TWI253003B - Antenna layout and coordinate positioning method for electromagnetic-induction systems - Google Patents
Antenna layout and coordinate positioning method for electromagnetic-induction systems Download PDFInfo
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5~ι發明領域: 種電 2發明背景 = 取代滑鼠’並且較滑鼠更 手寫辨識電路裝置,來急劇發展的領域。最早的 昇使用老的π从置,為將滑鼠以筆取代,並且為了提 t 1 、呆乍便利性’通常是以電磁筆盥數位板( tablet )二去炎衝说取句 电峨罕…默徂坂( ^ ^ , 來取代7月鼠’且通常以電磁筆的筆尖針靡、、典 鼠的左鍵。雖麸僂统的整彳蛉> + 苹刃聿大對應滑 類產口比從:…式輸入產品已行之多年,然而同 口口白僅偏重於繪圖或中文輪入等單一功能的應用上。5~ι invention field: seed electric 2 invention background = replace the mouse 'and more handwriting recognition circuit device than the mouse, to the field of rapid development. The earliest liters use the old π slave, in order to replace the mouse with a pen, and in order to mention t 1 , the convenience of staying 'usually using the electromagnetic pen 盥 digital tablet ( tablet ) two to Yan Chong said to take the sentence ... 默默 ( ^ ^ , to replace the 7 month mouse 'and usually with the pen tip of the electromagnetic pen, the left button of the classic rat. Although the whole glutinous rice 彳蛉 + + + + 对应 对应 对应 对应The mouth-to-mouth ratio has been implemented for many years, but the same mouth white is only focused on single-function applications such as drawing or Chinese wheeling.
* μ ί、克的電磁感應系統備有一數位板和一滑鼠或筆之型 =敕、此态/游標設備。眾所皆知,決定一描點設備在電 ^位板之表面上的位置有兩種的運作模式。一種為相對 二2,而另一種為絕對模式。一般滑鼠設備係以相對模式 §滑鼠在數位板系統表面上滑行時,電腦系統接收 A。自⑺鼠的輸入。只能辨識該滑鼠在X和γ方向的相對移動 種普遍的技術是在該滑鼠内利用一感應裝置以形成一* μ ί, gram of electromagnetic induction system is equipped with a digital tablet and a mouse or pen type = 敕, this state / cursor device. It is well known that there are two modes of operation for determining the position of a device on the surface of a plate. One is relative to two 2, and the other is absolute mode. The general mouse device is in relative mode. § The computer system receives A when the mouse slides on the surface of the tablet system. From (7) mouse input. Only the relative movement of the mouse in the X and γ directions can be recognized. A common technique is to use a sensing device in the mouse to form a
酿: i 號 91Ί_ 五、發明說明(2) 曰 修正 對相互垂直的轡拖 、 橫向沾全 、°〜’這對訊號對應於該滑鼠之縱向和 電::移動。同樣地,☆數位板系統中的游標設備,例如 ’:係於絕對模式下運作。假若提起該游標設備 腦系π至二所支持的數位板表面上之另一位置時,對該電 月白糸統而言,JL却缺肢a 的奶1 ,、也就將會改變以便於反應該游標設備之新 :::位置。J見今,已有多種方法用來決定該游標設備在 ΛΑ、之數位板表面上的位置,而其中普遍應用於絕對模 式的技術係為一種電磁感應的技術。 期的換 並經由 中。在 由使用 非方位 ,或類 相位的 、電磁 的數位 位板系 備,此 資訊。 早 位板, 腦系統 ,曾藉 功能的 的壓力 頻率和 、雜訊 在較大 良的數 描點設 位置的 月匕為/游標設備係藉由多導體電纜連接至數 此電纜將位置與按鈕/壓力的資訊傳送至電 某些傳統技術中的電磁式換能器/游標設備 頻率且/或相位改變來傳送換能器/游標設備 狀態,通常這些功能具有··按下之按鈕、筆 似的功能等。然而,若是沒有審慎的處理, 改變很容易因為多種外在因素,如金屬物品 波專專,因而導致錯誤的讀取訊號。特別是 板上,這些問題會變得越來越明顯。傳統改 統之技術允許使用者在雙模式的運作下使用 在使用者的控制下可提供相對移動或是絕對 現行之筆式輸入產品通常係為一種電磁感應電路裝置 參考第一圖所示,其係為一習知電磁電磁感應裝置之電Brewing: i No. 91Ί_ V. Invention description (2) 修正 Correction For each other, the vertical and horizontal, the ~~’ signal corresponds to the longitudinal and electric of the mouse:: Move. Similarly, vernier devices in the ☆ tablet system, such as ': operate in absolute mode. If the position of the brain device of the cursor device is raised to another position on the surface of the tablet supported by the brain, the JL is not the milk of the limb a, and will change to facilitate the reverse. Should be new to the cursor device::: location. J. Nowadays, there are various methods for determining the position of the cursor device on the surface of the tablet, and the technology widely used in the absolute mode is an electromagnetic induction technology. The exchange of the period is through. This information is provided by a non-azimuth or phase-like, electromagnetic digital tablet. The early position board, the brain system, the pressure frequency of the function that has been borrowed, and the moonlight in the position of the large number of traces of the noise are / the vernier equipment is connected by a multi-conductor cable to several cables to position and button / The information of the pressure is transmitted to the electromagnetic transducer/cursor device frequency and/or phase change in some conventional technologies to transmit the transducer/cursor device state. Usually, these functions have a button, a pen button Features, etc. However, if it is not handled with care, the change is easily due to a variety of external factors, such as metal object wave, which leads to erroneous read signals. Especially on the board, these problems will become more and more obvious. The traditionally modified technology allows the user to use a dual mode operation to provide a relatively mobile or absolute current pen input product under the control of the user. The product is typically an electromagnetic induction circuit device as shown in the first figure. Is a conventional electromagnetic electromagnetic induction device
第7頁 1253003 91109743 五、發明說明(3) 路方塊圖。電磁感應 digital tablet ) 〇 所組成之震盪線路, ,因而使得震盪頻率 大則電感量之變化越 以由頻率變化量之大 的側邊上亦有兩個開 電容震盪器中電容的 不同變化可測知使用 (tablet)亦包含了偵 )、類比數位轉換器 域係為感應迴路,在 排列之單向天線。此 專用的電磁筆所發射 時’單向天線將會接 感應的方式取得相關 號偵測的方式而言, 而降低中央處理器的 座標準確率仍是業界 裝置包含了:一電磁筆 電磁筆内具有一係由電 當碰觸筆尖時,將產生 亦隨之產生變化。碰撞 大’因而震盪頻率之變 小可知施於筆尖壓力之 關按鍵’由按鍵之接合 變化而改變筆的發射頻 者所按下之開關按鍵。 測器(detector)、放大 等元件。此類傳統之手 感應迴路的雙面具有以 單向天線迴路的主要用 的電磁波訊號。當電磁 收遠電磁波,並經由數 的資料。一般以傳統的 其所得到的座標準確率 效能與回報率。迄今, 最重要的發展目標之一 與一數位板( 感電容(LC ) 電感量之變化 筆尖之壓力越 化置越大’所 大小。電磁筆 離開產生電感 率,由頻率之 此外,數位板 器(Amp 1i f i er 寫板的中央區 陣列方式等距 途僅在於接收 筆發射電磁波 位板利用電磁 天線佈局與訊 通常不佳,因 對於如何提高 鑑於上述種種原因,本發明提供一種電磁感應系統之 天線佈局及其座標定位法,以提升座標定位之準確率並強 化電磁感應系統之效能。Page 7 1253003 91109743 V. Description of the invention (3) Road block diagram. Electromagnetic induction digital tablet ) 震 〇 组成 , , , , , , , , , , digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital digital The use of the tablet also includes the detection, the analog digital converter domain is the inductive loop, and the unidirectional antenna is arranged. When the dedicated electromagnetic pen is launched, the unidirectional antenna will be connected to the sensing method to obtain the correlation number detection method, and the reduction of the standard accuracy of the central processing unit is still included in the industry device: an electromagnetic pen electromagnetic pen There is a series of electricity that will generate and change when it touches the tip of the pen. The collision is large, and thus the oscillation frequency is small. It is known that the button applied to the pen tip pressure is changed by the engagement of the button to change the switch button pressed by the pen's transmission frequency. Detector, magnifying and other components. The double-sided side of such a conventional hand sensing circuit has a primary electromagnetic wave signal for a one-way antenna loop. When the electromagnetic is far away, the electromagnetic wave is passed through the number of data. The performance and return rate are generally determined by the traditional seat standard. So far, one of the most important development goals is the size of a digital tablet (the capacitance of the sensing capacitor (LC) changes the pressure of the nib." The electromagnetic pen leaves to generate the inductivity, and by the frequency, the tablet (Amp 1i fi er write board central area array mode is equidistant only in the receiving pen emission electromagnetic wave board using electromagnetic antenna layout and communication is generally poor, because for how to improve, in view of the above various reasons, the present invention provides an electromagnetic induction system Antenna layout and its coordinate positioning method to improve the accuracy of coordinate positioning and enhance the performance of the electromagnetic induction system.
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鑒於上述之發明背 應裝置的座標準確率 11〜為了強化與增加傳統電磁感 系統之天線佈局及其二j,、’本發明提供一種電磁感應 磁感應裝置的座標^ 2 f法可用以增加與改善傳統電 平及具效能。 本發明之一目的传捭In view of the above-mentioned invention, the standard deviation rate of the device is 11~~ In order to strengthen and increase the antenna layout of the conventional electromagnetic induction system, the present invention provides a coordinate of the electromagnetic induction magnetic induction device, which can be used to increase Improve traditional levels and performance. One of the objectives of the present invention
程序。本發明係採用種電磁感應系統之座標定 的準確性,並使JL成# 式座標定位法以提高座標定 符合產業上標回報率更加快速。因此,本發明 本發明之另一目的係提供 座標定位法。本發明係藉由一 置的计异能更為精準。據此, )的處理時間,並可避免手寫 強化電磁感應系統之效能。 一種電磁感應系統之五段式 座標計算程式以使得座標位 本發明可減少微控制器(CPU 輪入時的線性不良之問題以program. The invention adopts the accuracy of the calibration of the electromagnetic induction system, and makes the JL into the # coordinate coordinate positioning method to improve the coordinate of the coordinate to meet the industrial benchmark return rate. Accordingly, another object of the present invention is to provide a coordinate positioning method. The present invention is more accurate by the ability to measure the difference. According to this, the processing time can be avoided and the performance of the hand-held enhanced electromagnetic induction system can be avoided. A five-stage coordinate calculation program of an electromagnetic induction system to make a coordinate position. The present invention can reduce the problem of a linear controller (the problem of linearity when the CPU is wheeled)
本發明之再一目的係提供一種電磁感應系統之天線佈 1。本發明係採用一四四分式天線佈局以降低天線佈局之 密度。因此’本發明可縮減印刷電路板(Printed Circuit Board ; PCB )的面積,並減少生產工時,以達到縮減產品 尺寸的目的。據此,本發明能符合經濟上的效益。Still another object of the present invention is to provide an antenna cloth 1 for an electromagnetic induction system. The present invention employs a four-quarter antenna layout to reduce the density of the antenna layout. Therefore, the present invention can reduce the area of the printed circuit board (PCB) and reduce the production man-hours for the purpose of reducing the size of the product. Accordingly, the present invention is economically advantageous.
第9頁 1253003 修正Page 9 1253003 Revision
Afe 91109743 五'發明說明(5) 根據 統之四四 四分式天 佈列於電 路,以便 線迴路可 具有等間 路與降低 複數個天 ,亦即一 ,則只會 線迴圈的 當電磁場 感應訊號 =士所述之目的,本發明揭示了一種電磁 :式天線佈局與五段式座標定位法。本發明:二 故佈局係將電磁感應系統的感應天線依序等距地 板的兩面,並以二維陣列的方式組成一天線迴 乂在電磁場變化時能得到較為清楚的訊號。此天 ς為X方向與γ方向兩群組,同一群組皆為同向且 „移之天線迴路。& 了能均句地配置天線迴 各佈局之在度’每個方向群内的天線迴路包含 二,圈,例如,以4條天線迴圈組成一 /天線迴路 $ 7虎發射源置於天線迴圈之主要區域的正上方時 =3條天線迴圈把發射源包在圈内。而每一條天 =成^含自身密集多次重覆绛圈的方法。因此, :生變化時,圈數較多的天線可產生相對較強的 步驟:首先η之五段 程序至少包含下列 切《 啼 程序為「全域掃描」,以便於確 μ的電壓振幅強度大於訊號識別準位下限值; = …中域確認掃描」,以便於確認 天線迴圏去存在,亚確認與發射源最接近之 ,以便於取二r L,進了 一第三程序為「局部確認掃描」 哭可侬櫨据:圭標值;冑後,電磁感應系統之内部微處理 W 了依據振幅之座標值計算出一組絕對座標。Afe 91109743 five 'inventive description (5) according to the unified four four four-pointed sky cloth listed in the circuit, so that the line circuit can have an equal path and reduce the number of days, that is, one, only the line of the loop when the electromagnetic field Inductive signal = the purpose of the description, the present invention discloses an electromagnetic: antenna layout and five-segment coordinate positioning method. The invention has the following advantages: the illuminating system of the electromagnetic induction system sequentially aligns the two sides of the slab, and forms an antenna in a two-dimensional array to obtain a clear signal when the electromagnetic field changes. This day is two groups of X direction and γ direction, the same group are all in the same direction and the antenna loop is moved. & The antenna can be arranged in the same way as the antennas in each direction group. The loop consists of two loops, for example, consisting of four antenna loops forming an antenna loop. $7 The tiger emitter is placed directly above the main area of the antenna loop = 3 antenna loops enclose the source in the loop. And each day = Cheng ^ contains its own method of densely repeating the circle. Therefore, when the change occurs, the antenna with more turns can produce relatively strong steps: first, the five-segment program of η contains at least the following cuts. The 啼 program is a “global scan” so that the voltage amplitude of the μ is greater than the lower limit of the signal recognition level; = ... the medium-area confirmation scan, in order to confirm that the antenna is present, the sub-confirmation is closest to the source. In order to take two r L, a third program is called "local confirmation scan". The crying can be based on: the value of the standard; after that, the internal micro-processing of the electromagnetic induction system is calculated based on the coordinate value of the amplitude. A set of absolute coordinates.
I 1253003 Λ. 修正 五 、發明說明(6) 5 - 4發明的詳細說明: 本發明在此所探討的方向為一種電磁感應系統之天線 佈局及其座標定位法。為了能徹底地瞭解本發明,將在下 列的描述中提出詳盡的發明步驟或結構元件。顯然地,本 發明的施行並未限定於電路系統之技藝者所熟習的特殊細 卽。另一方面,眾所周知的步驟或元件並未描述於細節中 ,以避免造成本發明不必要之限制。本發明的較佳實施例 會詳細描述如下,然而除了這些詳細描述之外,本發明還 可以廣泛地施行在其他的實施例中,且本發明的範圍不受 限定,其以之後的專利範圍為準。 參考第二Α圖所示,在本發明之一實施例中,首先提 供一電磁感應系統2 0 0,電磁感應系統2 〇 〇至少包含:一天 線次電路205、一内部電路2 10與一微處理次電路21 5,其 中’内部電路210更包含一渡波次電路、一放大次電路、 一整流次電路與一數位-類比轉換次電路。微處理次電路 215至少包含複數個暫存器225,且微處理次電路215内部 可設定儲存一電壓參考值,此即為訊號識別準位下限值, 其中,訊號識別準位下限值係用以區別所接收之訊號是否 為雜訊。此外,訊號識別準位下限值的設定係在電磁感應 系統20 0的附近無任何明顯電波發射源時,電磁感應系統I 1253003 Λ. Amendment 5, Invention Description (6) 5 - 4 Detailed Description of the Invention: The invention is directed to an antenna layout of an electromagnetic induction system and its coordinate positioning method. In order to fully understand the present invention, detailed inventive steps or structural elements are set forth in the description below. Obviously, the implementation of the present invention is not limited to the particular details familiar to those skilled in the art of circuitry. On the other hand, well-known steps or elements are not described in detail to avoid unnecessarily limiting the invention. The preferred embodiments of the present invention are described in detail below, but the present invention may be widely practiced in other embodiments, and the scope of the present invention is not limited by the scope of the following patents. . Referring to the second figure, in an embodiment of the present invention, an electromagnetic induction system 200 is first provided, and the electromagnetic induction system 2 includes at least: an antenna sub-circuit 205, an internal circuit 2 10 and a micro The secondary circuit 21 5 is processed, wherein the 'internal circuit 210 further includes a wave sub-circuit, an amplifying sub-circuit, a rectifying sub-circuit and a digital-analog conversion sub-circuit. The micro-processing sub-circuit 215 includes at least a plurality of registers 225, and the micro-processing sub-circuit 215 can be internally configured to store a voltage reference value, which is a signal recognition level lower limit value, wherein the signal recognition level lower limit value is It is used to distinguish whether the received signal is noise. In addition, the setting of the lower limit value of the signal recognition level is in the vicinity of the electromagnetic induction system 20 0 without any obvious radio wave emission source, and the electromagnetic induction system
第11頁 1253003 —----- 銮號 911097“_年 月 日___ 五、發明說明(7) 2 0 0經由自身天線接收及内部電路21 〇處理之後所得到的雜 訊之最大電壓值,因此,訊號識別準位下限值大於一般雜 訊電壓值。據此,電磁感應系統2 0 0内的微處理次電路21 5 K需定時檢查所收得的電壓值是否大於訊號識別準位下限 值’如果接收的電壓值大於訊號識別準位下限值,即可判 定有一訊號發射源接近電磁感應系統2 〇 〇。一般而言,電 磁感應具有電磁訊號的強度與其距離平方成反比之特性。 對接收瑞而言,當發射源遠離接收天線時,其訊號之電壓 的^幅強度會小於雜訊之電壓的振幅強度;相對地,對接 收3而而言’當發射源接近接收天線時,其訊號之電壓的振 幅強度會大於雜訊之電壓的振幅強度。 參考第圖與第·二C圖所示,在本實施例中,本發明 之電磁感應系統2〇〇的天線次電路2〇5至少包含一四四分式 天線佈局’其中’四四分式天線佈局的天線配置方法更包 a —一維陣列式配置法,其座標位置可採用笛卡兒二維座 不(two dimensi〇nai cartesian coordinates),例如, 四四分_式天線佈局可將複數個具有不同方向之天線群組 以一維卩列式配置法等距排列於電路板的兩面,以便 205之複數條天線 應線圈的材質更包八3 一迴圈式感應線圈,且迴圈式感 複數個具有不同銅料線。根據笛卡紅維座標, 22ΠΑ ^ ^ ^向之天線群組220包含一X方向天線群組 ’、 ° 線群組22〇Β·,其中,同方向之天線群組Page 11 1253003 —----- 911 911097 “ _ _ _ _ _ _ _ 5, invention description (7) 2 0 0 through the self-antenna receiving and internal circuit 21 〇 processing after the maximum voltage value of the noise Therefore, the lower limit value of the signal recognition level is greater than the general noise voltage value. Accordingly, the micro-processing sub-circuit 21 5 K in the electromagnetic induction system 200 needs to periodically check whether the received voltage value is greater than the signal recognition level. The lower limit value 'If the received voltage value is greater than the lower limit value of the signal recognition level, it can be determined that a signal source is close to the electromagnetic induction system 2 一般. Generally, the electromagnetic induction has an electromagnetic signal whose intensity is inversely proportional to the square of its distance. For receivers, when the source is far away from the receiving antenna, the amplitude of the voltage of the signal will be less than the amplitude of the voltage of the noise; in contrast, for the receiver 3, when the source is close to the receiving antenna When the amplitude of the voltage of the signal is greater than the amplitude of the voltage of the noise, as shown in the figure and the second C, in the present embodiment, the antenna of the electromagnetic induction system of the present invention The sub-circuit 2〇5 includes at least a four-four-four antenna layout. The antenna configuration method of the 'four-quarter antenna layout is more a-one-dimensional array configuration method, and the coordinate position can be used by the Cartesian two-dimensional seat. (two dimensi〇nai cartesian coordinates), for example, a four-quarter antenna array layout can arrange a plurality of antenna groups with different directions in a one-dimensional array configuration on both sides of the circuit board, so as to have a plurality of 205 The antenna of the strip antenna should be composed of eight 3 loop-type induction coils, and the loop-shaped multiples have different copper wires. According to the Cartesian red-dimensional coordinates, the antenna group 220 contains an X. Directional antenna group ', ° line group 22〇Β·, where antenna groups in the same direction
1253003 _ _案號91109743 年月日 修,下 五、發明說明(8) 220A與220B内的天線迴路23 0A與230B皆為同向且具有等間 距性位移。再者,X方向天線群組22 0A與Y方向天線群組 220B分別包含N/4組X方向天線迴路230A與M/4組Y方向天線 迴路23 0B。此外,每組X方向天線迴路230A與Y方向天線迴 路2 3 0B皆包含四條天線迴圈235 A與2 35B,以便於能夠均句 佈置天線迴圈於電路板的兩面。因此,N/4組X方向天線迴 路230A的天線迴圈235A總數係為N,且M/4組Y方向天線迴 路2 30B的天線迴圈235B總數係為Μ。以同方向之天線迴圈 2 3 5Α或235Β而言,若一訊號發射源置於一天線迴圈235八或 2 3 5Β的主要區域之正上方時,則約有三條天線迴圈235人或 23 5Β把發射源包於其内。另一方面,每條天線迴圈235人與 235Β更包含一多重迴圈式感應天線,其方法係將同一天^ 迴圈以密集多次重覆繞圈的方式形成一感應天線,例如, 四迴圈式感應天線,此係由於在電磁場發生變化時,圈數 較多的天線可產生相對較強的感應訊號,如第二D圖所示 ⑨參考第二Ε圖所示,在本實施例中,根據笛卡兒二維 座4不本&月之電磁感應糸統2 0 0所進行的座標定位法至 少包含一五段式座標定位法,五段式座標定位法如下所述 。百先,進行一第一全域掃描程序24〇,其係針對义方向天 線群組2 2 0 A進行全方位掃描的程序,以便於確認具有大於 Λ號識別準位下限值之天線迴圈的位址。第一全域掃描程 序240的方法係藉由依時分序的方式進行χ方向天線群組1253003 _ _ Case No. 91109743 Rev. 5, Inventor's Note (8) The antenna loops 23 0A and 230B in 220A and 220B are in the same direction and have an equidistant displacement. Furthermore, the X-direction antenna group 22 0A and the Y-direction antenna group 220B respectively include N/4 sets of X-direction antenna circuits 230A and M/4 sets of Y-direction antenna circuits 23 0B. In addition, each set of X-direction antenna loop 230A and Y-direction antenna loop 2 3 0B includes four antenna loops 235 A and 2 35B, so that the antenna loops can be arranged on both sides of the board. Therefore, the total number of antenna loops 235A of the N/4 group X-direction antenna loop 230A is N, and the total number of antenna loops 235B of the M/4 group Y-direction antenna loops 2 30B is Μ. In the same direction of the antenna loop 2 3 5 Α or 235 ,, if a signal source is placed directly above the main area of an antenna loop 235 eight or 2 3 5 ,, then there are about three antenna loops of 235 people or 23 5ΒPack the source in it. On the other hand, each antenna loop 235 people and 235 Β includes a multiple loop-type sensing antenna. The method is to form an inductive antenna in a densely repeated manner on the same day, for example, Four-loop type induction antenna, because the antenna with a larger number of turns can generate a relatively strong induction signal when the electromagnetic field changes, as shown in the second D figure, the reference to the second figure is shown in this embodiment. In the example, the coordinate positioning method according to the Cartesian two-dimensional seat 4 and the monthly electromagnetic induction system 2000 includes at least a five-segment coordinate positioning method, and the five-segment coordinate positioning method is as follows. Hundreds of first, a first global scanning procedure is performed, which is a program for omnidirectional scanning of the antenna group 2 2 0 A in the sense direction, in order to confirm the antenna loop having a lower limit value than the nickname identification level. Address. The method of the first global scanning program 240 performs the χ direction antenna group by means of time division
第13頁 1253003 η 修正 曰 五、發明說明(9) 2 2 0 Α的所有w | 方式係在间_條天線迴圈235A之掃描,其中,依時分序的 圈係為關閉夺,内只開啟一條天線迴圈且其餘的天線迴 迴圈,斷路的狀態。首先’僅開啟第一條天線 210求π ★條天線迴圈所取得之信號經由内部電路 搜、第一條天線迴圈的訊號之最大電壓振幅’且將其 H微處理次電路215中進行一第一比對程序245以比較 條天線迴圈的訊號之最大電壓振幅與訊號識別準位下 If =的大小。然後’依序開啟每一條天線迴圈並反覆進行 上述的第一全域掃描程序24 0與第一比對程序245,直到X 方向天線群組22 0A的所有N條天線迴圈235A皆開啟一次, 並取得N個訊號之電壓振幅。在N個訊號之電壓振幅皆與訊 號:識別準位下限值比較後,將具有最大電壓振幅大於訊號 識別準位下限值之天線迴圈的編號值χρ記錄於一暫存器χ_ 中。若沒有任一天線迴圈的訊號振幅值大於訊號識別準位 下限值時,則再反覆進行第一全域掃描程序240與第一比 對程序245直到出現最大電壓振幅大於訊號識別準位下限 值之一訊號為止。 參考第二Ε圖與第二F圖所示,在本實施例中,進行一 中域確認掃描程序2 5 0,以確認前次掃描X方向天線群組 220Α的具有最大電壓振幅強度之訊號是否仍然存在,並找 出發射源與哪條天線迴圈最接近,以避免具有最大電壓振 幅強度之訊號係為環境中瞬間出現的雜訊突波。中域確認 掃描程序250的方法如下所述:首先,微處理次電路21 5取Page 13 1253003 η 曰 、, invention description (9) 2 2 0 所有 all w | mode is in the scanning of the _ antenna loop 235A, wherein the time-series circle is closed Turn on one antenna loop and the rest of the antennas return to the loop, the state of the open circuit. First, 'only open the first antenna 210 to obtain π ★ the signal obtained by the antenna loop is searched via the internal circuit, the maximum voltage amplitude of the signal of the first antenna loop' and the H micro-processing sub-circuit 215 is performed. The first comparison program 245 compares the maximum voltage amplitude of the signal of the loop back of the strip antenna with the magnitude of If = under the signal recognition level. Then, each antenna loop is sequentially turned on and the first global scanning program 240 and the first comparison program 245 are repeatedly performed until all N antenna loops 235A of the X-direction antenna group 22 0A are turned on once. And obtain the voltage amplitude of N signals. After the voltage amplitudes of the N signals are compared with the signal: the lower limit of the identification level, the number value χρ of the antenna loop having the maximum voltage amplitude greater than the lower limit of the signal recognition level is recorded in a register χ_. If the signal amplitude value of any of the antenna loops is greater than the signal recognition level lower limit value, then the first global scan program 240 and the first comparison program 245 are repeatedly performed until the maximum voltage amplitude is greater than the signal recognition level lower limit. One of the values is the signal. Referring to the second and second F diagrams, in the present embodiment, a mid-field confirmation scan program 250 is performed to confirm whether the signal having the maximum voltage amplitude intensity of the previous scan X-direction antenna group 220A is It still exists and finds which antenna is closest to the antenna's loop, so that the signal with the maximum voltage amplitude is the instantaneous noise burst in the environment. The method of the middle field confirmation scanning program 250 is as follows: First, the micro processing sub circuit 21 5 takes
第14頁 1253003 j 案號91109743 年月曰 修正 五、發明說明(10) "Page 14 1253003 j Case No. 91109743 Year Month Revisions V. Inventions (10) "
出記錄於暫存器Xt〇p之天線迴圈編號&,並將此天線迴圈& 設定為中域確認掃描基準;然後,以天線迴圈&為中心, 重新依序掃描X方向天線群組220Α内包含天線迴圈&在内 的半數天線迴圈’亦即Ν / 2條天線;接著,在取得X方向天 線群組220Α之Ν/2條天線迴圈的ν/2個訊號振幅後,再傳送 至微處理次電路215進行一第二比對程序255以比較Ν/2個 訊號之最大電壓振幅與訊號識別準位下限值的大小;若有 另一天線迴圈的訊號之電壓振幅大於訊號識別準位下限值 時’則更新暫存器Xt〇p之天線迴圈的編號值;相對地,若 無任一天線迴圈的訊號振幅值大於訊號識別準位下限值 曰守’則再重新進行第一全域掃描程序2 4 〇與第一比對程序 2 4 5直到出現最大電壓振幅大於訊號識別準位下限值之一 訊號為止。此外,若是p + ( N/4 )大;或p — ( N/4 )小 於1時,則中域確認掃描程序250之範圍係以天線佈局之邊 界為限,掃描包含天線迴圈Xp在内的N/2條天線迴圈。Output the antenna loop number & recorded in the register Xt〇p, and set the antenna loop & to the mid-field confirmation scan reference; then, scan the X direction sequentially with the antenna loop & The antenna group 220Α contains half of the antenna loops of the antenna loop & that is, Ν / 2 antennas; then, ν/2 of the loop antennas of the X-direction antenna group 220Α After the signal amplitude is transmitted to the microprocessor sub-circuit 215, a second comparison program 255 is performed to compare the maximum voltage amplitude of the Ν/2 signals with the lower limit value of the signal recognition level; if there is another antenna loop When the voltage amplitude of the signal is greater than the lower limit of the signal recognition level, the number of the antenna loop of the register Xt〇p is updated; in contrast, if the amplitude of the signal without any antenna loop is greater than the signal recognition level The limit value is followed by 'the first global scan program 2 4 〇 and the first comparison program 2 4 5 until the maximum voltage amplitude is greater than one of the lower limit of the signal recognition level. In addition, if p + ( N / 4 ) is large; or p - ( N / 4 ) is less than 1, the range of the medium-area confirmation scan program 250 is limited to the boundary of the antenna layout, and the scan includes the antenna loop Xp. N/2 antenna loops.
隨後,進行一第一局部確認掃描程序26〇以掃描χ方向 天線群組2 2 0 A中具有最大訊號振幅值的天線迴圈&之局部 區域,並取得X方向的座標值。首先,取出儲存於暫存器 Xt〇P中的具有最大電壓振幅之天線迴圈編號值χρ,並依據訊 號強度與距離平方成反比的物理特性,可判定訊號發射源 敢接近天線迴圈Χρ,亦即訊號發射源係位於天線迴圈^的 正上方範圍内;然後,再依序進行一掃描程序,其範圍包 含天線迴圈Xp在内的5條天線迴圈,亦即逐一掃描天線迴Then, a first partial confirmation scanning program 26 is performed to scan the local area of the antenna loop & which has the largest signal amplitude value in the antenna group 2 2 0 A, and obtain the coordinate value in the X direction. First, the antenna loop number value χρ having the maximum voltage amplitude stored in the register Xt〇P is taken out, and according to the physical characteristic that the signal intensity is inversely proportional to the square of the distance, it can be determined that the signal source dares to approach the antenna loop Χρ, That is, the signal source is located directly above the antenna loop ^; then, a scanning process is performed in sequence, which includes five antenna loops including the antenna loop Xp, that is, scanning the antenna one by one.
第15頁 1253003 曰 修正 五、發明說明(11) 圈Χρ_2 Xp-l、Χρ、Xp+l、Xp + 2專五條天線迴圈以取得五個訊號 振幅值,並分別存入複數個暫存器χΐ、χ2、χ3、以與“ 中。然後,進行一第二全域掃描程序2 6 5,其係針對Υ方向 天線群組22 〇 Β進行全方位的掃描程序以確認發射源最接近 之天線迴圈,其中,第二全域掃描程序2 65的施行方式如 第一全域掃描程序2 4 0所述,亦需藉由依時分序的方法進 行掃描程序以取得Μ條天線迴圈2 35Β之Μ個訊號振幅值,並 進行一第三比對程序2 7 0以比對μ個訊號振幅值彼此之間的 大小’且取得具有最大訊號振幅值之天線迴圈位置。因 此,第二全域掃描程序265不同於第一全域掃描程序24〇者 係在於Μ條天線迴圈235Β之Μ個訊號振幅值並不需與訊號識 別,位下限值進行比較,而是以Υ方向天線群組22〇β之^個 訊號振幅值進行比較。當γ方向天線群組22〇β之%條天線迴 圈的Μ個訊號振幅值皆被取得之後,可找出具有最大訊號 振幅值之天線迴圈γρ並儲存於微處理次電路215之一暫存 其-人,進行一第二局部確認掃描程序2 7 5以掃描Y方向 天線群組220B中具有最大訊號振幅值的天線迴圈γρ之局部 區域,並取得Υ方向的座標值。首先,取出儲存於Ρ暫存器 Yt〇P中具有最大訊號振幅之天線迴圈編號值&,並依據訊號 強度與距離平方成反比的物理特性,可判定訊號發射源最 接近天線迴圈γρ,亦即訊號發射源位於天線迴圈γ的正上 方範圍内H,再次依序進行另一掃描程序,?其範圍包Page 15 1253003 曰Revision 5, invention description (11) Χρ_2 Xp-l, Χρ, Xp+l, Xp + 2 special five antenna loops to obtain five signal amplitude values, and respectively stored in a plurality of registers Χΐ, χ2, χ3, and "中. Then, a second global scanning procedure 2 6 5 is performed, which performs a omnidirectional scanning procedure for the Υ direction antenna group 22 以 to confirm the antenna back closest to the source. The circle, wherein the second global scanning program 2 65 is implemented as described in the first global scanning program 240, and the scanning procedure is also performed by the time-sequential method to obtain the loop antenna loop 2 35 Β The signal amplitude value is subjected to a third comparison program 270 to compare the magnitudes of the μ signal amplitude values with each other and obtain the antenna loop position having the largest signal amplitude value. Therefore, the second global scanning procedure 265 Different from the first global scanning program, the amplitude of the signal amplitude of the 天线 antenna loop 235Β does not need to be compared with the signal identification, the lower limit value, but the antenna group 22〇β in the Υ direction. ^ signal amplitude values are compared. After all the signal amplitude values of the γ-directional antenna group 22 〇β of the antenna loop are obtained, the antenna loop γρ having the largest signal amplitude value can be found and stored in one of the micro-processing sub-circuits 215. The person-in-person performs a second partial confirmation scanning procedure 275 to scan a local region of the antenna loop γρ having the largest signal amplitude value in the Y-direction antenna group 220B, and obtains the coordinate value in the Υ direction. First, the storage is taken out. The antenna loop number value & with the maximum signal amplitude in the buffer Yt〇P, and according to the physical characteristics of the signal intensity inversely proportional to the square of the distance, can determine that the signal source is closest to the antenna loop γρ, that is, the signal The emission source is located in the range directly above the antenna loop γ, and another scanning procedure is performed in sequence, and the range is packaged.
.二.丄.丄 1253003.二.丄.丄 1253003
含天線迴圈γρ在内的5條天線迴圈,亦即逐一掃描天線迴 圈γρ_2、Υρ-ι、Υρ ' γρ+1、γρ+2等五條天線迴圈以取得五個訊號 振幅值,並分別存入複數個暫存器Y1、Υ2、Υ3、Υ4、Υ5 中。 參考第二F圖所示,在本實施例中,當完成上述程序 之後’可依據各方向所取得之振幅值(XI、χ3、Χ4、 Χ5)與(γΐ、Υ2、γ3、γ4、γ5)分別進行一χ座標定位程 序280與一Υ座標定位程序28 5,以計算出一組絕對座標。 因此’經由第一局部確認掃描程序2 6〇與第二局部確認掃 描程序275取得最大振幅值,且依據訊號強度與距離成反 比的特性’可判定具有振幅最大值之天線迴圈的相鄰兩天 ,迴圈應具有振幅的葶二大值及第三大值。據此,χ座標 定位程序280的施行方法如下所述:首先,進行一第四比 對程序280Α以比較暫存器Χ1、χ2、χ3、χ4、χ5内所儲存之 複,個振幅值彼此之間的大小,並儲存振幅最大值於一暫 存=Xmax中,且儲存具有振幅最大值之天線迴圈編號於暫 存益x:p中。接著,進行一第一邏輯判斷程序28〇B以判斷 2存益XI、X2、X3、X4、X5之電壓振幅的最大值為何者。 當電壓振幅之最大值判斷為暫存器^或“的資料,則進行 一第二邏輯判斷程序28〇c以判別暫存器χι或“所對應之 線迴圈的位址是否為X方向天線群組22〇A之第一條天^線迴 圈或第N條天線迴圈;若為是,則可直接判定訊號發射源 係位於X方向天線群組22 〇A兩側邊緣區上280D ;若為否,Five antenna loops including antenna loop γρ, that is, five antenna loops such as γρ_2, Υρ-ι, Υρ ' γρ+1, γρ+2 are scanned one by one to obtain five signal amplitude values, and They are stored in a plurality of registers Y1, Υ2, Υ3, Υ4, Υ5, respectively. Referring to the second F diagram, in the present embodiment, after the above procedure is completed, the amplitude values (XI, χ3, Χ4, Χ5) and (γΐ, Υ2, γ3, γ4, γ5) which can be obtained according to the respective directions are obtained. A coordinate positioning program 280 and a coordinate positioning program 28 5 are separately performed to calculate a set of absolute coordinates. Therefore, the maximum amplitude value is obtained by the first partial confirmation scanning program 206 and the second partial confirmation scanning program 275, and the adjacent two of the antenna loops having the amplitude maximum can be determined according to the characteristic of the signal intensity inversely proportional to the distance. Days, the loop should have the largest value and the third largest value of the amplitude. Accordingly, the method for performing the χ coordinate positioning program 280 is as follows: First, a fourth comparison program 280 is performed to compare the complex values stored in the registers Χ1, χ2, χ3, χ4, χ5 with each other, and the amplitude values are mutually The size of the interval, and store the amplitude maximum in a temporary storage = Xmax, and store the antenna loop number with the maximum amplitude in the temporary benefit x: p. Next, a first logic determination program 28A is performed to determine the maximum value of the voltage amplitudes of the two benefits XI, X2, X3, X4, and X5. When the maximum value of the voltage amplitude is judged as the data of the register or "", a second logic determining program 28〇c is performed to determine whether the address of the corresponding line loop or the corresponding line loop is an X-direction antenna. The first day of the group 22〇A loop or the Nth antenna loop; if yes, it can be directly determined that the signal source is located at 280D on both sides of the X-direction antenna group 22 〇A; If no,
第17頁 1253003 r----9110咖 t 1日 條正 五、發明酬(13) -------- 再次回到中域確認掃描程序250。當電壓振幅之最大 =判斷不為暫存器X1 4X5的資料,則進行一第一資料儲存 $ =28 0^以便於分別儲存電壓振幅之第二大值與第三大值 、存器tnd與Ird中;例如,具有振幅最大值的天線迴圈 D相鄰兩天線迴圈與X州的振幅值分別儲存於複數個 子器Ind與\Γ(1中,其中,天線迴圈&之振幅最大值係儲 子於一暫存器xmax中,而天線迴圈χ之編號係儲存 Φ p u 八top 然後,可藉由微處理次電路215進行一第一運算程序 280F,其運异方式如下所述:首先,藉由電壓振幅之最大 值Xmax分別減去電壓振幅之第二大值與第三大值,以 =得一第一電壓振幅差距值(X隨—Xw )與一第二電d壓振 中田差距值(Xmax 一 Ird );然後,以第一電壓振幅差距值, 、(、X2nd )與第二電壓振幅差距值(一 Id )的和作 為^母,=及第一電壓振幅差距值(—kd )為分子得 出一具有最大電壓振幅之彼此相鄰的三條天線迴圈χ 、χ 與Xp+l之電壓振幅斜率值;接著,將電壓振幅斜率值^上P 一基本解析度常數值Kr以得到一X方向之相對座標值Xr, 其中,基本解析度常數值Kr的定義係為單一條天線迴圈彼 此^間的解析度,其定義為一英吋的期望解析度點數除以 一英忖之内的天線數目,亦即每固定距離内的座標點數, 且基本解析度常數值Kr通常設定且儲存於微處理次電路 2 1 5中;據此,本發明之運算式如下所述··Page 17 1253003 r----9110 coffee t 1 day Article 5, invention reward (13) -------- Return to the middle field confirmation scan program 250 again. When the maximum voltage amplitude = the data of the scratchpad X1 4X5 is determined, a first data storage $=28 0^ is performed to store the second largest value and the third largest value of the voltage amplitude, respectively. In Ird; for example, the antenna loop D with the maximum amplitude is adjacent to the two antenna loops and the amplitude values of the X state are stored in a plurality of sub-injectors Ind and \Γ (1, where the amplitude of the antenna loop & The value is stored in a register xmax, and the number of the antenna loop is stored as Φ pu 八top. Then, the first operation program 280F can be performed by the micro-processing sub-circuit 215. First, the second largest value and the third largest value of the voltage amplitude are respectively subtracted by the maximum value Xmax of the voltage amplitude, and a first voltage amplitude difference value (X with -Xw) and a second electric d voltage are obtained. Zhenzhongtian gap value (Xmax-Ird); then, the sum of the first voltage amplitude difference value, (, X2nd) and the second voltage amplitude difference value (Id) as the mother, = and the first voltage amplitude difference value (—kd ) is a molecule that gives a three-day adjacent to each other with the largest voltage amplitude The voltage amplitude slope value of the loops χ, χ and Xp+l; then, the voltage amplitude slope value is added to P a basic resolution constant value Kr to obtain an X coordinate relative coordinate value Xr, wherein the basic resolution constant value Kr is defined as the resolution between the loops of a single antenna, which is defined as the number of points of the desired resolution divided by one inch divided by the number of antennas within one inch, that is, the number of coordinates per fixed distance. And the basic resolution constant value Kr is normally set and stored in the micro-processing secondary circuit 2 15; accordingly, the arithmetic expression of the present invention is as follows...
第18頁 1253003 五、發明說明(14) 曰 修正 此外,相對座標值Xr係利 天線迴圈Χη、χρ與^+1所計算局°卩掃描彼此相鄰之三條 相對座標值xr換算成真實的絕目對座標。因此必須將 二運算程序280G,其運算方式。最後’進行一第 條天線迴圈Χρ1'χ盥X距猎由相對座標值Xr加上三 ^ ^ ^ ^ 異的MX方向天線群組22 0A之原點 m真實座標值xa ’因此,相對座標值xr加上基底座 =的和即為真實座標值或絕對座標xa,第二運算程 序280G之方程式如下所示:Page 18 1253003 V. INSTRUCTIONS (14) 曰Correction In addition, the relative coordinate value Xr is converted into the actual coordinate value of the antenna coordinates Χη, χρ and ^+1 calculated by the relative coordinates xr adjacent to each other. The target is perfect. Therefore, the second operation program 280G must be used. Finally, 'perform a first antenna loop Χρ1'χ盥X from the relative coordinate value Xr plus three ^ ^ ^ ^ different MX direction antenna group 22 0A origin m true coordinate value xa ' Therefore, relative coordinates The sum of the value xr plus the base base = is the true coordinate value or the absolute coordinate xa, and the equation of the second operation program 280G is as follows:
Xr +Xbase ’且Xbase = (χ_ — 1 ) X κΓ 如上所述,根據本發明之座標計算程式之一實施例如 下·若(X1、X2、X3、X4、X5) = (3〇、60、85、70、 45),且(XI、X2、X3、X4、X5)分別對應之天線編號= (6、7、8、9、1〇 ),而Kr =1〇〇 ;則xt〇p = 8、X· = 85、 X2nd = 7 0 > X3rd =60; 因此, ,Xr +Xbase 'and Xbase = (χ_-1) X κΓ As described above, one of the coordinates calculation programs according to the present invention is implemented as follows (X1, X2, X3, X4, X5) = (3〇, 60, 85, 70, 45), and (XI, X2, X3, X4, X5) correspond to the antenna number = (6, 7, 8, 9, 1 〇), and Kr = 1 〇〇; then xt 〇 p = 8, X· = 85, X2nd = 7 0 > X3rd = 60; therefore,
Xbase = (8—1) X 100=700 ,與 Xa = 700 + 3 7.5 = 73 7. 5Xbase = (8-1) X 100=700 , with Xa = 700 + 3 7.5 = 73 7. 5
第19頁 1253003Page 19 1253003
___藍號 9110Q743 五、發明說明(15) 參考第二G圖所示,在本實施例中,γ座標定位 2 8 5的施行方法如下所述··首先,進行一第六比對程序 285A以比較暫存器γΐ、Y2、Y3、Υ4、Y5内所儲存之°複數個 振幅值彼此之間的大小,並儲存振幅最大值於_暫存器 Yniax中’且儲存具有振幅最大值之天線迴圈編號於暫存"器 Ytop中。接著,進行一第三邏輯判斷程序28 5B以判斷暫疒 器Yl、Y2、Y3、Y4、Y5之電壓振幅的最大值為何者。/ 壓振幅之最大值判斷為暫存器丫丨4Υ5的資料,則進―二# 四邏輯判斷程序28 5C以判別暫存器γι或γ5所對應之$線= 圈的位址是否為Υ方向天線群組22〇Β之第一條天線迴圈23 第Μ條天線迴圈;若為是,則可直接判定訊號發射源係1 於Υ方向天線群組2 20Β兩側邊緣區上28gD ;若為否,則兩 再次回到第二全域掃描程序26 5。當電壓振幅之最大值: 斷不為暫存器Y1或Y5的資料,則進行一第二資料儲1 285E以便於分別儲存電壓振幅之第二大值與第三大值於 存器And與Ird中;例如,具有振幅最大值的天線迴圈γ、 =鄭兩天線迴圈Υρ—1與\+1的振幅值分別儲存於複數個4存 f 與中,其中,天線迴圈Υρ之振幅最大值係儲存於 一暫存器Ymax中,而天線迴圈γ之編號係儲存於γ φ。、 . top 丁。 如上所述’可藉由微處理次電路215進行一第三運瞀 ,序28 5F,其運算方式如下所述:首先,藉由電壓-振幅^ 取大值Ymax分別減去電壓振幅之第二大值乙以與第三大值 1253003 _MM 91109743 ^ 修正__e 五、發明說明(16)___Blue No. 9110Q743 V. Inventive Description (15) Referring to the second G diagram, in the present embodiment, the γ coordinate positioning 285 is performed as follows. First, a sixth comparison program 285A is performed. Comparing the magnitudes of the complex amplitude values stored in the registers γΐ, Y2, Y3, Υ4, Y5 with each other, and storing the amplitude maximum in the _ register Yniax' and storing the antenna with the amplitude maximum The loop number is in the temporary storage "Ytop. Next, a third logic decision program 28 5B is performed to determine the maximum value of the voltage amplitudes of the buffers Y1, Y2, Y3, Y4, and Y5. / The maximum value of the pressure amplitude is judged as the data of the register 丫丨4Υ5, and the second-two logic determination program 28 5C is used to determine whether the address of the $ line = circle corresponding to the register γι or γ5 is the Υ direction The first antenna loop 23 of the antenna group 22〇Β is the loop antenna loop; if yes, it can directly determine that the signal source system 1 is 28gD on both side edge regions of the antenna group 2 20Β; If not, then both return to the second global scanning program 26 5 again. When the maximum value of the voltage amplitude is not the data of the register Y1 or Y5, a second data storage 1 285E is performed to store the second largest value and the third largest value of the voltage amplitude respectively in the registers And and Ird. For example, the amplitude of the antenna loop γ, = Zheng two antenna loops Υ ρ1 and \ +1 with the maximum amplitude are stored in a plurality of 4 stores f and respectively, wherein the antenna loop Υ ρ has the largest amplitude The value is stored in a register Ymax, and the number of the antenna loop γ is stored in γ φ. , . As described above, a third operation can be performed by the micro-processing sub-circuit 215, the sequence 28 5F, which is calculated as follows: First, the second value of the voltage amplitude is subtracted by the voltage-amplitude ^ large value Ymax Large value B with the third largest value 1253003 _MM 91109743 ^ Amendment __e V. Invention description (16)
Yid ’以取得一第三電壓振幅差距值(Ymax — Yw )與一第 四電壓振幅差距值(Ymax —Y3rd );然後,以第三電壓振幅 差距值(Ymax — Y2nd )與第四電壓振幅差距值(Yfflax — Yhd ) 的和作為分母,以及第三電壓振幅羞距值(Ymax — Y^d )為 分子得出一具有最大電壓振幅之彼此相鄰的三條天線迴圈 Yp-l、Yp與Yp+1之電壓振幅斜率值;接著,將電壓振幅斜率 值乘上基本解析度常數值K r以得刻,Υ方向之相對座標值 Y r ;據此,本發明之運算式如下所述: 最後,進行一第四運算裎序285G,其運算方式係藉由 相對座標值Yi:加上三條天線迴圈Yp i、Yp與¥州距離γ方向天 線群組220Β之原點的基底座標值,才是真正的以γ方向 天線群組220Β之原點為零點的真實座標值,因此,Yid 'to obtain a third voltage amplitude difference value (Ymax — Yw ) and a fourth voltage amplitude difference value (Ymax — Y3rd ); then, the third voltage amplitude difference value (Ymax — Y2nd ) and the fourth voltage amplitude difference The sum of the values (Yfflax - Yhd ) as the denominator and the third voltage amplitude shame value (Ymax - Y^d ) are molecules to obtain a three antenna loop Yp-l, Yp adjacent to each other with the largest voltage amplitude The voltage amplitude slope value of Yp+1; then, the voltage amplitude slope value is multiplied by the basic resolution constant value Kr to obtain the relative coordinate value Yr of the Υ direction; accordingly, the arithmetic expression of the present invention is as follows: Finally, a fourth operation sequence 285G is performed, which is calculated by the relative coordinate value Yi: plus the base point value of the origin of the three antenna loops Yp i, Yp and the state distance γ direction antenna group 220Β, It is the true coordinate value of the zero point of the original Β 天线 antenna group 220Β, therefore,
Ya =Yr +Ybase,且Ybase =勝力:上ίί座標值u和即為真實座標值或絕對 座標Ya,第四運鼻程序2 85G之方程式如下所示:Ya = Yr + Ybase, and Ybase = Victory: The ίί coordinate value u is the true coordinate value or the absolute coordinate Ya, and the fourth nose program 2 85G equation is as follows:
(Y top x Kr 如上所通,在本發明的實施例 :免式座標定:法=提高座標定位的準確性:“: 採Ξ此’本發明能符合產業上的利用性:、為 者,本發明係抹用一四四分式丟始 ^ 四刀式天線佈局以降低天線佈局之(Y top x Kr as above, in the embodiment of the present invention: free seat calibration: method = improve the accuracy of coordinate positioning: ": pick this" the invention can meet the industrial applicability: The invention uses a four-four-four-type throwing four-blade antenna layout to reduce the antenna layout.
第21頁 蘭003 修正 案號91109743 _年 月 a 五、發明說明(17) 密度。因此,本發明可縮減印刷電路板(printedPage 21 Lan 003 Amendment Case No. 91109743 _ Year Month a V. Description of invention (17) Density. Therefore, the present invention can reduce printed circuit boards (printed
Cycui t Board ; PCB )的面積,並減少生產工時,以達到 縮減產品尺寸的目的。據此,本發明能符合經濟上的效益 。此=a’本發明係藉由一座標計算程式,以使得座標位置 1計算能更為精準。據此,本發明可減少微處理器的處理 日令間並可避免手寫輸入時的線性不良之問題以強化電磁 感應系統之效能。 备然,本發明除了可能應用在電磁感應系統之天線佈 局上,也可能用在任何電磁感應系統之座標定位法上。而 f,本發明藉由四四分式天線佈局以降低 與一座標計算程式以使得座標位置的計算 $ 今仍未發展用在關於?磁感應系統方::"更為精準,- # μ ί然地,依照上面實施例中的描述,本發明可能有_ ==•除了上述詳細的描述外,本發 地在其他的實施例中施行。 /之 發明= =之較佳實施例而。,並非用以限定本 下所完成的等$文改變或修 =月所揭不之精神 圍内。 ^飾句應匕3在下述申請專利範 第22頁 1253003Cycui t Board; PCB) area and reduce production time to reduce product size. Accordingly, the present invention is economically advantageous. This = a' invention is based on a standard calculation program to make the coordinate position 1 calculation more accurate. Accordingly, the present invention can reduce the processing time of the microprocessor and avoid the problem of linearity in handwriting input to enhance the performance of the electromagnetic induction system. Incidentally, the present invention may be applied to the coordinate positioning of any electromagnetic induction system in addition to the antenna layout of the electromagnetic induction system. And f, the present invention uses a four-quarter antenna layout to reduce the calculation of the coordinate calculation with a standard calculation program. The calculation of the coordinate position has not yet been developed for the magnetic induction system side::" more precise, - # μ ί However, in accordance with the description in the above embodiments, the present invention may have _ ==• In addition to the above detailed description, the present invention is implemented in other embodiments. / The invention = = the preferred embodiment. It is not intended to limit the scope of the texts that have been completed in the current period. ^ decorated sentence should be 3 in the following patent application page 22 1253003
修正 圖式簡單說明 第-圖係為傳統的習知電磁電磁感應裝置之, 不意圖; 路方塊 第二A圖係為根據本發明之一較佳實施例中 應系統之簡易電路方塊示意圖; 、 第二B圖係為根據本發明之一較佳實施例中 應系統之X方向天線佈局示意圖; 第二C圖係為根據本發明之一較佳實施例中 應糸統之Y方向天線佈局示意圖; 、 第二D圖係為根據本發明之—較佳實施例中 應糸統之天線佈局所形成的天線迴圈之纟士構示音 第二E圖係為根據本發明之一較佳實施例中 應系統的座標定位法之流程圖; 、 第二F圖係為根據本發明之一較佳實施例中 應系統的座標定位法之中域確認掃描程序; 第二G圖係為根據本發明之一較佳實施例中 應糸統的座4示疋位法之X座標的定位流程圖;與 電磁感 電磁感 電磁感 電磁感 電磁感 電磁感 電磁感BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a conventional conventional electromagnetic electromagnetic induction device, and is not intended to be; FIG. 2A is a simplified circuit block diagram of a system according to a preferred embodiment of the present invention; 2B is a schematic diagram of an X-direction antenna layout according to a preferred embodiment of the present invention; and FIG. 2C is a schematic diagram of a Y-direction antenna layout according to a preferred embodiment of the present invention. The second diagram is a gentleman's structure of the antenna loop formed by the antenna layout of the preferred embodiment of the present invention. The second E diagram is a preferred embodiment of the present invention. A flowchart of a coordinate positioning method of the system in the example; and a second F diagram is a domain confirmation scanning procedure in the coordinate positioning method of the system according to a preferred embodiment of the present invention; the second G diagram is based on the present In a preferred embodiment of the invention, the seat 4 of the system is shown in the positioning flowchart of the X coordinate of the clamp method; and the electromagnetic sense electromagnetic sense electromagnetic sense electromagnetic sense electromagnetic sense electromagnetic sense
1253003 __ 案號91109743_年月日 修正_ 圖式簡單說明 第二Η圖係為根據本發明之一較佳實施例中,電磁感 應系統的座標定位法之Υ座標的定位流程圖。 主要部分之代表符號: 200 電磁感應系統 205 天線次電路 210 内部電路 215 微處理次電路 220 天線群組 22 0Α X方向天線群組 22 0Β Y方向天線群組 225 暫存器 ^max、 ^2nd Λ ^3rd 暫存裔 Xtop ' XI、X2、X3、X4、X5 23 0A X方向天線迴路 23 0B Y方向天線迴路 23 5A X方向天線迴圈 23 5B Υ方向天線迴圈 24 0 第一全域掃描程序 245 第一比對程序 250 中域確認掃描程序 255 第二比對程序 260 第一局部確認掃描程序 265 第二全域掃描程序1253003 __ Case No. 91109743_年月日日 Revision _ BRIEF DESCRIPTION OF THE DRAWINGS The second diagram is a flow chart for the positioning of the coordinates of the coordinate positioning method of the electromagnetic induction system in accordance with a preferred embodiment of the present invention. Representative symbols of the main parts: 200 Electromagnetic induction system 205 Antenna sub-circuit 210 Internal circuit 215 Micro-processing sub-circuit 220 Antenna group 22 0Α X-direction antenna group 22 0Β Y-direction antenna group 225 Registers ^max, ^2nd Λ ^3rd Temporary Xtop 'XI, X2, X3, X4, X5 23 0A X-direction antenna loop 23 0B Y-direction antenna loop 23 5A X-direction antenna loop 23 5B Υ directional antenna loop 24 0 First global scan procedure 245 The first comparison program 250 in the field confirmation scan program 255 the second comparison program 260 the first partial confirmation scan program 265 the second global scan program
第24頁 I ί函(k)3 ,Page 24 I ί letter (k) 3 ,
l—一一' 一 案9114)分74¾ 年月 曰 f多 JL 圖式簡單說明 27 0 第三比對程序L—一一' case 9114) minute 743⁄4 year month 曰 f more JL schema simple description 27 0 third comparison program
Ytop、Yl、Y2、Y3、Y4、Y5 暫存器Ytop, Yl, Y2, Y3, Y4, Y5 register
Yfliax、Y2nd、丫31^ 暫存器 27 5 第二局部確認掃描程序Yfliax, Y2nd, 丫31^ Register 27 5 Second Partial Confirmation Scanner
Xp_2、Xp-i、Xp、ΧρΗ、Xp + 2 X 方向之天線迴圈 ΥΡ-2、ΥΡ-1、Yp、Yp+l、Yp + 2 Y 方向之天線迴圈 28 0 X座標定位程序 28 0Α 第四比對程序 28 0B 第一邏輯判斷程序 28 0C 第二邏輯判斷程序 28 0D 判定發射源位於天線群組之邊緣區 28 0E 第一資料儲存程序 28 0F 第一運算程序 28 5 Y座標定位程序Xp_2, Xp-i, Xp, ΧρΗ, Xp + 2 X-direction antenna loop ΥΡ-2, ΥΡ-1, Yp, Yp+l, Yp + 2 Y direction antenna loop 28 0 X coordinate positioning program 28 0Α The fourth comparison program 28 0B first logic determination program 28 0C second logic determination program 28 0D determines that the transmission source is located in the edge region of the antenna group 28 0E first data storage program 28 0F first operation program 28 5 Y coordinate positioning program
28 5 第六比對程序A 28 5B 第三邏輯判斷程序 28 5C 第四邏輯判斷程序 2 8 5 D 判定訊號發射源係位於天線群組邊緣區上 28 5E 第二資料儲存程序 28 5F 第三運算程序 28 5G 第四運算程序28 5 Sixth comparison program A 28 5B Third logic judgment program 28 5C Fourth logic judgment program 2 8 5 D Judgment signal transmission source is located on the edge group of the antenna group 28 5E Second data storage program 28 5F Third operation Program 28 5G fourth arithmetic program
第25頁Page 25
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Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
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CN102243558A (en) * | 2010-05-12 | 2011-11-16 | 太瀚科技股份有限公司 | Electromagnetic input device and electromagnetic antenna loop layout thereof |
TWI512540B (en) * | 2009-09-22 | 2015-12-11 | Hanwang Technology Co Ltd | A method of measuring the distance between the coordinate indicator and the coordinate input device |
TWI550497B (en) * | 2012-03-09 | 2016-09-21 | 和冠股份有限公司 | Sensor of electromagnetic induction type coordinate input device |
TWI754954B (en) * | 2020-03-06 | 2022-02-11 | 大陸商深圳普贏創新科技股份有限公司 | Electromagnetic coordinate positioning device |
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Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
TWI512540B (en) * | 2009-09-22 | 2015-12-11 | Hanwang Technology Co Ltd | A method of measuring the distance between the coordinate indicator and the coordinate input device |
CN102243558A (en) * | 2010-05-12 | 2011-11-16 | 太瀚科技股份有限公司 | Electromagnetic input device and electromagnetic antenna loop layout thereof |
TWI550497B (en) * | 2012-03-09 | 2016-09-21 | 和冠股份有限公司 | Sensor of electromagnetic induction type coordinate input device |
TWI754954B (en) * | 2020-03-06 | 2022-02-11 | 大陸商深圳普贏創新科技股份有限公司 | Electromagnetic coordinate positioning device |
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