JPH0210443B2 - - Google Patents

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Publication number
JPH0210443B2
JPH0210443B2 JP59088176A JP8817684A JPH0210443B2 JP H0210443 B2 JPH0210443 B2 JP H0210443B2 JP 59088176 A JP59088176 A JP 59088176A JP 8817684 A JP8817684 A JP 8817684A JP H0210443 B2 JPH0210443 B2 JP H0210443B2
Authority
JP
Japan
Prior art keywords
magnetic
detection
lines
excitation
line
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 - Lifetime
Application number
JP59088176A
Other languages
Japanese (ja)
Other versions
JPS60231231A (en
Inventor
Yoshinori Taguchi
Tsugunari Yamanami
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.)
Wakomu KK
Original Assignee
Wakomu KK
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 Wakomu KK filed Critical Wakomu KK
Priority to JP59088176A priority Critical patent/JPS60231231A/en
Publication of JPS60231231A publication Critical patent/JPS60231231A/en
Publication of JPH0210443B2 publication Critical patent/JPH0210443B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 (技術分野) 本発明は位置指定用磁気発生器により磁界を加
えられた磁性体の透磁率の変化に基づいて位置指
定用磁気発生器で指定された位置を検出する位置
検出装置に関するものである。
Detailed Description of the Invention (Technical Field) The present invention detects a position specified by a position specifying magnetic generator based on a change in magnetic permeability of a magnetic body to which a magnetic field is applied by the position specifying magnetic generator. The present invention relates to a position detection device.

(従来技術と問題点) 従来の位置検出装置としては、磁歪伝達媒体の
一端または位置指示ペンの先端に設けた駆動コイ
ルにパルス電流を印加して前記磁歪伝達媒体に磁
歪振動波を生起させた時点より、位置指示ペンの
先端または磁歪伝達媒体の一端に設けた検出コイ
ルに前記磁歪振動波に基づく誘導電圧を検出する
までの時間を処理器等で測定し、これより位置指
示ペンの指示位置を算出する如くなしたものがあ
つた。この装置では位置検出精度は比較的良好で
あるが、ペンと処理器等との間でタイミング信号
等を授受するため、ペンと装置との間にコードを
必要としその取扱いが著しく制限されると共に、
他の機器から誘導を受けやすく誤動作したり、ま
た逆にノイズの発生源となる可能性もあり、更に
ペンを磁歪伝達媒体に対して垂直に保持し、かつ
かなり近持させて指示しなければならない等の問
題点があつた。
(Prior Art and Problems) Conventional position detection devices generate magnetostrictive vibration waves in the magnetostrictive transmission medium by applying a pulse current to a drive coil provided at one end of the magnetostrictive transmission medium or at the tip of a position indicating pen. From that point on, a processor or the like measures the time until an induced voltage based on the magnetostrictive oscillation waves is detected in a detection coil provided at the tip of the positioning pen or at one end of the magnetostrictive transmission medium, and from this time the indicated position of the positioning pen is determined. There was something that I did to calculate. Although this device has relatively good position detection accuracy, it requires a cord between the pen and the device in order to send and receive timing signals, etc. between the pen and the processor, which severely limits its handling. ,
It is susceptible to induction from other devices and may malfunction, or may even become a source of noise. Furthermore, the pen must be held perpendicular to the magnetostrictive transmission medium and very close to it. There were some problems, such as not being able to do so.

また、従来の他の位置検出装置としては、複数
の駆動線と検出線とを互いに直交して配置し、駆
動線に順次、電流を流すとともに検出線を順次選
択して誘導電圧を検出し、フエライトのような磁
性体を有する位置指示ペンで指定した位置を大き
な誘導電圧が誘起された検出線の位置より検出す
るようになしたものがあつた。この装置では位置
指示ペンをコードレスとすることができるが、座
標位置の分解能が線の間隔で決まり、分解能を上
げるために線の間隔を小さくするとSN比及び安
定度が悪くなり、従つて分解能を上げることが困
難であり、また駆動線と検出線の交点の真上の位
置検出が困難であり、更に位置指示ペンを線に極
く接近させなければならず入力面上に厚みのある
物を置いて使用できない等の問題点があつた。
In addition, as another conventional position detection device, a plurality of drive lines and detection lines are arranged perpendicularly to each other, and current is sequentially applied to the drive lines and detection lines are sequentially selected to detect induced voltage. There is a device in which a position specified by a position indicating pen made of a magnetic material such as ferrite is detected from the position of a detection line where a large induced voltage is induced. With this device, the positioning pen can be made cordless, but the resolution of the coordinate position is determined by the line spacing, and if you reduce the line spacing to increase the resolution, the signal-to-noise ratio and stability will deteriorate, and therefore the resolution will decrease. In addition, it is difficult to detect the position directly above the intersection of the drive line and the detection line, and the position indicator pen must be placed extremely close to the line, making it difficult to place thick objects on the input surface. There were some problems, such as not being able to use it by leaving it in place.

(発明の目的) 本発明はこのような従来の欠点を改善したもの
であり、位置指定用磁気発生器がどこにも接続さ
れず操作性が良く、また外部からの誘導に強く且
つノイズを放出することのない高精度な位置検出
装置を提供することを課題としている。
(Object of the Invention) The present invention improves these conventional drawbacks, and the magnetic generator for position designation is not connected anywhere, has good operability, is resistant to external guidance, and emits noise. Our goal is to provide a highly accurate position detection device that never fails.

(実施例) 第1図は本発明の一実施例を示す一部切欠分解
斜視図である。同図において、10はX方向位置
検出部、20はY方向位置検出部、30は駆動電
流源、41,42は信号選択手段,例えばマルチ
プレクサ、50は位置指定用磁気発生器,例えば
棒磁石、60は処理装置である。
(Embodiment) FIG. 1 is a partially cutaway exploded perspective view showing an embodiment of the present invention. In the figure, 10 is an X-direction position detection section, 20 is a Y-direction position detection section, 30 is a driving current source, 41 and 42 are signal selection means, such as a multiplexer, and 50 is a position designating magnetic generator, such as a bar magnet. 60 is a processing device.

X方向位置検出部10は平板状の磁性体11と
励磁線12a〜12iと検出線13a〜13hと
絶縁シート14,15とからなつている。磁性体
11は絶縁シート14,15間に挾まれている。
また、磁性体11としては磁石を接近させても磁
化され難く、即ち保持力が小さく且つ透磁率
(μ)の高い材料、例えばアモルフアス合金、パ
ーマロイ合金等が好ましい。アモルフアス合金と
しては、例えばFe79B16Si5(原子%)(保持力
0.2e、透磁率(μ)=14000)等が使用できる。ま
た、磁性体11は平板(シート)状であるが、ア
モルフアス合金は製造上、厚さが20〜50μmの簿
いものを作れるので、これをそのまま適用しても
よい。また、長尺の磁性体、例えば断面長方形の
簿帯状か断面円形の線状のアモルフアス合金を多
数互いにかつ密接させてシート状となしたものを
用いることもできる。なお、この場合は各磁性体
の長手方向と位置検出方向(ここではX方向)と
が一致するように配置した方が良い結果が得られ
る。
The X-direction position detection section 10 includes a flat magnetic body 11, excitation lines 12a to 12i, detection lines 13a to 13h, and insulating sheets 14 and 15. The magnetic body 11 is sandwiched between insulating sheets 14 and 15.
The magnetic material 11 is preferably a material that is difficult to be magnetized even when a magnet is brought close to it, that is, has a small coercive force and has a high magnetic permeability (μ), such as an amorphous alloy or a permalloy alloy. As an amorphous amorphous alloy, for example, Fe 79 B 16 Si 5 (atomic %) (coercive force
0.2e, magnetic permeability (μ) = 14000), etc. can be used. Further, although the magnetic material 11 is in the form of a flat plate (sheet), since an amorphous alloy can be manufactured into a compact material with a thickness of 20 to 50 μm, this may be used as is. Further, it is also possible to use a long magnetic material, for example, a sheet-like material in which a large number of amorphous alloys in the form of strips with a rectangular cross section or linear amorphous alloys with a circular cross section are brought close together and in close contact with each other. In this case, better results can be obtained by arranging the magnetic bodies so that the longitudinal direction of each magnetic body coincides with the position detection direction (in this case, the X direction).

各励磁線12a〜12iは、絶縁シート14の
上面に配設された部分(以下、上半部と称す。)
と絶縁シート15の下面に配設された部分(以
下、下半部と称す。)とが、それらの一端でそれ
ぞれ連続してなつており、励磁線12a,12
b,12c,12d,12e,12f,12g,
12hの下半部の他端と、励磁線12b,12
c,12d,12e,12f,12g,12h,
12iの上半部の他端とがそれぞれ接続され、即
ち励磁線12a〜12iは直列に接続され、励磁
線12aの上半部の他端と励磁線12iの下半部
の他端は駆動電流源30に接続される。また、各
励磁線12a〜12iはX方向と直交する方向、
即ちY方向に沿つて所定間隔をおいて互いに平行
に配置されている。
Each of the excitation wires 12a to 12i is a portion disposed on the upper surface of the insulating sheet 14 (hereinafter referred to as an upper half portion).
and a portion disposed on the lower surface of the insulating sheet 15 (hereinafter referred to as the lower half) are continuous at one end thereof, and the excitation wires 12a, 12
b, 12c, 12d, 12e, 12f, 12g,
The other end of the lower half of 12h and the excitation wires 12b, 12
c, 12d, 12e, 12f, 12g, 12h,
The other end of the upper half of the excitation wire 12i is connected to the other end of the upper half of the excitation wire 12i, that is, the excitation wires 12a to 12i are connected in series, and the other end of the upper half of the excitation wire 12a and the other end of the lower half of the excitation wire 12i are connected to each other. source 30. Moreover, each excitation line 12a to 12i is directed in a direction perpendicular to the X direction,
That is, they are arranged parallel to each other at predetermined intervals along the Y direction.

各検出線13a〜13hは、絶縁シート14の
上面に配設された部分(以下、上半部と称す。)
と絶縁シート15の下面に配設された部分(以
下、下半部と称す。)とが、それらの一端でそれ
ぞれ連続してなつており、検出線13a〜13h
の上半部の他端はそれぞれマルチプレクサ41に
接続され、検出線13a〜13hの下半部の他端
は共通に接地される。また、各検出線13a〜1
3hはそれぞれ励磁線12a〜12iのそれぞれ
の間に互いに平行に配置されている。
Each of the detection lines 13a to 13h is located on the upper surface of the insulating sheet 14 (hereinafter referred to as the upper half).
and a portion disposed on the lower surface of the insulating sheet 15 (hereinafter referred to as the lower half) are continuous at one end thereof, and the detection lines 13a to 13h
The other ends of the upper halves are respectively connected to the multiplexer 41, and the other ends of the lower halves of the detection lines 13a to 13h are commonly grounded. In addition, each detection line 13a to 1
3h are arranged parallel to each other between each of the excitation lines 12a to 12i.

Y方向位置検出部20は平板状の磁性体21と
励磁線22a〜22iと検出線23a〜23hと
絶縁シート24,25とからなつており、その細
部の構造はX方向位置検出部10と同様である。
Y方向位置検出部20はX方向位置検出部10の
下部に、図示しない絶縁シート等を介して、励磁
線及び検出線が互いに直交する如くできるだけ近
接して重ね合わされる(但し、図面では構造をわ
かりやすくするため、X方向位置検出部10とY
方向位置検出部20とは離して描いている。)。ま
た各励磁線22a〜22iは駆動電流源30に接
続され、各検出線23a〜23hはマルチプレク
サ42に接続される。
The Y-direction position detection section 20 consists of a flat magnetic body 21, excitation lines 22a to 22i, detection lines 23a to 23h, and insulating sheets 24 and 25, and its detailed structure is similar to the X direction position detection section 10. It is.
The Y-direction position detection section 20 is superimposed on the lower part of the X-direction position detection section 10 via an insulating sheet (not shown) as close as possible so that the excitation line and the detection line are orthogonal to each other (however, the structure is not shown in the drawings). For clarity, the X-direction position detection unit 10 and the Y
It is drawn apart from the direction position detection section 20. ). Further, each excitation line 22a to 22i is connected to a drive current source 30, and each detection line 23a to 23h is connected to a multiplexer 42.

駆動電流源30は所定周期の交番電流(ここで
いう交番電流とは正弦波、短形波、三角波等の全
てを含む)を常時、励磁線12a〜12i及び2
2a〜22iに送出する。また、マルチプレクサ
41,42は処理装置60からの制御信号に従つ
て検出線13a〜13h及び23a〜23hの出
力信号を処理装置60へ選択的に送出する如くな
つている。
The drive current source 30 constantly supplies an alternating current with a predetermined period (the alternating current here includes all of sine waves, rectangular waves, triangular waves, etc.) to the excitation lines 12a to 12i and 2.
2a to 22i. Further, the multiplexers 41 and 42 are configured to selectively send the output signals of the detection lines 13a to 13h and 23a to 23h to the processing device 60 in accordance with a control signal from the processing device 60.

このような構成において、検出線13a〜13
h及び23a〜23hには前記励磁線12a〜1
2i及び22a〜22iを流れる交番電流に基づ
く電磁誘導により誘導電圧が発生する。この電磁
誘導は磁性体11及び21を介して行なわれるた
め、磁性体11及び21の透磁率が大きい程、前
記誘導電圧の電圧値は大きくなる。ところで、磁
性体11及び21の透磁率は外部から加わる磁気
バイアスによつて大きく変化する。その変化のよ
うすは磁性体の組成、前記交流電流の周波数、あ
るいは磁性体に熱処理を加えること等によつて異
なり、第2図に示すようにある磁気バイアスを加
えた時に最大となるように設定することができ
る。従つてこの場合、磁性体11及び21に磁気
バイアスを加えると、励磁線12a〜12i,2
2a〜22iから検出線13a〜13h,23a
〜23hへ誘起する電圧も大きくなる。
In such a configuration, the detection lines 13a to 13
h and 23a to 23h are the excitation lines 12a to 1
An induced voltage is generated by electromagnetic induction based on the alternating current flowing through 2i and 22a to 22i. Since this electromagnetic induction occurs via the magnetic bodies 11 and 21, the higher the magnetic permeability of the magnetic bodies 11 and 21, the greater the voltage value of the induced voltage. Incidentally, the magnetic permeability of the magnetic bodies 11 and 21 changes greatly depending on the magnetic bias applied from the outside. The state of the change varies depending on the composition of the magnetic material, the frequency of the alternating current, the heat treatment applied to the magnetic material, etc., and is set so that it becomes maximum when a certain magnetic bias is applied, as shown in Figure 2. can do. Therefore, in this case, when a magnetic bias is applied to the magnetic bodies 11 and 21, the excitation lines 12a to 12i, 2
Detection lines 13a to 13h, 23a from 2a to 22i
The voltage induced to ~23h also increases.

今、第1図において、位置指定用棒磁石50が
N極を下にして検出線13aからX方向の距離
Xs及び検出線23aからY方向の距離ysだけ隔
てたX方向位置検出部10の位置A上にあり、透
磁率が大きくなる程度の磁気バイアスを磁性体1
1及び21に加えているものとする。
Now, in FIG. 1, the position specifying bar magnet 50 is located at a distance in the X direction from the detection line 13a with its N pole facing down.
It is located on position A of the X - direction position detection unit 10, which is separated by a distance ys in the Y direction from Xs and the detection line 23a, and applies a magnetic bias to the extent that the magnetic permeability increases.
1 and 21.

この時、X方向の検出線13a〜13hには第
3図に示すような誘導電圧V1〜V8が発生する。
第3図において、横軸は検出線13a〜13hの
位置をそれぞれx1〜x8とするX方向の座標位置を
示し、縦軸は電圧値を示しているが、前記各電圧
V1〜V8は位置A直下で最大値(極大値)となる。
前記各電圧V1/V8はマルチプレクサ41より得
られるので、これらより誘起電圧が極大値となる
X座標値を処理装置60で演算して求めれば、棒
磁石50のX座標値xsを求めることができる。
At this time, induced voltages V1 to V8 as shown in FIG. 3 are generated in the detection lines 13a to 13h in the X direction.
In FIG. 3, the horizontal axis indicates coordinate positions in the X direction, where the positions of the detection lines 13a to 13h are x 1 to x 8 , respectively, and the vertical axis indicates voltage values.
V 1 to V 8 reach their maximum values (local maximum values) directly below position A.
Since each of the voltages V 1 /V 8 is obtained from the multiplexer 41, if the processing device 60 calculates the X coordinate value at which the induced voltage becomes the maximum value from these, the X coordinate value x s of the bar magnet 50 is determined. be able to.

座標値xsを求める算出方法の一つとして、第3
図における極大値付近の波形を適当な函数で近似
し、その函数の極大値の座標を求める方法があ
る。例えば、各検出線13a〜13hの間隔を
Δxとし、第3図において座標x3から座標x5まで
を2次函数(図中、実線で示す)で近似すると、
次のようにして算出することができる。まず、各
検出線の電圧と座標値より V3=a(x3−xs2+b ……(1) V4=a(x4−xs2+b ……(2) V5=a(x5−xs2+b ……(3) となる。ここで、a,bは定数(a<0)であ
る。
As one of the calculation methods for determining the coordinate value x s , the third
There is a method of approximating the waveform near the maximum value in the figure with an appropriate function and finding the coordinates of the maximum value of that function. For example, if the interval between each detection line 13a to 13h is Δx, and the coordinates from coordinate x 3 to coordinate x 5 in FIG. 3 are approximated by a quadratic function (indicated by a solid line in the figure), then
It can be calculated as follows. First, from the voltage and coordinate values of each detection line, V 3 = a (x 3 - x s ) 2 + b ... (1) V 4 = a (x 4 - x s ) 2 + b ... (2) V 5 = a( x5xs ) 2 +b...(3). Here, a and b are constants (a<0).

また、 x4−x3=Δx ……(4) x5−x3=2Δx ……(5) となる。(4),(5)式を(2),(3)式に代入して整理する
と、 xs=x3+Δx/2(3V3−4V4+V5/V3−2V4+V5)…(6
) となる。従つて、検出線13c,13d,13e
に誘起する電圧V3,V4,V5、及び検出線13c
の座標値x3(既知)から処理装置60で(6)式の演
算を行なうことにより棒磁石50のX座標値を算
出できる。また、棒磁石50をY軸に沿つて動か
しても同一のX座標値が得られる。
Also, x 4 −x 3 =Δx ……(4) x 5 −x 3 =2Δx ……(5). Substituting equations (4) and (5) into equations (2) and (3) and rearranging, x s = x 3 + Δx/2 (3V 3 −4V 4 +V 5 /V 3 −2V 4 +V 5 )… (6
) becomes. Therefore, the detection lines 13c, 13d, 13e
Voltages V 3 , V 4 , V 5 induced in and the detection line 13c
The processing device 60 calculates the X coordinate value of the bar magnet 50 from the coordinate value x 3 (known) by calculating equation (6). Further, even if the bar magnet 50 is moved along the Y axis, the same X coordinate value can be obtained.

また、Y方向の検出線23a〜23hにも第3
図と同様な誘導電圧が得られ、前記同様の演算処
理によつてY座標値ysを求めることができる。
Also, a third
An induced voltage similar to that shown in the figure is obtained, and the Y coordinate value ys can be determined by the same calculation process as described above.

位置指定用棒磁石50の先端から発せられる磁
界は、第4図に示すように該棒磁石50の中心線
の延長上の一点rから発する如く近似される。従
つて磁性体11及び21より前記点rまでの距離
に相当する位置に入力面100を形成すれば、棒
磁石が磁性体11及び21に対して傾いても(但
し、図示例では二点鎖線で示す磁性体11を基準
として棒磁石50が傾いた状態にあることを示し
ている。)磁性体の同一位置に対する磁界の方向
は変わらず、その検出位置も変わらず、従つて、
棒磁石50の傾きに影響されず位置指定が可能と
なる。なお、実験では傾きが±30゜以内で、誤差
±0.5mm以下を達成している(入力面の高さ12
mm)。
The magnetic field emitted from the tip of the position specifying bar magnet 50 is approximated to be emitted from a point r on the extension of the center line of the bar magnet 50, as shown in FIG. Therefore, if the input surface 100 is formed at a position corresponding to the distance from the magnetic bodies 11 and 21 to the point r, even if the bar magnets are tilted with respect to the magnetic bodies 11 and 21 (however, in the illustrated example, the two-dot chain line (This shows that the bar magnet 50 is tilted with reference to the magnetic body 11 shown in .) The direction of the magnetic field with respect to the same position of the magnetic body does not change, and the detection position also does not change.
The position can be specified without being affected by the inclination of the bar magnet 50. In experiments, the tilt was within ±30° and the error was less than ±0.5mm (height of the input surface was 12mm).
mm).

第5図は駆動電流源30の具体例を示すもので
ある。同図において、31はフアンクシヨンジエ
ネレータ、例えばインターシル製IC、8038であ
り、コンデンサCと抵抗Rの値で定まる所定の周
波数の正弦波信号を出力する。また32はパワー
ドライバであり、オペアンプ電流増幅器とからな
つており、前記正弦波信号を電流増幅して励磁線
12a〜12i,22a〜22iへ送出する。
FIG. 5 shows a specific example of the drive current source 30. In the figure, numeral 31 is a function generator, for example, Intersil IC 8038, which outputs a sine wave signal of a predetermined frequency determined by the values of capacitor C and resistor R. Further, 32 is a power driver, which is composed of an operational amplifier and a current amplifier, and amplifies the current of the sine wave signal and sends it to the excitation lines 12a to 12i and 22a to 22i.

第6図は位置指定用磁気発生器50の具体例を
示す断面図、第7図はその電気回路図である。同
図において、51は合成樹脂等からなるペン状の
容器であり、その一端には先端先細状の棒磁石5
2が軸方向に摺動自在に収容されている。また、
53は操作スイツチで、棒磁石52の他端に対向
して取り付けられている。また、54は超音波信
号の送信機、55は超音波の送波器で、電池56
とともに容器51内の適所に収納されている。前
記容器51を保持しゴムカバー57を取り付けた
棒磁石52の先端を入力面に押し当てれば、該棒
磁石52がスライドしてスイツチ53がオンし、
これによつて、送信機54内の発振回路54a及
び増幅器54bが動作し、送波器55より測定開
始を示す信号,例えば所定周波数の連続パルス信
号を超音波信号に変えて発信する。
FIG. 6 is a sectional view showing a specific example of the position designating magnetic generator 50, and FIG. 7 is an electric circuit diagram thereof. In the figure, 51 is a pen-shaped container made of synthetic resin, etc., and a bar magnet 5 with a tapered tip is attached to one end of the pen-shaped container.
2 is accommodated so as to be slidable in the axial direction. Also,
Reference numeral 53 denotes an operation switch, which is attached opposite to the other end of the bar magnet 52. Further, 54 is an ultrasonic signal transmitter, 55 is an ultrasonic transmitter, and a battery 56
It is stored in a proper place in the container 51. When the tip of the bar magnet 52 that holds the container 51 and has the rubber cover 57 attached is pressed against the input surface, the bar magnet 52 slides and the switch 53 is turned on.
As a result, the oscillation circuit 54a and amplifier 54b in the transmitter 54 operate, and the transmitter 55 transmits a signal indicating the start of measurement, for example, a continuous pulse signal of a predetermined frequency, by converting it into an ultrasonic signal.

第8図は処理装置60の具体的構成を示す回路
ブロツク図である。同図において、前述した送波
器55より測定開始を示す超音波信号が送出され
ると、該超音波信号は受波器61で受波され、更
に受信器62で増幅・波形整形されて入力バツフ
ア63に送出される。演算処理回路64は入力バ
ツフア63より前記測定開始信号を読み取り、測
定開始を認識すると、出力バツフア65を介して
切換回路66及びマルチプレクサ41へ制御信号
を送り、X方向の検出線13a〜13hの誘導電
圧を増幅器67へ順次入力する。前記各誘導電圧
は増幅器67で増幅され検波器68で整流されて
直流電圧に変換され、更にアナログ―デイジタル
(A/D)変換器69にてデイジタル値に変換さ
れ入力バツフア63を介して演算処理回路64に
送出される。演算処理回路64では前記各誘導電
圧(デイジタル値)をメモリ70に一時記憶し、
これらの中よりピーク付近の電圧値を検出する。
この検出方法としては、例えば各誘導電圧の大小
を順次比較し、ある電圧,仮りにVkが直前の電
圧Vk-1より大きく、かつ次の電圧Vk+1よりも大
きい時、(Vk-1<Vk>Vk+1)に電圧Vkをピーク
電圧として検出することができる。演算処理回路
64は前記電圧Vk-1,Vk,Vk+1を取り出し、こ
れらをそれぞれ前記(6)式における電圧V3,V4
V5として(6)式の演算処理を行ない、X座標値を
求める。
FIG. 8 is a circuit block diagram showing a specific configuration of the processing device 60. In the figure, when an ultrasonic signal indicating the start of measurement is sent out from the above-mentioned transmitter 55, the ultrasonic signal is received by a receiver 61, further amplified and waveform-shaped by a receiver 62, and then inputted. It is sent to the buffer 63. The arithmetic processing circuit 64 reads the measurement start signal from the input buffer 63, and when recognizing the start of measurement, sends a control signal to the switching circuit 66 and the multiplexer 41 via the output buffer 65 to guide the detection lines 13a to 13h in the X direction. The voltages are sequentially input to the amplifier 67. Each of the induced voltages is amplified by an amplifier 67, rectified by a detector 68, converted into a DC voltage, further converted into a digital value by an analog-digital (A/D) converter 69, and processed through an input buffer 63. The signal is sent to circuit 64. The arithmetic processing circuit 64 temporarily stores each of the induced voltages (digital values) in a memory 70,
Among these, the voltage value near the peak is detected.
This detection method involves, for example, sequentially comparing the magnitude of each induced voltage, and if a certain voltage, V k , is larger than the immediately preceding voltage V k-1 and larger than the next voltage V k+1 , then (V k-1 <V k >V k+1 ), voltage V k can be detected as a peak voltage. The arithmetic processing circuit 64 takes out the voltages V k-1 , V k , V k+1 and converts them into the voltages V 3 , V 4 , V 4 and
As V5 , perform the arithmetic processing of equation (6) to obtain the X coordinate value.

次に演算処理回路64は出力バツフア65を介
して切換回路66及びマルチプレクサ42に制御
信号を送り、Y方向の検出線23a〜23hの誘
導電圧を順次入力し、前述と同様の処理を行ない
Y座標値を求める。このようにして求められたデ
イジタル値のX及びY座標値は出力バツフア71
を介してデイジタル表示器(図示せず)に送出さ
れ表示され、またはコンピユータ(図示せず)に
送出され処理されたり、あるいはデイジタル―ア
ナログ(D/A)変換器72を介してアナログ信
号に変換され処理される。
Next, the arithmetic processing circuit 64 sends a control signal to the switching circuit 66 and the multiplexer 42 via the output buffer 65, sequentially inputs the induced voltages of the detection lines 23a to 23h in the Y direction, performs the same processing as described above, and Find the value. The X and Y coordinate values of the digital values obtained in this way are output to the output buffer 71.
to a digital display (not shown) for display, or to a computer (not shown) for processing, or for conversion to an analog signal via a digital-to-analog (D/A) converter 72. and processed.

なお、実施例中の励磁線及び検出線の本数は一
例であり、これに限定されないことはいうまでも
ない。また、検出線の間隔は2〜6mm程度であれ
ば、比較的精度良く位置検出ができることが実験
により確められている。また、位置指定用磁気発
生器も棒磁石に限定されることはなく、板,リン
グ,角体等でもよく、あるいは電磁石でもよい。
Note that the numbers of excitation lines and detection lines in the examples are merely examples, and it goes without saying that the numbers are not limited thereto. Moreover, it has been confirmed through experiments that position detection can be performed with relatively high accuracy if the distance between the detection lines is about 2 to 6 mm. Furthermore, the magnetic generator for specifying the position is not limited to a bar magnet, and may be a plate, ring, square body, etc., or may be an electromagnet.

また、前記実施例において、測定開始を示す信
号を位置指定用磁器発生器50から処理装置60
まで超音波信号を用いて伝送したが赤外線等の光
信号を用いても良い。また、前記測定開始を示す
信号は単に座標検出のタイミングを演算処理回路
64に認識させる為のものであるから磁気発生器
50より送ることを要するものではなく、処理装
置60自体に設けたキーボードその他のスイツチ
回路より前記タイミングを認識させる信号を送る
如くなしても良い。
Further, in the embodiment, a signal indicating the start of measurement is transmitted from the position specifying ceramic generator 50 to the processing device 60.
Although ultrasonic signals have been used for transmission up to this point, optical signals such as infrared rays may also be used. Furthermore, since the signal indicating the start of measurement is simply for making the arithmetic processing circuit 64 recognize the timing of coordinate detection, it does not need to be sent from the magnetic generator 50, but rather from a keyboard or other device provided in the processing device 60 itself. The switch circuit may send a signal for recognizing the timing.

(発明の効果) 以上説明したように本発明によれば、平板状の
磁性体にその位置検出方向と直交する如く励磁線
とを交互に並設してなるX方向及びY方向位置検
出部と、前記X方向及びY方向の各励磁線に所定
周期の交番電流を加える駆動電流源と、前記X方
向及びY方向の各磁性体に局部的な磁気バイアス
を加え且つどこにも接続されない位置指定用磁気
発生器と、前記X方向及びY方向の各検出線にそ
れぞれ接続されたX方向及びY方向の信号選択手
段と、該X方向及びY方向の信号選択手段より取
り出される各誘導電圧から前記位置指定用磁気発
生器による指定位置のX方向及びY方向の座標値
を算出する処理装置とを具備したため、励磁線と
検出線との間の磁束変化が磁性体内でのみ行なわ
れ、その結合が密で検出電圧が大きくしかもSN
比が良く、また、外部からの誘導を受けにくくか
つ外部への誘導ノイズの発生が少なく、また、位
置指定用磁気発生器は位置検出のためのタイミン
グ信号等を装置側へ送る必要がなく、装置との間
をコードレスとすることができ、コードがその疲
労により断線したり、からみついたり、じやまし
たりすることがなく、従つて、操作性が良く、位
置指定用磁気発生器を任意の位置に容易に移動さ
せることができ、また、磁性体にわずかの磁気バ
イアスを加えるのみで位置指定できるため、位置
指定用磁気発生器をタブレツトに必ずしも近接さ
せる必要はなく、数cm以上の間隔をあけても良
く、また、磁性体以外の物体を介在させても良
く、これらの場合でも高い分解能で位置検出でき
る等の効果が得られる。
(Effects of the Invention) As explained above, according to the present invention, the X-direction and Y-direction position detection parts are formed by alternately arranging excitation lines in a flat magnetic body so as to be orthogonal to the position detection direction thereof. , a drive current source that applies an alternating current at a predetermined period to each of the excitation lines in the X and Y directions, and a position specifying source that applies a local magnetic bias to each of the magnetic bodies in the X and Y directions and is not connected anywhere. A magnetic generator, X-direction and Y-direction signal selection means connected to the X-direction and Y-direction detection lines, respectively, and the position determined from each induced voltage extracted from the X-direction and Y-direction signal selection means. Since it is equipped with a processing device that calculates the coordinate values in the X and Y directions of the specified position by the specified magnetic generator, the magnetic flux change between the excitation line and the detection line occurs only within the magnetic body, and the coupling is tight. The detection voltage is large and the SN
It has a good ratio, is less susceptible to external induction and generates less external induction noise, and the magnetic generator for position specification does not need to send timing signals etc. to the equipment side for position detection. The connection between the device and the device can be made cordless, and the cord will not break, become tangled, or become loose due to fatigue. Therefore, it is easy to operate, and the magnetic generator for position specification can be used freely. The position can be easily moved to the desired position, and the position can be specified by simply applying a slight magnetic bias to the magnetic material, so the magnetic generator for position specification does not necessarily need to be close to the tablet, and can be placed at a distance of several centimeters or more. Alternatively, an object other than a magnetic material may be interposed, and even in these cases, effects such as position detection with high resolution can be obtained.

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

図面は本発明の説明に供するもので、第1図は
本発明の一実施例を示す一部切欠分解斜視図、第
2図は磁気バイアス対透磁率の特性図、第3図は
X方向の各検出線に発生する誘導電圧の一例を示
すグラフ、第4図は位置指定用棒磁石より磁性体
に印加される磁束のようすを示す説明図、第5図
は駆動電流源の具体例を示す電気回路図、第6図
は位置指定用磁気発生器の具体例を示す断面図、
第7図はその電気回路図、第8図は処理装置の具
体的構成を示す回路ブロツク図である。 10…X方向位置検出部、20…Y方向位置検
出部、30…駆動電流源、41,42…マルチプ
レクサ、50…位置指定用磁気発生器、60…処
理装置、11,21…磁性体、12a〜12i,
22a〜22i…励磁線、13a〜13h,23
a〜23h…検出線。
The drawings are for explaining the present invention, and FIG. 1 is a partially cutaway exploded perspective view showing an embodiment of the present invention, FIG. 2 is a characteristic diagram of magnetic bias versus magnetic permeability, and FIG. 3 is a diagram showing characteristics of magnetic bias in the X direction. A graph showing an example of the induced voltage generated in each detection line, Fig. 4 is an explanatory diagram showing the magnetic flux applied to the magnetic material from the position specifying bar magnet, and Fig. 5 shows a specific example of the drive current source. Electric circuit diagram, FIG. 6 is a sectional view showing a specific example of a magnetic generator for position designation,
FIG. 7 is an electric circuit diagram thereof, and FIG. 8 is a circuit block diagram showing a specific configuration of the processing device. DESCRIPTION OF SYMBOLS 10... X direction position detection part, 20... Y direction position detection part, 30... Drive current source, 41, 42... Multiplexer, 50... Magnetic generator for position specification, 60... Processing device, 11, 21... Magnetic body, 12a ~12i,
22a-22i...Excitation line, 13a-13h, 23
a to 23h...detection line.

Claims (1)

【特許請求の範囲】 1 平板状の磁性体にその位置検出方向と直交す
る如く励磁線と検出線とを交互に並設してなるX
方向及びY方向位置検出部と、 前記X方向及びY方向の各励磁線に所定周期の
交番電流を加える駆動電流源と、 前記X方向及びY方向の各磁性体に局部的な磁
気バイアスを加え且つどこにも接続されない位置
指定用磁気発生器と、 前記X方向及びY方向の各検出線にそれぞれ接
続されたX方向及びY方向の信号選択手段と、 該X方向及びY方向の信号選択手段より取り出
される各誘導電圧から前記位置指定用磁気発生器
による指定位置のX方向及びY方向の座標値を算
出する処理装置とを具備した ことを特徴とする位置検出装置。
[Claims] 1.
a drive current source that applies an alternating current at a predetermined period to each of the excitation lines in the X and Y directions; and a drive current source that applies a local magnetic bias to each of the magnetic bodies in the X and Y directions. and a magnetic generator for position designation that is not connected to anywhere; X-direction and Y-direction signal selection means connected to each of the X-direction and Y-direction detection lines, respectively; and the X-direction and Y-direction signal selection means. A position detection device comprising: a processing device that calculates coordinate values in the X direction and Y direction of the position designated by the position designation magnetic generator from each induced voltage taken out.
JP59088176A 1984-05-01 1984-05-01 Position detector Granted JPS60231231A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59088176A JPS60231231A (en) 1984-05-01 1984-05-01 Position detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59088176A JPS60231231A (en) 1984-05-01 1984-05-01 Position detector

Publications (2)

Publication Number Publication Date
JPS60231231A JPS60231231A (en) 1985-11-16
JPH0210443B2 true JPH0210443B2 (en) 1990-03-08

Family

ID=13935592

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59088176A Granted JPS60231231A (en) 1984-05-01 1984-05-01 Position detector

Country Status (1)

Country Link
JP (1) JPS60231231A (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5510608A (en) * 1978-07-07 1980-01-25 Kokusai Denshin Denwa Co Ltd <Kdd> Coordinate reader
JPS578884A (en) * 1980-06-20 1982-01-18 Sony Corp Position detecting device
JPS58123184A (en) * 1982-01-16 1983-07-22 Graphtec Corp Digitizer

Also Published As

Publication number Publication date
JPS60231231A (en) 1985-11-16

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