JPH10288523A - Moving body azimuth detector - Google Patents

Moving body azimuth detector

Info

Publication number
JPH10288523A
JPH10288523A JP9750797A JP9750797A JPH10288523A JP H10288523 A JPH10288523 A JP H10288523A JP 9750797 A JP9750797 A JP 9750797A JP 9750797 A JP9750797 A JP 9750797A JP H10288523 A JPH10288523 A JP H10288523A
Authority
JP
Japan
Prior art keywords
azimuth
geomagnetic
moving body
sensor
angular velocity
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
JP9750797A
Other languages
Japanese (ja)
Inventor
Satoshi Saito
聡 斎藤
Norihiro Ashizuka
紀尋 芦塚
Toshihiko Ishikawa
俊彦 石川
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.)
Hitachi Cable Ltd
Original Assignee
Hitachi Cable 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 Hitachi Cable Ltd filed Critical Hitachi Cable Ltd
Priority to JP9750797A priority Critical patent/JPH10288523A/en
Publication of JPH10288523A publication Critical patent/JPH10288523A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To minimize the influence of disturbance and reduce the accumulation of errors by composing the geomagnetic azimuth from a geomagnetic azimuth detecting means with the rotating angle from a rotating angle detecting means in a frequency area to determine the azimuth of a moving body. SOLUTION: This moving body azimuth detector has a geomagnetic sensor 1 constituting geomagnetic azimuth detecting means, an optical fiber gyro (angle speed sensor) 2 constituting rotating angle detecting means, and a computer 3 constituting azimuth composing means. The computer 3 combines the change portions in a fixed time of the azimuth and angle by the respective sensor in a frequency area when the azimuth of a moving body is calculated. At this time, the rotating angle and the geomagnetic azimuth are differently weighted depending on frequency, respectively, such that the angle sensor 2 is weighted in high frequency area, and the geomagnetic sensor 1 is weighted in low frequency area, and outputs the resulting combined value as the azimuth of the moving body. Further, the computer 3 has also the function of changing this ratio of weighting.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、地磁気検出による
方位と回転角速度検出による回転角度とを併用した移動
体方位検出装置に係り、特に、外乱の影響が少なく、誤
差の累積が少ない移動体方位検出装置に関するものであ
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a moving body direction detecting apparatus using both a direction based on geomagnetism detection and a rotation angle based on rotational angular velocity detection, and in particular, a moving body direction with less influence of disturbance and less error accumulation. The present invention relates to a detection device.

【0002】[0002]

【従来の技術】車両の中で使用される方位計や車載用の
走行軌跡表示に用いる移動体方位検出装置として、従
来、車体の前後方向及び左右方向の地磁気成分を出力す
る地磁気センサを利用したものや、この地磁気センサに
地磁気の影響を受けない角速度センサを組み合わせたも
のがある。
2. Description of the Related Art Conventionally, a geomagnetic sensor that outputs geomagnetic components in the front-rear direction and the left-right direction of a vehicle body has been used as a compass or a moving body direction detecting device used for displaying a traveling locus for a vehicle or a vehicle. There is a sensor that combines a geomagnetic sensor with an angular velocity sensor that is not affected by geomagnetism.

【0003】後者の例として、一定の時間内に発生した
地磁気方位(絶対方位)の変化分と、同じく角速度セン
サより得た角度の変化分とを、それぞれ実験で求めた判
定値と比較し、どちらの変化分を採用するかを判定する
ものがある。
[0003] As an example of the latter, a change in the geomagnetic azimuth (absolute azimuth) generated within a fixed time and a change in the angle similarly obtained from the angular velocity sensor are compared with respective judgment values obtained by experiments. Some of them determine which change is to be adopted.

【0004】[0004]

【発明が解決しようとする課題】地磁気センサのみを利
用する方式は、検出した地磁気より絶対方位を演算し、
車体の進行方向の方位を求めるものであるが、踏切、橋
などを通過するときや、近くを着磁したトラックなどが
走行したときに生じる外乱磁界の影響を受けやすく、こ
のような外乱の影響により、検出した方位に誤差が生じ
る。
The method using only the geomagnetic sensor calculates the absolute azimuth from the detected geomagnetism,
The azimuth of the traveling direction of the vehicle body is obtained.However, it is susceptible to the disturbance magnetic field generated when passing a railroad crossing, a bridge, or when a nearby magnetized truck travels. This causes an error in the detected orientation.

【0005】地磁気センサと角速度センサとを組み合わ
せ、それぞれのセンサによる方位の変化分を判定値と比
較する方式では、車両が急カーブなどの急激な角度変化
を伴う軌跡を走行した場合に角速度センサの誤差が累積
してしまう。
In a system in which a terrestrial magnetism sensor and an angular velocity sensor are combined, and the change in the azimuth of each sensor is compared with a determination value, when the vehicle travels on a locus such as a sharp curve with a sharp angle change, the angular velocity sensor is used. Errors accumulate.

【0006】また、地磁気センサと角速度センサとを組
み合わせた方式では、角速度センサがドリフトしてしま
うと、誤差は時間とともに累積してしまう。このため、
長時間の運用の場合、低ドリフトな角速度センサが必要
となり、低ドリフトな角速度センサは高価であるから、
コスト面でも実用的でない。
[0006] In a system in which a geomagnetic sensor and an angular velocity sensor are combined, if the angular velocity sensor drifts, errors accumulate over time. For this reason,
For long-term operation, a low-drift angular velocity sensor is required, and a low-drift angular velocity sensor is expensive.
It is not practical in terms of cost.

【0007】そこで、本発明の目的は、上記課題を解決
し、外乱の影響が少なく、誤差の累積が少ない移動体方
位検出装置を提供することにある。
SUMMARY OF THE INVENTION It is an object of the present invention to solve the above problems and to provide a moving body direction detecting device which is less affected by disturbance and has less accumulated errors.

【0008】[0008]

【課題を解決するための手段】上記目的を達成するため
に本発明は、角速度センサにより移動体の回転角速度を
計測し、この回転角速度を時間で積分して回転角度を求
める回転角度検出手段と、地磁気センサにより移動体の
進行方向を検出する地磁気方位検出手段と、この地磁気
方位と上記回転角度とを周波数領域で合成して移動体の
方位とする方位合成手段とを備えたものである。
SUMMARY OF THE INVENTION In order to achieve the above object, the present invention relates to a rotational angle detecting means for measuring a rotational angular velocity of a moving body by an angular velocity sensor and integrating the rotational angular velocity with time to obtain a rotational angle. A geomagnetic azimuth detecting means for detecting the traveling direction of the moving object by a geomagnetic sensor, and an azimuth synthesizing means for synthesizing the geomagnetic azimuth and the rotation angle in the frequency domain to obtain the azimuth of the moving object.

【0009】上記方位合成手段は、上記回転角度と上記
地磁気方位とにそれぞれ周波数によって異なる重みを付
けて合成してもよい。
The azimuth combining means may combine the rotation angle and the geomagnetic azimuth with different weights depending on frequencies.

【0010】[0010]

【発明の実施の形態】以下、本発明の一実施形態を添付
図面に基づいて詳述する。
An embodiment of the present invention will be described below in detail with reference to the accompanying drawings.

【0011】図1に示されるように、本発明の移動体方
位検出装置は、地磁気方位検出手段を構成する地磁気セ
ンサ1と、回転角度検出手段を構成する光ファイバジャ
イロ(角速度センサ)2と、方位合成手段を構成する計
算機3と、結果を表示する表示器4とを備えている。
As shown in FIG. 1, a moving body direction detecting device according to the present invention includes a geomagnetic sensor 1 constituting geomagnetic direction detecting means, an optical fiber gyro (angular velocity sensor) 2 forming rotational angle detecting means, and The computer includes a computer 3 constituting the azimuth synthesizing means and a display 4 for displaying a result.

【0012】計算機3は、移動体の方位を演算する際、
それぞれのセンサによる方位・角度の一定時間における
変化分を周波数領域において結合させる。このとき高周
波領域では角速度センサ2に重みをおき、低周波領域で
は地磁気センサ1に重みをおくように、回転角度と地磁
気方位とにそれぞれ周波数によって異なる重みを付け、
合わせた値を移動体の方位として出力するようになって
いる。さらに、計算機3は、この重み付けの割合を変化
させる機能を持つ。例えば、地磁気の乱れを検出した場
合には回転角度への重みを大きくして真方位との誤差を
少なくする。
When calculating the azimuth of the moving object, the computer 3
Changes in the azimuth and angle of each sensor over a certain period of time are combined in the frequency domain. At this time, different weights are assigned to the rotation angle and the geomagnetic azimuth depending on the frequency so that the angular velocity sensor 2 is weighted in the high frequency region and the geomagnetic sensor 1 is weighted in the low frequency region.
The combined value is output as the direction of the moving object. Further, the computer 3 has a function of changing the weighting ratio. For example, when the disturbance of the geomagnetism is detected, the weight to the rotation angle is increased to reduce the error from the true azimuth.

【0013】回転角度と地磁気方位との周波数領域にお
ける結合による移動体の方位の算出演算は、次の手順に
よる。
The calculation of the azimuth of the moving object by the coupling between the rotation angle and the geomagnetic azimuth in the frequency domain is performed according to the following procedure.

【0014】(1)ある一定の時間間隔ΔTで地磁気セ
ンサ1及び角速度センサ2からデータを採取する。地磁
気データからは方位を算出し、これを地磁気方位θMi
する。角速度データは積分して角度に変換し、これを回
転角度θGiとする。ただし、添字i(i=0,1,2,
・・)は、データ採取順に付けた番号である。
(1) Data is collected from the geomagnetic sensor 1 and the angular velocity sensor 2 at a certain time interval ΔT. The azimuth is calculated from the terrestrial magnetism data, and this is set as the terrestrial magnetism azimuth θ Mi. The angular velocity data is integrated and converted into an angle, which is defined as a rotation angle θ Gi . Where the subscript i (i = 0, 1, 2,
・ ・) Are numbers assigned in the order of data collection.

【0015】(2)地磁気方位の低周波成分θMi (L)
次の式より算出する。
(2) The low frequency component θ Mi (L) of the geomagnetic azimuth is calculated by the following equation.

【0016】 θMi (L) =k×θMi+(1−k)×θMi-1 (L) ここで、kは係数で、次の式より算出する。Θ Mi (L) = k × θ Mi + (1−k) × θ Mi−1 (L) where k is a coefficient, which is calculated by the following equation.

【0017】 k=(2πfC ΔT)/(1+πfC ΔT) ここで、fC は予め決めておく遮断周波数である。ただ
し、計算機3は、この遮断周波数fC を変化させること
ができる。この遮断周波数fC が高いと地磁気センサ1
の重みが増し、低いと角速度センサ2の重みが増すこと
になる。
K = (2πf C ΔT) / (1 + πf C ΔT) Here, f C is a predetermined cutoff frequency. However, the computer 3 can change the cutoff frequency f C. If the cutoff frequency f C is high, the geomagnetic sensor 1
The weight of the angular velocity sensor 2 increases when the weight of the angular velocity sensor 2 increases.

【0018】(3)回転角度の低周波成分θGi (L) を次
の式より算出する。
(3) The low frequency component θ Gi (L) of the rotation angle is calculated by the following equation.

【0019】 θGi (L) =k×θGi+(1−k)×θGi-1 (L) (4)回転角度の高周波成分θGi (H) を次の式より算出
する。
Θ Gi (L) = k × θ Gi + (1−k) × θ Gi-1 (L) (4) The high frequency component θ Gi (H) of the rotation angle is calculated by the following equation.

【0020】θGi (H) =θGi−θGi (L) (5)移動体の方位θSiを次の式より算出する。Θ Gi (H) = θ Gi −θ Gi (L) (5) The direction θ Si of the moving object is calculated by the following equation.

【0021】θSi=θMi (L) +θGi (H) なお、移動体方位検出装置の立ち上げ時(i=0)には
次のように初期化する。
Θ Si = θ Mi (L) + θ Gi (H) When the moving body direction detecting device is started (i = 0), initialization is performed as follows.

【0022】θMi (L) =θMi θGi (L) =0 図2に、以上の合成式によって得られる出力の周波数特
性を示す。横軸は周波数を表し、縦軸はゲイン(重み)
を表す。図示されるように、低周波領域では地磁気セン
サ1の重みが大きく、磁気センサの特性曲線21で囲ま
れた面積が大きい。高周波領域では角速度センサ2の重
みが大きく、角速度センサの特性曲線22で囲まれた面
積が大きい。また、この2つの領域は図中のある1つの
周波数で分けられている。この周波数が遮断周波数fC
である。遮断周波数fC が高いと磁気センサの特性曲線
21で囲まれた面積が大きくなり、従って、出力におけ
る地磁気センサの重みが大きくなる。遮断周波数fC
低いと角速度センサの特性曲線22で囲まれた面積が大
きくなり、従って、出力における角速度センサの重みが
大きくなる。
Θ Mi (L) = θ Mi θ Gi (L) = 0 FIG. 2 shows the frequency characteristics of the output obtained by the above-described synthesis formula. The horizontal axis represents frequency, and the vertical axis represents gain (weight).
Represents As shown, the weight of the geomagnetic sensor 1 is large in the low frequency region, and the area surrounded by the characteristic curve 21 of the magnetic sensor is large. In the high frequency region, the weight of the angular velocity sensor 2 is large, and the area surrounded by the characteristic curve 22 of the angular velocity sensor is large. These two areas are separated by a certain frequency in the figure. This frequency is the cutoff frequency f C
It is. When the cutoff frequency f C is high, the area surrounded by the characteristic curve 21 of the magnetic sensor increases, and therefore, the weight of the geomagnetic sensor in the output increases. When the cutoff frequency f C is low, the area surrounded by the characteristic curve 22 of the angular velocity sensor increases, and therefore, the weight of the angular velocity sensor in the output increases.

【0023】図3に本発明の移動体方位検出装置の動作
の流れを示す。以下に、その動作を説明する。
FIG. 3 shows a flow of the operation of the moving body direction detecting apparatus of the present invention. The operation will be described below.

【0024】(1)初期設定を行う。即ち、磁気センサ
1の方位(地磁気方位)と角速度センサ2の角度(回転
角度)とのそれぞれ初回分を読み込み、出力方位θS0
は、その初回分の地磁気方位を代入する。
(1) Initial setting is performed. That is, the first azimuth of the magnetic sensor 1 (geomagnetic azimuth) and the angle of the angular velocity sensor 2 (rotation angle) are read, and the first terrestrial magnetic azimuth is substituted for the output azimuth θ S0 .

【0025】(2)ΔT秒待機する。(2) Wait for ΔT seconds.

【0026】(3)前記ΔT秒待機後の地磁気方位θMi
と回転角度θGiとを計算機3に読み込む。
(3) Geomagnetic orientation θ Mi after waiting for ΔT seconds
And the rotation angle θ Gi are read into the computer 3.

【0027】(4)ΔT秒間の地磁気方位の変化分Δθ
M を演算する。
(4) Change Δθ in geomagnetic azimuth during ΔT seconds
Calculate M.

【0028】(5)ΔT秒間の回転角度の変化分ΔθG
を演算する。
(5) Change Δθ G in rotation angle during ΔT seconds
Is calculated.

【0029】(6)ΔθM とΔθG との絶対差をとり、
この値としきい値A(例えば0.5度)とを比較する。
絶対差がしきい値Aより大きければ地磁気に乱れが生じ
ていると判断する。この判断に基づき、遮断周波数fC
を低くして地磁気センサの重みを小さくする。
(6) By taking the absolute difference between Δθ M and Δθ G ,
This value is compared with a threshold value A (for example, 0.5 degrees).
If the absolute difference is larger than the threshold value A, it is determined that the geomagnetism is disturbed. Based on this determination, the cutoff frequency f C
And the weight of the geomagnetic sensor is reduced.

【0030】(7)地磁気方位θMiと前回の出力方位θ
Si-1との絶対差をとり、この値としきい値B(例えば
1.0度)とを比較する。絶対差がしきい値Bより大き
ければ、車両が回転中であると判断する。この判断に基
づき、遮断周波数fC を低くして回転角度検出精度のよ
い角速度センサの重みを大きくする。
(7) Geomagnetic Direction θ Mi and Previous Output Direction θ
The absolute difference from Si-1 is obtained, and this value is compared with a threshold value B (for example, 1.0 degree). If the absolute difference is larger than the threshold value B, it is determined that the vehicle is rotating. Based on this determination, the cutoff frequency f C is lowered, and the weight of the angular velocity sensor with high rotation angle detection accuracy is increased.

【0031】(8)以上より決定した遮断周波数fC
用いて地磁気方位θMiと回転角度θGiとを合成し、これ
を今回の出力方位θSiとする。
(8) The terrestrial magnetic orientation θ Mi and the rotation angle θ Gi are synthesized using the cutoff frequency f C determined from the above, and this is set as the current output orientation θ Si .

【0032】(9)出力方位θSiを表示器に出力する。
以後、(3)以下を繰り返す。
(9) Output the output orientation θ Si to the display.
Thereafter, the following (3) is repeated.

【0033】本実施形態では、角速度センサとして光フ
ァイバジャイロを用いたが、このような光学式角速度セ
ンサの代わりに機械式角速度センサ(機械式ジャイロ、
振動式ジャイロ)を用いてもよい。
In this embodiment, an optical fiber gyro is used as the angular velocity sensor. However, instead of such an optical angular velocity sensor, a mechanical angular velocity sensor (mechanical gyro,
A vibration gyro may be used.

【0034】本発明の移動体方位検出装置を車両に搭載
することで、地磁気の乱れの影響を受けないカーナビゲ
ーション又はカーロケーションが実現できる。
By mounting the moving body direction detecting device of the present invention on a vehicle, it is possible to realize a car navigation or a car location which is not affected by disturbance of geomagnetism.

【0035】[0035]

【発明の効果】本発明は次の如き優れた効果を発揮す
る。
The present invention exhibits the following excellent effects.

【0036】(1)車両に搭載して走行軌跡表示に用い
る際、踏切その他の着磁磁性体に近付いても誤差を生じ
にくい。
(1) When mounted on a vehicle and used for displaying a traveling locus, errors are unlikely to occur even when approaching a railroad crossing or other magnetized magnetic material.

【0037】(2)カーブ走行などで角速度センサが誤
差を生じても、出力方位は地磁気方位によって次第に収
束し、角速度センサの誤差が出力方位に累積することが
ない。
(2) Even if an error occurs in the angular velocity sensor due to running on a curve or the like, the output azimuth gradually converges due to the geomagnetic azimuth, and the error of the angular velocity sensor does not accumulate in the output azimuth.

【0038】(3)角速度センサは低ドリフトなもので
なくても良いので、比較的安価な角速度センサが使用で
き、コスト面で効果がある。
(3) Since the angular velocity sensor does not need to have a low drift, a relatively inexpensive angular velocity sensor can be used, which is cost effective.

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

【図1】本発明の一実施形態を示す移動体方位検出装置
のブロック構成図である。
FIG. 1 is a block diagram of a moving body direction detecting apparatus according to an embodiment of the present invention.

【図2】本発明の周波数領域での合成における周波数特
性図である。
FIG. 2 is a frequency characteristic diagram in the synthesis in the frequency domain according to the present invention.

【図3】本発明の移動体方位検出装置の動作の流れ図で
ある。
FIG. 3 is a flowchart of the operation of the moving body direction detecting device of the present invention.

【符号の説明】[Explanation of symbols]

1 地磁気センサ 2 角速度センサ 3 計算機 1 geomagnetic sensor 2 angular velocity sensor 3 computer

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 角速度センサにより移動体の回転角速度
を計測し、この回転角速度を時間で積分して回転角度を
求める回転角度検出手段と、地磁気センサにより移動体
の進行方向を検出する地磁気方位検出手段と、この地磁
気方位と上記回転角度とを周波数領域で合成して移動体
の方位とする方位合成手段とを備えたことを特徴とする
移動体方位検出装置。
An angular velocity sensor measures a rotational angular velocity of a moving body, integrates the rotational angular velocity with time to determine a rotational angle, and a geomagnetic azimuth detection that detects a traveling direction of the moving body by a geomagnetic sensor. And a azimuth synthesizing means for synthesizing the terrestrial magnetic azimuth and the rotation angle in a frequency domain to obtain an azimuth of the mobile body.
【請求項2】 上記方位合成手段は、上記回転角度と上
記地磁気方位とにそれぞれ周波数によって異なる重みを
付けて合成することを特徴とする請求項1記載の移動体
方位検出装置。
2. The moving body direction detecting device according to claim 1, wherein the direction synthesizing unit combines the rotation angle and the geomagnetic direction with different weights depending on frequencies.
JP9750797A 1997-04-15 1997-04-15 Moving body azimuth detector Pending JPH10288523A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9750797A JPH10288523A (en) 1997-04-15 1997-04-15 Moving body azimuth detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9750797A JPH10288523A (en) 1997-04-15 1997-04-15 Moving body azimuth detector

Publications (1)

Publication Number Publication Date
JPH10288523A true JPH10288523A (en) 1998-10-27

Family

ID=14194180

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9750797A Pending JPH10288523A (en) 1997-04-15 1997-04-15 Moving body azimuth detector

Country Status (1)

Country Link
JP (1) JPH10288523A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012093152A (en) * 2010-10-26 2012-05-17 Aichi Micro Intelligent Corp Magnetic gyroscope
JP2014211324A (en) * 2013-04-17 2014-11-13 キヤノン株式会社 Information processing unit, control method of information processing unit, and program

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012093152A (en) * 2010-10-26 2012-05-17 Aichi Micro Intelligent Corp Magnetic gyroscope
JP2014211324A (en) * 2013-04-17 2014-11-13 キヤノン株式会社 Information processing unit, control method of information processing unit, and program

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