JPH063440A - Apparatus for measuring uneveness of ground surface or the like for missile - Google Patents
Apparatus for measuring uneveness of ground surface or the like for missileInfo
- Publication number
- JPH063440A JPH063440A JP4162977A JP16297792A JPH063440A JP H063440 A JPH063440 A JP H063440A JP 4162977 A JP4162977 A JP 4162977A JP 16297792 A JP16297792 A JP 16297792A JP H063440 A JPH063440 A JP H063440A
- Authority
- JP
- Japan
- Prior art keywords
- ground
- flying object
- missile
- altitude
- measuring
- 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.)
- Granted
Links
- 238000005259 measurement Methods 0.000 abstract description 4
- 238000010586 diagram Methods 0.000 description 6
- 238000000034 method Methods 0.000 description 3
- 230000002159 abnormal effect Effects 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
Landscapes
- Radar Systems Or Details Thereof (AREA)
- Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は飛翔体に取り付けた2個
の高度計の高度出力から飛翔体下の地形、地上構造物、
波浪等、地面あるいは海面の凹凸によるものを分離し、
これらを検出すると同時に飛翔体の絶対高度の変化を精
密に測定する高度測定装置に関わるものである。BACKGROUND OF THE INVENTION The present invention is based on the altitude output of two altimeters attached to a projectile, and determines the terrain under the projectile, the ground structure,
Separation of waves or other irregularities on the ground or sea surface,
The present invention relates to an altitude measuring device that detects these and at the same time accurately measures a change in absolute altitude of a flying object.
【0002】[0002]
【従来の技術】飛翔体の高度を測定する装置としては、
気圧高度計や電波高度計がある。気圧高度計は、飛翔体
下の地面あるいは海面(以後「地面等」という)の凹凸
には影響されにくいが飛翔体周辺の気流の変化に敏感で
あり、飛翔体の上昇中と下降中で同一高度であっても高
度出力が精密には一致しないことがある。また、旋回時
の不整な気流により異常な高度出力が出ることもあり飛
翔体の絶対高度の変化を精密に測定するには問題があ
る。また、電波高度計による高度測定は飛翔体と飛翔体
下の地面等との距離を測定するので飛翔体本体の絶対高
度の変化と飛翔体下の地面等の凹凸とを分離することが
できない。2. Description of the Related Art As a device for measuring the altitude of a flying object,
There are barometric altimeters and radio altimeters. The barometric altimeter is not affected by the unevenness of the ground or the sea surface (hereinafter referred to as "ground, etc.") below the flying object, but it is sensitive to changes in the air flow around the flying object, and is at the same altitude while the flying object is rising and falling. However, the altitude output may not exactly match. In addition, irregular airflow during turning may cause abnormal altitude output, which poses a problem in accurately measuring the change in absolute altitude of the flying object. Further, since the altitude measurement by the radio altimeter measures the distance between the flying body and the ground or the like below the flying body, it is impossible to separate the change in the absolute height of the flying body from the irregularity of the ground or the like below the flying body.
【0003】[0003]
【発明が解決しようとする課題】飛翔体に取り付けた、
ビームを発してその反射を用いて対地高度を測定する高
度計(以後「高度計」という。)の高度出力には、飛翔
体本体の絶対高度の変化に加え、飛翔体下の地面等の凹
凸が含まれている。この2つの情報を分離する方法とし
て飛行状態での飛翔体本体の運動及び姿勢の変化を加速
度計とジャイロとの出力から算出し、これによって高度
計出力を補正することが考えられるが、この方法では装
置が煩雑化し、また、異種の器材の特性の相違のため信
頼しうる結果を得ることが困難である。[Problems to be Solved by the Invention] Attached to a flying object,
The altitude output of the altimeter (hereinafter referred to as "altimeter"), which emits a beam and measures the ground altitude using its reflection, includes not only the change in the absolute altitude of the projectile body, but also irregularities such as the ground below the projectile. Has been. As a method of separating these two pieces of information, it is conceivable to calculate the change in the motion and attitude of the flying body in the flight state from the outputs of the accelerometer and the gyro and correct the altimeter output by this method. The device is complicated and it is difficult to obtain reliable results due to the difference in characteristics of different kinds of equipment.
【0004】本発明は、上記問題点に鑑みて成されたも
のであり、飛翔体の下の地面等の凹凸を精密測定及び飛
翔体の絶対高度の変化の精密測定を行える飛翔体用地面
等凹凸測定装置を提供することを目的としている。The present invention has been made in view of the above problems, and can be used to accurately measure unevenness of the ground or the like under a flying object and to accurately measure changes in absolute altitude of the flying object. It is an object of the present invention to provide an unevenness measuring device.
【0005】[0005]
【課題を解決するための手段】上記目的を達成するた
め、本発明の飛翔体用地面等凹凸測定装置は、請求項1
では、図1に示すように、電波、光波、音波等のビーム
を発し、その反射を用いて対地高度を測定する同一のも
の2個の高度計2,3を、前後方向にそれぞれのビーム
7,8が重なりあわないよう飛翔体1に取り付け、2個
の高度計2,3の高度出力を用いて計算する信号処理機
5により、飛行中に飛翔体1下の地面あるいは海面の凹
凸6と飛翔体1本体の絶対高度の変化を分離可能とする
ことを特徴としている。In order to achieve the above object, an apparatus for measuring unevenness of a ground for a flying object according to the present invention is defined by claim 1.
Then, as shown in FIG. 1, two identical altimeters 2 and 3 which emit beams of radio waves, light waves, sound waves, etc. and measure the altitude with respect to the ground by using their reflection 8 is attached to the flying body 1 so that they do not overlap with each other, and the signal processor 5 that calculates using the altitude output of the two altimeters 2 and 3 makes the flying body 1 and the unevenness 6 of the ground or sea under the flying body 1 in flight. The feature is that the change in absolute height of one body can be separated.
【0006】また、請求項2では、請求項1記載の信号
処理機5には、飛翔体1のピッチ角測定用ジャイロ4の
出力が加えられて計算する構成とすることもできる。In the second aspect, the signal processor 5 according to the first aspect may be configured such that the output of the gyro 4 for measuring the pitch angle of the flying object 1 is added to perform calculation.
【0007】[0007]
【作用】上記構成によれば、飛翔体1から地面あるいは
海面の凹凸6に向けて2個の高度計2,3からは、それ
ぞれビーム7,8が重なりあわないように発せられる。
したがって、ビーム7,8の反射状態を信号処理機5に
より計算することにより、飛翔体1下の地面あるいは海
面の凹凸6、および飛翔体1の絶対高度の変化を分離し
て得ることができる。According to the above structure, the two altimeters 2 and 3 are emitted from the flying body 1 toward the unevenness 6 on the ground or the sea so that the beams 7 and 8 do not overlap with each other.
Therefore, by calculating the reflection state of the beams 7 and 8 by the signal processor 5, it is possible to separately obtain the unevenness 6 of the ground or sea surface under the flying body 1 and the change in the absolute height of the flying body 1.
【0008】また、信号処理機5に対し、さらにピッチ
角測定用ジャイロ4の出力が得られれば、飛翔体1のピ
ッチ角の変化に対応でき、上記機能の精度を向上させる
ことができる。Further, if the output of the pitch angle measuring gyro 4 is further obtained with respect to the signal processor 5, it is possible to cope with the change in the pitch angle of the flying object 1 and improve the accuracy of the above-mentioned function.
【0009】[0009]
【実施例】図1は本発明の飛翔体用地面等凹凸測定装置
の実施例を示す構成図である。図において、1は飛翔
体、2と3はビームを発し、その反射により対地高度を
測定する高度計、4は飛翔体のピッチ運動測定用ジャイ
ロ、5は信号処理機、6は飛翔体下の地面等、7は高度
計2のビーム、8は高度計3のビームである。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a configuration diagram showing an embodiment of the unevenness measuring apparatus for the ground for a flying object of the present invention. In the figure, 1 is a flying object, 2 and 3 are altimeters that measure the altitude of the ground by reflecting the beams, 4 is a gyro for pitch motion measurement of the flying object, 5 is a signal processor, and 6 is the ground below the flying object. Etc., 7 is the beam of altimeter 2 and 8 is the beam of altimeter 3.
【0010】図1のように飛翔体1にその直下方向にビ
ーム7を向けて取り付けた高度計2に加えて、高度計2
の前方にビーム7とビーム8が重ならないように第2の
高度計3を取り付ける。これら、高度計2と高度計3の
ビームの間の角度をθとする。As shown in FIG. 1, in addition to an altimeter 2 attached to a flying body 1 with a beam 7 directed directly below it, an altimeter 2
The second altimeter 3 is attached so that the beams 7 and 8 do not overlap in front of. The angle between the beams of the altimeter 2 and the altimeter 3 is θ.
【0011】次に、図2の原理説明図に示すように、飛
翔体1の飛行方向をx軸に取り、飛翔体1のx軸上の位
置x0での高度計2の高度出力をf1、高度計3の高度
出力をf2とする。凹凸のある面上を飛翔体1が飛行す
る場合、仮想水準面に対し、飛翔体の絶対高度、地面等
の凹凸6をそれぞれx軸上の位置xの関数としてh
(x),g(x)とすると、高度計2の高度出力f1
は、次式で表される。Next, as shown in the principle explanatory view of FIG. 2, the flight direction of the flying object 1 is taken as the x-axis, and the altitude output of the altimeter 2 at the position x0 on the x-axis of the flying object 1 is f1, the altimeter. The altitude output of 3 is f2. When the flying object 1 flies over a surface having irregularities, the absolute height of the flying object, the irregularities 6 such as the ground, etc. are each expressed as a function of the position x on the x-axis with respect to the virtual level surface.
(X) and g (x), the altitude output f1 of the altimeter 2
Is expressed by the following equation.
【0012】[0012]
【数1】 [Equation 1]
【0013】一方、高度計3のビーム8は、次式で表さ
れるx軸上の位置x1の地点から反射する。On the other hand, the beam 8 of the altimeter 3 is reflected from the point of position x1 on the x-axis expressed by the following equation.
【0014】[0014]
【数2】 [Equation 2]
【0015】また、f2は、この地点での地面等の凹凸
g(x1)を用いて次式で表される。Further, f2 is expressed by the following equation using the unevenness g (x1) of the ground or the like at this point.
【0016】[0016]
【数3】 [Equation 3]
【0017】ここで数1と数3からh(x0)を抹消す
ると次式になる。When h (x0) is deleted from the equations 1 and 3, the following equation is obtained.
【0018】[0018]
【数4】 [Equation 4]
【0019】数4の左辺は数2の右辺第2項を微小量と
してg(x1)をテーラー展開し、微小量の1次の展開
まで取るとg(x)のx0での位置xによる微分を用い
て次のように表される。The left side of the equation 4 is obtained by Taylor-expanding g (x1) with the second term on the right side of the equation 2 as a minute amount, and taking the first-order expansion of a minute amount, the derivative of g (x) at the position x at x0. Is expressed as follows.
【0020】[0020]
【数5】 [Equation 5]
【0021】数5を用いて数4を書き直すと次のように
なる。Rewriting equation 4 using equation 5 yields the following.
【0022】[0022]
【数6】 [Equation 6]
【0023】即ち、地面等の凹凸g(x)の位置xによ
る微分が2個の高度出力f1,f2及び既知の量θによ
って表されている。そこで数6の右辺を刻々積分したも
のはg(x)となり、地面等の凹凸そのものである。That is, the differential of the unevenness g (x) of the ground or the like with respect to the position x is represented by two altitude outputs f1 and f2 and a known amount θ. Then, the product of the right side of Equation 6 is g (x), which is the unevenness of the ground itself.
【0024】したがって図3に示すように、信号処理機
5は、上記数6に基づき得られたg(x)により、地面
等の凹凸を得る。また、信号処理機5は、このg(x)
と数1を用いてh(x)を得るための演算を行って飛翔
体1の絶対高度h(x)を得ることができる。Therefore, as shown in FIG. 3, the signal processor 5 obtains the unevenness of the ground or the like by using g (x) obtained based on the above equation (6). Further, the signal processor 5 uses this g (x)
The absolute height h (x) of the flying object 1 can be obtained by performing a calculation to obtain h (x) by using Equation 1 and
【0025】次に、図4は、本発明の第2実施例を示す
原理説明図である。図4に示すように、この実施例で
は、前記第1実施例の構成とともに、ジャイロ4を用い
る。ジャイロ4により、飛翔体1の姿勢の変化、特にピ
ッチ運動によるビームの方向変化の補正のためにピッチ
角出力pが得られる。図4に示したように飛翔体1のピ
ッチ角がpの時、飛翔体1のx軸上の位置をx0、高度
計2のビーム7が地面等に当たる点のx軸上の位置をx
1、高度計3のビーム8が地面等に当たる点のx軸上の
位置をx2とするとx1は次式で表される。Next, FIG. 4 is a principle explanatory view showing a second embodiment of the present invention. As shown in FIG. 4, in this embodiment, a gyro 4 is used in addition to the structure of the first embodiment. The gyro 4 obtains the pitch angle output p for correcting the change in the attitude of the flying object 1, especially the change in the beam direction due to the pitch movement. As shown in FIG. 4, when the pitch angle of the flying object 1 is p, the position on the x axis of the flying object 1 is x0, and the position on the x axis of the point where the beam 7 of the altimeter 2 hits the ground or the like is x.
1. If x2 is the position on the x-axis of the point where the beam 8 of the altimeter 3 hits the ground or the like, x1 is expressed by the following equation.
【0026】[0026]
【数7】 [Equation 7]
【0027】また、x2は次式で表される。Further, x2 is expressed by the following equation.
【0028】[0028]
【数8】 [Equation 8]
【0029】数7と数8からx0を消去すると次式が得
られる。Eliminating x0 from the equations 7 and 8 gives the following equation.
【0030】[0030]
【数9】 [Equation 9]
【0031】高度計2と高度計3の高度出力f1、f2
の間には次の数10の関係が成り立つ。Altimeter outputs f1 and f2 of altimeter 2 and altimeter 3
The following relational expression 10 holds.
【0032】[0032]
【数10】 [Equation 10]
【0033】後の手段は、数9の右辺第2項と第3項を
微小量としてg(x)のx1での位置微分を用いてpを
含まない場合と同様にして数11が得られ、これを積分
することによりg(x)を求めることができる。尚、信
号処理機5は、図5に示される演算で上記数11に基づ
き得られたg(x)により、地面等の凹凸を得る。In the latter means, the second term and the third term on the right side of the equation 9 are used as minute amounts and the position differential of g (x) with respect to x1 is used to obtain the equation 11 in the same manner as in the case where p is not included. , G (x) can be obtained by integrating this. The signal processor 5 obtains the unevenness of the ground or the like from g (x) obtained by the calculation shown in FIG.
【0034】[0034]
【数11】 [Equation 11]
【0035】以上のようにして2個の高度計2,3の高
度出力とジャイロ4のピッチ角出力を信号処理機5で計
算処理することにより飛行中の飛翔体1にあって、その
絶対高度の変化を測定すると同時に、飛翔体1下の地面
等の凹凸を測定することができる。As described above, the signal processor 5 calculates the altitude output of the two altimeters 2 and 3 and the pitch angle output of the gyro 4 to calculate the absolute altitude of the flying object 1. At the same time as measuring the change, it is possible to measure the unevenness of the ground or the like under the flying body 1.
【0036】[0036]
【発明の効果】以上説明したように本発明の飛翔体用地
面等凹凸測定装置によれば、これまで困難であった飛行
中の飛翔体からの飛翔体の下の地面等の凹凸の精密測定
及び飛翔体の絶対高度の変化の精密測定を可能とした。
また、本方式は単純な器材の構成であるので小型の飛翔
体に搭載し上記の機能を果たさせることが可能である。As described above, according to the apparatus for measuring unevenness of the ground for a flying object of the present invention, it is possible to precisely measure the unevenness of the ground under the flying object from the flying object which is difficult in the past. It also enables precise measurement of changes in absolute altitude of a flying object.
Further, since this method has a simple equipment structure, it can be mounted on a small flying object to fulfill the above-mentioned functions.
【図1】本発明の飛翔体用地面等凹凸測定装置の構成例
を示す図である。FIG. 1 is a diagram showing a configuration example of an unevenness measuring device for a ground for a flying object of the present invention.
【図2】同装置の原理を示した説明図である。FIG. 2 is an explanatory diagram showing the principle of the device.
【図3】同装置の演算内容を示す図である。FIG. 3 is a diagram showing the contents of calculation of the device.
【図4】本発明の他の実施例をの原理を示す説明図であ
る。FIG. 4 is an explanatory diagram showing the principle of another embodiment of the present invention.
【図5】同装置の演算内容を示す図である。FIG. 5 is a diagram showing calculation contents of the apparatus.
1…飛翔体、2…高度計、3…高度計、4…ジャイロ、
5…信号処理機、6…地面又は海面、7…高度計2のビ
ーム、8…高度計3のビーム。1 ... Flying object, 2 ... Altimeter, 3 ... Altimeter, 4 ... Gyro,
5 ... Signal processor, 6 ... Ground or sea surface, 7 ... Beam of altimeter 2, 8 ... Beam of altimeter 3.
Claims (2)
の反射を用いて対地高度を測定する高度計のうち同一の
もの2個(2)(3)を、前後方向にそれぞれのビーム
(7)(8)が重なりあわないよう飛翔体(1)に取り
付け、2個の高度計(2)(3)の高度出力を用いて計
算する信号処理機(5)により、飛行中に飛翔体下の地
面あるいは海面の凹凸(6)と飛翔体(1)本体の絶対
高度の変化を分離可能とすることを特徴とする飛翔体用
地面等凹凸測定装置。1. Two altimeters (2) and (3) which emit the beam of radio waves, light waves, sound waves and the like and measure the altitude to the ground by using the reflection of the beams (2) and (3) respectively in the front and rear directions. ) (8) is attached to the projectile (1) so that they do not overlap, and a signal processor (5) that calculates using the altitude output of two altimeters (2) and (3) is used to A device for measuring unevenness of a ground such as a flying body, which is capable of separating changes in absolute height of the flying body (1) from unevenness (6) of the ground or sea surface.
飛翔体(1)のピッチ角測定用ジャイロ(4)の出力が
加えられて計算する飛翔体用地面等凹凸測定装置。2. The signal processor (5) according to claim 1, wherein
An unevenness measuring device for the ground for a flying object, which is calculated by adding the output of a gyro (4) for measuring the pitch angle of the flying object (1).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4162977A JP2560229B2 (en) | 1992-06-22 | 1992-06-22 | Measuring device for unevenness of the ground such as flying objects |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4162977A JP2560229B2 (en) | 1992-06-22 | 1992-06-22 | Measuring device for unevenness of the ground such as flying objects |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH063440A true JPH063440A (en) | 1994-01-11 |
JP2560229B2 JP2560229B2 (en) | 1996-12-04 |
Family
ID=15764878
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4162977A Expired - Lifetime JP2560229B2 (en) | 1992-06-22 | 1992-06-22 | Measuring device for unevenness of the ground such as flying objects |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2560229B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5811707A (en) * | 1994-06-24 | 1998-09-22 | Roland Kabushiki Kaisha | Effect adding system |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR101740538B1 (en) * | 2016-05-30 | 2017-06-08 | (주)다음기술단 | Method for Correction Shaking Image of Side-Scan Sonar |
-
1992
- 1992-06-22 JP JP4162977A patent/JP2560229B2/en not_active Expired - Lifetime
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5811707A (en) * | 1994-06-24 | 1998-09-22 | Roland Kabushiki Kaisha | Effect adding system |
Also Published As
Publication number | Publication date |
---|---|
JP2560229B2 (en) | 1996-12-04 |
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