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JPH0456928B2 - - Google Patents

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Publication number
JPH0456928B2
JPH0456928B2 JP24559684A JP24559684A JPH0456928B2 JP H0456928 B2 JPH0456928 B2 JP H0456928B2 JP 24559684 A JP24559684 A JP 24559684A JP 24559684 A JP24559684 A JP 24559684A JP H0456928 B2 JPH0456928 B2 JP H0456928B2
Authority
JP
Japan
Prior art keywords
light
optical fiber
axis
surveying
circuit
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.)
Expired
Application number
JP24559684A
Other languages
Japanese (ja)
Other versions
JPS61122514A (en
Inventor
Toshihiko Yoshino
Nobuaki Yoshida
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.)
Nikon Corp
Original Assignee
Nippon Kogaku KK
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 Nippon Kogaku KK filed Critical Nippon Kogaku KK
Priority to JP24559684A priority Critical patent/JPS61122514A/en
Publication of JPS61122514A publication Critical patent/JPS61122514A/en
Publication of JPH0456928B2 publication Critical patent/JPH0456928B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 (発明の技術分野) 本発明は光フアイバジヤイロを用いた測量装置
に関する。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field of the Invention) The present invention relates to a surveying device using an optical fiber gyro.

(発明の背景) 従来用いられている各種測量法のうち多角測
量、三角測量は比較的に良く用いられる測量法で
ある。これらの測量にはトランシツト(セオドラ
イト)が使用されるが、トランシツトは、機械式
の角度読み取り機構を備えているので重量が重
く、それに従い三脚も大型で重いものにせざるを
得ず、装置の大型化と重量化を招いていた。更に
目盛を読む為読み取り誤差を取り除く事が出来な
いと言う欠点を有している。又方位角(一定の方
位に対する角度)を直接測定出来ない等の為測量
に時間が掛かるという欠点を有している。更に、
方位角の測定の為に他の機器を必要とする為、運
搬する機材が増える。トランジツトに方位側測定
置を組み込んだものもあるが、重量が増し、且つ
大型化すると言う欠点を有している。
(Background of the Invention) Among various conventional surveying methods, polygonal surveying and triangulation are relatively commonly used surveying methods. A transit (theodolite) is used for these surveys, but since the transit is equipped with a mechanical angle reading mechanism, it is heavy, and accordingly the tripod must be large and heavy. This led to increased weight and weight. Furthermore, since the scale is read, it has the disadvantage that reading errors cannot be removed. Another drawback is that it takes time to survey, as the azimuth angle (angle relative to a certain direction) cannot be directly measured. Furthermore,
Since other equipment is required to measure the azimuth angle, the amount of equipment to be transported increases. Some transits have built-in azimuth measurement devices, but these have the drawbacks of increased weight and size.

(発明の目的) 本発明は上記欠点を解決するもので、操作が簡
単で小型軽量な読み取り誤差の無い測量装置を得
る事を目的とする。
(Object of the Invention) The present invention solves the above-mentioned drawbacks, and aims to provide a surveying device that is easy to operate, small and lightweight, and free from reading errors.

(発明の概要) 本発明は互いに直交する3面のそれぞれの面内
に巻回された光フアイバを中空の略球状に形成し
た3軸光フアイバジヤイロ(以下3軸光フアイバ
ジヤイロと称す)を測量装置に用いるものであつ
て、3軸光フアイバジヤイロと視準付望遠鏡とを
組合せる事を技術的要点としている。
(Summary of the Invention) The present invention provides a 3-axis optical fiber coil (hereinafter referred to as 3-axis optical fiber coil) in which optical fibers wound in each of three mutually orthogonal planes are formed into a hollow, substantially spherical shape for use in surveying equipment. The technical point is to combine a 3-axis optical fiber gyro and a collimating telescope.

(実施例) 第1図は本発明による測量装置の実施例であつ
てトランシツトに代替可能のものである。
(Embodiment) FIG. 1 shows an embodiment of a surveying device according to the present invention, which can be substituted for a transit.

1,2,3はボビンであつてそれぞれのボビン
には光フアイバが巻回されており、それぞれが光
フアイバジヤイロの一部を構成している。ボビン
1,2,3は、ボビン1の中にボビン2が、更に
ボビン2の中にボビン3が、それぞれの面が直交
する様に組み合わされて全体で中空の略球状を成
し(以下中空球状体と称す)、3軸光フアイバジ
ヤイロを構成している。それぞれのボビンの断面
は第2図に示す様に外縁凹部を有し、該凹部には
光フアイバが巻回されている。該中空球状体の中
空部には光フアイバジヤイロの構成要素である電
源、光源、受光器、信号処理系、発信機または表
示機が収納される。4は視準付望遠鏡であり、前
記3軸光フアイバジヤイロが一体的に固定ささて
いる。視準付望遠鏡4は、周知のように、三脚5
0上に鉛直軸まわりで回転自在に取付けられる自
在回転アーム53に、水平軸まわりで回転自在に
取付けられている。三脚50には気泡による水平
測定器8が組み込まれており、又自在回転アーム
53の三脚50への取付け軸と同軸に下げ振り8
0が取付けられる。
Reference numerals 1, 2, and 3 indicate bobbins, each of which is wound with an optical fiber, and each constitutes a part of an optical fiber coil. The bobbins 1, 2, and 3 are assembled such that the bobbin 2 is placed inside the bobbin 1, and the bobbin 3 is placed inside the bobbin 2, so that their respective surfaces are orthogonal to each other, forming a hollow approximately spherical shape as a whole (hereinafter referred to as hollow). (referred to as a spherical body), which constitutes a three-axis optical fiber gyroscope. The cross section of each bobbin has an outer edge recess as shown in FIG. 2, and an optical fiber is wound in the recess. The hollow portion of the hollow spherical body accommodates the components of the fiber optic gyroscope, such as a power source, a light source, a light receiver, a signal processing system, a transmitter, or a display. Reference numeral 4 denotes a collimating telescope, to which the three-axis optical fiber gyroscope is integrally fixed. As is well known, the sighting telescope 4 is equipped with a tripod 5.
The rotary arm 53 is rotatably mounted on the rotary arm 53, which is rotatably mounted on the rotary arm 53, rotatably around the horizontal axis. The tripod 50 has a level measuring device 8 built in using a bubble, and a plumb bob 8 is installed coaxially with the axis of attachment of the freely rotating arm 53 to the tripod 50.
0 is attached.

第3図は第1図に示す3軸光フアイバジヤイロ
の1軸要素についてその構造を示すもので、10
はボビン1に巻回された偏向保持の光フアイバ、
11は電源及び信号処理系を含む回路部、12は
スーパールミネツセンスダイオード、カツプラ、
導光用フアイバ、レンズを含む光源部、13はハ
ーフプリズムで光源12からの光を効率良く等量
に二手に分ける。従つて透過率及び反射率はそれ
ぞれ約50%である。14a,14bは偏光板、15a,
15bは光フアイバ10の両端に設けられる集光
用のレンズである。光フアイバ10はボビン1に
巻回されてサニヤツク効果を生ずるループをなし
ており、レンズ15a,15bで受けた光源12
からの光を該ループの両端から入射する様構成す
る。16は該ループの一端に設けられる位相変調
用のピエゾ素子であり、光フアイバー10が堅く
巻回されており、一定の交流信号を該ピエゾ素子
16に与えると光フアイバ10が伸縮する。これ
により光フアイバループの右回りと左回りとの干
渉出力は変調されて微小な回転角速度に対する測
定感度を上げる。前記ループを通って入射端と反
対側の端部に出射された光はそれぞれ再び偏光板
14a,14bを通りハーフプリズム17a,1
7bで反射され、各光デイスク18a,18bで
検出される。この光デイテクタ18a,18bに
よりサニヤツク干渉前の光量を知る事が出来る。
尚前記ハーフプリズム17a,17bの透過率は
高く、例えば90%程度に設定される。前記ハーフ
プリズム17a,17bを透過した光はハーフプ
リズム13でサニヤツク干渉し、該干渉光は光デ
イテクタ18cで検出される。サニヤツク干渉前
と干渉後の光信号は光デイテクタ18a,18
b,18cによつて光電変換され、回路部11に
送られる。回路部11では、干渉後の光量と干渉
前の光量との差動をとる事により、光源12のド
リフトを除去する。19は送信部で回路部11で
処理された信号を電波により受信部に送る。尚偏
光板14a,14bは光が光フアイバ10のルー
プを通過する際発生するノイズを除去する為に設
けられる。
Figure 3 shows the structure of the 1-axis element of the 3-axis optical fiber gyroscope shown in Figure 1.
is a polarization-maintaining optical fiber wound around bobbin 1,
11 is a circuit section including a power supply and a signal processing system, 12 is a super luminescence diode, a coupler,
A light source section 13 including a light guide fiber and a lens is a half prism that efficiently divides the light from the light source 12 into two equal parts. Therefore, the transmittance and reflectance are each about 50%. 14a, 14b are polarizing plates, 15a,
Reference numeral 15b denotes condensing lenses provided at both ends of the optical fiber 10. The optical fiber 10 is wound around the bobbin 1 to form a loop that produces a sannyac effect, and the light source 12 received by the lenses 15a and 15b is
The configuration is such that light from the loop enters from both ends of the loop. Reference numeral 16 denotes a phase modulation piezo element provided at one end of the loop, in which the optical fiber 10 is tightly wound.When a constant alternating current signal is applied to the piezo element 16, the optical fiber 10 expands and contracts. As a result, the clockwise and counterclockwise interference outputs of the optical fiber loop are modulated, increasing the measurement sensitivity to minute rotational angular velocities. The light that passes through the loop and is emitted to the end opposite to the incident end passes through the polarizing plates 14a and 14b again, respectively, and enters the half prisms 17a and 1.
7b and detected by each optical disk 18a, 18b. These optical detectors 18a and 18b make it possible to know the amount of light before sannyac interference.
The transmittance of the half prisms 17a and 17b is high, for example, set to about 90%. The light transmitted through the half prisms 17a and 17b undergoes sanitary interference at the half prism 13, and this interference light is detected by an optical detector 18c. The optical signals before and after the interference are sent to the optical detectors 18a and 18.
b, 18c photoelectrically converts the signal and sends it to the circuit section 11. The circuit section 11 removes the drift of the light source 12 by taking the difference between the amount of light after interference and the amount of light before interference. A transmitting section 19 sends the signal processed by the circuit section 11 to the receiving section by radio waves. The polarizing plates 14a and 14b are provided to remove noise generated when light passes through the loop of the optical fiber 10.

第4図は第1図に示す3軸光フアイバジヤイロ
の球状のフアイバループの内部に組み込まれてい
るハーフプリズム等の構成を示す図で一つの光源
12で三軸光フアイバージヤイロの光源を賄う一
実施例である。121,122は光分岐カプラ
で、融着、研磨・接着、エツチング・デイツピン
グ、プリズム、グレーテイング等によるものが考
えられる。光分岐カプラ121,122で3分岐
された光は、ハーフプリズム13,13′,1
3″に入射される。ハーフプリズム13,13′,
13″にはそれぞれハーフプリズム17a,17
a′17a″及び17b,17b′17b″が組み合わさ
れている。例えばハーフプリズム13に入射した
光は半々に17a,17bに進む。17aを殆ど
通過した光フアイバループ10を反時計回りに回
つてハーフプリズム17bに入る。ハーフプリズ
ム17bに入った光の一部が強度検出用として光
デイテクタ18bに進み、残りの殆どがハーフプ
リズム13に進む。一方ハーフプリズム17bを
殆ど通過した光はフアイバループ10を時計回り
に回つてハーフプリズム17aに入る。ハーフプ
リズム17aに入つた光の一部が強度検出用とし
て光デイテクタ18aに進み、残りの殆どがハー
フプリズム13に進む。ハーフプリズム13に戻
つた時計回りと反時計回りの二つによる光の干渉
光は、光デイテクタ18cで検出される。ここで
光源12に戻り光があるが、光源にスーパールミ
ネツセンスダイオードを使用すればコヒーレンス
長が数十ミクロン程度の為コヒーレンスノイズを
発生しない。第5,6図は本発明による測量装置
の回路系のそれぞれ一部を示すブロツク図であ
り、第5図は送信側、第6図は受信側をそれぞれ
表す。第5図に於いて181,182,183は
光デイテクタ18a,18b,18cからの信号
を増幅する増幅器である。184は乗算回路で,
増幅器181と182との信号の積、即ちサニヤ
ツクループである光フアイバループ10の時計回
りの反時計回りの光の強度の積で、これはサニヤ
ツク干渉前の光の強度である。183はサニヤツ
ク干渉後の光の強度を増幅する増幅器である。1
85は増幅器183と乗算回路184との比をと
る差動回路であり、これにより光源12の出力光
に含まれるドリフトを除去する為のものである。
このドリフト除去により測量装置の精度を向上す
ることができる。186は積分回路であり差動回
路185の出力である一軸分即ち一次元の角速度
信号を角度信号に直す。187,188はそれぞ
れ他の二軸分の角速度信号を角度信号に直す積分
回路である。19はそれぞれの信号の送信部、1
9aは送信アンテナである。
FIG. 4 is a diagram showing the configuration of a half prism etc. built into the spherical fiber loop of the triaxial fiber optic coil shown in FIG. 1. This is an example. Reference numerals 121 and 122 are optical branching couplers, which may be made by fusing, polishing/bonding, etching/dipping, prism, grating, or the like. The light branched into three by the optical branch couplers 121 and 122 is split into half prisms 13, 13', and 1.
3″.Half prisms 13, 13′,
13″ have half prisms 17a and 17, respectively.
a'17a'' and 17b, 17b'17b'' are combined. For example, the light incident on the half prism 13 travels equally to 17a and 17b. The optical fiber loop 10, which has almost passed through 17a, is rotated counterclockwise and enters the half prism 17b. A part of the light entering the half prism 17b goes to the optical detector 18b for intensity detection, and most of the rest goes to the half prism 13. On the other hand, most of the light that has passed through the half prism 17b goes around the fiber loop 10 clockwise and enters the half prism 17a. A portion of the light entering the half prism 17a passes to the optical detector 18a for intensity detection, and most of the remaining light passes to the half prism 13. The interference light of the clockwise and counterclockwise lights returning to the half prism 13 is detected by the optical detector 18c. Here, there is light returning to the light source 12, but if a superluminescence diode is used as the light source, coherence noise will not be generated because the coherence length is about several tens of microns. 5 and 6 are block diagrams showing a part of the circuit system of the surveying apparatus according to the present invention, with FIG. 5 showing the transmitting side and FIG. 6 showing the receiving side, respectively. In FIG. 5, 181, 182, and 183 are amplifiers that amplify the signals from the optical detectors 18a, 18b, and 18c. 184 is a multiplication circuit,
The product of the signals of the amplifiers 181 and 182, that is, the product of the clockwise and counterclockwise light intensities of the optical fiber loop 10, which is a sannyac loop, is the light intensity before sannyac interference. Reference numeral 183 denotes an amplifier that amplifies the intensity of the light after the sannyac interference. 1
85 is a differential circuit that takes the ratio between the amplifier 183 and the multiplier circuit 184, and is used to remove the drift contained in the output light of the light source 12.
By removing this drift, the accuracy of the surveying device can be improved. Reference numeral 186 denotes an integrating circuit which converts the one-axis, ie, one-dimensional, angular velocity signal output from the differential circuit 185 into an angle signal. Reference numerals 187 and 188 are integration circuits that convert the angular velocity signals of the other two axes into angle signals. 19 is a transmitter for each signal, 1
9a is a transmitting antenna.

第6図に於いて21は受信部、21aは受信ア
ンテナ、22は受信部21からの信号を処理する
処理回路、23は処理回路からの信号を受けてプ
リンタ231やデイスプレイ232等の装置にデ
ータを表示する出力部である。
In FIG. 6, 21 is a receiving section, 21a is a receiving antenna, 22 is a processing circuit that processes the signal from the receiving section 21, and 23 is a device that receives the signal from the processing circuit and sends the data to a device such as a printer 231 or a display 232. This is an output section that displays.

第6図において222は3次元の角度決定回路
であり、前記積分回路186,187,188か
らの直交する3成分の角度信号から方位を3次元
のデータとして演算し出力する。223は手動の
切換スイツチで真北決定回路224か座標変換回
路225のいずれかを択一的に接続可能となつて
いる。即ち切換スイツチ223を真北決定回路2
24側に接続した時、ある方向を向いて静止して
いる本測量装置には地球の自転の検出により西の
方位が出力される為三脚50に取付けられている
水平測定器8からの位置関係から真北が決定され
る。このデータはメモリ227aに記憶される。
次に、或る方位の測定の為に切換スイツチ223
を座標変換回路225側に接続すると前述のメモ
リ227aに記憶された真北のデータは座標変換
データとして使われて、3次元の角度決定回路2
22のデータを座標変換回路225で座標変換し
て真の方位を算出し、メモリ227bで記憶す
る。メモリ227a及び227bに記憶されたデ
ータは、インターフエース226を通つて随時出
力部23のうちのプリンタ231やデイスプレイ
232に出力される。第1〜6図によつてしめさ
れる測量装置は従来のトランシツト測量をより簡
素化できる。以下に本発明の測量装置を用いた測
量の手順をしめす。
In FIG. 6, 222 is a three-dimensional angle determination circuit, which calculates and outputs the orientation as three-dimensional data from the orthogonal three-component angle signals from the integrating circuits 186, 187, and 188. Reference numeral 223 is a manual changeover switch that can be selectively connected to either the true north determination circuit 224 or the coordinate conversion circuit 225. That is, the changeover switch 223 is set to the true north determination circuit 2.
When connected to the 24 side, this surveying device, which is stationary facing a certain direction, outputs the west direction by detecting the rotation of the earth, so the positional relationship from the horizontal measuring device 8 attached to the tripod 50 is True north is determined from This data is stored in memory 227a.
Next, select switch 223 for measurement in a certain direction.
When connected to the coordinate conversion circuit 225 side, the due north data stored in the memory 227a mentioned above is used as coordinate conversion data, and the three-dimensional angle determination circuit 2
The coordinate conversion circuit 225 converts the coordinates of the data No. 22 to calculate the true orientation, which is stored in the memory 227b. The data stored in the memories 227a and 227b is output to the printer 231 or display 232 of the output section 23 at any time through the interface 226. The surveying apparatus shown in FIGS. 1-6 can simplify conventional transit surveying. The following is a survey procedure using the surveying device of the present invention.

第7図は本発明の測量装置による測量の概要を
説明する図である。以下第1〜7図を用いて本発
明の測量装置の動作を説明する。
FIG. 7 is a diagram illustrating an overview of surveying by the surveying device of the present invention. The operation of the surveying apparatus of the present invention will be explained below using FIGS. 1 to 7.

AB間は基線長であり、適当な方法(巻尺に
よる実測や測距儀による計測)により正確な距
離を測定しておく。
The distance between A and B is the base line length, and the accurate distance is measured by an appropriate method (actual measurement with a tape measure or measurement with a rangefinder).

本測量装置を略B点上に置き下げ振りがB点
を指す様に三脚を調整する。
Place this surveying device approximately above point B and adjust the tripod so that the down swing points to point B.

A点を視準付望遠鏡4で観測し、視準をA点
に合う様に調節する。
Point A is observed with a sighting telescope 4, and the sight is adjusted to match point A.

前記調節後測量装置の第1のメモリ書込み操
作を行い、直線ABの方位角Θ0(真北に対する
水平面内の角度)及び仰角又は俯角Θ1(水平面
に対する角度/以下単に仰角という)がメモリ
ーに記憶される。A点からB点を含む水平面上
に下ろした垂線の足をDとするとΘ1=∠ABD
である。
A first memory write operation of the surveying device after adjustment is performed, and the azimuth angle Θ0 (angle in the horizontal plane with respect to true north) and the elevation angle or depression angle Θ1 (angle with respect to the horizontal plane/hereinafter simply referred to as elevation angle) of the straight line AB are stored in the memory. Ru. If the foot of the perpendicular drawn from point A to the horizontal plane including point B is D, then Θ1 = ∠ABD
It is.

次に測量装置を回動させてC点を視準付望遠
鏡4で観測し、視準をC点に合う様に調節す
る。
Next, the surveying device is rotated to observe point C with the collimating telescope 4, and the collimation is adjusted to match point C.

前記調節後測量装置の第2のメモリ書込み操
作を行い、直線BCの方位角Θ2と仰角Θ3がメモ
リーに記憶される。C点からB点を含む水平面
上に下ろした垂線の足をEとするとΘ3=∠
CBEである。
After said adjustment, a second memory write operation of the surveying device is performed, and the azimuth angle Θ2 and the elevation angle Θ3 of the straight line BC are stored in the memory. If the leg of the perpendicular drawn from point C to the horizontal plane including point B is E, then Θ3=∠
He is a CBE.

前記第1及び第2のメモリ書込み操作による
データより∠ABCの値が演算されその結果等
が記憶され、表示される。
The value of ∠ABC is calculated from the data obtained by the first and second memory write operations, and the results are stored and displayed.

次に測量装置をA点上に置き、前述の様にB
点及びC点を観測して∠CABが演算され、そ
の結果等が記憶され、表示される。
Next, place the surveying device on point A and place it on point B as described above.
∠CAB is calculated by observing the point and C point, and the results are stored and displayed.

△ABC及びそれらの方位が特定される。 ΔABC and their orientations are identified.

以上の手順により三角測量が行われる。 Triangulation is performed through the above steps.

第8図、第9図は第4図に示す光源の分岐のや
り方の他の実施例を示し、第8図は光源の分岐を
プリズムで行うものでハーフプリズム127に入
射した入射光の1/3はハーフプリズム131に進
み残りの2/3はハーフプリズム128に進む。該
ハーフプリズム128に進んだ光はハーフプリズ
ム132,133に等分に進む。以上により光源
12の光は3等分され以降は第4図に示すプリズ
ムの構成と同様に構成される。この分岐方式によ
ると各プリズムでの不要光が他の次元用の干渉計
に悪影響を及ぼさない点で優れている。第9図は
光源の分岐をグレーテイング(回折格子)で行う
もので123はグレーテイング、124,12
5,126は干渉プリズム、141,142,1
43は導光ガイドである。グレーテイング123
で0次光、±1次光に分岐された光は、導光ガイ
ド141,142,143に入射する。導光ガイ
ドは、集光レンズ等でフアイバに入射させる機能
を持つ部分と、フアイバからプリズム124,1
25,126に入射するときに平行光を作る機能
を持つ部分とを含む。
8 and 9 show other embodiments of the method of branching the light source shown in FIG. 3 goes to the half prism 131 and the remaining 2/3 goes to the half prism 128. The light that has traveled to the half prism 128 travels equally to the half prisms 132 and 133. As described above, the light from the light source 12 is divided into three equal parts, and the subsequent structure is similar to that of the prism shown in FIG. This branching method is advantageous in that unnecessary light from each prism does not adversely affect interferometers for other dimensions. In Figure 9, the light source is branched using a grating (diffraction grating), 123 is the grating, 124, 12
5,126 is an interference prism, 141,142,1
43 is a light guide. grating 123
The light branched into zero-order light and ±first-order light enters light guides 141, 142, and 143. The light guiding guide includes a part that has a function of making the light enter the fiber using a condensing lens, etc., and a part that has a function of making the light enter the fiber with a condensing lens, etc.
25, 126.

(発明の効果) 上記説明で明らかな様に3軸光フアイバジヤイ
ロを用いている事から、方位を測定する必要が無
いので測量の手順が簡単であり角度読み取り用目
盛等が無い為小型軽量であり、方位測定の為の装
置をトランジツトに組み込んだり方位測定装置を
測量作業の為に運搬する必要が無く、又従来のト
ランシツトの様に目盛が無いので重量が軽く、又
目盛を読む事も無いので(表示手段で直読)読み
取り誤差も無く、測量が簡単になる。
(Effects of the invention) As is clear from the above explanation, since the 3-axis optical fiber gyro is used, there is no need to measure the direction, so the surveying procedure is simple, and there is no scale for reading angles, so it is small and lightweight. There is no need to incorporate a direction measuring device into the transit or to transport the direction measuring device for surveying work, and since there is no scale like conventional transits, it is light in weight, and there is no need to read the scale. (Direct reading using display means) There is no reading error, making surveying easier.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の一実施例の外観図、第2図は
ボビンの断面図、第3図は3軸光フアイバジヤイ
ロの1軸要素の構造を示す図、第4図は光源の分
岐の一例を示す図、第5図は送信側の回路系を示
すブロツク図、第6図は受信側の回路系を示すブ
ロツク図、第7図は本発明の測量装置による測量
の一例を示す図、第8図は光源の分岐の他の例を
示す図、第9図は光源の分岐の他の例を示す図 (主要な符号の説明)、1,2,3……ボビン、
8……水平測定器、10……光フアイバ、50…
…三脚、53……自在回転アーム、80……下げ
振り、13,13′,13″……ハーフプリズム、
17a,17b,17b′,17b″……ハーフプリ
ズム。
Fig. 1 is an external view of one embodiment of the present invention, Fig. 2 is a sectional view of a bobbin, Fig. 3 is a diagram showing the structure of a single-axis element of a triaxial optical fiber coil, and Fig. 4 is an example of a branching of a light source. 5 is a block diagram showing the circuit system on the transmitting side, FIG. 6 is a block diagram showing the circuit system on the receiving side, and FIG. 7 is a diagram showing an example of surveying using the surveying device of the present invention. Figure 8 is a diagram showing another example of branching of the light source, Figure 9 is a diagram showing another example of branching of the light source (explanation of main symbols), 1, 2, 3... bobbin,
8... Horizontal measuring device, 10... Optical fiber, 50...
...Tripod, 53...Freely rotating arm, 80...Plumb bob, 13, 13', 13''...Half prism,
17a, 17b, 17b', 17b''...Half prism.

Claims (1)

【特許請求の範囲】[Claims] 1 3つの光フアイバをそれぞれ巻回すると共
に、前記巻回によつて形成する3面が互いに交差
するようにそれぞれの光フアイバが組み合わされ
た、3軸光フアイバジヤイロと、該3軸光フアイ
バジヤイロを水平軸及び垂直軸回りに回転自在に
支持する支持部材と、該支持部材の姿勢を検出す
る検出器と、前記3軸光フアイバジヤイロに一体
的に設けられた視準付望遠鏡と、を備えたことを
特徴とする光フアイバジヤイロを用いた測量装
置。
1. A 3-axis optical fiber coil in which three optical fibers are wound, and the respective optical fibers are combined so that the three planes formed by the windings intersect with each other, and the 3-axis optical fiber coil is horizontally wound. A support member that is rotatably supported around an axis and a vertical axis, a detector that detects the attitude of the support member, and a collimating telescope that is integrally provided with the three-axis optical fiber gyroscope. A surveying device using a characteristic optical fiber gyroscope.
JP24559684A 1984-11-20 1984-11-20 Surveying device using optical fiber gyroscope Granted JPS61122514A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24559684A JPS61122514A (en) 1984-11-20 1984-11-20 Surveying device using optical fiber gyroscope

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24559684A JPS61122514A (en) 1984-11-20 1984-11-20 Surveying device using optical fiber gyroscope

Publications (2)

Publication Number Publication Date
JPS61122514A JPS61122514A (en) 1986-06-10
JPH0456928B2 true JPH0456928B2 (en) 1992-09-10

Family

ID=17136077

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24559684A Granted JPS61122514A (en) 1984-11-20 1984-11-20 Surveying device using optical fiber gyroscope

Country Status (1)

Country Link
JP (1) JPS61122514A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105021162B (en) * 2015-07-24 2017-05-10 西安航光仪器厂 New gyro theodolite locking device

Also Published As

Publication number Publication date
JPS61122514A (en) 1986-06-10

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