JPH0210968B2 - - Google Patents
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- Publication number
- JPH0210968B2 JPH0210968B2 JP59149053A JP14905384A JPH0210968B2 JP H0210968 B2 JPH0210968 B2 JP H0210968B2 JP 59149053 A JP59149053 A JP 59149053A JP 14905384 A JP14905384 A JP 14905384A JP H0210968 B2 JPH0210968 B2 JP H0210968B2
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- JP
- Japan
- Prior art keywords
- magnetic
- detection
- directions
- applies
- magnetic material
- 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.)
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Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は任意の指示位置の座標値を簡易かつ正
確に検出し得る位置検出装置に関するものであ
る。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a position detection device that can easily and accurately detect the coordinate values of any indicated position.
(従来の技術)
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、その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
や、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等があつた。(Prior Art) A conventional position detection device applies a pulse current to a drive coil provided at one end of a magnetostrictive transmission medium or the tip of a position indicating pen to generate magnetostrictive vibration waves in the magnetostrictive transmission medium, and A processor or the like measures the time until an induced voltage based on the magnetostrictive vibration 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 the indicated position of the positioning pen is calculated. In some cases, a plurality of drive lines and detection lines are arranged orthogonally to each other, and the induced voltage is detected by sequentially passing current through the drive lines and sequentially selecting the detection lines. There was a device in which a position specified by a position indicating pen having a position indicator was detected from the position of a detection line where a large induced voltage was induced.
(発明が解決しようとする問題点)
前者の装置は位置検出精度が比較的良好である
が他の機器からの誘導を受けやすく誤動作した
り、逆にノイズの発生源となる恐れがあり、また
後者の装置は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、かつ駆動線と検出線の交
点の真上の位置検出が困難であり、更にこれらの
装置では位置指示ペンを磁歪伝達媒体や検出線等
に極く接近させなければ位置検出の精度が極端に
低下したり、または検出不能となるため入力板面
上の高さ方向を含めた、いわゆる3次元的な位置
検出ができないという問題点があつた。(Problems to be Solved by the Invention) Although the former device has relatively good position detection accuracy, it is susceptible to guidance from other devices and may malfunction, or may even become a source of noise. In the latter device, the resolution of the coordinate position is determined by the line spacing, and if the line spacing is made small to increase the resolution, the signal-to-noise ratio and stability deteriorate, making it difficult to increase the resolution. It is difficult to detect the position directly above the intersection of the lines, and in addition, with these devices, the accuracy of position detection will be extremely reduced or the detection will be difficult if the position indicating pen is not brought very close to the magnetostrictive transmission medium or the detection line. Therefore, there was a problem that so-called three-dimensional position detection including the height direction on the input board surface was impossible.
本発明は前述したような従来の問題点を解決
し、位置指定用磁気発生器がどこにも接続されず
操作性がよく、しかも外部からの誘導ノイズ等に
強い高精度な位置検出装置、並びにこれに加えて
X方向及びY方向の座標値とともにZ方向の座標
値を検出し得る位置検出装置を提供することを目
的とするものである。 The present invention solves the conventional problems as described above, and provides a high-precision position detection device that has a magnetic generator for position specification that is not connected anywhere, has good operability, and is resistant to external induced noise, etc. It is an object of the present invention to provide a position detection device capable of detecting coordinate values in the Z direction as well as coordinate values in the X and Y directions.
(発明の構成)
本発明は前記問題点を解決するため、平板状の
磁性体11か又は、複数の長尺の磁性体片を互い
にほぼ平行に配列してなる磁性体片群2組を互い
に直角方向に重ね合わせて構成した磁性体16の
上下両面を一連に覆う如くX方向及びY方向に
各々、励磁線122a〜122i及び132a〜
132iと検出線123a〜123h及び133
a〜133hとを交互に配設してなるタブレツト
部10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20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31,32
と、前記磁性体11あるいは16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40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し、またはこれに加えて
X方向及びY方向の各誘導電圧のうちで最も大き
な電圧値を、予め設定した少なくとも1つの閾値
と比較することにより、前記位置指定用磁気発生
器による指定位置のZ方向の座標値を求める処理
装置50とを具備したことを特徴とするものであ
る。(Structure of the Invention) In order to solve the above-mentioned problems, the present invention has a flat magnetic body 11 or two sets of magnetic body pieces each formed by arranging a plurality of elongated magnetic body pieces substantially parallel to each other. Excitation lines 122a to 122i and 132a to 132a are arranged in the X direction and the Y direction so as to continuously cover both the upper and lower surfaces of the magnetic body 16, which are stacked at right angles.
132i and detection lines 123a to 123h and 133
a to 133h arranged alternately, a drive current source 20 that applies an alternating current at a predetermined period to each excitation line in the X direction and the Y direction, and each detection device in the X direction and the Y direction. X-direction and Y-direction signal selection means 31, 32 connected to the lines, respectively.
, a position designating magnetic generator 40 that applies a local magnetic bias to the magnetic body 11 or 16 and is not connected anywhere, and the position designation from each induced voltage taken out from the X-direction and Y-direction signal selection means. Calculate the coordinate values in the X and Y directions of the designated position by the magnetic generator, or in addition, calculate the largest voltage value among the induced voltages in the X and Y directions at least one preset threshold value. The present invention is characterized by comprising a processing device 50 that calculates the Z-direction coordinate value of the position designated by the position designating magnetic generator by comparing with the position designation magnetic generator.
(実施例)
第1図は本発明の一実施例の要部構成を示すも
ので、図中、10はタブレツト部、20は駆動電
流源、31,32は信号選択手段、例えばマルチ
プレクサ、40は位置指定用磁気発生器、例えば
棒磁石、50は処理装置である。(Embodiment) FIG. 1 shows the main part configuration of an embodiment of the present invention, in which 10 is a tablet section, 20 is a drive current source, 31 and 32 are signal selection means, for example, a multiplexer, and 40 is a A magnetic generator for position designation, for example a bar magnet, 50 is a processing device.
タブレツト部10は、平板状の磁性体11とX
方向導体部12とY方向導体部13とからなつて
いる。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
0.2Oe、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
薄いものを作れるので、これをそのまま適用して
もよい。 The tablet part 10 includes a flat magnetic body 11 and an
It consists of a direction conductor section 12 and a Y direction conductor section 13. 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
0.2Oe, magnetic permeability (μ) = 14000), etc. can be used.
Moreover, although the magnetic body 11 is in the shape of a flat plate (sheet),
Amorphous alloys can be manufactured to be as thin as 20 to 50 μm, so they may be used as they are.
X方向導体部12は、銅線のような線状導体を
多数平行にプラスチツクフイルム121等でラミ
ネートしたものからなつており、該線状導体が励
磁線122a〜122iと検出線123a〜12
3hを構成する如くなつている。このX方向導体
部12は長手方向の略中央付近で二つ折りにさ
れ、その間に前記磁性体11が収納される如くな
つている。X方向導体部12の磁性体11の下面
11bの下に位置する部分12b側の各励磁線1
22a,122b,122c,122d,122
e,122f,122g,122hの一端は、磁
性体11の上面11aの上に位置する部分12a
側の励磁線122b,122c,122d,12
2e,122f,122g,122h,122i
の一端にそれぞれ接続され、即ち励磁線122a
〜122iは直列に接続され、励磁線122aの
他端と励磁線122iの他端は駆動電流源20に
接続される。また、各励磁線122a〜122i
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。部
分12a側の各検出線123a〜123hの一端
はそれぞれマルチプレクサ31に接続され、部分
12b側の一端は共通に接地される。また、各検
出線123a〜123hはそれぞれ励磁線122
a〜122iのそれぞれの間に互いに平行に配置
されている。 The X-direction conductor section 12 is made up of a large number of linear conductors such as copper wires laminated in parallel with a plastic film 121 or the like, and the linear conductors are connected to excitation lines 122a to 122i and detection lines 123a to 12.
It seems to constitute 3h. This X-direction conductor portion 12 is folded in two near the approximate center in the longitudinal direction, and the magnetic material 11 is housed in between. Each excitation line 1 on the side of the portion 12b located under the lower surface 11b of the magnetic body 11 of the X-direction conductor portion 12
22a, 122b, 122c, 122d, 122
One end of e, 122f, 122g, 122h is a portion 12a located above the upper surface 11a of the magnetic body 11.
Side excitation lines 122b, 122c, 122d, 12
2e, 122f, 122g, 122h, 122i
are respectively connected to one end of the excitation line 122a, that is, the excitation line 122a
122i are connected in series, and the other end of the excitation line 122a and the other end of the excitation line 122i are connected to the drive current source 20. In addition, each excitation line 122a to 122i
are arranged parallel to each other at predetermined intervals in a direction perpendicular to the X direction, that is, along the Y direction. One end of each of the detection lines 123a to 123h on the portion 12a side is connected to the multiplexer 31, and one end on the portion 12b side is commonly grounded. In addition, each detection line 123a to 123h is connected to an excitation line 122, respectively.
They are arranged parallel to each other between each of a to 122i.
Y方向導体部13は、プラスチツクフイルム1
31と励磁線132a〜132iと検出線133
a〜133hとからなつており、その細部の構造
はX方向導体部12と同様である。第2図に示す
ように、Y方向導体部13の磁性体11の上面1
1aの上に位置する部分13aはX方向導体部1
2の部分12aの上に、またY方向導体部13の
磁性体11の下面11bの下に位置する部分13
bはX方向導体部12の部分12bの上になる如
く配置される。また各励磁線132a〜132i
は駆動電流源20に接続され、各検出線133a
〜133hはマルチプレクサ32に接続される。
なお、X方向導体部12とY方向導体部13との
配置は、部分13aの上に部分12aが位置し、
部分13bの上に部分12bが位置する如くなし
ても良い。また、これらタブレツト部10は、外
部からの誘導やノイズの発散を防ぐため、第3図
に示すように非磁性の金属、例えばアルミ板14
でその上部を覆う如くなしても良い。なお、15
は合成樹脂等からなる保持板である。 The Y-direction conductor portion 13 is made of plastic film 1
31, excitation lines 132a to 132i, and detection line 133
a to 133h, and its detailed structure is the same as that of the X-direction conductor section 12. As shown in FIG. 2, the upper surface 1 of the magnetic body 11 of the Y direction conductor section 13
The portion 13a located above 1a is the X direction conductor portion 1
A portion 13 located above the portion 12a of No. 2 and below the lower surface 11b of the magnetic body 11 of the Y-direction conductor portion 13
b is arranged so as to be above the portion 12b of the X-direction conductor portion 12. In addition, each excitation line 132a to 132i
are connected to the drive current source 20, and each detection line 133a
~133h are connected to multiplexer 32.
Note that the arrangement of the X-direction conductor portion 12 and the Y-direction conductor portion 13 is such that the portion 12a is located above the portion 13a,
The portion 12b may be positioned above the portion 13b. In addition, these tablet parts 10 are made of non-magnetic metal, for example, an aluminum plate 14, as shown in FIG.
The upper part may be covered with In addition, 15
is a holding plate made of synthetic resin or the like.
駆動電流源20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122a〜122i及
び132a〜132iに送出する。また、マルチ
プレクサ31,32は処理装置50からの制御信
号に従つて検出線123a〜123h及び133
a〜133hの出力信号を処理装置50へ選択的
に送出する如くなつている。 The drive current source 20 always sends out an alternating current of a predetermined period (the alternating current here includes all of sine waves, rectangular waves, triangular waves, etc.) to the excitation lines 122a to 122i and 132a to 132i. Further, the multiplexers 31 and 32 operate on the detection lines 123a to 123h and 133 according to the control signal from the processing device 50.
The output signals of a to 133h are selectively sent to the processing device 50.
このような構成において、検出線123a〜1
23h及び133a〜133hには前記励磁線1
22a〜122i及び132a〜132i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を介して行な
われるため、磁性体11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4
図に示すように所定量の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
てこの場合は、磁性体11に前記所定量程度の磁
気バイアスを加えると、励磁線122a〜122
i,132a〜132iから検出線123a〜1
23h,133a〜133hへ誘起する電圧が大
きくなる。 In such a configuration, the detection lines 123a to 1
The excitation line 1 is connected to 23h and 133a to 133h.
An induced voltage is generated by electromagnetic induction based on the alternating current flowing through 22a to 122i and 132a to 132i. Since this electromagnetic induction occurs via the magnetic body 11, the higher the magnetic permeability of the magnetic body 11, the greater the voltage value of the induced voltage. By the way, the magnetic permeability of the magnetic body 11 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, heat treatment applied to the magnetic material, etc.
As shown in the figure, it can be set so that it becomes maximum when a predetermined amount of magnetic bias is applied. Therefore, in this case, if a magnetic bias of the predetermined amount is applied to the magnetic body 11, the excitation lines 122a to 122
i, 132a to 132i to detection lines 123a to 1
The voltage induced to 23h, 133a to 133h increases.
今、第1図において位置指定用棒磁石40がN
極を下にして検出線123aからX方向の距離
xs、また検出線133aからY方向の距離ysだけ
隔てたY方向導体部13の位置A(Z方向の距離
は0とする。)上にあり、前記所定量程度の磁気
バイアスを磁性体11に加えているものとする。 Now, in FIG. 1, the position specifying bar magnet 40 is
Distance in the X direction from the detection line 123a with the pole facing down
x s , and is located on position A of the Y-direction conductor section 13 separated by a distance y s in the Y direction from the detection line 133a (the distance in the Z direction is 0), and applies a magnetic bias of about the predetermined amount to the magnetic material. 11.
この時、X方向の検出線123a〜123hに
は第5図に示すような誘導電圧V1〜V8が発生す
る。第5図において、横軸は検出線123a〜1
23h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3
1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50で演算して求め
れば、棒磁石40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. 5 are generated in the detection lines 123a to 123h in the X direction. In FIG. 5, the horizontal axis is the detection line 123a to 1
The coordinate positions in the X direction are shown with the positions of 23h being x 1 to x 8 , respectively, and the vertical axis shows the voltage value, and each of the voltages V 1 to V 8 has a maximum value (maximum value) directly below position A.
becomes. Each of the voltages V 1 to V 8 is supplied to multiplexer 3.
1, the X coordinate value xs of the bar magnet 40 can be determined by calculating and determining the X coordinate value at which the induced voltage becomes the maximum value using the processing device 50.
座標値xsを求める算出方法の一つとして、第5
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123a〜123hの間隔
をΔxとし、第5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−xs)2+b …(1)
V4=a(x4−xs)2+b …(2)
V5=a(x5−xs)2+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 fifth
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 123a to 123h is Δx and the coordinates x 3 to x 5 in FIG. 5 are approximated by a quadratic function (indicated by a solid line in the figure), the calculation can be performed as follows. Can be done. 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 ( x 5 −x s ) 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123c,123d,1
23eに誘起する電圧V3,V4,V5、及び検出線
123cの座標値x3(既知)から処理装置50で
(6)式の演算を行なうことにより棒磁石40のX座
標値を算出できる。また、棒磁石40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). Therefore, the detection lines 123c, 123d, 1
The processing device 50 uses the voltages V 3 , V 4 , V 5 induced in 23e and the coordinate value x 3 (known) of the detection line 123c.
The X coordinate value of the bar magnet 40 can be calculated by calculating equation (6). Further, even if the bar magnet 40 is moved along the Y axis, the same X coordinate value can be obtained.
また、Y方向の検出線133a〜133hにも
第5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。 Further, induced voltages similar to those shown in FIG. 5 are obtained on the detection lines 133a to 133h in the Y direction, and the Y coordinate value ys can be determined by the same calculation process as described above.
また、前述したように位置指定するためには磁
性体11に局部的に数0e程度の磁気バイアスを与
えるのみで良いから、位置指定用棒磁石40を磁
性体11よりZ方向に多少離隔させて用いること
もできる。ここで、位置指定用棒磁石40のN極
側の一端より磁性体11に加わる磁気バイアス量
(即ち、磁界強さ)は該磁性体11と棒磁石40
の一端との間の距離、即ちZ方向の距離の2乗に
反比例する。従つて、位置指定用棒磁石40のZ
方向の距離を0とした時、例えば第6図に示すよ
うにタブレツト部10の上部に通常形成される入
力面70上に棒磁石40の一端が接した時に、該
棒磁石40より磁性体11に加えられる磁気バイ
アスが前記透磁率を最大とする値になるよう棒磁
石40の磁界強さを設定すれば、該棒磁石40の
Z方向の距離の略2乗に反比例して透磁率が減少
し、検出線123a〜123h,133a〜13
3hへの誘導電圧が減少する。第5図において、
V3〜V5は棒磁石40のN極側の一端を前記位置
A上でZ方向にわずかの距離(5mm程度)をおい
て保持した場合の誘導電圧を示すものである。 In addition, as mentioned above, in order to specify the position, it is sufficient to locally apply a magnetic bias of several tens of e to the magnetic body 11, so the position specifying bar magnet 40 may be separated from the magnetic body 11 by some distance in the Z direction. It can also be used. Here, the amount of magnetic bias (that is, the magnetic field strength) applied to the magnetic body 11 from one end of the N-pole side of the position specifying bar magnet 40 is between the magnetic body 11 and the bar magnet 40.
It is inversely proportional to the square of the distance between the two ends of the line, that is, the distance in the Z direction. Therefore, Z of the position designating bar magnet 40
When the distance in the direction is 0, for example, when one end of the bar magnet 40 comes into contact with the input surface 70 normally formed on the upper part of the tablet part 10 as shown in FIG. If the magnetic field strength of the bar magnet 40 is set so that the magnetic bias applied to the bar magnet 40 has a value that maximizes the magnetic permeability, the magnetic permeability decreases in inverse proportion to approximately the square of the distance of the bar magnet 40 in the Z direction. Detection lines 123a to 123h, 133a to 13
The induced voltage to 3h is reduced. In Figure 5,
V 3 to V 5 indicate induced voltages when one end of the N pole side of the bar magnet 40 is held at the position A at a short distance (about 5 mm) in the Z direction.
指示位置における誘導電圧値Vsは磁性体11
の透磁率の変化特性、棒磁石40の磁界強さ及び
Z方向の距離で決まるから、該電圧Vsがわかれ
ば棒磁石40のZ方向の距離(位置)を算出する
ことができる。しかしながら、実際には該電圧
Vsを電圧V3〜V5より式を用いて算出することが
困難であるので、棒磁石40のZ方向の正確な距
離を知ることはできない。そこで電圧Vsの代り
に指示位置に最も近い検出線の電圧、即ち誘導電
圧V1〜V8の中で最も大きな電圧値(第5図の例
ではV4)を取り出し、これを予めいくつか設定
した閾値電圧VTと比較し、その結果より棒磁石
40のZ方向のおおよその距離を求めることがで
きる。なお、棒磁石40の指示位置が各検出線の
中間付近に位置する場合と各検出線付近に位置す
る場合とでは、Z方向の距離が同一でも前記最も
大きな誘導電圧の電圧値にかなりの相違が生じる
ことになるが、予めその差を考慮して閾値を設定
しておくこともでき、また検出線及び励磁線の本
数を増し間隔を詰めて差を少なくすることもでき
る。 The induced voltage value V s at the indicated position is the magnetic material 11
, the magnetic field strength of the bar magnet 40, and the distance in the Z direction. Therefore, if the voltage Vs is known, the distance (position) of the bar magnet 40 in the Z direction can be calculated. However, in reality the voltage
Since it is difficult to calculate V s from the voltages V 3 to V 5 using a formula, it is not possible to know the exact distance of the bar magnet 40 in the Z direction. Therefore, instead of the voltage V s , take the voltage of the detection line closest to the indicated position, that is, the largest voltage value among the induced voltages V 1 to V 8 (V 4 in the example in Figure 5), and set several of these in advance. It is compared with the set threshold voltage VT , and from the result, the approximate distance of the bar magnet 40 in the Z direction can be determined. Note that even if the distance in the Z direction is the same, there is a considerable difference in the voltage value of the largest induced voltage between when the indicated position of the bar magnet 40 is located near the middle of each detection line and when it is located near each detection line. However, the difference can be set in advance by taking this difference into account, or the difference can be reduced by increasing the number of detection lines and excitation lines and reducing the spacing between them.
第7図は駆動電流源20の具体例を示すもので
ある。同図において、21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22はパワー
ドライバであり、オペアンプと電流増幅器とから
なつており、前記正弦波信号を電流増幅して励磁
線122a〜122i,132a〜132iへ送
出する。 FIG. 7 shows a specific example of the drive current source 20. In the figure, reference numeral 21 denotes a function generator, such as Intersil IC 8038, which outputs a sine wave signal of a predetermined frequency determined by the values of capacitor C and resistor R. A power driver 22 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 122a to 122i and 132a to 132i.
第8図は位置指定用磁気発生器40の具体例を
示す断面図、第9図はその電気回路図である。同
図において、41は合成樹脂等からなるペン状の
容器であり、その一端には同じく合成樹脂等から
なる先端先細状の中空スライド管42が軸方向に
摺動自在に収容されている。また、43は前記ス
ライド管42内に収納される如く容器41の一端
に取り付けられた棒磁石である。また、44は容
器41の側面より操作可能な位置に取り付けられ
た操作スイツチであり、45は超音波信号の送信
機、46は超音波の送波器で、電池47とともに
容器41内の適所に収納されている。前記容器4
1を保持し中空スライド管42の先端を入力面に
接触させ位置指定し、スイツチ44を操作すれ
ば、送信機45内の発振回路45a及び増幅器4
5bが動作し、送波器46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。この時、容器41を入力
面に対して強く押し付けると、スライド管42が
容器41内にスライドし棒磁石43の先端が入力
面に近接し、また逆に軽く押し付けるとスライド
管42がスプリング48の弾撥力により突出した
ままとなり棒磁石43の先端が入力面より離れる
ことになり、従つて棒磁石43のZ方向の指示位
置を容易に変えることができる。 FIG. 8 is a sectional view showing a specific example of the position specifying magnetic generator 40, and FIG. 9 is an electric circuit diagram thereof. In the figure, reference numeral 41 denotes a pen-shaped container made of synthetic resin or the like, and a hollow slide tube 42 made of synthetic resin or the like with a tapered tip is accommodated in one end of the pen-shaped container so as to be slidable in the axial direction. Further, 43 is a bar magnet attached to one end of the container 41 so as to be housed in the slide tube 42. Further, 44 is an operation switch attached to a position that can be operated from the side of the container 41, 45 is an ultrasonic signal transmitter, and 46 is an ultrasonic wave transmitter, which is attached to a suitable place in the container 41 together with a battery 47. It is stored. Said container 4
1, touch the tip of the hollow slide tube 42 to the input surface to specify the position, and operate the switch 44, the oscillation circuit 45a in the transmitter 45 and the amplifier 4
5b is activated, and the transmitter 46 converts a signal indicating the start of measurement, for example, a continuous pulse signal of a predetermined frequency, into an ultrasonic signal and transmits it. At this time, when the container 41 is strongly pressed against the input surface, the slide tube 42 slides into the container 41 and the tip of the bar magnet 43 approaches the input surface. The tip of the bar magnet 43 remains protruded due to the repulsive force and moves away from the input surface, so that the indicated position of the bar magnet 43 in the Z direction can be easily changed.
第10図は処理装置50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46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51で受波され、
更に受信器52で増幅・波形整形されて入力バツ
フア53に送出される。演算処理装置54は入力
バツフア53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55を介し
て切換回路56及びマルチプレクサ31へ制御信
号を送り、X方向の検出線123a〜123hの
誘導電圧を増幅器57へ順次入力する。前記各誘
導電圧は増幅器57で増幅され検波器58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59にてデイジタル値に
変換され入力バツフア53を介して演算処理回路
54に送出される。演算処理回路54では前記各
誘導電圧(デイジタル値)をメモリ60に一時記
憶し、これらの中より最大の電圧値を有する誘導
電圧Vk(k=1、2…8)を検出する。更に演算
処理回路54はメモリ60内より前記誘導電圧
Vkとその前後の誘導電圧Vk-1,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。また一方、前記最大の誘導電圧Vkと予
め閾値メモリ61内に記憶させた所定の閾値電圧
VTとを比較し、棒磁石40のZ座標値を求める。 FIG. 10 is a circuit block diagram showing a specific configuration of the processing device 50. In the figure, when an ultrasonic signal indicating the start of measurement is transmitted from the above-mentioned transmitter 46, the ultrasonic signal is received by a receiver 51,
Furthermore, the signal is amplified and waveform-shaped by the receiver 52 and sent to the input buffer 53. The arithmetic processing unit 54 reads the measurement start signal from the input buffer 53,
When the start of measurement is recognized, a control signal is sent to the switching circuit 56 and the multiplexer 31 via the output buffer 55, and the induced voltages of the detection lines 123a to 123h in the X direction are sequentially input to the amplifier 57. Each of the induced voltages is amplified by an amplifier 57, rectified by a detector 58, converted into a DC voltage, further converted into a digital value by an analog-digital (A/D) converter 59, and processed through an input buffer 53. The signal is sent to circuit 54. The arithmetic processing circuit 54 temporarily stores each of the induced voltages (digital values) in the memory 60, and detects the induced voltage V k (k=1, 2...8) having the maximum voltage value among them. Further, the arithmetic processing circuit 54 receives the induced voltage from within the memory 60.
Take out V k and the induced voltages V k-1 and V k+1 before and after it,
These are respectively the voltages V 3 , V 4 , and
As V5 , perform the arithmetic processing of equation (6) to obtain the X coordinate value. On the other hand, the maximum induced voltage V k and a predetermined threshold voltage stored in the threshold memory 61 in advance
V T and the Z coordinate value of the bar magnet 40 is determined.
次に演算処理回路54は出力バツフア55を介
して切換回路56及びマルチプレクサ32に制御
信号を送り、Y方向の検出線133a〜133h
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。 Next, the arithmetic processing circuit 54 sends a control signal to the switching circuit 56 and the multiplexer 32 via the output buffer 55, and sends a control signal to the detection lines 133a to 133h in the Y direction.
The induced voltages are sequentially input, and the same processing as described above is performed to obtain the Y coordinate value.
このようにして求められたデイジタル値のX、
Y及びZの座標値は出力バツフア62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63を介してアナログ信号に変
換され処理される。前記Z座標値は立体物(但
し、高さの極く低いものに限る。)を入力面上に
載置してその形状を入力する場合の他、入力図形
の線の太さのパラメータ等として用いることもで
きる。なお、Y方向の誘導電圧よりZ座標値を求
めることができるのはいうまでもない。 The digital value X obtained in this way,
The Y and Z coordinate values are sent via output buffer 62 to a digital display (not shown) for display, or sent to a computer (not shown) for processing, or digital-to-analog (D/A). It is converted into an analog signal via a converter 63 and processed. The Z coordinate value is used not only when placing a three-dimensional object (limited to extremely low height objects) on the input surface and inputting its shape, but also as a parameter for the line thickness of the input figure. It can also be used. It goes without saying that the Z coordinate value can be determined from the induced voltage in the Y direction.
また、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
により確かめられている。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。 Further, the numbers of excitation lines and detection lines in the embodiments are merely examples, and it goes without saying that the numbers are not limited thereto. Further, it has been confirmed through experiments that position detection can be performed with relatively high accuracy if the distance between the detection lines is approximately 2 to 6 mm. Further, 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.
前記実施例において、測定開始を示す信号を位
置指定用磁気発生器40から処理装置50まで超
音波信号を用いて伝送したのは、位置指定用磁気
発生器40をコードレスとし操作性を良くするた
めであつて、コードを用いて電気信号のまま伝送
しても良いことはいうまでもない。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54に認識させる為のものであるか
ら特に磁気発生器40より送ることを要するもの
ではなく、処理装置50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。 In the above embodiment, the signal indicating the start of measurement was transmitted from the position specifying magnetic generator 40 to the processing device 50 using an ultrasonic signal in order to make the position specifying magnetic generator 40 cordless and improve operability. However, it goes without saying that the electric signal may be transmitted as it is using a code. Furthermore, since the signal indicating the start of measurement is simply for making the arithmetic processing circuit 54 recognize the timing of coordinate detection, it is not necessary to send it from the magnetic generator 40, but rather from the keyboard provided in the processing device 50 itself. A signal for recognizing the timing may be sent from another switch circuit.
第11図は本発明の磁性体の別の実施例を示す
ものである。同図において、16は磁性体であつ
て、例えば直径が0.13mmのアモルフアスワイヤ
(磁性体片)161を複数本、所定間隔(1〜2
mm)をおいて互いにほぼ平行に配列し、これ(磁
性体片群)をプラスチツクフイルム162等でラ
ミネートしたシート163を2枚、そのワイヤが
X方向及びY方向に沿つて互いに直交する如く重
ね合わせてなつており、より検出精度を上げるこ
とができる。 FIG. 11 shows another embodiment of the magnetic material of the present invention. In the same figure, reference numeral 16 is a magnetic material, for example, a plurality of amorphous wires (magnetic material pieces) 161 with a diameter of 0.13 mm are arranged at predetermined intervals (1 to 2
Two sheets 163 are arranged approximately parallel to each other with a distance of This increases the detection accuracy.
(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
磁性体か又は、複数の長尺の磁性体片を互いにほ
ぼ平行に配列してなる磁性体片群2組を互いに直
角方向に重ね合わせて構成した磁性体の上下両面
を一連に覆う如くX方向及びY方向に各々、励磁
線と検出線とを交互に配設してなるタブレツト部
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、前記磁性体に局部
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、
X方向及びY方向の励磁線並びに検出線を共通の
磁性体の周囲に配設したため、X方向及びY方向
の励磁線並びに検出線と位置指定用磁気発生器と
の間の距離がほぼ同一となり、その検出出力がX
方向及びY方向でほぼ同一となり、従つて、検出
精度が向上し、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。(Effects of the Invention) As explained above, according to the present invention, two sets of magnetic material pieces each formed by arranging a flat magnetic material or a plurality of elongated magnetic material pieces substantially parallel to each other are arranged at right angles to each other. a tablet portion in which excitation lines and detection lines are arranged alternately in the X direction and the Y direction so as to continuously cover both upper and lower surfaces of magnetic bodies configured by overlapping each other in the X direction and the Y direction; a drive current source that applies an alternating current with a predetermined period to each excitation line; a signal selection means in the X and Y directions connected to each of the detection lines in the X and Y directions; and local magnetism in the magnetic body. A position designating magnetic generator to which a bias is applied and not connected to any other location, and the X direction of the designated position by the position designating magnetic generator from each induced voltage taken out from the X direction and Y direction signal selection means.
Equipped with a processing device that calculates the coordinate values in the direction and Y direction, the magnetic flux change between the excitation line and the detection line occurs only within the magnetic body, and the coupling is tight, resulting in a large detection voltage and a good signal-to-noise ratio. In addition, it is less susceptible to external induction and generates less external induction noise.Furthermore, the magnetic generator for position specification does not need to send timing signals etc. for position detection to the equipment side, making it easier to communicate with the equipment. The cable 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 placed in any position. Can be easily moved and
Because the excitation lines and detection lines in the X and Y directions are arranged around a common magnetic body, the distances between the excitation lines and detection lines in the X and Y directions and the magnetic generator for position specification are almost the same. , its detection output is
It is almost the same in both the direction and the Y direction, therefore, the detection accuracy is improved, and the position can be specified by simply applying a slight magnetic bias to the magnetic material, so it is not necessary to place the magnetic generator for position specification close to the tablet. It is okay to leave a distance of several centimeters or more,
Further, an object other than a magnetic material may be interposed, and even in these cases, the position can be detected with high resolution.
また、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とともに、
X方向またはY方向の各誘導電圧のうちで最も大
きな電圧値を、予め設定した少なくとも1つの閾
値と比較することにより、位置指定用磁気発生器
による指定位置のZ方向の座標値を求める処理装
置を具備したものによれば、前述した効果に加え
てX方向及びY方向のいわゆる2次元の座標値と
ともにこれらに直交するZ方向の座標値を入力す
ることができ、立体物の形状を直接入力したり、
2次元の座標値以外のパラメータを位置指定とと
もに変化させることができる等の効果が得られ
る。 In addition, while calculating the coordinate values in the X direction and Y direction of the designated position by the position designating magnetic generator,
A processing device that calculates the Z-direction coordinate value of the specified position by the position-specifying magnetic generator by comparing the largest voltage value among the induced voltages in the X-direction or the Y-direction with at least one preset threshold value. In addition to the above-mentioned effects, it is possible to input the so-called two-dimensional coordinate values in the X and Y directions as well as the coordinate values in the Z direction perpendicular to these, making it possible to directly input the shape of a three-dimensional object. or
Effects such as being able to change parameters other than two-dimensional coordinate values together with position designation can be obtained.
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図はタブレツト部のY方向の励磁線に沿う断面
図、第3図はタブレツト部にアルミ板による覆い
を取りつけた状態を示す一部切欠斜視図、第4図
は磁気バイアス対透磁率の特性図、第5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6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7図は駆
動電流源の具体例を示す電気回路図、第8図は位
置指定用磁気発生器の具体例を示す断面図、第9
図はその電気回路図、第10図は処理装置の具体
的構成を示す回路ブロツク図、第11図は磁性体
の別の実施例を示す一部切欠斜視図である。
10……タブレツト部、20……駆動電流源、
31,32……マルチプレクサ、40……位置指
定用磁気発生器、50……処理装置、11,16
……磁性体、122a〜122i,132a〜1
32i……励磁線、123a〜123h,133
a〜133h……検出線。
The drawings are for explaining the present invention, and FIG. 1 is a partially cutaway exploded perspective view showing one embodiment of the present invention, FIG. 2 is a cross-sectional view of the tablet portion along the excitation line in the Y direction, and FIG. Figure 4 is a partially cutaway perspective view showing the tablet part covered with an aluminum plate, Figure 4 is a characteristic diagram of magnetic bias versus magnetic permeability, and Figure 5 is an example of the induced voltage generated in each detection line in the X direction. 6 is an explanatory diagram showing the state of the magnetic flux applied to the magnetic material from the bar magnet for position designation, Figure 7 is an electric circuit diagram showing a specific example of the drive current source, and Figure 8 is a diagram showing the position designation. Cross-sectional view showing a specific example of a magnetic generator for use, No. 9
10 is a circuit block diagram showing a specific configuration of the processing device, and FIG. 11 is a partially cutaway perspective view showing another embodiment of the magnetic material. 10... Tablet part, 20... Drive current source,
31, 32... Multiplexer, 40... Magnetic generator for position specification, 50... Processing device, 11, 16
...Magnetic material, 122a-122i, 132a-1
32i...excitation line, 123a to 123h, 133
a~133h...Detection line.
Claims (1)
片を互いにほぼ平行に配列してなる磁性体片群2
組を互いに直角方向に重ね合わせて構成した磁性
体の上下両面を一連に覆う如くX方向及びY方向
に各々、励磁線と検出線とを交互に配設してなる
タブレツト部と、 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、 前記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。 2 タブレツト部の周囲を非磁性金属で覆うよう
になしたことを特徴とする特許請求の範囲第1項
記載の位置検出装置。 3 平板状の磁性体か又は、複数の長尺の磁性体
片を互いにほぼ平行に配列してなる磁性体片群2
組を互いに直角方向に重ね合わせて構成した磁性
体の上下両面を一連に覆う如くX方向及びY方向
に各々、励磁線と検出線とを交互に配設してなる
タブレツト部と、 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、 前記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
算出するとともに、X方向またはY方向の各誘導
電圧のうちで最も大きな電圧値を、予め設定した
少なくとも1つの閾値と比較することにより、前
記位置指定用磁気発生器による指定位置のZ方向
の座標値を求め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。 4 タブレツト部の周囲を非磁性金属で覆うよう
になしたことを特徴とする特許請求の範囲第3項
記載の位置検出装置。[Claims] 1. A flat magnetic material or a group of magnetic material pieces 2 formed by arranging a plurality of elongated magnetic material pieces substantially parallel to each other.
a tablet portion in which excitation wires and detection wires are arranged alternately in the X direction and the Y direction so as to continuously cover both upper and lower surfaces of a magnetic body formed by overlapping pairs of magnetic materials in a perpendicular direction; and a drive current source that applies an alternating current with a predetermined period to each excitation line in the X and Y directions; signal selection means in the X and Y directions connected to each of the detection lines in the X and Y directions, respectively; a position designating magnetic generator that applies a local magnetic bias and is not connected to any other location; and a position designating magnetic generator that applies a local magnetic bias and is not connected to any part; and a processing device that calculates coordinate values in the Y direction. 2. The position detection device according to claim 1, wherein the tablet portion is covered with a non-magnetic metal. 3 Magnetic material piece group 2 made of a flat magnetic material or a plurality of long magnetic material pieces arranged substantially parallel to each other
a tablet portion in which excitation wires and detection wires are arranged alternately in the X direction and the Y direction so as to continuously cover both upper and lower surfaces of a magnetic body formed by overlapping pairs of magnetic materials in a perpendicular direction; and a drive current source that applies an alternating current with a predetermined period to each excitation line in the X and Y directions; signal selection means in the X and Y directions connected to each of the detection lines in the X and Y directions, respectively; a position designating magnetic generator that applies a local magnetic bias and is not connected to any other location; and a position designating magnetic generator that applies a local magnetic bias and is not connected to any part; and Y-direction coordinate values, and by comparing the largest voltage value of each induced voltage in the X-direction or Y-direction with at least one preset threshold value, the magnetic generator for position designation 1. A position detection device comprising: a processing device for determining a Z-direction coordinate value of a specified position. 4. The position detection device according to claim 3, wherein the tablet portion is covered with a non-magnetic metal.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14905384A JPS6128121A (en) | 1984-07-18 | 1984-07-18 | Position detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14905384A JPS6128121A (en) | 1984-07-18 | 1984-07-18 | Position detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6128121A JPS6128121A (en) | 1986-02-07 |
| JPH0210968B2 true JPH0210968B2 (en) | 1990-03-12 |
Family
ID=15466625
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14905384A Granted JPS6128121A (en) | 1984-07-18 | 1984-07-18 | Position detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6128121A (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS53125726A (en) * | 1977-04-11 | 1978-11-02 | Kokusai Denshin Denwa Co Ltd | Code generator |
| JPS5953569B2 (en) * | 1977-06-07 | 1984-12-26 | 日本電信電話株式会社 | tablet input device |
-
1984
- 1984-07-18 JP JP14905384A patent/JPS6128121A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6128121A (en) | 1986-02-07 |
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