:一筆直光束的發生器(亦稱雷射模組 和一光束擴展器,光束擴展器為一頂角為9 〇度的 、二 射面,它將雷射模組所發射的光束’沿其對稱軸 入射角呈垂直的一光學參考平面。 谀展成與 1相關雷射水平儀等諸多前案設計’概利用馬達 得:::稜鏡吨整體係受雲檯式支撑座所浮載,以確實1 何·水平角位,唯諸前索斗古 % X獲 k成使用上不夠輕巧利便等缺失。 禾螓疋善, 【本發 因 半反射 方式, 主要目 本 指向地 幅,可 本 面,為 方式, 直角關 本 帶動光 :及垂直基準’經偏轉器或 U光束,再藉各別光擴展 先幅和垂直面參考光幅為其 之擴展器,可依據 产’藉以聯動垂直面之光 衩周圍任一位置。 2:光學偏轉器所射反射 八古 ’可採半反射鍍膜 接穿透,藉以同步獲得 2器之實施,可採由馬達 ’或利用圓錐形反射錐 明之内容】 此,本發明 方式,獲得 而同步獲得 的。 發明之再一 心的垂直軸 在環狀任一 發明之再二 了同步形成 提供光束部 係之二道激 發明之第三 束進行掃描 特別針對水 一角向垂直 水平面參考 目的為垂直 線為中心而 角位照向環 目的為在相 =道垂直關 分折射及部 光束。 目的為該光 形成一光學V. Description of the invention (2) The case number of the month; · 10/310894) has described another kind of energy line to produce a hurricane road -· Yi 2, ~ to Xie Yi, including: a straight beam generator (also The laser module and a beam expander, the beam expander is a 9-degree apex angle, and the beam emitted by the laser module is perpendicular to the incident angle of the beam along its axis of symmetry. Reference plane. 谀 成 与 与 相关 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷 雷The front of the squadrons of the ancients X is not enough to be used in light and easy to use. He is good, [this is due to the semi-reflective method, the main target is pointing to the ground, the surface can be used, the way, the right angle is the light : and the vertical reference 'transformer or U beam, and then extend the first and vertical reference beam as its expander by the respective light, according to the position of the origin of the vertical plane of the light. 2: The optical deflector reflects the reflection of the eight ancient 'can be semi-reflective coating Through the synchronization to obtain the implementation of the two devices, the motor can be used or the content of the cone-shaped reflection cone can be used. The method of the present invention is obtained synchronously. The vertical axis of the invention is in the ring of any invention. Secondly, the third beam of the invention is provided to simultaneously form a beam beam system for scanning, especially for the vertical direction of the water angle to the vertical horizontal reference, and the angular position to the ring is for the vertical phase separation of the phase and the channel a beam of light. The purpose is to form an optical
第7頁 1252907 五、發明說明(3) 體,以直角關係擴展出光學平面 【本發 本 模組改 射錐體 別沿其 學平面 為 第一和 別稱為 的儀器 來的細 到垂直 反射鏡 射光束 該 穩定地 個反射 兩個反 夾角為 射角度 夾角偏 明之實施方式】 發明是使用一雷射模組,對上述水平及垂直的兩組 變、簡化。為線述方便,將空心馬達及錐形光束反 稱為光束擴展器。將兩上模組以垂直關係放置,分 旋轉對稱軸射入細光束就會產生兩個相互垂直的光 描述方便 第二光束 第二光學 產生兩個 至少通過 器方向。 學偏轉器 直角稜鏡 角。 法雖然簡 垂直狀態 的工作原 續作兩次 射面之夾 這時,光 這反射面 了以下 垂直的 第一和 將同時 光束將 的擴展 裏的光 ,或是 呈90 〇 分光方 保持在 面。它 射面連 itb兩反 無關。 差。當 ’兹將這兩個模組分別稱為水平的 擴展器;它們所產生的光學平面分 平面(光幅)。由於本發明所確定 相互垂直的光學平面,從雷射模組 一個光學偏轉器偏轉提供另一光束 可以是一個和入射光成45°的平面 ,利用其反射面使投出之光束與入 單,但是兩束光難以高精度準確而 ,為了克服這個問題,通常使用兩 理是基於這樣一個事實:當光線被 反射後,其出射光與入射光之間的 角的兩倍,而且與入射光本身的入 線偏轉的誤差僅取線於它們之間的 之間的夾角為45 °時,這兩束光將Page 7 1252907 V. Description of the invention (3) Body, extending the optical plane in a right angle relationship [The fine-to-vertical mirror of the module of the present invention is modified to be the first and other instruments along its learning plane. The embodiment of the present invention is to use a laser module to change and simplify the two levels of the above horizontal and vertical. For convenience of description, the hollow motor and the cone beam are referred to as beam expanders. Placing the two upper modules in a vertical relationship and splitting the symmetry axis into the beamlets produces two mutually perpendicular lights. Description The second beam The second beam produces two at least the director directions. Learn the deflector at right angles. Although the work of the simple vertical state is continued for two times of the face-to-face, at this time, the light reflects the following vertical first and will simultaneously hold the light in the extended beam or 90 〇 splitting. Its face is not related to itb. difference. When the two modules are referred to as horizontal expanders, respectively, the optical planes they produce are divided into planes (light amplitudes). Due to the mutually perpendicular optical plane determined by the present invention, the deflection of one optical deflector from the laser module provides that the other beam may be a plane at 45° to the incident light, and the reflected beam is used to make the projected beam and the input sheet. However, the two beams are difficult to be accurate and accurate. To overcome this problem, the two principles are usually based on the fact that when the light is reflected, the angle between the emitted light and the incident light is twice, and the incident light itself. The error of the incoming line deflection is only taken when the angle between them is 45 °, the two beams will
第8頁 1252907 五、發明說明(4) 有效相互垂直。 通過一整塊導光材質,我們將上述兩個反射面做成一 體,就形成了更為穩定的的五角稜鏡。這種偏轉器有四個 光學表面:兩個折射面相互垂直而兩個反射面成45 ,光 束經兩次折射、兩次反射作用後的光束與原入射光束當能 有效呈垂直。 本發明之光學偏轉器的應用,放射端亦可是同時產生 兩束相互垂直的分光光學元件,這種分光光學元件可以是 和入射光成4 5 °的半反射艘膜的平面平行透明平板,這 樣,入射光的一部分,如5 0 %被反射到與入射垂直的方向 上,而另餘下部分,如5 0%則沿入射方向穿過該膜,形成 直向光束。 上述分光光學元件可以是立方稜鏡:它為兩個直角稜 鏡沿其斜面膠合而成,其中至少一個斜面鍍有半反膜。這 樣,入射光的部分,如50%被反射到與入射垂直的方向 上,而餘下5 0 %則沿入射方向同軸穿透該稜鏡。 但是由於將該鍍膜平行平板厚度的影響,兩束光之間 將有一平行平移。為了消除兩光之間的位置偏差,引入一 補償平面平行透明平板,由它的厚度所引起的光線之間的 位移來抵消上述分光鏡帶來的位移。 同樣,為了兩束光難以高精度準確而穩定地保持在垂 直狀態,在本發明應用的分光光學元件亦可用兩片夾角為 4 5 °的平面平行透明平板,其中面對從光源入射光的平面 平行透明平板鍍有半反膜,而另一平面鍍有反射膜。入射Page 8 1252907 V. Description of invention (4) Effectively perpendicular to each other. Through a single piece of light guiding material, we make the two reflecting surfaces into one body, which forms a more stable pentagonal 稜鏡. The deflector has four optical surfaces: the two refractive surfaces are perpendicular to each other and the two reflecting surfaces are 45. The beam after two refractions and two reflections is effectively perpendicular to the original incident beam. In the application of the optical deflector of the present invention, the radiating end may simultaneously generate two mutually perpendicular spectroscopic optical elements, and the spectroscopic optical element may be a plane parallel transparent flat plate of a semi-reflective film which is at a temperature of 45° with incident light, such that A portion of the incident light, such as 50%, is reflected in a direction perpendicular to the incident, while the remaining portion, such as 50%, passes through the film in the incident direction to form a straight beam. The above-mentioned spectroscopic optical element may be a cubic crucible: it is formed by gluing two right-angle prisms along a slope thereof, at least one of which is plated with a semi-reflective film. Thus, a portion of the incident light, such as 50%, is reflected in a direction perpendicular to the incident, and the remaining 50% is coaxially penetrated in the incident direction. However, due to the effect of the parallel plate thickness of the coating, there will be a parallel translation between the two beams. In order to eliminate the positional deviation between the two lights, a compensation plane parallel transparent plate is introduced, and the displacement between the rays caused by the thickness thereof is offset to offset the displacement caused by the above-mentioned beam splitter. Similarly, in order to prevent the two beams from being accurately and accurately maintained in a vertical state, the spectroscopic optical element to which the present invention is applied may also use two plane-parallel transparent plates having an angle of 45°, in which a plane that faces light from the light source is faced. The parallel transparent plate is plated with a semi-reflective film while the other plane is plated with a reflective film. Incident
1252907 五、發明說明(5) 光首先射向鍍有半反膜的爭行透明平板,其一部分如 5 0 % ’沿入射方向穿過該不彳于透明平板沿原方向行進,餘 下5 0 %,則被它反射到鍍反射膜的平行平板上,經兩次連 續的反射形成與入射光垂直的光束。 在五角稜中,為了使部分光線沿原方向穿過該稜鏡, 其中正對從雷射模組來的光反射面改鍍半反膜。從它反射 的光被隨後的反射面再次反射成與原光束垂直的光束,而 透過半反膜的光因折射而偏離原入射方向,為了保持原方 向不變,在鍍以分光膜的卒面固定一光楔,光楔的角度被 選擇,使得這部分光束透過該光楔後形成一光束,與原射 向五角稜鏡的光束在同一直線上。 利用兩組光束擴展器及光學偏轉器就可以建立起自動 或手動的水平儀。 在本發明的第一個實施中,將雷射模組發出的細光 首先射向第一光束擴展器。第一光束擴展器一部分入射光 擴展為第一光學平面,而另一部分將穿過此擴展器保持 方向射向光學偏轉器,並由該偏轉器偏轉9 0。射向第二^ 束擴展器形成與第一光學平面垂直的第二光學平面。 光 上述實施,第一個光束偏轉器必須同時有光學分光 1展功能:其分光功能是將入射光分為兩部分,其中—^ 刀’士原方向不變;另一部份利用光束擴展功能將 與原入射方向垂直的光學平面。 擴展為 在本發明的第二個實施中,可將雷射模組發出的細“ 束’首先由分光光學元件以前置性分解為兩束相互垂=光 I的1252907 V. Description of invention (5) The light is first directed to a transparent plate coated with a semi-reflective film, a part of which is like 50% 'passing in the incident direction, which is not in the transparent plate, travels in the original direction, leaving the remaining 50%. Then, it is reflected on the parallel plate of the reflective film, and two consecutive reflections form a beam perpendicular to the incident light. In the pentagonal rib, in order to pass part of the light through the cymbal in the original direction, the light reflecting surface from the laser module is reformed with a semi-reflective film. The light reflected from it is reflected again by the subsequent reflecting surface into a beam perpendicular to the original beam, and the light transmitted through the semi-reflective film deviates from the original incident direction by refraction, and in order to maintain the original direction, the surface of the spectroscopic film is plated. A wedge is fixed, and the angle of the wedge is selected such that the beam passes through the wedge to form a beam that is in line with the beam that is directed toward the pentagon. An automatic or manual level can be established using two sets of beam expanders and optical deflectors. In a first implementation of the invention, the fine light from the laser module is first directed toward the first beam expander. A portion of the incident light of the first beam expander expands into a first optical plane, and another portion passes through the expander holding direction toward the optical deflector and is deflected 90 by the deflector. A second optical plane is formed perpendicular to the first optical plane toward the second beam expander. In the above implementation, the first beam deflector must have the function of optical splitting at the same time: its splitting function divides the incident light into two parts, wherein -^ the knife's original direction is unchanged; the other part utilizes the beam expanding function. An optical plane that is perpendicular to the original incident direction. Expanding In the second implementation of the present invention, the thin "beam" emitted by the laser module can be first decomposed by the spectroscopic optical element into two bundles of light = light I
1252907 五、發明說明 光束。這 擴展成相 以下 在描 如笫 束Bo成4 5 垂直。當 掃描出一 笫一 21,2 2 和 述平面成 沒有偏離 面上被反 與原入射 射光束B 〇 上述 確而穩定 問題,通 3 1 和 3 2 0 們相對入 夾角的誤 更準 所示,該 的光學折 (6) 兩束光分別指向第一 4结 互垂直的和第一光束擴展器,由它們 光學平面。 為备種實施範例: 述本發明之前 一圖3所+ 1 ,先描述本發明的光學偏轉器。 。的反射浐' f簡,單的光學偏轉器為一和入射光 反射鏡1 1 5人i從它反射的光束Br和入射光束β〇 ik ^ ix ^ ^ 射光束β〇為軸旋轉時,反射光束Br :4釉一垂直的水平平面光幅。 圖Μ。斤I為一直角棱鏡偏轉器20 ’它有三個平面 45。,、中平面21和22相互垂直,而平面23與上 、平面垂直的入射光束Bo在通過該面後 、方向而射向平面23,由於全反射,光線在該平 =f直射向平面22,穿透該平面所形成的光束& " 〇垂直,並如前述,當偏轉器20被帶動以入 1軸旋轉,則同掃描出平面光幅。 适,光學偏轉元件雖然簡單,但是難以高精度準 $安裝在和入射光成4 5。方向上,為了克服這個 常使用如圓一 c所示的兩個夾角為45。的反射平面 該裝置中入射光束Bo和出射光束βΓ的垂直度和它 射光的方向無關,在誤差僅取線於它們之間4 5。 差。 確而穩定的光學偏轉器為五角稜鏡。如第一d圖 稜鏡40的五個平面41-45,其中有兩個相互垂直 射面··入射平面4 1和出射平面4 2 ;兩個光學夾角1252907 V. Description of the invention Beam. This expands to the phase below, which is described as 笫 bundle Bo into 4 5 vertical. When scanning a 笫21, 2 2 and the plane is not deviated from the original incident beam B 〇 the above is stable and stable, the errors of the relative angles of the 3 1 and 3 2 0 are more accurate. The optical fold (6) is directed to the first 4 junctions perpendicular to each other and to the first beam expander, respectively, by their optical planes. For the purpose of preparing the example: Before the present invention, Fig. 3 + 1 , the optical deflector of the present invention will be described first. . The reflection 浐' f simple, single optical deflector is one and the incident light mirror 1 1 5 people i from which the reflected light beam Br and the incident beam β〇ik ^ ix ^ ^ beam β 〇 as the axis rotates, the reflection Beam Br: 4 glazes a vertical horizontal plane of light. Figure Μ. The jin I is a right-angle prism deflector 20' which has three planes 45. , the intermediate planes 21 and 22 are perpendicular to each other, and the incident beam Bo of the plane 23 perpendicular to the upper and the plane is directed toward the plane 23 after passing through the plane, and the light is directed to the plane 22 at the level = f due to total reflection. The beam &" 穿透 formed by penetrating the plane is vertical, and as described above, when the deflector 20 is driven to rotate in one axis, the planar light amplitude is scanned. Appropriate, although the optical deflecting element is simple, it is difficult to mount it at 45 with the incident light. In the direction, in order to overcome this, the two angles shown as circle one c are 45. Reflecting plane The perpendicularity of the incident beam Bo and the outgoing beam βΓ in the device is independent of the direction in which it is emitted, and the error is only taken between them 4 5 . difference. A sure and stable optical deflector is a pentagonal cymbal. For example, the five planes 41-45 of the first d-figure 40 have two mutually perpendicular planes · the incident plane 4 1 and the exit plane 4 2 ; two optical angles
第11頁 1252907 五、發明說明(7) 為4 5 的反射平面:第一 其中切割平面45為非光學射平面43和第二反射平面44。 41上射進入該稜鏡成為第一=,、’,光束Bo首先在入射平面 光束Bi又為第二反射平面 /平面44的入射光,其反射 為光束Br離開該稜鏡,入射=,出射平面42,經折射作 直。 束B〇與偏轉光束βΓ相互垂 對上述光學偏轉器加以改 垂直光線的分光光學元件。 P T以同時產生兩束相互 用半透膜取代如圖一 示羋品屯―丁 的反射膜,即成為最簡單的分光光:一仃、’板反射鏡1 1上 ® b ^ Λ ^ ^ .t #15^45 Λ ^ 分光膜1 6反射成與入射光垂直的光走、 〇、邛刀被其 υ生且的九束Br,而另餘下部分, 則沿=射方向穿過該膜成為光束β卜由於平板厚度t的影 響,這兩束光束Bo和Bt有一個平行平移距離e,當該雙反 射片以入射光束Bo為軸心轉動時,指向光束Br將圍繞該光 束Bt轉動而形成光柱,這是在使用中所不希望的。 為此我們可使用一補償用二相對為平行平面之光學平 板1 7 ’透過分光元件1 5之分光臈1 6並穿過此元件丨5後,其 出射光束B t與入射光偏離了一個距離β,它又通過另一平 板1 7 (如第二b圖)。小心選擇光學平板1 7的厚度折射率4 及取向’可以使因平行平板元件1 5的厚度所引起的出射光 束Bn相對入射光束B〇的偏離,為平板17的厚度所引起的偏 離所抵消,從而Bo與B t兩光束共線。 用兩個直角稜鏡250及260沿其斜面膠合而成為立方Page 11 1252907 V. Description of the invention (7) is a reflection plane of 4 5: first, wherein the cutting plane 45 is a non-optical plane 43 and a second reflection plane 44. 41 is incident into the crucible to become the first =,, ', the beam Bo first in the incident plane beam Bi is the incident light of the second reflection plane / plane 44, which is reflected as the beam Br leaves the crucible, incident =, exit Plane 42, refracted straight. The beam B 〇 and the deflected beam β Γ are mutually perpendicular to the optical deflector to change the vertical light splitting optical element. PT replaces the reflective film with two semi-permeable films at the same time as shown in Figure 1. It becomes the simplest spectroscopic light: a 仃, 'plate mirror 1 1 on the b ^ Λ ^ ^. t #15^45 Λ ^ The splitting film 16 is reflected as a beam of light that is perpendicular to the incident light, nine beams of Br, which are generated by the file, and the remaining part is passed through the film in the direction of the radiation. The beam βb has a parallel translation distance e due to the thickness t of the plate. When the double reflection plate rotates with the incident beam Bo as the axis, the directed beam Br will rotate around the beam Bt. Light column, which is not desirable in use. For this purpose, we can use a compensating optical plate 1 7 ' with a parallel plane to pass through the splitter 16 of the splitting element 15 and pass through the component 丨5, the outgoing beam B t is offset from the incident light by a distance. β, which in turn passes through another plate 1 7 (as in the second b-picture). Careful selection of the thickness index 4 and orientation ' of the optical plate 17 can offset the deviation of the exit beam Bn from the incident beam B 引起 due to the thickness of the parallel plate member 15 as a result of the deviation caused by the thickness of the plate 17. Thus, the two beams of Bo and Bt are collinear. Glue with two right angles 稜鏡250 and 260 along its slope
1252907 五、發明說明(8) 棱鏡(第二c圖)。其中至少一個鍍有半反射膜之斜面形成 分光膜2 7,這樣入射光束β〇進入稜鏡2 5 〇後,在分光膜2 7 上一部分’如約5 0 %,被反射到與入射垂直的方向光束 Br ’而另餘下部分,則透過該分光膜27沿入射方向同軸穿 過棱鏡2 6 0,而成為與入射光束β〇共線的光束Bt。 為了產生與原入射光共處一線的光束B t,我們也可將 圖一 c的反射平面3 2改為鍍半透膜的分光膜,部分入射光 束Bo將被該分光膜反射,經反射平面3丨再次反射而形成偏1252907 V. Invention description (8) Prism (second c diagram). At least one of the inclined surfaces coated with the semi-reflective film forms the spectroscopic film 2, 7 such that after the incident beam β〇 enters the 稜鏡25 〇, a portion of the spectroscopic film 27 is “about 50%, and is reflected perpendicular to the incident. The directional beam Br' and the remaining portion pass through the prism 260 in the incident direction through the spectroscopic film 27, and become a beam Bt collinear with the incident beam β〇. In order to generate a beam B t co-located with the original incident light, we can also change the reflection plane 3 2 of FIG. 1 c into a semi-transparent film splitting film, and part of the incident beam Bo will be reflected by the spectroscopic film through the reflection plane 3丨 re-reflecting and forming a partial
轉光束Br。另一部分將穿過該平板形成與入射光平行的指 向光束B t。The light beam Br. Another portion will form a pointing beam B t parallel to the incident light through the plate.
然而同樣由於平板厚度t的影響,這兩束光也有一個 平行平移距離e,為此,也可以如第二圖d的同附加的平面 平行平板所產生的平移來抵消這個平行平移,因為在在這 光學系統中使用有兩片相成9 〇度的平面平行平板,係作適 當的組合即可以產生無偏移的光束B t,鍍分光膜3 7的平行 平面平板35和平面平行平板36之間的夾角為45。,平板36 的出射平面3 9鍍以反射膜,入射光束β 0首先穿過平行平板 36射向平行平板35的分光入射分光膜37。由於其平板的厚 度tl影響,其出射光束Bt,與之有一個平移距離el,當該 光束Bt’透過分光膜37穿越透過平板35後,其出射光ϋ 又將為其厚度t的影響而反向偏回一個平移距離^,小心選 擇平行平板35和36的厚度折射率以及取向,因平行平板36 的厚度所引起的出射光束Bt,相對入射光束B〇的偏離el, 可為平板3 5的厚度所引起的偏離距離e所抵消,從而兩光However, due to the influence of the thickness t of the flat plate, the two beams also have a parallel translation distance e. For this reason, the parallel translation can also be offset by the translation produced by the same plane parallel plate of the second figure d, because In this optical system, two plane parallel plates of 9 turns are used, and a suitable combination can produce a non-offset beam B t , a parallel flat plate 35 of the plated light film 37 and a plane parallel plate 36. The angle between the two is 45. The exit plane 39 of the flat plate 36 is plated with a reflective film, and the incident beam β 0 is first passed through the parallel plate 36 to the split-light incident spectroscopic film 37 of the parallel flat plate 35. Due to the influence of the thickness t1 of the flat plate, the outgoing beam Bt has a translational distance el. When the beam Bt' passes through the spectroscopic film 37 and passes through the transillumination plate 35, the exit pupil will be opposite to the thickness t. To offset a translation distance ^, carefully select the thickness refractive index and orientation of the parallel plates 35 and 36. The deviation of the exit beam Bt due to the thickness of the parallel plate 36, relative to the incident beam B〇, may be the plate 35. The deviation caused by the thickness is offset by the distance e, so that the two lights
1252907 五、發明說明(9) 束Bo和Bt同軸。 將第一d圖五角稜鏡的第一反射平面“鍍以分光膜, 该面因此標以反射平面46。如第二e圖所示,光束β〇的一 部分將在反射平面4 6反射而形成光束β丨。另一部分B t將穿 出該稜鏡。由於反射平面46不與入射光束B〇垂直,離開該 面的光束B t將偏離該軸一個角度。為了使兩光束在同一直 線上,在反射平面4 6上附一光楔4 7,該光楔4 7有兩個光學 折射平面48和49’其中平面48與反射平面46貼合。在光楔 4 7的光學材料和五角稜鏡一樣時,光楔4 7的夾角平面4 9得 與稜鏡的入射平面41平行,兩者的組合相當於一光學平面 平行平板’透過稜鏡4 0之反射平面4 6的部分光將進入光楔 4 7 ’經其平面4 9離開該稜鏡組合成為光束b t,當入射光束 B 〇與入射平面4 1垂直時,兩光束B 〇、B t同軸。 利用上述光學偏轉器和不同的光束擴展器,產生本發 明之能同時產生兩個相互垂直的光學平面的裝置。 主要係利用上述最佳實施之偏轉器,間接於光束擴展 系統之前置或中段光學路徑,提供同步獲得水平之第一光 學平面,或垂直之第二光學平面,以下首先對光束擴展器 作簡述,如第三圖及第四圖令對所指錐形光束擴展器。 第三a圖為一反射錐體50,它有一錐頂角為90度與軸 5 2旋轉對稱的反射面平5 1。入射光束B〇沿該軸射向錐面’ 經它反射圓形擴展形成一光平面Be。 第三b圖中顯示的為一全反射型的光學透明内錐形光 束擴展器60,具有一光學入射平面62、,一與轴61旋轉對稱1252907 V. Description of invention (9) Beam Bo and Bt are coaxial. The first reflective plane of the pentagonal 第一 of the first d-graph is "plated with a beam splitting film, which is thus labeled with a reflecting plane 46. As shown in the second e-figure, a portion of the beam β〇 will be reflected at the reflecting plane 46 to form The beam β丨. The other part B t will pass through the pupil. Since the reflection plane 46 is not perpendicular to the incident beam B〇, the beam B t leaving the plane will deviate from the axis by an angle. In order to make the two beams on the same line, Attached to the reflecting plane 46 is a wedge 47. The wedge 47 has two optically refractive planes 48 and 49', wherein the plane 48 is attached to the reflecting plane 46. The optical material and the pentagonal ridge at the wedge 47 In the same case, the angle plane 4 of the wedge 47 is parallel to the incident plane 41 of the crucible, and the combination of the two corresponds to an optical plane parallel plate. Part of the light passing through the reflection plane 46 of the 稜鏡40 will enter the light. The wedge 4 7 'is separated from the crucible by its plane 4 9 into a beam bt, and when the incident beam B 垂直 is perpendicular to the incident plane 4 1 , the two beams B 〇 , B t are coaxial. Using the above optical deflector and different beam extensions Producing the present invention capable of simultaneously producing two mutually perpendicular The apparatus of the optical plane mainly utilizes the deflector of the above-described best implementation, indirectly to the optical path of the front or middle section of the beam expanding system, to provide a first optical plane that simultaneously obtains a level, or a second optical plane that is perpendicular, first The beam expander is briefly described, as shown in the third and fourth figures for the pointed cone expander. The third a diagram is a reflection cone 50 having a cone apex angle of 90 degrees and a rotational rotation of the shaft 5 2 The reflecting surface is flat 5 1. The incident beam B 射 is directed toward the tapered surface along the axis. The circular expansion is formed by its reflection to form a light plane Be. The third b-picture shows a totally reflective optically transparent inner cone beam. The expander 60 has an optical incident plane 62, and is rotationally symmetric with the shaft 61.
第14頁 =錐面63、以此軸為旋轉對稱軸的光學 ,面62和旋轉對稱軸61垂直。當光束“入硯窗66。入 ”入平面62時,光束越過該面進入透:光沿軸61垂 二要透明體的光學折射率大於某值,該光在=向錐面63, μ =射。對於反射光要求和入射光垂直的情線面上會發生 :的折射率不小於丨,4142。絕大多數的光風払,光學透明 :璃和塑膠的折射率大多都大於此值,為:】質,如光學 擴展成第一光平面心。, 〃、反射的光束將 對上述錐形反射鏡作改變即可以同時 ,,並進一步如第四圓所示,可形成有:個光平 光束擴展器。 先作用於錐形 如第四a圖描述的分光錐形鏡為一 7〇,它是一與軸7〗斿赭料p伯& 尤予透明擴展器 0疋兴釉u旋轉對稱,頂角為90度的籴錢、头 體。其錐面7 2鑛有反射膜,麻面7 q4 予透明錐形 面,盆雜τη It 為與軸71垂直的光學平 面其錐頂為一與底面73的光學小平面74平行,=学+ 平面74大的光束Bo沿軸71入射到該元件上,一,=比小 平面74與底面73的光束Bt穿射方向不冑,餘下過小 射的光線擴展成第一光平面Bc。 ,,、、、隹面72反 第四b圖描述的分弁4鱼# g p i , 展謂,它是有-光學入Λ 射型的錐形光束擴 内錐面82、以此軸為旋轉對稱軸的光學圓柱面8 :面 82頂端有一與入射平面85平行的小平面84,入射平=面 旋轉對稱軸81垂直。當直徑大於小平面84的光束Β ;Page 14 = Conical surface 63, optics with this axis as the axis of rotational symmetry, face 62 and axis of rotational symmetry 61 are perpendicular. When the beam enters the plane 66 into the plane 62, the beam passes through the surface to enter: the optical refractive index of the transparent body along the axis 61 is greater than a certain value, the light is at the cone 63, μ = Shoot. For the reflected light requirement and the incident light perpendicular to the line of sight will occur: the refractive index is not less than 丨, 4142. Most of the light winds, optically transparent: the refractive index of glass and plastic are mostly greater than this value, which is: quality, such as optical expansion into the first light plane heart. The 〃, reflected beam will change the above-mentioned cone mirror at the same time, and further as shown by the fourth circle, a flat beam expander can be formed. Firstly, the spectroscopic cone mirror described in the fourth diagram is a 7 〇, which is a shaft 7 斿赭 p 伯 & & 尤 尤 尤 尤 尤 尤 尤 尤 尤 尤 釉 釉 旋转 旋转 旋转 旋转 旋转It is a 90-degree money and head. The conical surface of the conical surface has a reflective film, the surface 7 q4 is a transparent conical surface, and the basin is τη It is an optical plane perpendicular to the axis 71. The cone top is parallel to the optical facet 74 of the bottom surface 73. The light beam Bo having a large plane 74 is incident on the element along the axis 71. One, the light beam Bt is smaller than the light beam Bt of the facet 74 and the bottom surface 73, and the remaining light beam is expanded into the first light plane Bc. ,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, The optical cylindrical surface 8 of the shaft: the top end of the surface 82 has a facet 84 parallel to the plane of incidence 85, and the incident plane = plane rotational axis of symmetry 81 is perpendicular. When the diameter is larger than the plane of the plane 84;
沿轴81垂直進入平面85時,-部分光穿過小平面84保持J 彡、發明說明(11) ~ ' " " ----------η 方向不變成直線光束Bt,其餘的入射光會進入透明體射向 雜面2,只要透明體的光學折射率大於某值,該光在錐面 82上w發生全反射,為其反射的光線擴展成光平面。 本發明能同時產生兩個相互垂直的光學平面的第一種 實施中,光學偏轉器在光學路徑上置於第一光束擴展器之 後。 、 _ · 弟五圖4田述了本專利第一種實體使用旋轉光學偏轉器. 的裝置。它是第8 9 1 2 3 9 0 1號專利案所描述的能產生指示光― 的雷射掃描模組的改進。圖中1 〇 〇就是這種雷射掃描模 錐:它由一個雷射模組1 1 〇,一個空心馬達丨丨3及一個固定着, 在馬達之空心轉軸上的五角稜鏡1 1 4組成,雷射模組π 〇和 矣心馬達1 1 3由一機殼11 5固定在一起並使雷射模組11 Q發 出的光束與空心馬達11 3的轉軸重合。 , 雷射模組1 1 0含有一個半導體雷射1 1 1和一個筆直光學 -聚焦系統1 1 2。從半導體雷射11 1發出的擴散之雷射光為垂人 真光學聚焦糸統112聚焦形成一束光束Bo,光束通過空 心馬達旋轉軸的通孔(未畫)射向旋轉的帶補償光楔的五角 棱鏡114。從其分光膜反射的光束Brl形成第一光學面。穿 過分光膜的光束B t ’進入光學偏轉器2 6,(圖中為分光立 方稜鏡偏轉器2 6 ),反射的光通過另一水平向之空心馬達 1 2 3的中心沿其旋轉抽的通孔(未畫)射向旋轉的五角稜鏡 124。為此五角稜鏡反射的光束Br2形成垂直之第二光學平 _ 面。穿越分光偏轉器26的光束Bt與原入射光束B〇的方向重 合0When the axis 81 enters the plane 85 perpendicularly, part of the light passes through the facet 84 to maintain J 彡, invention description (11) ~ ' """ ---------- η direction does not become a straight beam Bt, the rest The incident light enters the transparent body and is incident on the surface 2, and as long as the optical refractive index of the transparent body is greater than a certain value, the light is totally reflected on the tapered surface w, and the reflected light is expanded into a light plane. The first embodiment of the invention capable of simultaneously producing two mutually perpendicular optical planes, the optical deflector being placed behind the first beam expander in the optical path. _ · 弟五图4 The device of the first entity of this patent uses a rotating optical deflector. It is an improvement of the laser scanning module capable of producing indicator light as described in the Patent No. 8 9 1 2 3 0 0 1 . In the figure, 1 〇〇 is the laser scanning die cone: it consists of a laser module 1 1 〇, a hollow motor 丨丨 3 and a fixed, five-corner 稜鏡 1 1 4 on the hollow shaft of the motor. The laser module π 〇 and the centroid motor 1 1 3 are fixed together by a casing 11 5 and the beam emitted by the laser module 11 Q coincides with the rotating shaft of the hollow motor 11 3 . The laser module 110 includes a semiconductor laser 1 1 1 and a straight optical-focus system 1 1 2 . The diffused laser light emitted from the semiconductor laser 11 1 is focused by a vertical optical focusing system 112 to form a beam Bo, which is directed through a through hole (not shown) of the rotating shaft of the hollow motor toward the rotating compensated wedge. Pentagonal prism 114. The light beam Brl reflected from its spectroscopic film forms a first optical surface. The light beam B t ' passing through the beam splitting film enters the optical deflector 2 6 (in the figure, the splitting cube 稜鏡 deflector 2 6 ), and the reflected light is drawn along the center of the hollow motor 1 2 3 A through hole (not shown) is directed toward the rotating pentagonal 稜鏡 124. For this purpose, the light beam Br2 reflected by the pentagonal ridge forms a vertical second optical plane. The beam Bt passing through the spectroscopic deflector 26 coincides with the direction of the original incident beam B〇.
第16頁 1252907 五、發明說明(12) 光學偏轉器26及第二光束擴展器位置為機構116所固 定。為了不遮阻光束B r 1,此組合可用透明窗1 1 7與雷射模 組1 1 0結合在一起。 當為機構11 6所組合的光學偏轉器2 6及第二光束擴展 器可以圍繞入射光束B 〇同軸旋轉時,也就是橫向設置之空 心馬達123或稜鏡124,可偏心圍繞光束Bo之軸心,而作外 圍走動,則第二光學平面則可被調整照射於周圍環境任一 角位,提供任一標示點皆可取得垂直線依據,換句話說第 二平面可任意出現在與第一平面垂直的任一角位上。 前述所有相關之光學偏轉器,均可以取代圖中的分 立方稜鏡狀之偏轉器2 6。 刀 第六a圖顯示的裝置的第一光束擴展元件為一全反 型的錐形光束擴展器8〇。光束Bo入射光沿軸8 1射入該元件 時,一部分光束Bt穿過它。餘下的光在其内錐面上= 反射而擴展成第一光平面Bc卜不偏轉的光束^為偏王 2 6 (圖中為立方稜鏡)所反射射向水平擺置之第二 ° 器60。該光释此擴展器擴展為第二光平面β〇2。—束擴展 二光束擴展器60為全反射型的内錐面反射鏡。 、 將第一光束擴展器80及第二光束擴展器6〇分 偏轉器26的入射與出射平面結合在一起成為 =先: 第六b圖所示,再與雷射模組11〇結合在一 ,。如 但可以同時產生兩相互直角關係的光學平面、:^ :: 一平面法線(垂直線)的模組。 此產生 有關第六c圖係在重複說明如第五圖所述之第二光束Page 16 1252907 V. INSTRUCTION DESCRIPTION (12) The position of the optical deflector 26 and the second beam expander is fixed by the mechanism 116. In order not to block the beam B r 1, this combination can be combined with the laser module 1 1 0 by the transparent window 1 17 . When the optical deflector 26 and the second beam expander combined for the mechanism 116 can rotate coaxially around the incident beam B ,, that is, the laterally disposed hollow motor 123 or 稜鏡 124, the eccentric surrounding the beam Bo can be eccentrically For the peripheral movement, the second optical plane can be adjusted to illuminate any corner of the surrounding environment, and any marked point can be used to obtain the vertical line basis. In other words, the second plane can appear arbitrarily perpendicular to the first plane. Any corner position. All of the aforementioned optical deflectors can be substituted for the sub-cube-shaped deflectors 26 in the figure. Knife The first beam expanding element of the device shown in Figure 6a is a full-reflex cone beam expander 8〇. When the incident light of the beam Bo is incident on the element along the axis 81, a part of the beam Bt passes through it. The remaining light is reflected on its inner cone surface = reflected and expanded into the first light plane Bc. The beam that is not deflected is the second reflector that is reflected by the king 26 6 (cube in the figure). 60. The light release expander expands to a second light plane β〇2. - Beam Expansion The two beam expander 60 is a total reflection type inner cone mirror. Combining the incident and exit planes of the first beam expander 80 and the second beam expander 6 to the deflector 26 becomes = first: as shown in the sixth b diagram, and then combined with the laser module 11 ,. For example, it is possible to simultaneously generate optical planes of two mutually orthogonal angles: a module of: ^ :: a plane normal (vertical line). This generation is related to the sixth c-ray in repeating the second beam as described in the fifth figure.
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ΐΐΞ可射光束β。同軸旋轉,進而獲得第二光 ^ 卜圍调動,而在任一角位皆可取得第-光學 m黛: 思 圖上所示,該雷射模組110 L Γ所發出—Λ束擴展器8 °,該光束擴展器8 °可由雷射模 L 110所發出之雷激光擴展成第一光平面Bci, 光束擴展器8 0之光| Rt,目,ι φ吉& & Μ & 牙、丄弟 哭W 則垂直射向偏轉器26,藉由偏轉 益26再k向轉折射向第二光束擴展 — + f弟一先千 其中第二光束擴展器 〇 了圍、:者=射模組110 (或是相同垂直地表的軸心線,ΐΐΞ can emit beam β. The coaxial rotation is performed to obtain the second optical transmission, and the first optical optical 黛 can be obtained at any angular position: as shown in the figure, the laser module 110 L 发出 is issued - the Λ bundle expander 8 ° The beam expander 8° can be expanded by the laser light emitted by the laser mode L 110 into a first light plane Bci, the beam expander 80 light | Rt, M, φ φ 吉 && amp & When the younger brother is crying W, it is directed to the deflector 26 vertically, and is extended to the second beam by the deflection benefit 26 and k to the refraction - + f is a thousand, and the second beam expander is surrounded by: 110 (or the same vertical axis axis,
:Γ i係Γ:光束Μ “作為中心點進行外圍的弧向調轉 心ί:由二不),由第六d圖俯視觀之’其中第二擴展 裔6桃0可及由调校方式沿著Bt的軸心而作圍繞轉動,因此相 同帶動第二光平面Bc2形成不同角位的變化,於此而使第 二光平面可投射在任一角位,獲得任一角位的垂直線參 考0: Γ i system Γ: beam Μ "As the center point for the peripheral arc to turn the heart ί: by the two no), from the sixth d figure overlooking the view of which the second extended 6 peach 0 is accessible by the adjustment method The axis of Bt is rotated around, so that the second light plane Bc2 is driven to form a different angular position change, so that the second light plane can be projected at any angular position, and the vertical line reference of any angular position is obtained.
第七a圖的裝置使用了反射型的分光式錐形第一擴展 器70,光束Bo沿輛71入射到該元件上。軸71附近的一部分 透過該元件射向光學偏轉器20 (此圖為直角稜鏡)。餘下 的為錐面72反射形成第一光平面Bcl。為直角稜鏡所反射 的光進而為第二光擴展器60擴展而形成第二光平面以2。 圖中使用的第一光擴展器70是一全反射錐形鏡。它的 優點是可以將第_ ,二光束擴展器7〇及6〇及直角稜鏡偏轉 :2〇集成為單一整體的光學元件。將第一光擴展器7〇的底 3與直角稜鏡偏轉器2〇的入射平面重合,將偏轉器“的The apparatus of the seventh diagram uses a reflective spectroscopic cone-shaped first expander 70 to which the light beam Bo is incident on the element 71. A portion of the vicinity of the shaft 71 is directed through the element toward the optical deflector 20 (this figure is a right angle 稜鏡). The remaining reflection of the tapered surface 72 forms a first light plane Bcl. The light reflected by the right angle 进而 further expands the second light expander 60 to form a second light plane of two. The first light expander 70 used in the figure is a total reflection cone mirror. It has the advantage that the _ and 2 beam expanders 7〇 and 6〇 and the right angle 稜鏡 can be deflected: 2〇 integrated into a single integral optical component. The bottom 3 of the first light expander 7〇 coincides with the plane of incidence of the right angle 稜鏡 deflector 2〇, and the deflector is
1252907___ 五、發明說明(14) 出射平面與第二光擴展器60的底面(入射面)重合就形成如 第七b圖所示的可以同時產生兩個相互垂直光平面的單一 光學元件1 7 0。 該元件為一光學透明體,它有四個光學表面··一個鍍 反射膜的錐形面1 7 1,一個全反射的内錐形面1 7 2,它們的 對稱軸相互垂直;一個在錐形面i 7 1錐頂上與其對稱轴垂 直的小平面1 7 3,一個與兩對稱均成4 5度的全反射平面! 7 4 和一以全反射面對稱軸為軸的光學圓柱面1 7 5。 本發明能同時產生兩個相互垂直的光學平面的第二種 實施中,分光光學偏轉器在光學路徑上置於第一光束擴展 器之前’如第八a圖所描述的是此實體中的使用兩個旋轉 光束擴展器210及220的裝置。從雷射模組11〇發出的細光 束Bo首先射向有分光作用的光學偏轉器470 (圖中為帶光 楔的五角稜鏡4 0 ),且與其入射面垂直。為光學偏轉器 470折射出的光為第一旋轉擴展器210掃描擴展成垂直的光 平面Bel。透過該光學偏轉器470的光為第二旋轉擴展器 2 2 0掃描擴展成光平面Be2。 第八b圖是這種裝置組合的水平儀的模組。指示水平 位置的水泡211通過一圓柱型透明窗212與機殼213固定在 一起。在儀器校正中,將第一光平面B c 1校正到水平位 置,而第二光平面Bc2自動處於垂直位置。 圖中第二旋轉擴展器210連同光學偏轉器所設光楔47 及棱鏡40可以通過一個機殼213固定在一起。如第八c圖所 示,通過一個偏移機構2〇〇,由軸承214活固第二旋轉擴展1252907___ V. DESCRIPTION OF THE INVENTION (14) The exit plane coincides with the bottom surface (incident surface) of the second light expander 60 to form a single optical element 1 7 0 which can simultaneously produce two mutually perpendicular light planes as shown in FIG. . The element is an optically transparent body having four optical surfaces, a tapered surface of a reflective film 173, a totally reflective inner tapered surface 172, and their axes of symmetry are perpendicular to each other; Shape i i 1 The facet on the top of the cone perpendicular to its axis of symmetry 1 7 3, one and two symmetry is a total reflection plane of 45 degrees! 7 4 and an optical cylindrical surface 175 with the axis of symmetry of the total reflection plane as the axis. In a second implementation of the invention capable of simultaneously producing two mutually perpendicular optical planes, the spectroscopic optical deflector is placed in front of the first beam expander on the optical path, as described in Figure 8a, which is used in this entity. Two means for rotating the beam expanders 210 and 220. The fine beam Bo emitted from the laser module 11 is first directed toward the optical deflector 470 having a splitting action (in the figure, a pentagonal 稜鏡40 with a wedge) and perpendicular to its incident surface. The light refracted by the optical deflector 470 is scanned for expansion by the first rotary expander 210 into a vertical light plane Bel. The light transmitted through the optical deflector 470 is scanned into a light plane Be2 for the second rotary expander 220. Figure 8b is a block diagram of the level of such a device combination. The blisters 211 indicating the horizontal position are fixed to the casing 213 through a cylindrical transparent window 212. In the instrument calibration, the first light plane B c 1 is corrected to the horizontal position, and the second light plane Bc2 is automatically in the vertical position. The second rotary expander 210 together with the optical wedges and prisms 40 provided by the optical deflector can be fixed together by a casing 213. As shown in the eighth c-figure, the second rotation extension is alive by the bearing 214 through an offset mechanism 2〇〇
第19頁 1252907Page 19 1252907
器210,使該擴展器21 0可依入射光束β〇作水平向掃動,它 所產生的第二光平面Bc2則可以出現任何與第一光平面Bci 垂直的方向上(除受機殼機構限制外)。 第八d圖的自動水平儀中的雷射模組1 1 〇懸置在一個可 以圍繞兩個相互垂直而與地心引力垂直的軸轉平臺23〇 上。雪射模組1 1 〇通過懸臂2 4 1與一重錘2 4 2相連。重錐 24 2處於平衡位置時雷射模組11〇產生的細光束此與地心引 力重合。重錘2 4 2偏離平衡位置時,雷射模組i丨〇在重力作The apparatus 210 is configured to enable the expander 210 to horizontally sweep according to the incident beam β〇, and the second light plane Bc2 generated by the expander 210 can appear in any direction perpendicular to the first light plane Bci (except for the housing mechanism). Restricted). The laser module 1 1 自动 in the automatic level of the eighth figure is suspended on a pivoting platform 23 可 which can be perpendicular to the two perpendicular to the gravity. The snow shooting module 1 1 〇 is connected to a weight 2 4 2 through a cantilever 2 4 1 . When the weight cone 24 2 is in the equilibrium position, the beamlet generated by the laser module 11 重 coincides with the gravity of the earth. When the weight 2 4 2 deviates from the equilibrium position, the laser module i is in gravity
用下將返回平衡位置,直到它產生的細光束β〇與地心弓丨力 重合。 正對重錘242下方可設有一靜止的鐵盤243,上面固定 至少一個永磁體2 4 4。它和重錘2 4 2組成一電磁掣動系統。 ®重錘擺動時,它將切割永磁體2 4 4的磁力線而產生舉動 力使之快速回到平衡位置。The lower part will return to the equilibrium position until it produces a beamlet β〇 that coincides with the geocentric force. A stationary iron plate 243 may be disposed under the counterweight 242, and at least one permanent magnet 24 4 is fixed thereon. It and the weight 2 4 2 form an electromagnetic sway system. When the weight swings, it cuts the magnetic lines of the permanent magnets 24 4 and generates a force to quickly return to the equilibrium position.
第九圖是第二個實施的另一種裝置,它使用了兩個對 稱軸相互垂直的錐形光束擴展器6 0 a和6 Ob。從雷射模組 110來的光束經光學偏轉器25反射的光為第二光束擴展器 60b反射為第二光平面Bc2。而透過此偏轉器25的光為第一 光束擴展器60a反射為第一光平面Bel。圖中的水泡可以將 光平面Bel定向為水平面,而bc2為垂直光平面。 本發明之所有錐形擴束器均可以用作第一和第二光束 擴展器,其中錐形擴展器可以與所描述的光學偏轉器作各 種組合和變型,特別是如其中第二光束擴展器可與光學偏 轉益圍繞入射光束β 〇轴心線轉動’從而產生與第一光束擴The ninth diagram is another apparatus of the second embodiment which uses two cone beam expanders 60a and 6 Ob which are perpendicular to each other. The light reflected by the laser beam from the laser module 110 is reflected by the second beam expander 60b as the second light plane Bc2. The light transmitted through the deflector 25 is reflected by the first beam expander 60a as the first light plane Bel. The blisters in the figure can orient the light plane Bel to a horizontal plane, and bc2 to a vertical plane. All of the conical beam expanders of the present invention can be used as first and second beam expanders, wherein the conical expanders can be variously combined and modified with the described optical deflectors, particularly as the second beam expander Can be rotated with the optical deflection around the incident beam β 〇 axis to generate a first beam expansion
第20頁 1252907 五、發明說明(16) 展器所發生的 取向的第二光 此外,本 手動地同步產 本發明之 偏轉器同時產 本發明實施表 1. 結構精 學平面的光學 2. 發明簡 及另一個與之 3. 於利用 同步產生垂直 綜上所述 諸公開使用, 便0 第一擴展平面垂直5可獲得投光角位能任意 學面 發明 生一 基本 生兩 現之 簡、 系統 單可 垂直 光學 光幅 ,本 合於Page 20 1252907 V. INSTRUCTIONS (16) Second Light of Orientation Occurred in the Extensor In addition, the present invention simultaneously produces the deflector of the present invention simultaneously and produces the embodiment of the present invention. 1. Structured Fine Plane Optics 2. Invention Jane and the other 3. In the use of synchronization to produce the vertical use of the above-mentioned public use, then 0 the first expansion plane vertical 5 can obtain the projection angle can be any way to invent a basic life and two simple, system Single vertical optical light, this is in
可以用於具體的水平儀,它可以自動或 個水平面和一個垂直面。 點:係使用兩個光束擴展器,通過光學 個相互垂直的光學平面。 優點有: 功耗小、可同時產生相互垂直的二個光 〇 靠的可產生一個光學平面(光幅),以 且方向可變化的光學平面的光學系統; 系統,發明全新既可產生水光幅,又可 的雷射光學參考光學平面發生儀。 發明能確實改善習見之缺失,其並未見 專利法之規定,懇請賜准專利,實為德It can be used for a specific level, it can be automatic or horizontal and a vertical. Point: Two beam expanders are used to optically oppose the optical planes that are perpendicular to each other. The advantages are: low power consumption, simultaneous generation of two optical beams that are perpendicular to each other, can produce an optical plane (optical amplitude), and an optical system with a variable optical plane; the system, the invention is new, can produce water light A wide range of laser optical reference optical plane generators. The invention can indeed improve the lack of understanding, and it does not see the provisions of the patent law.
第21頁 1252907 圖式簡單說明 第一 a圖係本發明之4 5 °反射鏡光學偏轉器。. 第一 b圖係本發明之直角棱鏡。 · 第一 c圖係本發明之雙反射鏡光學偏轉器 第一 d圖係本發明之五角梭鏡光學偏轉器。 第二a圖係本發明之45 °分光偏轉器。 第二b圖係本發明之帶光束平行偏移校正的4 5 °分光偏 轉器。 第二c圖係本發明之立方棱鏡。 第二d圖係本發明之鍍分光膜的雙反射鏡光學偏轉 器。 第二e圖係本發明之轉軸指向光被校正了的雙反射鏡 偏轉器。 第三a圖係本發明之錐形反射鏡。 第三b圖係本發明之錐形全反射鏡。 第四a圖係本發明之分光錐形反射鏡。 第四b圖係本發明之分光錐形全反射鏡。 第五圖係本發明之使用旋轉五角棱鏡的第一種實體。 第六a圖係本發明之使用全反射錐形鏡的第一種實 第六b圖係本發明之使用全反射錐形鏡的第一種實體Page 21 1252907 Brief Description of the Drawings The first a drawing is a 4 5 ° mirror optical deflector of the present invention. The first b is a right angle prism of the present invention. The first c-picture is the dual-mirror optical deflector of the present invention. The first d-figure is the pentagonal shuttle optical deflector of the present invention. The second a diagram is a 45° spectroscopic deflector of the present invention. The second b-picture is a 45 ° split-light deflector with beam parallel offset correction of the present invention. The second c-picture is a cube prism of the present invention. The second graph is a double mirror optical deflector for the plated split film of the present invention. The second e-picture is a dual-mirror deflector in which the rotating shaft of the present invention is directed to light. The third a diagram is a conical mirror of the present invention. The third b-picture is a tapered total reflection mirror of the present invention. The fourth a diagram is a spectroscopic cone mirror of the present invention. The fourth b-picture is a spectroscopic cone-shaped total reflection mirror of the present invention. The fifth figure is the first entity of the present invention using a rotating pentagonal prism. Figure 6a is a first embodiment of the present invention using a total reflection conical mirror. The first embodiment is a first entity using a total reflection conical mirror of the present invention.
第22頁 1252907 圖式簡單說明 的 模組。 第六C圖係本發明相關第二擴展器與垂直地表之軸心 線 偏轉立體示意圖。 第六d圖係為第六c圖之俯視圖。 第七a圖係本發明之使用一個反射鏡和一個全反射錐 形 鏡的第一種實體。 第七b圖係本發明之含一個反射鏡、一個全反射錐形 鏡 和一光學偏轉器的第一種實體的集成塊。 第八a圖係本發明之使用旋轉五角棱鏡的第二種實施 的 模組。 第八b圖係本發明之使用旋轉五角棱鏡的第二種實體 的 能同時產生水平面及垂直面的模組。 第八c圖係本發明之使用旋轉五角棱鏡的第二種實體 的 能同時產生水平面及旋轉垂直面的模組。 第八d圖係本發明之使用旋轉五角棱鏡的第二種實體 的 能自動同時產生水平面及旋轉垂直面的模組。Page 22 1252907 A simple description of the module. The sixth C is a perspective view of the axial extension of the second expander and the vertical surface of the present invention. The sixth diagram is a top view of the sixth c diagram. Figure 7a is a first entity of the present invention using a mirror and a total reflection cone. Figure 7b is an integrated block of the first entity of the present invention comprising a mirror, a total reflection cone and an optical deflector. The eighth diagram is a module of the second embodiment of the present invention using a rotating pentagonal prism. The eighth b-picture is a module of the second entity of the present invention which uses a rotating pentagonal prism to simultaneously produce a horizontal plane and a vertical plane. The eighth c-picture is a module of the second entity of the present invention using a rotating pentagonal prism capable of simultaneously generating a horizontal plane and a rotating vertical plane. The eighth drawing is a module of the second entity of the present invention which uses a rotating pentagonal prism to automatically generate both a horizontal plane and a rotating vertical plane.
第23頁 1252907___ 圖式簡單說明 第九圖係本發明之使用全反射錐形鏡的第二種實施例 〈圖示符號說明>: 11 :反射鏡 1 5、1 7 0 :元件 1 7、3 5、3 6 :平板 20、26、4 7 0 :偏轉器 2 5 0、2 6 0、4 0、1 1 4、1 2 4 :稜鏡 21 、 22 、 23 、 31 、 32 、 39 、 41 、 42 、 43 、 45 、 46 、 48、49、51、62、74、84、85、173、174、21 0、2 2 0 :平 面 1 6、2 7、3 7 :分光膜 4 7 :光楔 5 0 :反射錐體 60、60a、60b、70、80、210、2 2 0 ··擴張器 52、61、71、81 :車由 63、 72、 82:錐面 6 6 :圓柱視窗 7 3 :底面 83、175:光學圓柱面 I 0 0 ·雷射掃描模組 II 0雷射模組 1 1 1 :半導體雷射Page 23 1252907___ BRIEF DESCRIPTION OF THE DRAWINGS FIG. 9 is a second embodiment of the present invention using a total reflection conical mirror. <Illustration of Symbols>: 11: Mirrors 1 5, 1 7 0: Element 1 7. 3 5, 3 6 : plate 20, 26, 4 7 0 : deflector 2 5 0, 2 6 0, 4 0, 1 1 4, 1 2 4 : 稜鏡 21 , 22 , 23 , 31 , 32 , 39 , 41, 42 , 43 , 45 , 46 , 48 , 49 , 51 , 62 , 74 , 84 , 85 , 173 , 174 , 21 0 , 2 2 0 : plane 1 6 , 2 7 , 3 7 : beam splitting film 4 7 : Wedge 50: Reflecting cones 60, 60a, 60b, 70, 80, 210, 2 2 0 · Dilators 52, 61, 71, 81: Cars 63, 72, 82: Cone 6 6 : Cylindrical window 7 3 : bottom surface 83, 175: optical cylindrical surface I 0 0 · laser scanning module II 0 laser module 1 1 1 : semiconductor laser
第24頁 1252907_;_ 圖式簡單說明 1 1 2 :光學聚焦系統 1 1 3、1 2 3 :空心馬達 1 1 5、2 1 3 :機殼 1 1 6、2 0 0 ··機構 1 1 7 :透明窗 171 >172 :錐形面 2 1 1水泡: 2 1 2 :透明窗 2 1 4 :軸承 2 3 0 :軸轉平臺 2 4 1 :懸臂 242 :重錘 2 4 3 :鐵盤 2 4 4 :永磁體Page 24 1252907_; _ Simple description of the diagram 1 1 2 : Optical focusing system 1 1 3, 1 2 3 : Hollow motor 1 1 5, 2 1 3 : Enclosure 1 1 6 , 2 0 0 · · Mechanism 1 1 7 : Transparent window 171 > 172 : Conical surface 2 1 1 Blisters: 2 1 2 : Transparent window 2 1 4 : Bearing 2 3 0 : Axle-turning platform 2 4 1 : Cantilever 242: Heavy hammer 2 4 3 : Iron plate 2 4 4 : Permanent magnet
Bo、Br、Bt、Bi、Bt’ 、Bn、Brl、Br2:光束 Be 、 Bel 、 Bc2 :光平面 t 、 tl :厚度 e、el :距離Bo, Br, Bt, Bi, Bt', Bn, Brl, Br2: beam Be, Bel, Bc2: light plane t, tl: thickness e, el: distance
第25頁Page 25
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