JP2016161363A - Optical coordinate measurement device - Google Patents
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Abstract
Description
本発明は、任意の箇所を原点とする座標系において光によって対象点の座標を測定する装置に関するものである。 The present invention relates to an apparatus for measuring the coordinates of a target point with light in a coordinate system having an arbitrary point as an origin.
三次元座標を得る手段としては、光学式・超音波式・電波式・機械式・磁気式・GPS(グローバルポジショニングシステム)などの様々な方式がある。しかし、どの方式にも一長一短があり、安価で使いやすく且つ精度が良い方式が実用化されておらず、製品としても存在しない。 As means for obtaining the three-dimensional coordinates, there are various methods such as optical, ultrasonic, radio, mechanical, magnetic, and GPS (global positioning system). However, each system has advantages and disadvantages, and an inexpensive, easy-to-use and accurate system has not been put into practical use and does not exist as a product.
住宅などの建設業界の基礎工事測量分野では、測量対象点を反射プリズムが装着された指示器(ポールなど)で指し示し、本体内蔵のカメラから得られる画像を解析することでその反射プリズムを追尾しレーザー計測により得られる距離情報と内蔵された2軸のサーボモーターそれぞれから得られる角度情報から三次元座標を導出する製品がある。 In the field of basic construction surveying in the construction industry such as housing, the surveying point is pointed by an indicator (such as a pole) equipped with a reflecting prism, and the reflecting prism is tracked by analyzing the image obtained from the built-in camera. There are products that derive three-dimensional coordinates from distance information obtained by laser measurement and angle information obtained from each built-in two-axis servo motor.
しかしながら、同方式では、極めて高性能なエンコーダーが必要となるためコストが高額となってしまう。また、計測においては、上記の通りモーターを使って計測点指示器を追尾する必要があるので追尾可能な範囲内で指示器を移動せざるをえず使い勝手が悪い。加えて、複数箇所を複数人で同時計測することも不可能である。 However, this method requires a very high-performance encoder, which increases the cost. In measurement, it is necessary to track the measurement point indicator using the motor as described above, and thus the indicator must be moved within a trackable range, which is inconvenient. In addition, it is impossible to simultaneously measure a plurality of locations by a plurality of people.
そこで本願発明者はこれらの問題を解決すべく発明を成し、特願2012−227909(特開2014−081232)「無線による座標測定装置」を出願した。 Accordingly, the inventor of the present application has made an invention to solve these problems, and has applied for Japanese Patent Application No. 2012-227909 (Japanese Patent Application Laid-Open No. 2014-081232) “Wireless Coordinate Measuring Device”.
特許文献1の技術は無線を使用するものである。無線は障害物の影響が軽微であり三次元座標測定を行う上では好適な手段の一つであるが、どの周波数帯であっても混信や高調波などのノイズの影響があり、またマルチパスといった問題があり、運用するフィールドに制限を設ける必要があり、汎用性が低下してしまう。 The technique of Patent Document 1 uses radio. Wireless is less affected by obstacles and is one of the preferred means for 3D coordinate measurement, but it is affected by noise such as interference and harmonics in any frequency band, and multipath Therefore, it is necessary to limit the field to be used, and the versatility is lowered.
そこで上述の諸問題を解決すべく本発明が成された。
本発明による座標測定装置は、
「光を発光する発光部と、
任意の空間座標系において既知の座標に配置され且つ発光部が発光した光を受光する複数の受光部と、
複数の受光部のうちの任意の二つの受光部からなる受光部対を複数有し、受光部対に含まれる受光部で受光した光に基づいて、発光部から受光部対の第一の受光部までの距離と発光部から受光部対の第二の受光部までの距離との差である伝播行路距離差を算出する伝播行路距離差算出部と、
複数の受光部の既知の座標と、複数の受光部対についてそれぞれ算出された伝播行路距離差と、に基づいて発光部の座標を算出する発光部座標算出部と、
を具備する」
ことを特徴としている。
Therefore, the present invention has been made to solve the above problems.
The coordinate measuring device according to the present invention is:
“A light emitting part that emits light,
A plurality of light receiving units arranged at known coordinates in an arbitrary spatial coordinate system and receiving light emitted by the light emitting unit;
Based on the light received by the light receiving unit included in the light receiving unit pair, the first light reception of the light receiving unit pair from the light emitting unit based on the light received by the light receiving unit included in the light receiving unit pair. A propagation path distance difference calculating unit that calculates a propagation path distance difference that is a difference between a distance from the light emitting unit and a distance from the light emitting unit to the second light receiving unit of the light receiving unit pair;
A light emitting unit coordinate calculating unit that calculates the coordinates of the light emitting unit based on the known coordinates of the plurality of light receiving units and the propagation path distance difference calculated for each of the plurality of light receiving unit pairs;
With "
It is characterized by that.
また、本発明の座標測定装置の発光部は、
「発光部は複数の受光部とは別体に設けられている」
ことを特徴としている。
The light emitting unit of the coordinate measuring device of the present invention is
"The light emitting part is provided separately from the plurality of light receiving parts."
It is characterized by that.
更に、本発明の座標測定装置は、
「光は、特定の周波数の正弦波で振幅変調されている」
ことを特徴としている。
Furthermore, the coordinate measuring apparatus of the present invention is
“Light is amplitude modulated with a sine wave of a certain frequency”
It is characterized by that.
本発明により、特定の周波数の正弦波で振幅変調されている光によって三次元座標測定が可能となる。 According to the present invention, three-dimensional coordinate measurement can be performed using light that is amplitude-modulated with a sine wave having a specific frequency.
詳細な説明の前に、本明細書内で共通の事項について説明する。
本発明において、発光部が発光する光は可視光・赤外線・紫外線・エックス線などであり、座標とは特に断りの無い限り立体(三次元)空間の直交座標系の座標を意味するものとする。
Before the detailed description, common matters in the present specification will be described.
In the present invention, the light emitted from the light emitting unit is visible light, infrared light, ultraviolet light, X-rays, and the like, and the coordinates mean coordinates in a three-dimensional (three-dimensional) space orthogonal coordinate system unless otherwise specified.
図1は、本発明の基本的な概念を示している。
基準モジュールは、一連の座標測定を行う間は移動させないよう扱うものであり、仮想座標系の原点(もしくは特定の座標)と看做すことができる。基準モジュールには複数の受光部があり、図1では5つの受光部としてあるが、特にこれに限定されない。
仮想座標系は、仮に、左右水平方向をX軸、垂直方向をY軸、奥行水平方向をZ軸、としている。
計測モジュールは、座標を計測したい点を指し示す計測点指示部、光を発光する発光部、座標計測を行った結果を表示する計測結果表示部から構成される。使用者はこの計測モジュールを持って移動し、座標計測を行いたい点を測定点指示部で指し示すようにし、図示しない計測開始スイッチを押下することにより計測を開始するよう計測モジュールに指示する。仮想座標系における座標計測の結果は計測結果表示部に表示される。
FIG. 1 illustrates the basic concept of the present invention.
The reference module is handled so as not to move during a series of coordinate measurements, and can be regarded as the origin (or specific coordinates) of the virtual coordinate system. The reference module has a plurality of light receiving portions, and in FIG. 1, there are five light receiving portions. However, the reference module is not particularly limited to this.
The virtual coordinate system assumes that the horizontal direction is the X axis, the vertical direction is the Y axis, and the depth horizontal direction is the Z axis.
The measurement module includes a measurement point indicating unit that indicates a point whose coordinates are to be measured, a light emitting unit that emits light, and a measurement result display unit that displays a result of coordinate measurement. The user moves with this measurement module, points to the point to be coordinate-measured by the measurement point instruction unit, and instructs the measurement module to start measurement by pressing a measurement start switch (not shown). The result of coordinate measurement in the virtual coordinate system is displayed on the measurement result display unit.
図2は、基準モジュールの受光部の構造について示している。
まず、計測モジュールの発光部より光が発光される。図2では、例として1GHzの正弦波で振幅変調された光としているが、もちろんこれに限定される理由は無い。また、自明ながら、計測モジュール内には図示していない1GHzの局部発振器を具備している。
基準モジュールには受光部が5つあり、それぞれ受光部R1〜R5としている。
各受光部R1〜R5では計測モジュールの発光部より発光された光をそれぞれ受光する。
FIG. 2 shows the structure of the light receiving portion of the reference module.
First, light is emitted from the light emitting unit of the measurement module. In FIG. 2, the light is amplitude-modulated with a 1 GHz sine wave as an example, but of course there is no reason limited to this. As is obvious, a 1 GHz local oscillator (not shown) is provided in the measurement module.
The reference module has five light receiving portions, which are light receiving portions R1 to R5, respectively.
Each of the light receiving portions R1 to R5 receives light emitted from the light emitting portion of the measurement module.
各受光部R1〜R5で受光された光は電気信号に変換され、振幅変調に用いられた信号成分(本実施例では1GHz正弦波)が抽出されて、ミキサーへ入力される。
基準モジュール内には1.00001GHz(=1GHz+10kHz)のクロック(局部発振器)を具備しており、この局部発振器が生成した正弦波信号を受光部R1〜R5で受光した1GHz正弦波信号に対し各ミキサーにて混合する。尚、図中では局部発振器からミキサーまでの線路長が全て異なっているが、実際には各ミキサー全てに同じタイミングで信号が到達するよう回路を調整してある。
各ミキサーで混合された信号はA/D(アナログ−ディジタル)変換器を通してマイコンに読取られる。マイコンでは読み取った信号をデータとして処理する。
The light received by each of the light receiving portions R1 to R5 is converted into an electrical signal, and a signal component (1 GHz sine wave in this embodiment) used for amplitude modulation is extracted and input to the mixer.
In the reference module, a clock (local oscillator) of 1.00001 GHz (= 1 GHz + 10 kHz) is provided, and each mixer is applied to the 1 GHz sine wave signal received by the light receiving units R1 to R5 of the sine wave signal generated by the local oscillator. Mix with. Although the line lengths from the local oscillator to the mixer are all different in the figure, the circuits are actually adjusted so that the signals reach all the mixers at the same timing.
A signal mixed by each mixer is read by a microcomputer through an A / D (analog-digital) converter. The microcomputer processes the read signal as data.
図3は、ミキサーで1GHzの正弦波と1.00001GHz(=1GHz+10kHz)の正弦波を混合した際の波形について示している。
周波数の近い2つの正弦波を混合すると、周波数差を周期として振幅が変動する信号(所謂「うねり」)となる。周波数差は10kHzなので、うねりの周波数は10kHzとなる。前述のマイコンは、この振幅変動の包絡線を検出し、その波形を解析する。
以下、前述の先行技術文献(特願2012−227909/特開2014−081232)に基づき、共通点については参照のみで扱い、異なる点を中心に説明する。
FIG. 3 shows a waveform when a sine wave of 1 GHz and a sine wave of 1.00001 GHz (= 1 GHz + 10 kHz) are mixed by a mixer.
When two sine waves having similar frequencies are mixed, a signal whose amplitude varies with a frequency difference as a period (so-called “swell”) is obtained. Since the frequency difference is 10 kHz, the swell frequency is 10 kHz. The aforementioned microcomputer detects the envelope of this amplitude variation and analyzes the waveform.
Hereinafter, based on the above-mentioned prior art document (Japanese Patent Application No. 2012-227909 / Japanese Patent Application Laid-Open No. 2014-081232), common points will be treated only by reference and different points will be mainly described.
先行技術の要旨は、4つの受信部対を想定し、受信部対の2つの受信部それぞれと送信部との距離の差を算出し、4つの受信部対の距離差を以って送信部の三次元座標を求める、というものである。
4つの受信部対を構成するためにコスト低減を踏まえて4つの受信部を三角錐状に配置する方式を採用したが、本発明ではより計測精度を高めるために5つの受光部を四角錐状に配置する方式とした。
まず、前述の通り、ミキサーで混合された信号は10kHzのうなりを持つものとなり、この信号の包絡線波形に対してマイコンでFFT(高速フーリエ変換)処理を施すことにより、包絡線の周波数とミキサーに混合した2つの信号の位相差を求めることができる。
The gist of the prior art is to assume four receiving unit pairs, calculate the difference in distance between each of the two receiving units of the receiving unit pair and the transmitting unit, and calculate the transmitting unit with the difference in distance between the four receiving unit pairs. The three-dimensional coordinates are obtained.
In order to construct four receiver pairs, a system in which four receivers are arranged in a triangular pyramid shape was adopted in consideration of cost reduction. However, in the present invention, five light receiving parts are arranged in a quadrangular pyramid shape in order to improve measurement accuracy. It was set as the method to arrange in.
First, as described above, the signal mixed by the mixer has a beat of 10 kHz. By applying FFT (Fast Fourier Transform) processing to the envelope waveform of this signal by a microcomputer, the frequency of the envelope and the mixer The phase difference between the two signals mixed together can be obtained.
この際、発光部が発光する光の振幅変調をする正弦波の周波数をf、光速をc、ミキサーに混合する信号のうち基準となる信号の位相値をθ1、もう片方の信号の位相値をθn、発光部とθ1の信号を受光する受光部の距離をd1、発光部とθnの信号を受光する受光部の距離をdn、とした場合、距離差Dm=dn―d1は次の式で算出できる(m=1〜4となる)。
なお、以降の数式で多用する添え字nとmについては以下の通りである。
nは、複数の受光部のうちの特定の1つを示す数字であり、本実施例では受光部が5つあるので、nは1〜5の範囲となる。
このうち、n=1の受光部を中心的に扱い、n=1以外の受光部(n=2〜5)との組み合わせで受光部対を構成することとする。すなわち、受光部をRnと表記すると、受光部対は「R1対R2」「R1対R3」「R1対R4」「R1対R5」の4つが存在することになる。受光部対のこれらの4通り組み合わせをmで示す。例えば「R1対R2」はm=1である。受光部が5つある場合、mは1〜4の範囲となる。mを用いた違う書き方をすると、受光部対「R1対R(m+1)」を示しているという意味でもある。
At this time, the frequency of the sine wave for amplitude modulation of the light emitted from the light emitting unit is f, the speed of light is c, the phase value of the reference signal among the signals mixed in the mixer is θ1, and the phase value of the other signal is When θn, the distance between the light emitting unit and the light receiving unit that receives the θ1 signal is d1, and the distance between the light emitting unit and the light receiving unit that receives the θn signal is dn, the distance difference Dm = dn−d1 is expressed by the following equation. Can be calculated (m = 1 to 4).
The subscripts n and m frequently used in the following formulas are as follows.
n is a number indicating a specific one of the plurality of light receiving portions. In this embodiment, there are five light receiving portions, and therefore n is in the range of 1 to 5.
Among these, a light receiving unit with n = 1 is treated as a center, and a light receiving unit pair is configured by a combination with light receiving units other than n = 1 (n = 2 to 5). In other words, when the light receiving part is represented as Rn, there are four light receiving part pairs: “R1 pair R2”, “R1 pair R3”, “R1 pair R4”, and “R1 pair R5”. These four combinations of light receiving part pairs are denoted by m. For example, “R1 vs. R2” is m = 1. When there are five light receiving parts, m is in the range of 1-4. If the writing method is different using m, it also means that the light receiving unit pair “R1 pair R (m + 1)” is shown.
このことより、発光部が発光する光の振幅変調をする正弦波の周波数fと基準モジュール内の局部発振器の周波数(=ミキサーで混合した際のうねり周波数を決定する)が既知であれば、「発光部と受光部対のうちの片方の受光部との距離」と「発光部と受光部対のうちのもう片方の受光部との距離」の差Dがわかるのである。
他の受光部の信号との関係性についても同じことがいえるので、発光部を基準として受光部R1〜R5相互の距離差も同様に求まることになる。
From this, if the frequency f of the sine wave that modulates the amplitude of the light emitted from the light emitting unit and the frequency of the local oscillator in the reference module (= determines the swell frequency when mixed by the mixer) are known, The difference D between the “distance between the light emitting part and one light receiving part of the light receiving part pair” and the “distance between the light emitting part and the other light receiving part in the light receiving part pair” is known.
Since the same can be said for the relationship with the signals of the other light receiving parts, the difference in distance between the light receiving parts R1 to R5 with respect to the light emitting part is also obtained in the same manner.
先行技術では4つの受信部で4つの受信部対を構成していたが、本発明では5つの受光部で4つの受光部対を構成するようにしたため、先行技術文献の式4に該当する部分は以下のようになる。 In the prior art, four receiving units are configured by four receiving units. However, in the present invention, four light receiving units are configured by five light receiving units, and therefore a part corresponding to Equation 4 in the prior art document. Is as follows.
ここまでの内容に基づき、距離差Dmから発光部の座標を求める方法を説明する。
発光部lの座標をl(x,y,z)とする。
受光部R1〜R5の座標は既知でありこれをRn(x,y,z)とする(n=1〜5)。
受光部Rnと発光部lとの直線距離をdnとする(n=1〜5)。
d1とd2〜d4の差(距離差)をrmとする(m=1〜4)。
受光部R1とRnの間に生じる既知の回路上の遅延要因を距離に換算したものをAm(m=1〜4)とする。
ミキサー出力波形をA/D変換しFFTを施して得られた位相値をθnとする(n=1〜5)。
Based on the contents so far, a method for obtaining the coordinates of the light emitting unit from the distance difference Dm will be described.
The coordinates of the light emitting unit l are assumed to be l (x, y, z).
The coordinates of the light receiving parts R1 to R5 are known, and this is assumed to be Rn (x, y, z) (n = 1 to 5).
The linear distance between the light receiving part Rn and the light emitting part 1 is dn (n = 1 to 5).
The difference (distance difference) between d1 and d2 to d4 is rm (m = 1 to 4).
Am (m = 1 to 4) is obtained by converting a known delay factor on the circuit generated between the light receiving portions R1 and Rn into a distance.
A phase value obtained by subjecting the mixer output waveform to A / D conversion and FFT is θn (n = 1 to 5).
この時、
T1=D1−A1
T2=D2−A2
T3=D3−A3
T4=D4−A4
とすると、
中間変数としてC・X・Y・Zを以下のように定義できる。
At this time,
T1 = D1-A1
T2 = D2-A2
T3 = D3-A3
T4 = D4-A4
Then,
C, X, Y, and Z can be defined as intermediate variables as follows.
上述の中間変数を元に発光部の座標l(x,y,z)は以下の式により求まる。 Based on the above-mentioned intermediate variables, the coordinates l (x, y, z) of the light emitting unit are obtained by the following equations.
このようにして、5つの受光部の既知の座標と、各受光部より構成される受光部対それぞれにおいて測定された伝播行路距離差と、を数式に代入することで発光部の座標を求めることが可能となる。 In this way, the coordinates of the light emitting unit are obtained by substituting the known coordinates of the five light receiving units and the propagation path distance difference measured in each pair of the light receiving units composed of the respective light receiving units into the mathematical formula. Is possible.
図1の計測モジュールにおいて、三次元座標測定の対象になるのは発光部の存在する部位となるが、計測モジュール内に加速度センサーなどを設けて重力方向に対する姿勢を取得するようにすれば、発光部から計測点指示部までの距離は既知であるので、計測点指示部の座標も算出することが可能となる。 In the measurement module of FIG. 1, the target of the three-dimensional coordinate measurement is a part where the light emitting unit exists. However, if an accelerometer or the like is provided in the measurement module so as to acquire a posture in the direction of gravity, light emission Since the distance from the unit to the measurement point instruction unit is known, the coordinates of the measurement point instruction unit can also be calculated.
更に、計測は基準モジュール側で行うが、計測結果は計測モジュール側へ通信手段をもって通知しても良い。図2に示してある例ではBluetooth(登録商標)を用いて計測した結果を計測モジュールへ送信している。 Further, although the measurement is performed on the reference module side, the measurement result may be notified to the measurement module side by communication means. In the example shown in FIG. 2, the result of measurement using Bluetooth (registered trademark) is transmitted to the measurement module.
以上、本発明について好適な実施例を挙げて説明したが、本発明はこれらの実施例に限定されるものではなく、発明の精神を逸脱しない限り多くの改変を施すことが可能であるのは勿論である。 The present invention has been described with reference to preferred embodiments. However, the present invention is not limited to these embodiments, and many modifications can be made without departing from the spirit of the invention. Of course.
量産可能な発光部および受光部を用いて特定箇所の座標測定を簡便に行うことができ、寸法測定や測量などの作業の効率を向上させるなどの効果を有している。 Coordinate measurement at a specific location can be easily performed by using a light emitting unit and a light receiving unit that can be mass-produced, and there is an effect of improving the efficiency of operations such as dimension measurement and surveying.
Claims (3)
任意の空間座標系において既知の座標に配置され且つ前記発光部が発光した光を受光する複数の受光部と、
前記複数の受光部のうちの任意の二つの受光部からなる受光部対を複数有し、該受光部対に含まれる受光部で受光した光に基づいて、前記発光部から該受光部対の第一の受光部までの距離と前記発光部から該受光部対の第二の受光部までの距離との差である伝播行路距離差を算出する伝播行路距離差算出部と、
前記複数の受光部の既知の座標と、前記複数の受光部対についてそれぞれ算出された前記伝播行路距離差と、に基づいて前記発光部の座標を算出する発光部座標算出部と、
を具備することを特徴とする座標測定装置。 A light emitting unit that emits light;
A plurality of light receiving units arranged at known coordinates in an arbitrary spatial coordinate system and receiving light emitted from the light emitting unit;
A plurality of light receiving unit pairs each including two arbitrary light receiving units among the plurality of light receiving units, and based on light received by the light receiving units included in the light receiving unit pair, A propagation path distance difference calculation unit that calculates a propagation path distance difference that is a difference between a distance to the first light receiving unit and a distance from the light emitting unit to the second light receiving unit of the light receiving unit pair;
A light emitting unit coordinate calculating unit that calculates coordinates of the light emitting unit based on known coordinates of the plurality of light receiving units and the propagation path distance difference calculated for each of the plurality of light receiving unit pairs;
A coordinate measuring apparatus comprising:
The coordinate measuring apparatus according to claim 1, wherein the light is amplitude-modulated with a sine wave having a specific frequency.
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| JP2015039712A JP2016161363A (en) | 2015-02-28 | 2015-02-28 | Optical coordinate measurement device |
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| JP2015039712A JP2016161363A (en) | 2015-02-28 | 2015-02-28 | Optical coordinate measurement device |
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Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7499393B1 (en) | 2023-09-19 | 2024-06-13 | 直之 村上 | Fiber optic distance measuring instrument |
| WO2025063241A3 (en) * | 2023-09-19 | 2025-05-22 | 直之 村上 | Optical fiber distance measurement |
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Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7499393B1 (en) | 2023-09-19 | 2024-06-13 | 直之 村上 | Fiber optic distance measuring instrument |
| JP2025044082A (en) * | 2023-09-19 | 2025-04-01 | 直之 村上 | Optical fiber distance measuring instrument |
| WO2025063241A3 (en) * | 2023-09-19 | 2025-05-22 | 直之 村上 | Optical fiber distance measurement |
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