TWI242636B - An optical angle encoder - Google Patents
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1242636 玖、發明說明: 【發明所屬之技術領域】 本發明係關於一種光學式角度繞 » 扁馬器,尤指一種適用 於鬲精度旋轉軸之光學式角度編碼器。 【先前技術】 目前半導體業、薄膜電晶體顯示器等光電產業正不斷 成長’奈米科技也已成為全球最熱門的研究方向之一,技 術水準之要求,也日益提高,而這些產業均為光機電整合 10型產業’為了達此技術要求,精密機械工業相形之下更為 人所重視。精密機械工業常使用到是高精度研磨機、CNC 車床、CNC銑床等’這些加卫機器除需要有準確的位移外, 同時必需高精度之角度旋轉軸來配合加工需求。此外,在 航空上因其觀測之距離相當遠,亦需要高精度之角度旋轉 15 量測,以防止誤差產生。 現有高精度旋轉軸其角度定位感測器都採用編碼器 (Encoder),其包括一片具有無數夾縫之圓盤(或稱為光 柵),在圓盤的兩側裝置發光器與感測器,當移動時帶動 光柵圓盤,光柵會阻斷光線,感測器便會收到間斷之光源, 20電腦即憑藉光感測器收到之信號推算出位移。 隶間單型之光學角度編碼器為將一薄圓盤等角度輻 射狀開細縫槽,再以感測器檢出光束通過細縫的明暗變 化’如應用在滑鼠之編碼器,但其能感應明暗變化之狹縫 大小有限,亦即狹縫太小,便無法感測;在工業上使用的光 1242636 學編碼器如圖i所示,包含主光拇戦副光拇2〇,主光拇ι〇 如同-薄圓盤,圓盤上有等角度輻射狀之刻線,而副光拇 20則只有主光栅U)圓盤之⑽或1/2()的大小,光源%通過 主光柵H)後’再通過副光油,使用—光感測器(讀取頭) 5 4(H貞測光訊號變化,兩光栅之刻線平行,當對圓心有旋轉 方向轉動時,會產生週期性明暗變化,就是所謂莫爾(m。㈣ 條紋,由計算莫爾條紋數就可換算出對應轉動角度;近來 另有採用不同光學方式,應用光學繞射干涉,來產生干涉 條紋,由計算干涉條紋數換算出對應轉動角度。以上這些 10光學編碼器都含有加工與組裝所造成之角度誤差,對於高1242636 发明 Description of the invention: [Technical field to which the invention belongs] The present invention relates to an optical angle winding »flat horse, especially an optical angle encoder suitable for a high-precision rotary shaft. [Previous technology] At present, the optoelectronic industry such as the semiconductor industry and thin film transistor display is constantly growing. Nano technology has also become one of the world's most popular research directions, and the technical standards are also increasing. These industries are all optoelectronics Integrating the 10-type industry 'In order to meet this technical requirement, the precision machinery industry has been paid more attention by comparison. In the precision machinery industry, high-precision grinding machines, CNC lathes, CNC milling machines, etc. are often used. These guarding machines, in addition to requiring accurate displacement, must also have high-precision angular rotation axes to meet processing requirements. In addition, because of the distance of observation in aviation, it is also necessary to measure with a high degree of angular rotation to prevent errors. Existing high-precision rotating shafts use encoders for their angular positioning sensors. They include a disc (or grating) with countless gaps. Light emitters and sensors are installed on both sides of the disc. When moving the grating disk, the grating will block the light, and the sensor will receive the intermittent light source. The 20 computer will use the signal received by the light sensor to calculate the displacement. The optical angle encoder of the single-unit type is a thin slot with a thin disk and other angles, and then the sensor detects the light and dark changes of the light beam through the slit. For example, it is used in a mouse encoder, but its The size of the slit that can sense the change of light and darkness is limited, that is, the slit is too small to be sensed; the light 1242636 learning encoder used in industry is shown in Figure i, which contains the main light thumb and the auxiliary light thumb 20. The light thumb is like a thin disk, with equal angle radial engraved lines on the disk, while the auxiliary light thumb 20 is only the size of the main grating U) or 1/2 () of the disk, and the light source% passes through the main After the grating H) ', then pass through the secondary varnish, use-light sensor (reading head) 5 4 (H 测 measuring light signal changes, the two grating lines are parallel, when the rotation of the center of the circle direction, a cycle will occur The change in the lightness and darkness is the so-called Moire (m.㈣ fringe). The corresponding rotation angle can be converted by calculating the number of Moire fringes. Recently, different optical methods have been used to apply optical diffraction interference to generate interference fringes. The number of stripes is converted to the corresponding rotation angle. These 10 optical encoders Both include angular errors caused by processing and assembly.
精度之旋轉角度要求時,設法消除這些角度誤差就變得Z 重要。 為了解決偏心所造成角度誤差,Can0n Inc•設計一款 k-1光路型光學編碼器,其特點是兩條干涉光路分別入射到 15對稱位置(相位差180。)之反射面後,反射回來再聚集一起 產生干涉,當偏心是發生在對稱位置所構成向量方向,誤 差會自動補償,減少偏心影嚮量。另外德國聯邦物理技術 院有設計8個讀頭的光學編碼器,來抵消角度誤差。 理’上而g ’光學編碼器的讀頭愈多,愈能減少角度 20誤差影響,所以本發明採用光學方式,設計出擬似無限: 讀頭,就能完全抵消角度誤差影響。 【發明内容】 1242636 哭,二f:之主要目的係在提供一種光學式角度編碼 使編碼器在量測上,完全消除加卫與組裝所造成 i ’以達到零誤差角度量測。 10 15 外一為達成上述目的,本發明之光學式角度編碼器包括一 =圓形編料栅,具有呈輻射狀排列之複數個細縫槽, :。该任二相鄰之細縫槽延伸至圓心之夾角均相等;一第 二圓形編碼光柵,具有呈輻射狀排列之複數個細縫槽,其 了》亥任—相鄰之細縫槽延伸至圓心之夾角均相等,並與該 第-圓形編碼光柵互相平行排列,且共用一中心軸;二轉 軸,與該第二圓形編碼光栅互相連接,用以帶動該第二圓 形編碼光柵轉動;—本體’用以完全或部分容置該轉軸, 亚固定該第-圓形編碼光栅;-光源,產生-光束,在到 達該第一圓形編碼光柵與該第二圓形編碼光柵時,該光束 路徑平行該圓形編碼光栅之射心、軸,且騎範圍覆蓋該 第一圓形編碼光栅之周長;—聚线鏡,在該平行光束行 經該第-圓形編碼光柵與該第二圓形編碼光柵之該複數個 細縫槽後’以使該平行光束聚焦;以及—光感測器,置放 於該聚焦透鏡之聚;t位置’則貞知莫爾條紋之變化,以將 光訊號轉為電訊號。 【實施方式】 在2001年國際光學工程會議(pr〇c· spiE)第44〇1期第 267 〜274 頁由 Tsukasa Watanabe所提出之”Automatic high precision calibration system f〇r angle enc〇der"中,假設角 20 1242636 度編碼器因加工與組裝所造成之 哭 用度誤差為5,因為編碼 裔方疋I 一圈疋2π,所以角度誤葚括 叙 . 、差值5疋週期為2π之週期函 数,5可以η階之傅立業铋 „ 一、、及數展開(Fourier SeriesWhen the rotation angle of accuracy is required, it becomes important to try to eliminate these angle errors. In order to solve the angular error caused by eccentricity, Can0n Inc • designed a k-1 optical path type optical encoder, which is characterized in that two interference optical paths are incident on the reflecting surface of 15 symmetrical positions (phase difference 180.), and then reflected back. Gather together to generate interference. When the eccentricity occurs in the direction of the vector formed by the symmetrical position, the error will be automatically compensated to reduce the eccentric shadow vector. In addition, the German Federal Institute of Physics and Technology has designed an optical encoder with 8 read heads to offset the angular error. The more the read head of the optical encoder, the more the g 'optical encoder can reduce the effect of the angle 20 error, so the present invention adopts an optical method to design a pseudo-infinite: the read head can completely offset the effect of the angle error. [Summary of the invention] 1242636 Cry, two f: The main purpose is to provide an optical angle coding to enable the encoder to completely eliminate i ′ caused by guarding and assembly to achieve zero error angle measurement. 10 15 In order to achieve the above object, the optical angle encoder of the present invention includes a circular weaving grid with a plurality of fine slit grooves arranged in a radial pattern:. The angle between any two adjacent narrow slits extending to the center of the circle is equal; a second circular coded grating has a plurality of thin slits arranged in a radial pattern. The included angles to the center of the circle are all equal, and are arranged parallel to the first-round coded grating and share a central axis; two rotation axes are connected to the second round-coded grating to drive the second round-coded grating Rotate;-the body is used to fully or partially accommodate the rotating shaft, sub-fixing the first circular coded grating;-light source, generating-a light beam, when reaching the first circular coded grating and the second circular coded grating , The beam path is parallel to the center and axis of the circular encoding grating, and the riding range covers the perimeter of the first circular encoding grating; a condenser lens, the parallel beam passes through the first circular encoding grating and the The plurality of narrow slit grooves of the second circular coded grating are used to focus the parallel beam; and-a light sensor is placed at the focus of the focusing lens; t position is used to know the change of the moire fringe, and Turn optical signals into telecommunications signals. [Embodiment] In the 2001 International Optical Engineering Conference (pr〇c · spiE) No. 44〇1, pages 267 ~ 274, "Automatic high precision calibration system f0r angle enc〇der" proposed by Tsukasa Watanabe, Suppose that the angle 20 1242636 degree encoder has an error of 5 due to processing and assembly. Because the encoder is 疋 I one circle 疋 2π, the angle is misunderstood. The difference 5 is a periodic function with a period of 2π. , 5 can be expanded by Fourier bismuth of order η
Expansion)來表示,可以得如式1之定理: 5 10 15 s =ζΈΕ]ύηϋ~+β.) ,上 其中Ej為第j項次之振幅,已為 价為第J項次之相位角。當在2π 把圍内’平均取m個點,即每一 f, A ^ ^ 點間距相位差為k/m,該 ”,、占對應之函數值&如式2所示: .(式 2) •0 ::' m 1將坆m個點之對應函數值相加後,取平均 干^=均值等於傅立#序列巾所有_倍數項總和,表 :除=序列中m之倍數項外,其他項次會 掉。以方程式表示如式3: m m τ Ύα :I〜sin(加苧+〜).............................. 3) 讀 下 在圓周:此:疋理在編碼器設計上’若有。1個等間距分饰 頭:U值2頌’編碼11之角度誤差讀值平均值為秦 m之^數項的均值,原有角度駐部份會抵消掉,只剩下 益窮I/ ’此時角度誤差即如式3所示,若m趨近 數之無二::有傅立業項次都抵消掉’只剩下傅立業級 、人,對於貫際系統而言,愈高項次之振幅會 20Expansion), we can get the theorem of formula 1: 5 10 15 s = ζΈΕ] ύηϋ ~ + β.), Where Ej is the amplitude of the jth term, and is the phase angle of the jth term. When the average 'm points are taken within the range of 2π, that is, the phase difference between each f, A ^ ^ point is k / m, the function value of the corresponding function & is shown in Equation 2: 2) • 0 :: 'm 1 After adding the corresponding function values of 坆 m points, take the average dry ^ = mean is equal to the sum of all _ multiple items of the Fu Li # sequence towel, table: Divide = multiple items of m in the sequence In addition, other terms will be lost. Expressed as an equation: mm τ Ύα: I ~ sin (plus 苎 + ~) ............ ........ 3) Read on the circle: This: The reason for the encoder design 'if there is. 1 equidistant sub-head: U value 2 homing' the average value of the angular error reading of the code 11 It is the mean value of several terms of Qin m, the original angle resident part will be offset, and only the residual I / 'is left. At this time, the angle error is as shown in Equation 3. If m is close to the number of two :: Yes Fourier items are offset. Only the Fourier class and people are left. For the trans system, the amplitude of the higher item will be 20
I 1242636 4 '、’所以無窮大項次之彳振幅趨近於零,此時誤差δ趨近 為零。例如德國聯邦物理技術院設計之8個讀頭的光學編碼 裔’則角度誤差的傅立業級數0〜7階倍數項之振幅皆為零, 剩下8倍數項之振幅不為零(即第8、16、24、32…階振幅 5不為零),整體之角度誤差小於〇.〇〇6”。 4 本t明之光學式編碼器,第一圓形編碼光柵與第二圓 $編碼光柵較佳都為—透明基板上有等間距線條之光拇, 第圓$、扁碼光柵與第二圓形編碼光栅相對位移時,會產 生週期I*生明暗變化,就是莫爾(M〇ire)條紋,莫爾條紋之光 10訊號偵測,可應用穿透光或反射光,再計算莫爾條紋數就 可換算出對應轉動角度。 本t明之光學式角度編碼器中,轉轴較佳為穿過第二 圓形編碼光柵之中心軸,或以第二圓形編碼光拇之外_ 連接,而光源較佳為一點光源,經由一准直透鏡產生平行 光束。當點光源位在非中心軸位置時,其先經由一分光 折鏡片將光束導向朝向於第一 矛llj形編碼光柵,並延伸聚焦 之中心轴。 M、 20I 1242636 4 ',' Therefore, the amplitude of 彳 next to the infinite term approaches zero, and the error δ approaches zero at this time. For example, the optical encoder of the 8 read heads designed by the German Federal Institute of Physics and Technology has the amplitudes of the Fourier series 0 to 7 multiples of the angular error are zero, and the amplitudes of the remaining 8 multiples are not zero (that is, the first 8, 16, 24, 32 ... order amplitude 5 is not zero), the overall angular error is less than 0.006 ". 4 Optical encoders of this specification, the first circular encoder grating and the second circular encoder encoder It is preferred that there is a light-equivalent line on the transparent substrate. When the first circle $, the flat code grating and the second circular code grating are displaced relative to each other, the period I * produces a change in light and shade, which is Moire. ) Streak, Moire fringe light 10 signal detection, you can use transmitted light or reflected light, and then calculate the moire fringe number to convert the corresponding rotation angle. In this optical angle encoder, the rotation axis is better In order to pass through the central axis of the second circular coded grating, or to be connected outside the thumb of the second circular coded light source, the light source is preferably a point light source, and a parallel light beam is generated through a collimating lens. When the central axis position, it first guides the light beam through a refractive lens Llj lance toward the first encoder plate-shaped, and extends through the center axis of the focus. M, 20
杨明純用反射光計算莫爾條紋數,以換 轉動角度,此時光源與光感剛器位在第-圓形編:光柵 同-側,則該光束經由第1形編碼光栅與第= 光栅後,反射回第二圓形編 *7 跚興弟一圓形編 以被光感測器㈣。本發明若使用穿透n 數,以換算出對應轉動角廑,旲爾條¥ 月度此時光源與光感测器位在; 10 1242636 圓形編碼光栅 —圓形編碼光柵之異侧,則該光束穿透第一 與第二圓形編碼光栅,以被光感測器偵測。 在本發明之光路上,光束是平行人射第__編碼光 冊/、苐一圓形編碼光拇後,得到穿透或反射之莫爾條紋的 光訊號,在離開第一圓形編碼光柵與第二圓形編碼 後,經過準直透鏡,光束會聚焦到光感測器,如此相當於 有無數個光感測器讀頭之訊號聚集後由光感田山 式3可知為無窮大時,則所有傅立業項次都抵== 時誤差5為零。 10 為能讓貴審查委員能更瞭解本發明之技術内容,特 舉二較佳具體實施例說明如下。 實施例1 在本實施例中之光學式角度編碼器如圖2所示,包括一 15於等角度位置具有呈輻射狀排列之複數個細縫槽之第一圓 形編碼光柵110;—於等角度位置具有呈輻射狀排列之複數 個細縫槽之第二圓形編碼光栅12〇,其與第—圓形編碼光拇 110互相平行排列’且共用—中々軸;_與第二圓形編碼光 栅120外緣相連接之轉軸13〇,用以帶動第二圓形編碼光栅 20 120之轉動,亦與第一圓形編碼光栅11〇共用一中心軸,·一 用以70王谷置轉軸130並固定該第一圓形編碼光柵丨丨〇之 本體140。一光束係由位於該第一圓形編碼光柵“ο之外側 並偏離中心軸之點光源15〇產生,經由一分光轉折鏡片16〇 將該光束導向朝第一圓形編碼光柵11〇之方向,該光束並延 25伸聚焦於第一圓形編碼光栅11 〇中心軸,再經由一准直透鏡 1242636 170轉為平行光束,該光束照射範圍完全覆蓋第一圓形編碼 光柵110與第一圓形編碼光柵i 20,隨後反射回第二圓形編 碼光柵120與第-圓形編碼光柵11〇,再行經分光轉折鏡片 160以被置放於分光轉折鏡片16〇之聚焦位置之光感測器 5 偵知莫爾條紋之變化,以將光訊號轉為電訊號。 由於點光源15 0與光感測器丨8 〇位在第一圓形編碼光柵 110之同一側,故使得帶動第二圓形編碼光柵1之轉軸1 並無轉動上之阻礙,較容易被使用者操控。其中在本實施 例中,帶動第二圓形編碼光柵12〇之轉軸13〇亦可為與第二 10圓形編碼光柵120之内緣相接,並穿過第二圓形編碼光栅 120之中心軸。 在本實施例中,由於所偵測之光束為照射範圍覆蓋圓 形編碼光柵之全週長,再聚焦到光感測器以取得平均值, 故相當於有無數個光感測器讀頭之訊號聚集後由光感測器 U輸出,由式3可知,此時誤差占為零,故可消除因製造時光 柵分畫線位置之誤差,以及消除因安裝編碼器時量測中心 線與轉軸中心線之不一致(即所謂偏心)所造成之誤差。 實施例2 20 在本實施例中之光學式角度編碼器如圖3所示,包括一 於等角度位置具有呈輻射狀排列之複數個細縫槽之第一圓 形編碼光柵210;—於等角度位置具有呈輻射狀排列之複數 個細缝槽之第二圓形編碼光柵220,其與第一圓形編碼光柵 210互相平行排列,且共用一中心軸;一與第二圓形編碼光 25柵220外緣相連接之轉軸230,用以帶動第二圓形編碼光柵 12 1242636 220之轉動,亦與第一圓形編碼光栅21〇共用一中心軸;一 用以完全容置轉軸230並固定該第一圓形編碼光柵21〇之 本體240。一光束由位於第一圓形編碼光栅之中心軸上之點 光源250產生,先經一准直透鏡27〇轉為平行光束,隨後穿 5越第一圓形編碼光栅210與第二圓形編碼光柵22〇,經由一 聚=透鏡260,將該平行光束聚焦於—置放於聚焦透鏡26〇 之承焦位置光感測28G,以偵知莫爾條紋之變化,以將光 訊號轉為電訊號。Yang Mingchun uses the reflected light to calculate the number of Moire fringes in exchange for the rotation angle. At this time, the light source and the light sensor are located in the -circular series: the grating is on the same side, and the beam passes through the first-shaped encoding grating and the third grating. , Reflected back to the second circular series * 7 A young circular group was used to be pinched by a light sensor. According to the present invention, if the number of penetration n is used to convert the corresponding rotation angle 廑, the bar is at this time. The light source and the light sensor are located at this time. 10 1242636 Circular coded grating—the opposite side of the circular coded grating, then The light beam penetrates the first and second circular coded gratings for detection by a light sensor. On the light path of the present invention, the light beam is shot by a human in parallel with the first __coded light album /, and a circular coded light beam is obtained, and a light signal with a moiré pattern that penetrates or reflects is obtained. After encoding with the second circle, after collimating the lens, the light beam will be focused on the light sensor. This is equivalent to the signal of countless light sensor read heads. When the light sensor Tianshan type 3 is known to be infinite, then All Fourier terms are offset == when the error 5 is zero. 10 In order to allow your review committee to better understand the technical content of the present invention, the second preferred embodiment is described below. Embodiment 1 The optical angle encoder in this embodiment is shown in FIG. 2 and includes a first circular encoding grating 110 having a plurality of fine slits arranged radially at equal angular positions; The angular position has a second circular coded grating 12 with a plurality of fine slits arranged in a radial pattern, which are arranged parallel to the first-rounded coded thumb 110 and share the middle axis; and the second-rounded code The rotating shaft 13o connected to the outer edge of the grating 120 is used to drive the rotation of the second circular coded grating 20 120. It also shares a central axis with the first circular coded grating 110, and a rotary shaft 130 is set for 70 Wanggu The body 140 of the first circular encoding grating 丨 丨 0 is fixed. A light beam is generated by a point light source 15 located outside the first circular coded grating “ο and deviated from the central axis, and directs the light beam in the direction of the first circular coded grating 11 through a spectroscopic conversion lens 16o. The light beam is extended and focused on the central axis of the first circular coded grating 11 °, and then converted into a parallel light beam through a collimating lens 1242636 170. The irradiation range of the light beam completely covers the first circular coded grating 110 and the first circular The coded grating i 20 is then reflected back to the second circular coded grating 120 and the first-rounded coded grating 11 10, and then passes through the spectroscopic conversion lens 160 to be placed in the light sensor 5 at the focusing position of the spectroscopic conversion lens 160. Detect changes in moire fringes to convert optical signals into electrical signals. Because the point light source 150 and the light sensor 丨 800 are on the same side of the first circular encoder grating 110, the second circle is driven. The rotation axis 1 of the encoder grating 1 is not obstructed by rotation, and is relatively easy to be controlled by the user. In this embodiment, the rotation axis 13 of the second circular encoder grating 12 can also be encoded with the second 10 circle. Inner edge phase of the grating 120 And pass through the central axis of the second circular encoding grating 120. In this embodiment, since the detected light beam covers the entire circumference of the circular encoding grating in the irradiation range, it is then focused on the light sensor to obtain an average Value, so it is equivalent to the signals from countless light sensor read heads, which are output by the light sensor U after being gathered. According to Equation 3, the error account is zero at this time, so the position of the grating sub-drawing line at the time of manufacture can be eliminated. Error, and eliminate the error caused by the inconsistency between the measured centerline and the centerline of the rotating shaft when the encoder is installed (the so-called eccentricity). Embodiment 2 20 The optical angle encoder in this embodiment is shown in Figure 3. A first circular encoding grating 210 having a plurality of fine slit grooves arranged radially at an equiangular position; a second circular encoding grating 220 having a plurality of fine slit grooves arranged radially at an angular position It is arranged parallel to the first circular encoding grating 210 and shares a central axis; a rotating shaft 230 connected to the outer edge of the second circular encoding light 25 grid 220 is used to drive the second circular encoding grating 12 1242636 The rotation of 220 is also related to A circular coded grating 21 0 shares a central axis; a body 240 for completely accommodating the rotating shaft 230 and fixing the first circular coded grating 21 0. A light beam is located on the central axis of the first circular coded grating. Generated by the point light source 250, it is first converted into a parallel beam by a collimating lens 27, and then passes through the first circular coded grating 210 and the second circular coded grating 22, and passes through a focusing lens 260 to convert the parallel beam. Focus on-The 28G light sensor placed at the focusing position of the focusing lens 260 is used to detect the change of the moire fringe to convert the optical signal into a telecommunication signal.
/由於光束離開第-圓形編碼光栅與第二圓形編碼光拇 10後’會聚焦到光感測器’如同實施例i所示,其誤差占為零。 此光學式角度編碼器在量測時,可完全消除加工與組 而舉例而已,本發明所 圍所述為準,而非僅限 15 上述實施例僅係為了方便說明 主張之權利範圍自應以申請專利範 於上述實施例。 20 【圖式簡單說明】 圖1係習知光學式角度編碼器之示意圖/ Because the light beam leaves the first and second rounded coding gratings 10 and 10, it will be 'focused to the light sensor' as shown in the embodiment i, and its error will be zero. This optical angle encoder can completely eliminate processing and grouping during measurement. For example, the scope of the present invention is not limited to the above. The above embodiments are only for the convenience of explanation of the scope of the claimed rights. The patent application is based on the above embodiments. 20 [Schematic description] Figure 1 is a schematic diagram of a conventional optical angle encoder
圖2係本發明光學式角度編碼器一 圖3係本發明光學式角度編碼器另 較佳實施例之示意圖 一較佳實施例之示意Fig. 2 is a diagram of an optical angle encoder according to the present invention Fig. 3 is a diagram of another preferred embodiment of the optical angle encoder according to the present invention
【圖號說明】 30光源 10 ±光^冊 20副光柵 40 光感測器 13 1242636 110 第一圓形編碼 120 第二圓形編碼 130 轉軸 光栅 光柵 140 本體 150 點光源 160 分光轉折鏡片 170 准直透鏡 180 光感測器 210 第一圓形編碼 220 第二圓形編碼 230 轉軸 光柵 光栅 240 本體 250 點光源 260 聚焦透鏡 270 准直透鏡 280 光感測器[Illustration of drawing number] 30 light source 10 ± light ^ book 20 pairs of grating 40 light sensor 13 1242636 110 first circular code 120 second circular code 130 rotary grating grating 140 body 150 point light source 160 splitting lens 170 collimation Lens 180 Light sensor 210 First circular code 220 Second circular code 230 Rotary axis grating grating 240 Body 250 Point light source 260 Focusing lens 270 Collimation lens 280 Light sensor
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