JPH0510708A - Position detector - Google Patents

Position detector

Info

Publication number
JPH0510708A
JPH0510708A JP3161298A JP16129891A JPH0510708A JP H0510708 A JPH0510708 A JP H0510708A JP 3161298 A JP3161298 A JP 3161298A JP 16129891 A JP16129891 A JP 16129891A JP H0510708 A JPH0510708 A JP H0510708A
Authority
JP
Japan
Prior art keywords
signal
transducer
magnetic
magnetic element
magnet
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.)
Pending
Application number
JP3161298A
Other languages
Japanese (ja)
Inventor
Kimio Uchida
公雄 内田
Katsuhiko Ariga
勝彦 有賀
Makoto Ozaki
眞 尾崎
Masahiko Miyahara
雅彦 宮原
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.)
Denso Corp
Original Assignee
NipponDenso Co 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 NipponDenso Co Ltd filed Critical NipponDenso Co Ltd
Priority to JP3161298A priority Critical patent/JPH0510708A/en
Publication of JPH0510708A publication Critical patent/JPH0510708A/en
Pending legal-status Critical Current

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  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)

Abstract

PURPOSE:To provide a position detector at which a linear sphere usable for position detection is made wide. CONSTITUTION:At a rotation position detector, a transducer 1 having magnetic resistance elements 11, 12, 13 generating output voltages V11, V12, V13 that are according to the rotation positions of permanent magnets and the permanent magnets rotating at positions opposite to the magnetic resistance elements 11, 12, 13 are equipped. In addition, an operation circuit 3 which superimposes output voltages V12, V13 that are correction signals on the output voltage V11 that is a basic signal, and realizes linearization between the minimum and maximum of the output voltage V11, is equipped.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、非接触式の位置検出装
置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a non-contact type position detecting device.

【0002】[0002]

【従来の技術】図6に示すように、磁気素子400を、
中心421を中心に回転する磁界420中に置き、磁気
素子400と磁石との回転位置を求める位置検出装置が
知られている。
2. Description of the Related Art As shown in FIG.
There is known a position detecting device that is placed in a magnetic field 420 that rotates around a center 421 to obtain the rotational positions of the magnetic element 400 and the magnet.

【0003】[0003]

【発明が解決しようとする課題】しかるに、直線性±3
%F,Sを示す直線領域は、磁気素子400がホール素
子の場合約70°、磁気抵抗素子の場合は約35°であ
り、直線領域にて位置を検出するようにした上記従来の
位置検出装置は位置検出範囲が狭い、という課題があ
る。本発明の目的は、位置検出に使用できる直線領域を
広くした位置検出装置の提供にある。
However, the linearity ± 3
The linear area indicating% F, S is approximately 70 ° when the magnetic element 400 is a Hall element and approximately 35 ° when the magnetic element 400 is a magnetoresistive element, and the above-mentioned conventional position detection in which the position is detected in the linear area is shown. The device has a problem that the position detection range is narrow. An object of the present invention is to provide a position detection device in which a linear area that can be used for position detection is widened.

【0004】[0004]

【課題を解決するための手段】上記課題を解決する為、
本発明は、磁界強度の変化を受ける磁気素子を有し、前
記磁界強度を電気信号に変換するトランスデューサと、
前記磁気素子に対向する位置に配される磁石と、前記ト
ランスデューサ及び磁石の内、一方を回転させる回転部
材とを備え、前記トランスデューサからの電気信号に基
づき、前記トランスデューサと磁石との相対回転位置を
検出する位置検出装置において、前記トランスデューサ
は、前記相対回転位置に応じた大きさの基本信号が生じ
る基本信号用磁気素子と、前記基本信号を補正する、前
記相対回転位置に応じた大きさの補正信号が生じる補正
信号用磁気素子とを有し、前記補正信号を前記基本信号
に重畳して、前記基本信号の極小〜極大間の直線化を図
る波形整形手段を備えた構成を採用した。
[Means for Solving the Problems] In order to solve the above problems,
The present invention has a magnetic element that receives a change in magnetic field strength, and a transducer that converts the magnetic field strength into an electric signal,
A magnet disposed at a position facing the magnetic element and a rotating member that rotates one of the transducer and the magnet are provided, and a relative rotational position between the transducer and the magnet is determined based on an electric signal from the transducer. In the position detecting device for detecting, the transducer is a basic signal magnetic element for generating a basic signal having a size corresponding to the relative rotational position, and a correction having a size corresponding to the relative rotational position for correcting the basic signal. A magnetic signal shaping magnetic element for generating a signal is provided, and the correction signal is superimposed on the basic signal to provide a waveform shaping means for linearizing the minimum and maximum of the basic signal.

【0005】[0005]

【作用】回転部材により、トランスデューサまたは磁石
が回転すると、基本信号用磁気素子には、トランスデュ
ーサと磁石との相対回転位置に応じて波状に変化する基
本信号が生じ、補正信号用磁気素子には、相対回転位置
に応じて波状に変化する補正信号が生じる。波形整形手
段は、補正信号を基本信号に重畳し、基本信号の極小〜
極大間の波形を直線化する。
When the transducer or the magnet is rotated by the rotating member, the basic signal magnetic element produces a basic signal which changes in a wave shape in accordance with the relative rotational position of the transducer and the magnet, and the correction signal magnetic element is A correction signal that changes in a wave shape according to the relative rotational position is generated. The waveform shaping means superimposes the correction signal on the basic signal to minimize the basic signal.
Linearize the waveform between maxima.

【0006】[0006]

【発明の効果】基本信号の極小〜極大間の波形が直線化
されるので、トランスデューサと磁石との相対回転位置
を検出するのに使用できる直線領域が広くなる。
Since the waveform between the minimum and maximum of the basic signal is linearized, the linear region that can be used to detect the relative rotational position between the transducer and the magnet is widened.

【0007】[0007]

【実施例】本発明の一実施例を図1〜図4に基づいて説
明する。回転位置検出装置は、図1および図2に示すご
とく、磁気抵抗素子11、12、13(薄膜のNi- C
o強磁性合金)を有するトランスデューサ1と、磁気抵
抗素子11、12、13に対向して位置する永久磁石2
と、演算回路3と、前記永久磁石2を回転させるロータ
4とを備える。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described with reference to FIGS. As shown in FIGS. 1 and 2, the rotational position detecting device includes magnetoresistive elements 11, 12, and 13 (thin film Ni-C).
Transducer 1 having a (ferromagnetic alloy), and a permanent magnet 2 located opposite to the magnetoresistive elements 11, 12, and 13.
A computing circuit 3 and a rotor 4 for rotating the permanent magnet 2.

【0008】トランスデューサ1は、素子短手方向と磁
界方向との鎖交角度θの変化に拠り電気抵抗値が増減す
る磁気抵抗素子11、12、13と、これら素子の抵抗
値変化を電圧変化として取り出す為の定電流源14とか
らなる。磁気抵抗素子11は、基本信号用磁気素子であ
り、図3に示す様に、基板取付部材100に固着された
絶縁基板110上に、蒸着およびホトエッチング技術
(他の素子も同様)により櫛形状(折返し回数は2回)
に膜付けされ、永久磁石2との回転位置に応じた大きさ
の出力電圧V11を発生する。磁気抵抗素子12は、補正
信号用磁気素子であり、長手方向の長さが磁気抵抗素子
11よりやや短くされ、磁気抵抗素子11と平行に、櫛
形状(折返し回数は1回)に膜付けされている。磁気抵
抗素子13は、補正信号用磁気素子であり、長手方向の
長さが磁気抵抗素子12よりやや短くされ、磁気抵抗素
子11、12と45°の角度を付けて、櫛形状(折返し
回数は1回)に膜付けされている。ここで、各磁気抵抗
素子11ないし13の折返しは、上記回数に限定される
ものではない。
The transducer 1 includes magnetoresistive elements 11, 12 and 13 whose electric resistance values increase and decrease due to a change in the interlinking angle θ between the element short-side direction and the magnetic field direction, and the resistance value change of these elements as a voltage change. And a constant current source 14 for taking out. The magnetoresistive element 11 is a basic signal magnetic element, and as shown in FIG. 3, is formed into a comb shape on the insulating substrate 110 fixed to the substrate mounting member 100 by vapor deposition and photoetching techniques (similar to other elements). (Twice the number of turns)
And an output voltage V 11 having a magnitude corresponding to the rotational position of the permanent magnet 2 is generated. The magnetoresistive element 12 is a magnetic element for correction signal, has a length in the longitudinal direction slightly shorter than that of the magnetoresistive element 11, and is filmed in parallel with the magnetoresistive element 11 in a comb shape (the number of folding is once). ing. The magnetoresistive element 13 is a magnetic element for a correction signal, has a length in the longitudinal direction slightly shorter than that of the magnetoresistive element 12, and forms an angle of 45 ° with the magnetoresistive elements 11 and 12, and has a comb shape (the number of folding times is Once). Here, the folding back of each of the magnetoresistive elements 11 to 13 is not limited to the above number.

【0009】永久磁石2(矩形柱状)は、ハウジング
(非磁性体)200に枢着されたロータ4の図示上部中
央に固定され、平行な均一磁界で満たされる磁気抵抗素
子11、12、13と平行状態を保持しロータ4ととも
に回転する。なお、この永久磁石2は、間隔21を隔て
て位置する磁気抵抗素子11、12、13に作用する回
転磁界の強度が、磁気抵抗素子11、12、13の飽和
磁界以上となる様な強力磁石である。
The permanent magnet 2 (rectangular columnar shape) is fixed to the center of the upper portion of the rotor 4 pivotally mounted on the housing (non-magnetic body) 200 in the figure and is filled with a parallel uniform magnetic field. The parallel state is maintained and the rotor 4 rotates together. The permanent magnet 2 is a strong magnet such that the strength of the rotating magnetic field acting on the magnetoresistive elements 11, 12, 13 located at a distance 21 is equal to or higher than the saturation magnetic field of the magnetoresistive elements 11, 12, 13. Is.

【0010】演算回路3は、オペアンプ301、抵抗3
02、303からなり、出力電圧V 11を1倍に増幅して
出力信号V’11を得る緩衝増幅回路30と、コンデンサ
311、312を備え出力電圧V12、V13の中心値を一
定に調節するオフセット調整部31と、FET321、
抵抗322、323、オペアンプ324を備え位相が互
いに45°異なる出力電圧V12、V13を乗算して半周期
の波形に変換する半周期発生部32と、抵抗331、3
32、333、334、オペアンプ335を備え半周期
の波形に変換した補正信号Vhと出力信号V’11とを加
算し出力信号V out を出力する加算部33とを備える。
The arithmetic circuit 3 includes an operational amplifier 301 and a resistor 3.
02, 303, output voltage V 11Amplifies
Output signal V '11And a buffer amplifier circuit 30 for obtaining
Output voltage V with 311 and 31212, V13The central value of
An offset adjustment unit 31 for constant adjustment, an FET 321,
The resistors 322 and 323 and the operational amplifier 324 are provided so that the phases are the same.
Output voltage V differing by 45 °12, V13Half cycle by multiplying by
Half-cycle generating section 32 for converting into a waveform of
Half cycle with 32, 333, 334 and operational amplifier 335
Correction signal Vh and output signal V ′11And add
Output signal V outAnd an adding unit 33 that outputs

【0011】つぎに、回転位置検出装置の作動を説明す
る。ロータ4が回転すると、永久磁石2と磁気抵抗素子
11、12、13との位置関係が変化し、磁気抵抗素子
11、12、13が受ける磁界強度が変化する。磁気抵
抗素子11、12、13の両端には、以下の式で示され
る出力電圧V11、V12、V13が発生する。但し、R11
12、R13は磁気抵抗素子11、12、13の抵抗値、
θは各磁気抵抗素子11、12、13の短手方向と磁界
方向との鎖交角度、Iは定電流源14より各磁気抵抗素
子11、12、13に流れる定電流、(‖)、(⊥)は
各磁気抵抗素子11、12、13の長手方向(電流の流
れる方向)と磁界方向との位置関係を示す。但し、
(‖)、(⊥)は、位置関係がそれぞれ、平行、垂直で
あることを示す。 V11=R11(⊥)・SIN2 θ+R11(‖)・COS2
θ =A11・COS2θ+B11 なお、A11=〔{R11(‖)−R11(⊥)}/2〕×I B11=〔{R11(‖)+R11(⊥)}/2〕×I V12=R12(⊥)・SIN2 θ+R12(‖)・COS2
θ =A12・COS2θ+B12 なお、A12=〔{R12(‖)−R12(⊥)}/2〕×I B12=〔{R12(‖)+R12(⊥)}/2〕×I V13=R13(‖)・SIN2 (θ−45°) +R13(⊥)・COS2 (θ−45°) =A13・COS2(θ−45°)+B13 なお、A13=〔{R13(‖)−R13(⊥)}/2〕×I B13=〔{R13(‖)+R13(⊥)}/2〕×I オフセット調整部31は、交流信号のみ通すコンデンサ
311、312で構成されているため、実定数B12、B
13はゼロとなり、半周期発生部32のFET321のド
レイン、ゲートには以下の式で示される電圧V’12
V’13が印加される。 V’12=A12・COS2θ V’13=A13・COS2(θ−45°) 半周期発生部32は、電圧V’12と電圧V’13とを乗算
し、以下の式で示される半周期の補正信号Vhを得る。 Vh=A12・COS2θ×A13・COS2(θ−45
°) =A12・A13/2×SIN4θ 加算部33は、出力信号V’11と補正信号Vhとを合成
し、以下の式で示される極小〜極大間の直線化を図った
出力信号Vout を出力する。 Vout =V11+Vh =(A11・COS2θ+B11)+(A12・A13/2)×
SIN4θ
Next, the operation of the rotational position detecting device will be described. When the rotor 4 rotates, the positional relationship between the permanent magnet 2 and the magnetoresistive elements 11, 12, 13 changes, and the magnetic field strength received by the magnetoresistive elements 11, 12, 13 changes. Output voltages V 11 , V 12 , and V 13 represented by the following equations are generated at both ends of the magnetoresistive elements 11, 12 , and 13 . However, R 11 ,
R 12 and R 13 are resistance values of the magnetoresistive elements 11, 12 , and 13 ,
θ is the interlinking angle between the lateral direction and the magnetic field direction of each of the magnetoresistive elements 11, 12, and 13, I is the constant current flowing from the constant current source 14 to each of the magnetoresistive elements 11, 12, and 13, (‖), ( ⊥) indicates the positional relationship between the longitudinal direction (current flowing direction) of each of the magnetoresistive elements 11, 12, 13 and the magnetic field direction. However,
(‖) And (⊥) indicate that the positional relationships are parallel and vertical, respectively. V 11 = R 11 (⊥) ・ SIN 2 θ + R 11 (‖) ・ COS 2
θ = A 11 · COS 2 θ + B 11 A 11 = [{R 11 (‖) -R 11 (⊥)} / 2] × I B 11 = [{R 11 (‖) + R 11 (⊥)} / 2] × IV 12 = R 12 (⊥) ・ SIN 2 θ + R 12 (‖) ・ COS 2
θ = A 12 · COS 2 θ + B 12 A 12 = [{R 12 (‖) -R 12 (⊥)} / 2] × I B 12 = [{R 12 (‖) + R 12 (⊥)} / 2] × IV 13 = R 13 (‖) · SIN 2 (θ−45 °) + R 13 (⊥) · COS 2 (θ−45 °) = A 13 · COS 2 (θ−45 °) + B 13 Note that A 13 = [{R 13 (‖) -R 13 (⊥)} / 2] × I B 13 = [{R 13 (‖) + R 13 (⊥)} / 2] × I The offset adjustment unit 31 is an AC signal only. Since it is composed of passing capacitors 311, 312, the real constants B 12 , B
13 becomes zero, the voltage V '12 drains the FET321 half cycle generation unit 32, to the gate of the following formula,
V '13 is applied. V ′ 12 = A 12 · COS 2 θ V ′ 13 = A 13 · COS 2 (θ−45 °) The half-cycle generator 32 multiplies the voltage V ′ 12 and the voltage V ′ 13 by a half represented by the following formula. A cycle correction signal Vh is obtained. Vh = A 12 · COS 2 θ × A 13 · COS 2 (θ-45
°) = A 12 · A 13 /2 × SIN4θ addition section 33, the output signal V '11 and the correction signal and Vh are synthesized and output signal V which attained linearization between minimum-maximum of the following formula Output out . V out = V 11 + Vh = (A 11 · COS2θ + B 11) + (A 12 · A 13/2) ×
SIN4θ

【0012】つぎに、回転位置検出装置の作用効果を説
明する。 (ア)出力信号Vout は、図4に示す様に極小〜極大間
の直線化が図られ、直線性±3%F,Sを示す直線領域
が従来の約35°から90°以上に拡大した。 (イ)磁気抵抗素子11と同位相の磁気抵抗素子12の
出力電圧V12、および45°位相をずらした磁気抵抗素
子13の出力電圧V13を利用して補正信号Vhを生成す
る構成であるので演算回路3が簡単なもので済む。 (ウ)磁気抵抗素子11、12、13を固定し、永久磁
石2を回転させる構成であるので、出力電圧V11
12、V13の処理性に優れる。 (エ)磁気抵抗素子11、12、13は、飽和磁界中で
動作するので、鎖交角度θに関連しない磁界の強度変化
や回転方向以外の位置変動の影響を受けない。
Next, the function and effect of the rotational position detecting device will be described. (A) The output signal V out is linearized between the minimum and maximum as shown in FIG. 4, and the linear region showing the linearity ± 3% F, S is expanded from the conventional 35 ° to 90 ° or more. did. (B) is a configuration for generating a correction signal Vh using the output voltage V 13 of the magnetoresistive element 13 shifted output voltage V 12, and 45 ° phase of the magnetoresistive element 11 in phase magnetoresistive element 12 of Therefore, the arithmetic circuit 3 can be simple. (C) Since the magnetic resistance elements 11, 12 and 13 are fixed and the permanent magnet 2 is rotated, the output voltage V 11 ,
Excellent processability for V 12 and V 13 . (D) Since the magnetoresistive elements 11, 12 and 13 operate in a saturated magnetic field, they are not affected by changes in magnetic field strength unrelated to the interlinkage angle θ and position variations other than the rotation direction.

【0013】本発明は、上記実施例以外に、つぎの実施
態様を含む。 a.磁束の集中、均一化を図る為、図5に示す様に、永
久磁石2と、磁路を形成するための磁性体腕部22、2
3とを設ける構成にしても良い。 b.磁気素子は、本明細書中では、ホール素子も含む。 c.回転側に磁気素子を配し、磁石を固定する構成であ
っても良い。なお、この場合、ブラシ等で波形整形手段
と導通させる必要がある。 d.磁石は円盤状の永久磁石であっても良い。 また、電磁石であっても良い。なお、回転側が電磁石の
場合、ブラシ等で電源を供給する必要がある。 e.トランスデューサに定電圧源を組み込み、磁界強度
の変化を電流変化に変換しても良い。
The present invention includes the following embodiments in addition to the above embodiments. a. In order to concentrate and equalize the magnetic flux, as shown in FIG. 5, the permanent magnet 2 and the magnetic material arm portions 22 and 2 for forming the magnetic path are formed.
3 may be provided. b. The magnetic element also includes a Hall element in the present specification. c. The magnetic element may be arranged on the rotating side and the magnet may be fixed. In this case, it is necessary to connect the waveform shaping means with a brush or the like. d. The magnet may be a disk-shaped permanent magnet. It may also be an electromagnet. When the rotating side is an electromagnet, it is necessary to supply power with a brush or the like. e. A constant voltage source may be incorporated in the transducer to convert a change in magnetic field strength into a change in current.

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

【図1】本発明の一実施例に係る回転位置検出装置の電
気回路図である。
FIG. 1 is an electric circuit diagram of a rotational position detecting device according to an embodiment of the present invention.

【図2】本発明の一実施例に係る回転位置検出装置の構
造説明図である。
FIG. 2 is a structural explanatory view of a rotational position detecting device according to an embodiment of the present invention.

【図3】(a)はその装置における磁気抵抗素子の形成
状態、(b)はそれら素子の抵抗値変化を示す説明図で
ある。
FIG. 3A is an explanatory diagram showing a formation state of magnetoresistive elements in the apparatus, and FIG. 3B is a diagram showing changes in resistance values of the elements.

【図4】出力電圧V11、出力信号Vout を示すグラフで
ある。
FIG. 4 is a graph showing an output voltage V 11 and an output signal V out .

【図5】本発明の他の実施例に係る回転位置検出装置の
構造説明図である。
FIG. 5 is a structural explanatory view of a rotational position detecting device according to another embodiment of the present invention.

【図6】(a)〜(c)は従来技術を説明する為の図で
あって、(a)は磁気素子を回転する磁界中に置いたと
ころを示す説明図、(b)は磁気素子がホール素子であ
る場合の鎖交角度θ’とホール素子出力との関係を示す
グラフ、(c)は磁気素子が磁気抵抗素子である場合の
鎖交角度θと磁気抵抗素子出力との関係を示すグラフで
ある。
6 (a) to 6 (c) are views for explaining a conventional technique, FIG. 6 (a) is an explanatory view showing a magnetic element placed in a rotating magnetic field, and FIG. 6 (b) is a magnetic element. Is a Hall element, a graph showing the relationship between the interlinkage angle θ ′ and the Hall element output, and (c) shows the relationship between the interlinkage angle θ and the magnetoresistive element output when the magnetic element is a magnetoresistive element. It is a graph shown.

【符号の説明】[Explanation of symbols]

1 トランスデューサ 2 永久磁石(磁石) 3 演算回路(波形整形手段) 4 ロータ(回転部材) 11 磁気抵抗素子(基本信号用磁気素子) 12、13 磁気抵抗素子(補正信号用磁気素子) V11 出力電圧(基本信号) V12、V13 出力電圧(補正信号)DESCRIPTION OF SYMBOLS 1 Transducer 2 Permanent magnet (magnet) 3 Calculation circuit (waveform shaping means) 4 Rotor (rotating member) 11 Magnetoresistive element (magnetic element for basic signal) 12, 13 Magnetoresistive element (magnetic element for correction signal) V 11 Output voltage (Basic signal) V 12 , V 13 output voltage (correction signal)

───────────────────────────────────────────────────── フロントページの続き (72)発明者 宮原 雅彦 愛知県刈谷市昭和町1丁目1番地 日本電 装株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Masahiko Miyahara 1-1, Showa-cho, Kariya city, Aichi Nihon Denso Co., Ltd.

Claims (1)

【特許請求の範囲】 【請求項1】 磁界強度の変化を受ける磁気素子を有
し、前記磁界強度を電気信号に変換するトランスデュー
サと、 前記磁気素子に対向する位置に配される磁石と、 前記トランスデューサ及び磁石の内、一方を回転させる
回転部材とを備え、前記トランスデューサからの電気信
号に基づき、前記トランスデューサと磁石との相対回転
位置を検出する位置検出装置において、 前記トランスデューサは、前記相対回転位置に応じた大
きさの基本信号が生じる基本信号用磁気素子と、前記基
本信号を補正する、前記相対回転位置に応じた大きさの
補正信号が生じる補正信号用磁気素子とを有し、 前記補正信号を前記基本信号に重畳して、前記基本信号
の極小〜極大間の直線化を図る波形整形手段を備えたこ
とを特徴とする位置検出装置。
Claim: What is claimed is: 1. A transducer having a magnetic element that receives a change in magnetic field strength, converting the magnetic field strength into an electric signal, a magnet arranged at a position facing the magnetic element, A position detection device that includes a rotating member that rotates one of a transducer and a magnet, and detects a relative rotational position between the transducer and the magnet based on an electric signal from the transducer, wherein the transducer is the relative rotational position. A basic signal magnetic element that generates a basic signal having a magnitude corresponding to the correction signal, and a correction signal magnetic element that corrects the basic signal and that generates a correction signal having a magnitude corresponding to the relative rotational position. A position characterized by including a waveform shaping means for superimposing a signal on the basic signal to linearize the minimum and maximum of the basic signal. Detection device.
JP3161298A 1991-07-02 1991-07-02 Position detector Pending JPH0510708A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3161298A JPH0510708A (en) 1991-07-02 1991-07-02 Position detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3161298A JPH0510708A (en) 1991-07-02 1991-07-02 Position detector

Publications (1)

Publication Number Publication Date
JPH0510708A true JPH0510708A (en) 1993-01-19

Family

ID=15732456

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3161298A Pending JPH0510708A (en) 1991-07-02 1991-07-02 Position detector

Country Status (1)

Country Link
JP (1) JPH0510708A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012086658A (en) * 2010-10-19 2012-05-10 Bosch Corp Position detector of change lever, change lever unit having the same, and position detection method of change lever

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012086658A (en) * 2010-10-19 2012-05-10 Bosch Corp Position detector of change lever, change lever unit having the same, and position detection method of change lever

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