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JPS6035684B2 - Coordinate detection device - Google Patents
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JPS6035684B2 - Coordinate detection device - Google Patents

Coordinate detection device

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Publication number
JPS6035684B2
JPS6035684B2 JP7320383A JP7320383A JPS6035684B2 JP S6035684 B2 JPS6035684 B2 JP S6035684B2 JP 7320383 A JP7320383 A JP 7320383A JP 7320383 A JP7320383 A JP 7320383A JP S6035684 B2 JPS6035684 B2 JP S6035684B2
Authority
JP
Japan
Prior art keywords
magnetic field
phase
plane plate
circuit
region
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP7320383A
Other languages
Japanese (ja)
Other versions
JPS59200383A (en
Inventor
博 岩城
圭右 星野
利雄 津久井
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP7320383A priority Critical patent/JPS6035684B2/en
Publication of JPS59200383A publication Critical patent/JPS59200383A/en
Publication of JPS6035684B2 publication Critical patent/JPS6035684B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 ‘1} 発明の技術分野 本発明は座標説取装置、いわゆるディジタィザに関し、
複数の駆動コイルによって平面板上に形成された回転磁
界の位相から指定の位置の座標を謙取る形式の座標論取
装置に関する。
[Detailed Description of the Invention] '1} Technical Field of the Invention The present invention relates to a coordinate interpretation device, a so-called digitizer;
The present invention relates to a coordinate measuring device that obtains the coordinates of a specified position from the phase of a rotating magnetic field formed on a flat plate by a plurality of drive coils.

【2} 技術の背景 座標論取装置は、平面板上に置かれたペンの座標を読取
る装置であり、例えば自動設計・製図技術分野において
重要な役割を果す図形情報処理システムに用いられるも
のである。
[2] Background of the technology A coordinate reading device is a device that reads the coordinates of a pen placed on a flat board, and is used, for example, in graphical information processing systems that play an important role in the fields of automatic design and drafting technology. be.

この種の座標説取装置としては、第1に静電結合方法、
第2に電磁誘導方法、第3にオーミック方法が提案され
ているが、本発明はこの中で第2の電磁謙導方法をベー
スにし、特に回転磁界の位相から位置検出する形式の座
標論取装置に言及する。
As this type of coordinate reading device, the first method is an electrostatic coupling method,
A second method is an electromagnetic induction method, and a third method is an ohmic method. The present invention is based on the second electromagnetic induction method, and in particular, coordinate theory that detects a position from the phase of a rotating magnetic field. Refer to equipment.

{3} 従来技術と問題点 従来の上記形式の座標謙取装置は、平面坂上に並列して
配置された複数のコイルを有し、相互に位相のずれた複
数の駆動信号をそれぞれ談複数のコイルに通電すること
より前記平面板の上方に該平面坂上の位置に応じて位相
の異なる回転磁界を形成する交流磁界発生器があり、該
平面板の上方に位置して前記回転磁界を検出する磁界検
出器からなるものである。
{3} Prior Art and Problems The conventional coordinate sampling device of the above type has a plurality of coils arranged in parallel on a plane slope, and each transmits a plurality of drive signals out of phase with each other. There is an alternating current magnetic field generator above the plane plate that generates a rotating magnetic field with a different phase depending on the position on the plane slope by energizing a coil, and is located above the plane plate to detect the rotating magnetic field. It consists of a magnetic field detector.

この場合、平面坂上の一端側から池端側に向って丁度o
oから360oまで連続的に位相の変化する回転磁界を
形成しているので、前記磁界検出器(前述のペン)によ
って検出した磁界の位相を知り、これによって自己の置
かれた座標を知ることができる。ところが上記形式の座
標談取装置では精度に関し未だ十分でない。
In this case, from one end of the flat slope to the pond end,
Since it forms a rotating magnetic field whose phase changes continuously from o to 360 o, it is possible to know the phase of the magnetic field detected by the magnetic field detector (the aforementioned pen) and thereby know the coordinates where it is located. can. However, the above-mentioned type of coordinate negotiating device still does not have sufficient accuracy.

つまり、前記回転磁界の位相は、前記平面坂上の一端側
から池端側に向ってリニャに変化すきであるところ、実
際には大略S字状にうねりを含み、完全なりニャリティ
ーは望めなかった。ただし、平面板上の中央部分では良
好なりニャティ−を呈している。このため、本出願人は
、先に特鰯昭56−20978び号1こより平面板上の
端から端までどこをとっても高精度に位置検出のできる
座標論取装置を提案した。以下、先願について図面に従
って説明する。
That is, although the phase of the rotating magnetic field should change linearly from one end of the plane slope toward the pond end, in reality it included undulations in a roughly S-shape, and perfect linearity could not be expected. However, the central portion of the flat plate exhibits a good to poor quality. For this reason, the present applicant previously proposed a coordinate measuring device capable of highly accurate position detection anywhere on a flat plate from one end to the other from Tokusho Sho 56-20978 No. 1. The prior application will be explained below with reference to the drawings.

第1図は先願の第1実施例を示す穣式図である。本図に
おいて、座論取装置10は、交流磁界発生器11と、該
発生器11に位相のずれた駆動信号を供給する駆動部1
3と、いわゆるペンをなす磁界検出器12と協働する。
その他のブロックは、検出器12からの出力を処理して
、座標出力を生成する部分である。発生器11に設けた
平面板の上方には回転磁界Mが形成され、それぞれ矢印
で表示するように位相が異なる。この位相の変化からペ
ン12の位置が分る。このような回転磁界Mを分布形成
せしめるべく、発生器11には複数のコイル群が内蔵さ
れる。第2図は回転磁界を形成する複数のコイルの配列
を、一次元座標議取りについて示す平面図である。
FIG. 1 is a schematic diagram showing the first embodiment of the prior application. In this figure, the discussion device 10 includes an AC magnetic field generator 11 and a drive section 1 that supplies a drive signal out of phase to the generator 11.
3 and a magnetic field detector 12 forming a so-called pen.
The other blocks are those that process the output from the detector 12 and generate coordinate output. A rotating magnetic field M is formed above the flat plate provided in the generator 11, and the phases thereof differ as indicated by arrows. The position of the pen 12 can be determined from this change in phase. In order to distribute the rotating magnetic field M as described above, the generator 11 includes a plurality of coil groups. FIG. 2 is a plan view showing the arrangement of a plurality of coils forming a rotating magnetic field in terms of one-dimensional coordinates.

第2図中、21〜25が複数の駆動コイル群であり、相
互に位相のずれた駆動信号◇,〜で5を受信する。これ
ら相互に位相のずれた駆動信号を図示すると第3図の如
くなる。
In FIG. 2, reference numerals 21 to 25 represent a plurality of drive coil groups, which receive drive signals ◇ and 5 whose phases are shifted from each other. FIG. 3 shows these mutually phase-shifted drive signals.

第3図は第2図に示した駆動信号ぐ,〜ぐ5の波形を示
す波形図である。本図より明らかなとおり;各々の駆動
信号の位相は相互に一定量ずつシフトしている。この位
相のずれが、回転磁界Mの位相を連続的に変化させるこ
とになる。然しながら従来はその位相と平面坂上の位置
とのりニャリティ−が良好でなく精度が悪かつた。第4
A図、第4B図、第4C図および第40図はそれぞれ先
願による座標謙取装置の原理説明に用いるグラフである
FIG. 3 is a waveform diagram showing the waveforms of drive signals G to G5 shown in FIG. As is clear from this figure; the phases of the respective drive signals are mutually shifted by a certain amount. This phase shift causes the phase of the rotating magnetic field M to change continuously. However, in the past, the alignment between the phase and the position on the plane slope was not good, resulting in poor accuracy. Fourth
Fig. A, Fig. 4B, Fig. 4C, and Fig. 40 are graphs used to explain the principle of the coordinate sampling device according to the earlier application.

このうち第4B図のグラフは前述したりニャリティーに
相当するカーブを示しており、理想的な場合に相当する
。つまり、リニャリテイーは最良である。このようにリ
ニヤリテイーが良好ならば検出位相ox(回転磁界Mの
位相)から正確に位置xが求まる。ところが実際には、
そのカーブは第4B図の点線の如く両端近傍でうねりを
生じ、正確な位置xを全平面板に亘つて得ることは困難
であった。そこで先願では、第4B図のカーブを得るの
に用いた基本本波(第3図)の成分(例えば4k伍)に
加えて、第n次高調波成分を導入する。
Of these, the graph in FIG. 4B shows a curve corresponding to the above-mentioned nullity, and corresponds to an ideal case. In other words, linearity is the best. If the linearity is thus good, the position x can be accurately determined from the detection phase ox (the phase of the rotating magnetic field M). However, in reality,
The curve has undulations near both ends as shown by the dotted line in FIG. 4B, making it difficult to obtain an accurate position x over the entire plane plate. Therefore, in the prior application, in addition to the fundamental wave (FIG. 3) component (for example, 4k) used to obtain the curve in FIG. 4B, an n-th harmonic component is introduced.

周波数がn倍のものについて見ると、第4B図と同様の
カーブが繰り返しn回現われ、第4A図に示す領域1,
2・・・・・・nが定義される。各領域のピークは位相
2mに相当し、左から順次2汀、2×2作……かけと変
化する。このようにセグメント化した力−ブは、第4B
図のカーブに比して遥かにリニャリティーが良い。第4
C図はその2汀、2×2汀・・・・・・かけの変化を直
線的に引き伸ばして表わす。そこで先ず、ベン12の位
置が各領域内のどこにあるかを正確に知る。
When looking at the case where the frequency is n times higher, a curve similar to that shown in Fig. 4B appears repeatedly n times, and the areas 1 and 1 shown in Fig. 4A appear.
2...n is defined. The peak in each region corresponds to a phase of 2m, and changes sequentially from the left to 2 waves, 2×2 waves, and so on. The force segmented in this way is the 4th B
The linearity is much better than the curve shown in the figure. Fourth
Diagram C shows the changes in the 2 rows, 2×2 rows, etc. by stretching them linearly. Therefore, first, it is known exactly where Ben 12 is located within each area.

然しながら、この場合、当該領域が全体として何番目の
領域にあるかは分らない。このため、再びリニャリティ
−の良好でない基本波成分の信号を利用する。第4D図
は本発明の検出原理を簡略に示しており、ベン12の置
かれた位置を位相表示で8×(一点銀線)とすると、高
調波成分による該当領域のカーブCから正確に位置xを
読取り、次に当該領域が何番目の領域であるかを基本波
成分によるカーブC′から知る(図中○印の交点参照)
。かくして、どの領域内のどの位置かが高精度で割り出
される。再び第1図に戻ると、磁界検出器12内の検出
巻線14は基本波成分にのみ感応し、第4D図に示した
カーブ〇を第1検出器16より抽出する(これは従来ど
おり)。一方、磁界検出器12内の検出巻線15は第n
次高調波成分にのみ感応し、第40図に示したカーブC
を第1検出器17より抽出する。処理回路18は、これ
らカーブCおよびC′の情報をもとに、目的とする座標
位置を割り出す。検出巻線14が感応すべきものは、駆
動信号のうち基本波成分(例えば4k舷)のみである。
However, in this case, it is not known which region the region is located in as a whole. For this reason, a fundamental wave component signal with poor linearity is again used. Fig. 4D briefly shows the detection principle of the present invention. If the position where Ben 12 is placed is 8x (single dot silver line) in phase display, the position can be accurately determined from the curve C of the corresponding area due to the harmonic component. Read x, and then find out what number the region is from the curve C' based on the fundamental wave component (see the intersection marked with ○ in the figure)
. In this way, which position within which region is determined with high precision. Returning to FIG. 1 again, the detection winding 14 in the magnetic field detector 12 is sensitive only to the fundamental wave component, and the curve 〇 shown in FIG. 4D is extracted from the first detector 16 (this is the same as before). . On the other hand, the detection winding 15 in the magnetic field detector 12 is
Curve C shown in Figure 40 is sensitive only to harmonic components.
is extracted by the first detector 17. The processing circuit 18 determines the target coordinate position based on the information on these curves C and C'. What the detection winding 14 should be sensitive to is only the fundamental wave component (for example, 4K ship) of the drive signal.

この駆動信号は第3図に示す如く矩形波であるから、そ
の中に多数の高調波を必然的に内蔵している。その一部
を、例えば第8次高調波(4kHzの基本波に対して3
2k世)として検出巻線15から拾い出している。とこ
ろで、上記先願では、n次高調波成分の位相を検出する
ために、検出巻線の出力信号の内n次高調波成分を帯城
通猿波器により抽出し、基準信号の零クロス点から、該
高調波成分の奪クロス点までの時間差を位相として表わ
しているが、櫨波器あるいは、零クロス点を検出する比
較器などの温度特性および上記出力信号のS/Nが装置
全体の精度へ大きく依存するという欠′点がある。
Since this drive signal is a rectangular wave as shown in FIG. 3, it necessarily contains many harmonics. A part of it, for example, the 8th harmonic (3kHz for the 4kHz fundamental wave)
2k generation) from the detection winding 15. By the way, in the above-mentioned prior application, in order to detect the phase of the n-th harmonic component, the n-th harmonic component of the output signal of the detection winding is extracted by a bandpass filter, and the zero-crossing point of the reference signal is extracted. The time difference from to the zero-crossing point of the harmonic component is expressed as the phase, but the temperature characteristics of the waveform filter or the comparator that detects the zero-crossing point and the S/N of the output signal are dependent on the overall device. It has the disadvantage of being highly dependent on accuracy.

■ 発明の目的本発明は、この様な欠点を除去し、櫨波
器等を不要とし温度特性に依存しない座標検出装置を提
供することを目的とする。
(2) Purpose of the Invention The object of the present invention is to eliminate such drawbacks, to provide a coordinate detection device that does not require a waveform device or the like and does not depend on temperature characteristics.

{5} 発明の構成 上記目的は、本発明によれば、平面坂上に並列して配列
された複数のコイルを有し、相互に位相のずれた複数の
駆動信号をそれぞれ該複数のコイルに通電することによ
り、前記平面板の上方に該平面板上の位置に応じて位相
の異なる回転磁界を形成する交流磁界発生器と、前記平
面板の上方に位置して前記回転磁界を検出する磁界検出
器と、前記磁界検出器の出力から前記駆動信号の基本波
成分とその第n次高調波成分(nは2以上の整数)とを
取り出し、該n次高調波成分から前記平面板上の位置を
n個の連続した領域に区分して、各談領域内での位置を
読み取る一方、前記基本波成分を用いて当該領域が、n
個の中の何番目の領域であるかを判別して前記磁界検出
器の置かれた平面板の位置を読み取る処理回路とを有す
る座標検出装置において、該磁界検出器の出力をフーリ
エ変換して、2つのフーリエ係数an、bnを求め、該
フーリエ係数an、bnを該第n次高調波成分とし該平
面板上の位置を読み取る様にしたことを特徴とする座標
読取装置によって達成される。
{5} Structure of the Invention According to the present invention, the present invention has a plurality of coils arranged in parallel on a plane slope, and energizes each of the plurality of coils with a plurality of mutually phase-shifted drive signals. an alternating current magnetic field generator that forms a rotating magnetic field with a different phase depending on the position on the plane plate above the plane plate; and a magnetic field detector that is located above the plane plate and detects the rotating magnetic field. extracts the fundamental wave component of the drive signal and its n-th harmonic component (n is an integer of 2 or more) from the output of the magnetic field detector, and determines the position on the flat plate from the n-th harmonic component. is divided into n consecutive regions and the position within each region is read, while the fundamental wave component is used to divide the region into n consecutive regions.
A coordinate detection device includes a processing circuit that reads the position of the plane plate on which the magnetic field detector is placed by determining the number of the area in the area, and a processing circuit that reads the position of the flat plate on which the magnetic field detector is placed. , two Fourier coefficients an and bn are obtained, and the Fourier coefficients an and bn are used as the n-th harmonic components to read the position on the plane plate.

(6} 発明の実施例以下、本発明を実施例に基づいて
説明する。
(6} Examples of the Invention The present invention will be described below based on Examples.

第5図は本発明の一実施例を示す図で、図中14は増幅
器、15はAD変換器、16はフーリエ変換回路、17
は位相検出回路、18は減算回路、19は入力する位相
から離散値を発生する離散値発生回路、20‘ま乗算回
路、21は加算回路である。本発明において、検出巻線
の出力信号Vjは、図示しないフィル夕により、抽出さ
れたn−1、n次高調波成分で、増幅器14により増幅
されたA/D変換器15によりN個のデータSk(K:
0、1・・…・N−1)に標本化される。
FIG. 5 is a diagram showing an embodiment of the present invention, in which 14 is an amplifier, 15 is an AD converter, 16 is a Fourier transform circuit, and 17 is a diagram showing an embodiment of the present invention.
18 is a phase detection circuit, 18 is a subtraction circuit, 19 is a discrete value generation circuit that generates a discrete value from an input phase, 20' is a multiplication circuit, and 21 is an addition circuit. In the present invention, the output signal Vj of the detection winding is an n-1, n-th order harmonic component extracted by a filter (not shown), which is amplified by an amplifier 14 and converted into N data by an A/D converter 15. Sk(K:
0, 1...N-1).

ディジタル変換された信号Skはフーリエ変換回路16
によりm式に従って、離散的フーリエ変換が施され、n
次高調波のフーリエ係数an、bnが求められる。
The digitally converted signal Sk is sent to the Fourier transform circuit 16
A discrete Fourier transform is performed according to m formula, and n
The Fourier coefficients an and bn of the harmonics are determined.

an=声宅喜三郎‐COSか苦竹 bn=吉母亨j舷‐母N加持汀 …イ1’次にフーリエ
係数an、bnから位相Jnを求めるが、位相◇nは、
m式より{2}式で求められる。
an = Kisaburo Koetaku - COS or bitter bamboo bn = Yoshimo Toru - mother N Kajiten...I1' Next, find the phase Jn from the Fourier coefficients an and bn, but the phase ◇n is
It is determined by the {2} formula from the m formula.

◇n=はn−,生 肌帆an ここで{1’、■式の三角関数は、簡単のためテーブル
参照により求められる。
◇n= is n-, Namahaho an Here, the trigonometric function of the {1', ■ formula can be found by referring to a table for simplicity.

又、n−1次高調波のフーリエ係数an‐1、bn‐1
も同様にして求め、このフーリエ係数から位相検出回路
17により位相ぐn−1を求める。
In addition, the Fourier coefficients an-1 and bn-1 of the n-1th harmonic
is obtained in the same manner, and the phase n-1 is obtained from this Fourier coefficient by the phase detection circuit 17.

ここで、第4図で説明した如く、n次高調波の位相?n
(0〜2竹 rad)は、全タブレット領域において、
n回回転し、その区別がつかないため、その領域を判別
するために基本波成分の位相めを用いる。このため、減
算回路18よりぐn−でn−1なる減算を行なって、位
相0,を求める。
Here, as explained in Fig. 4, the phase of the nth harmonic? n
(0 to 2 bamboo rad) in all tablet areas,
Since it rotates n times and cannot be distinguished, the phase of the fundamental wave component is used to distinguish the region. Therefore, the subtraction circuit 18 performs subtraction of n-1 by n-1 to obtain the phase 0.

この位相で,は離散値発生回路19に入力し、位相の大
きさにより、0、1、2、・・・・・・n−1の値が出
力され、乗算回路2川こ入力する。
At this phase, is input to the discrete value generation circuit 19, and depending on the magnitude of the phase, values of 0, 1, 2, .

乗算回路20では、離散値発生回路19の出力に2mを
乗算する。従って、乗算回路20の出力は、上記領域を
示す。
The multiplication circuit 20 multiplies the output of the discrete value generation circuit 19 by 2m. Therefore, the output of the multiplier circuit 20 indicates the above region.

そして、位相ぐnと加算回路21で加算することにより
、座標を求める。
Then, the coordinates are determined by adding the phase gn and the adder circuit 21.

{7)発明の効果 以上の如く、本発明によればフーリエ係数を用いて、位
相を求めているため、従来の如く、猿波器、比較器等を
必要とせず、従って温度等による影響をなくすことが可
能となる。
{7) Effects of the Invention As described above, according to the present invention, the phase is determined using Fourier coefficients, so there is no need for a monkey waver, a comparator, etc. as in the past, and the influence of temperature etc. can be eliminated. It becomes possible to eliminate it.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は先願の実施例を示す図、第2図はコイル配列を
示す図、第3図は駆動信号を示す図、第4図は先願の原
理を示す図、第5図は本発明の実施例を示す図である。 図中、1 4は増幅器、15はAD変換器、16はフー
リエ変換回路、17は位相検出回路、18は減算回路、
19は入力する位相から離散値を発生する離散値発生回
路、2川ま乗算回路、21は加算回路である。※丁図 第2図 第3図 第4A図 第48図 第4C図 第4D図 努J図
Figure 1 is a diagram showing the embodiment of the earlier application, Figure 2 is a diagram showing the coil arrangement, Figure 3 is a diagram showing the drive signal, Figure 4 is a diagram showing the principle of the earlier application, and Figure 5 is a diagram of the present invention. It is a figure showing an example of the invention. In the figure, 14 is an amplifier, 15 is an AD converter, 16 is a Fourier transform circuit, 17 is a phase detection circuit, 18 is a subtraction circuit,
19 is a discrete value generation circuit that generates a discrete value from an input phase, a Futagawa multiplication circuit, and 21 is an addition circuit. *Figure 2Figure 3Figure 4AFigure 48Figure 4CFigure 4DFigure Tsutomu J figure

Claims (1)

【特許請求の範囲】[Claims] 1 平面板上に並列して配列された複数のコイルを有し
、相互に位相のずれた複数の駆動信号をそれぞれ該複数
のコイルに通電することにより、前記平面板の上方に該
平面板上の位置に応じて位相の異なる回転磁界を形成す
る交流磁界発生器と、前記平面板の上方に位置して前記
回転磁界を検出する磁界検出と、前記磁界検出器の出力
から前記駆動信号の基本波成分とその第n次高調波成分
(nは2以上の整数)とを取り出し、該n次高調波成分
から前記平面板上の位置をn個の連続した領域に区分し
て、各該領域内での位置を読み取る一方、前記基本波成
分を用いて当該領域が、n個の中の何番目の領域である
かを判別して前記磁界検出器の置かれた平面板の位置を
読み取る処理回路とを有する座標検出位置において、該
磁界検出回路の出力をフーリエ変換して、2つのフーリ
エ係数a_n、b_nを求め、該フーリエ係数a_n、
b_nを該第n次高周波成分とし該平面板上の位置を読
み取る様にしたことを特徴とする座標読取装置。
1 It has a plurality of coils arranged in parallel on a plane plate, and by applying a plurality of mutually phase-shifted drive signals to the plurality of coils, the plane plate is placed above the plane plate. an alternating current magnetic field generator that forms a rotating magnetic field with a different phase depending on the position of the plane, a magnetic field detector that is located above the plane plate and detects the rotating magnetic field, and a basis for generating the drive signal from the output of the magnetic field detector. A wave component and its n-th harmonic component (n is an integer of 2 or more) are extracted, and the position on the plane plate is divided into n consecutive regions based on the n-th harmonic component, and each region is divided into n consecutive regions. A process of reading the position of the flat plate on which the magnetic field detector is placed by determining which region out of n the region is, using the fundamental wave component. At a coordinate detection position having a circuit, the output of the magnetic field detection circuit is Fourier transformed to obtain two Fourier coefficients a_n, b_n, and the Fourier coefficients a_n,
A coordinate reading device characterized in that b_n is used as the n-th high frequency component to read a position on the plane plate.
JP7320383A 1983-04-26 1983-04-26 Coordinate detection device Expired JPS6035684B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7320383A JPS6035684B2 (en) 1983-04-26 1983-04-26 Coordinate detection device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7320383A JPS6035684B2 (en) 1983-04-26 1983-04-26 Coordinate detection device

Publications (2)

Publication Number Publication Date
JPS59200383A JPS59200383A (en) 1984-11-13
JPS6035684B2 true JPS6035684B2 (en) 1985-08-16

Family

ID=13511349

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7320383A Expired JPS6035684B2 (en) 1983-04-26 1983-04-26 Coordinate detection device

Country Status (1)

Country Link
JP (1) JPS6035684B2 (en)

Also Published As

Publication number Publication date
JPS59200383A (en) 1984-11-13

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