JP3515622B2 - Lightwave rangefinder - Google Patents
Lightwave rangefinderInfo
- Publication number
- JP3515622B2 JP3515622B2 JP33324894A JP33324894A JP3515622B2 JP 3515622 B2 JP3515622 B2 JP 3515622B2 JP 33324894 A JP33324894 A JP 33324894A JP 33324894 A JP33324894 A JP 33324894A JP 3515622 B2 JP3515622 B2 JP 3515622B2
- Authority
- JP
- Japan
- Prior art keywords
- light
- objective lens
- lens
- distance meter
- lens system
- 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 - Fee Related
Links
Landscapes
- Measurement Of Optical Distance (AREA)
- Optical Radar Systems And Details Thereof (AREA)
Description
【発明の詳細な説明】
【0001】
【産業上の利用分野】本発明は、視準望遠鏡により測量
点を視準し、その測量点との間で測距光を往復させるこ
とにより測量を行う光波距離計に関する。
【0002】
【従来の技術】従来の光波距離計のひとつに図9の概略
図に示すような単眼式の光波距離計1がある。この単眼
式の光波距離計1は、対物レンズの面積の半分を送光レ
ンズ系の対物レンズ5として、また残りの半分を受光レ
ンズ系の対物レンズ7として利用し、この対物レンズ全
体を視準望遠鏡21の対物レンズとしても利用してい
る。したがってこの対物レンズの後方には視準望遠鏡2
1の接眼レンズ23があるため、発光素子9および受光
素子10はこの対物レンズの焦点位置に配置することが
できない。したがって波長選択特性を持つプリズム41
を視準望遠鏡の光軸内に挿入し、送、受光レンズ系の光
軸を図示のように直角に折り曲げている。
【0003】次に従来の光波距離計の他の例として、図
10および図11の概略図に示すような複眼式の光波距
離計1がある。この複眼式の光波距離計1は、送光レン
ズ系の光軸31、受光レンズ系の光軸32および視準望
遠鏡の光軸33が上記単眼式の場合と異なって同一平面
内に存在しない。このため反射プリズム35にターゲッ
ト45を組み合せ、このターゲット45を視準すれば、
送光光軸31および受光光軸32が反射プリズム35の
入出射面の所定位置をそれぞれ貫くように構成してい
る。このため、発光素子9の漏光が受光素子10に入射
されるような不都合を容易に防ぐことができ、構造が簡
単で小型化しやすい。
【0004】
【発明が解決しようとする課題】しかしながら上記単眼
式光波距離計1の場合、送光レンズ系の対物レンズに
は、1つのレンズを受光レンズ系との間で折半した形で
使用しているから、発光素子9から出る光のほぼ半量
(図9の符号42で示す部分)が無駄になり、その結果
光量不足で測量距離が制限されるという問題があった。
【0005】また高価な波長選択特性を持つプリズム4
1が必要となるだけでなく、精密な組立て作業も必要に
なるから、製造コストが高くつくという問題もあった。
【0006】次に上記複眼式光波距離計1では反射プリ
ズム35に既述のごとくターゲット45を組み込まなけ
ればならない。このため製造コストが増すだけでなく、
測量精度の低下も生じる。特に後者については、反射プ
リズム35を測量点に配置しないで、光をこの測量点に
直接当て、測量する場合、視準点が測量点からずれてい
るために、単眼式の場合と較べると測定精度が低下する
という問題があった。
【0007】本発明は、製造コストを低減しかつ取り扱
いが容易で測量点に反射プリズムを配置する場合であっ
てもそのプリズムに視準望遠鏡用のターゲットを設ける
必要がない光波距離計を提供することを目的とする。
【0008】
【課題を解決するための手段】本発明の光波距離計は、
光軸が平行となるように配置された送光レンズ系および
受光レンズ系と、その光軸が上記送光および上記受光レ
ンズ系の光軸と平行になるように配置された視準望遠鏡
とを備え、上記送光レンズ系の対物レンズの外周縁上の
点と上記受光レンズ系の対物レンズの外周縁上の点とを
結ぶ線分のうち最大の長さが、測量点に配置される反射
プリズムの円形状入出射面の直径とほぼ等しい光波距離
計において、上記視準望遠鏡の対物レンズを上記送光レ
ンズ系の対物レンズと上記受光レンズ系の対物レンズと
の間に配置し、かつそれぞれのレンズの光軸が同一平面
内に含まれるように構成し、上記送光レンズ系の対物レ
ンズおよび上記受光レンズ系の対物レンズには、上記視
準望遠鏡の対物レンズを配置するための切り欠きをそれ
ぞれ形成したものである。
【0009】
【0010】
【実施例】以下、図面を参照して、本発明の光波距離計
の一実施例につき説明する。図1は光波距離計1の正面
図で、送光レンズ系の対物レンズ5(送光用対物レンズ
5)、受光レンズ系の対物レンズ7(受光用対物レンズ
7)および視準望遠鏡用対物レンズ22のレイアウトを
示している。
【0011】送光用対物レンズ5、受光用対物レンズ7
および視準望遠鏡用対物レンズ22はそれぞれ対物レン
ズユニット11の保持部12、13、14に位置決めさ
れて固定される。また送光用対物レンズ5および受光用
対物レンズ7は、1つの接線を共有するような大きさに
構成したから、両者には、視準望遠鏡用対物レンズ22
に対応して切り欠き6、8がそれぞれ形成されている。
【0012】ところでこれらの切り欠き6、8によって
送光用対物レンズ5および受光用対物レンズ7の有効面
積が若干減少し、測量に用いられる光量も少なくなる
が、例えば送光用対物レンズ5および受光用対物レンズ
7の直径がそれぞれ約25ミリ、視準望遠鏡用対物レン
ズ22の直径が約10ミリで、これら3つの対物レンズ
5、7、22のレンズ配置の最大幅が約50ミリ(これ
らの値は従来の複眼式のものとほぼ等しい)であったと
すると、この実施例の切り欠き6、8によって減少する
面積は、従来の複眼式光波距離計の送光および受光用対
物レンズのような切り欠き6、8が無いものの約7%に
過ぎない。
【0013】したがって従来の切り欠きが無いものと比
較しても、測量可能な距離は殆ど変わらず、3つの対物
レンズ5、7、22の光軸が同一平面内に含まれること
により、視準が正確に行えて迅速に測量ができるという
点を考慮すれば、実用上の問題は全く無い。なお上記送
光および受光用対物レンズ5、7の径は、視準望遠鏡用
対物レンズ22と接する大きさから、単眼式光波距離計
用対物レンズの径に近い大きさまでの範囲で選択可能で
ある。
【0014】図2は本発明の光波距離計1の平面図であ
る。光波距離計1の筐体2の一端には対物レンズユニッ
ト11の取付部3が形成されており、この取付部3に対
物レンズユニット11が取り付けられる。
【0015】図3は本発明の光波距離計1の側面図であ
る。従来の複眼式の光波距離計は視準望遠鏡が送光用対
物レンズ5および受光用対物レンズ7の中心を含む平面
に対してオフセットされている都合で筐体の上下高さを
あまり低くできなかったが、本発明の光波距離計1で
は、視準望遠鏡が送光用対物レンズ5および受光用対物
レンズ7の中心を含む平面に対してオフセットされてい
ないため、筐体の上下高さを非常に低くすることができ
る。
【0016】図4は図2のA−A線矢視による概略断面
図である。接眼レンズ23は筐体2の他端に形成された
取付部4に取り付けられ、接眼レンズ23と対物レンズ
22の間に鏡筒24が配置されている。
【0017】図5は図2のB−B線矢視による概略断面
図である。図4に示された受光素子10が図面上で鏡筒
24の奥側に配置され、鏡筒24を挟んで図5に示すよ
うに発光素子9が配置されている(これらの配置は、図
3のC−C線矢視による概略断面図である図6に示すと
おりである)。したがってこの鏡筒24により発光素子
9の漏光が受光素子10に入射されるのを防止できる。
【0018】図7は、本発明の光波距離計1と反射プリ
ズム35とを組み合わせて用いる場合の概略図である。
視準望遠鏡21にて反射プリズム35の中心部分を視準
すると、送光光軸31および受光光軸32が共に視準光
軸33と平行でかつ同一平面内に含まれるので、発光素
子9からの光は確実に反射プリズム35の入出射面に入
り、反射プリズム35の反射面で反射されて受光素子1
0に到達する。
【0019】図8は、反射プリズム35の入出射面に対
する送光用対物レンズ5、受光用対物レンズ7および視
準望遠鏡用対物レンズ22の位置関係を示す概略図であ
る。この図8に示すように、反射プリズム35の入出射
面が最大の面積を有し、対物レンズユニット11内に組
み合わされた送光用対物レンズ5、受光用対物レンズ7
および視準望遠鏡用対物レンズ22がその反射プリズム
35の入出射面内に含まれるようになっている。したが
ってこの図8から明らかなように、視準望遠鏡21で反
射プリズム35の入出射面の中心部分を視準すれば(視
準光軸33を反射プリズム35の入出射面の中心部分に
位置合わせすれば)送光光軸31および受光光軸32は
視準光軸33を中心にして左右方向に等しく振り分けら
れ、必ず反射プリズム35の入出射面内の所定位置をそ
れぞれ貫く。
【0020】以上、本発明の実施例について述べたが、
本発明は上記実施例に限定されるものではない。たとえ
ば、実施例では送光用対物レンズと受光用対物レンズと
が水平方向に並べられているが、これらを垂直方向に並
べてもよい。また、測量距離、気象条件、反射プリズム
の使用、不使用などに合わせて、最適な特性のレンズを
対物レンズユニットとして組み合せ、測量状況に応じて
特性の異なる対物レンズユニットを選択的に用いるよう
にしてもよい。
【0021】また、送光および受光用対物レンズの径を
大きくする場合、これらの対物レンズの焦点同士の間隔
が対物レンズの大径化に伴って接近するので、これらの
対物レンズの大径化は波長選択特性を有するプリズムな
どを用いずに発光素子と受光素子とを配置できる範囲で
行えばよい。
【0022】また実施例においては、送光および受光用
対物レンズのそれぞれに、視準望遠鏡用対物レンズを配
置するための円弧状の切り欠きを形成したが、この切り
欠きの形状は円弧状に限らず、他の形状であってもよ
い。
【0023】たとえば、送光および受光用対物レンズの
それぞれの中心を結ぶ線と直交する面を送光および受光
用対物レンズのそれぞれに形成してもよい。この場合、
送光および受光用対物レンズをそれらの半径方向に対し
て直交するように直線状に切り欠くだけでよいので、切
り欠き加工のコストを下げることができる。
【0024】なお、本発明の光波距離計に用いられる測
量用の制御回路、ディスプレイなどについては、従来と
同様の構成のものを用いることができるため、上記実施
例の説明においてその説明を省略した。また、これらの
制御回路やディスプレイは、光波距離計の筐体に内蔵さ
れるものあるいは、外部装置として光波距離計に接続さ
れるものであってもよい。
【0025】
【発明の効果】上述のように構成された本発明による光
波距離計によれば、視準望遠鏡により視準する位置が送
光レンズ系の光軸と受光レンズ系の光軸との間に位置
し、低コストで構造の簡単な複眼式の光波距離計であり
ながら視準誤差の少ない測量を簡単に行うことができ
る。しかも、3つの対物レンズの配置が非常にコンパク
トであるので、光波距離計を容易に小型化することがで
きる。
【0026】さらに、視準望遠鏡の対物レンズを配置す
るための切り欠きを送光用対物レンズと受光用対物レン
ズとに形成すれば、これらの対物レンズの面積を広くか
つ有効に利用することができ、測量に必要な光量を十分
に確保して、測量可能な距離が極端に短くなるような不
都合を解消することができる。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention performs a survey by collimating a survey point with a collimating telescope and reciprocating distance measuring light to and from the survey point. It relates to a lightwave distance meter. 2. Description of the Related Art As one of conventional lightwave distance meters, there is a monocular lightwave distance meter 1 as schematically shown in FIG. The monocular lightwave distance meter 1 uses half of the area of the objective lens as an objective lens 5 of a light transmitting lens system and the other half as an objective lens 7 of a light receiving lens system, and collimates the entire objective lens. It is also used as an objective lens of the telescope 21. Therefore, the collimating telescope 2 is located behind this objective lens.
Since there is one eyepiece lens 23, the light emitting element 9 and the light receiving element 10 cannot be arranged at the focal position of this objective lens. Therefore, prism 41 having wavelength selection characteristics
Is inserted into the optical axis of the collimating telescope, and the optical axis of the sending and receiving lens system is bent at a right angle as shown in the figure. Next, as another example of a conventional lightwave distance meter, there is a compound eye type lightwave distance meter 1 as shown in schematic views of FIGS. In the compound eye type optical wave distance meter 1, the optical axis 31 of the light transmitting lens system, the optical axis 32 of the light receiving lens system, and the optical axis 33 of the collimating telescope do not exist in the same plane unlike the case of the above-mentioned monocular type. Therefore, if the target 45 is combined with the reflecting prism 35 and this target 45 is collimated,
The light transmitting optical axis 31 and the light receiving optical axis 32 are configured to pass through predetermined positions of the input / output surface of the reflecting prism 35, respectively. For this reason, it is possible to easily prevent such a disadvantage that the light leakage of the light emitting element 9 is incident on the light receiving element 10, and the structure is simple and the size is easily reduced. [0004] However, in the case of the monocular lightwave distance meter 1 described above, one lens is used as the objective lens of the light transmission lens system in such a manner that it is split in half with the light reception lens system. Therefore, almost half of the light emitted from the light emitting element 9 (the portion indicated by reference numeral 42 in FIG. 9) is wasted, and as a result, there is a problem that the survey distance is limited due to insufficient light quantity. A prism 4 having an expensive wavelength selection characteristic
In addition to the necessity of (1), a precise assembling operation is also required, so that there is a problem that the manufacturing cost is high. Next, in the compound eye type optical wave distance meter 1, the target 45 must be incorporated in the reflecting prism 35 as described above. This not only increases manufacturing costs,
There is also a decrease in surveying accuracy. In particular, for the latter, when the reflecting prism 35 is not disposed at the surveying point, and the light is directly applied to the surveying point and the survey is performed, the collimation point is shifted from the surveying point, so that the measurement is performed in comparison with the monocular method. There was a problem that the accuracy was reduced. SUMMARY OF THE INVENTION The present invention provides a lightwave distance meter which reduces the manufacturing cost, is easy to handle, and does not require the provision of a collimating telescope target at the surveying point even when a reflecting prism is arranged at the surveying point. The purpose is to: [0008] The lightwave distance meter according to the present invention comprises:
A light transmitting lens system and a light receiving lens system arranged so that their optical axes are parallel, and a collimating telescope arranged so that their optical axes are parallel to the optical axes of the light transmitting and light receiving lens systems. The maximum length of a line segment connecting a point on the outer peripheral edge of the objective lens of the light transmitting lens system and a point on the outer peripheral edge of the objective lens of the light receiving lens system is a reflection arranged at the surveying point. In a light wave distance meter substantially equal to the diameter of the circular input / output surface of the prism, the objective lens of the collimating telescope is arranged between the objective lens of the light transmission lens system and the objective lens of the light reception lens system, and The optical axis of each lens is included in the same plane, and the objective lens of the light transmitting lens system is
Lens and the objective lens of the light-receiving lens system
Cut out the notch for placing the quasi-telescope objective lens
Each was formed . An embodiment of the present invention will be described below with reference to the accompanying drawings. FIG. 1 is a front view of a lightwave distance meter 1, and shows an objective lens 5 of a light transmission lens system (objective lens 5 for light transmission), an objective lens 7 of a light reception lens system (objective lens 7 of light reception), and an objective lens for a collimating telescope. 22 shows a layout of the second embodiment. Light transmitting objective lens 5, light receiving objective lens 7
In addition, the collimating telescope objective lens 22 is positioned and fixed to the holding portions 12, 13, and 14 of the objective lens unit 11, respectively. Further, since the light-transmitting objective lens 5 and the light-receiving objective lens 7 are configured to have a size that shares one tangent line, both the objective lens 22 and the objective lens 22 for the collimating telescope are provided.
Notches 6 and 8 are respectively formed corresponding to. By the way, the effective areas of the light transmitting objective lens 5 and the light receiving objective lens 7 are slightly reduced by these notches 6 and 8, and the amount of light used for surveying is also reduced. The diameter of the objective lens 7 for receiving light is about 25 mm, the diameter of the objective lens 22 for the collimating telescope is about 10 mm, and the maximum width of the lens arrangement of these three objective lenses 5, 7, 22 is about 50 mm. Is substantially equal to that of the conventional compound-eye type), the area reduced by the notches 6 and 8 of this embodiment is the same as that of the transmitting and receiving objective lenses of the conventional compound-eye type optical distance meter. Only about 7% of those without the notches 6,8. Therefore, the distance that can be measured is almost the same even when compared with the conventional one having no notch, and the optical axes of the three objective lenses 5, 7, 22 are included in the same plane, so that collimation is achieved. There is no practical problem in view of the fact that the measurement can be performed accurately and the survey can be performed quickly. The diameters of the light-transmitting and light-receiving objective lenses 5 and 7 can be selected from a size in contact with the collimating telescope objective lens 22 to a size close to the diameter of the monocular lightwave distance meter objective lens. . FIG. 2 is a plan view of the lightwave distance meter 1 of the present invention. At one end of the housing 2 of the optical distance meter 1, a mounting portion 3 for the objective lens unit 11 is formed, and the objective lens unit 11 is mounted on the mounting portion 3. FIG. 3 is a side view of the lightwave distance meter 1 of the present invention. In the conventional compound eye type optical distance meter, the vertical height of the housing cannot be reduced so much because the collimating telescope is offset with respect to a plane including the centers of the transmitting objective lens 5 and the receiving objective lens 7. However, in the electro-optical distance meter 1 of the present invention, since the collimating telescope is not offset with respect to the plane including the centers of the objective lens 5 for transmitting light and the objective lens 7 for receiving light, the vertical height of the housing is extremely low. Can be lowered. FIG. 4 is a schematic sectional view taken along line AA of FIG. The eyepiece 23 is attached to the attachment part 4 formed at the other end of the housing 2, and a lens barrel 24 is arranged between the eyepiece 23 and the objective lens 22. FIG. 5 is a schematic sectional view taken along line BB of FIG. The light receiving element 10 shown in FIG. 4 is arranged on the back side of the lens barrel 24 in the drawing, and the light emitting element 9 is arranged as shown in FIG. FIG. 6 is a schematic cross-sectional view taken along line CC of FIG. 3). Therefore, the light leakage of the light emitting element 9 can be prevented from being incident on the light receiving element 10 by the lens barrel 24. FIG. 7 is a schematic diagram showing a case where the lightwave distance meter 1 of the present invention and the reflecting prism 35 are used in combination.
When the collimating telescope 21 collimates the central portion of the reflecting prism 35, the light transmitting optical axis 31 and the light receiving optical axis 32 are both parallel to the collimating optical axis 33 and included in the same plane. Light surely enters the entrance / exit surface of the reflecting prism 35, is reflected by the reflecting surface of the reflecting prism 35, and
Reach 0. FIG. 8 is a schematic diagram showing the positional relationship between the light transmitting objective lens 5, the light receiving objective lens 7, and the collimating telescope objective lens 22 with respect to the entrance / exit surface of the reflecting prism 35. As shown in FIG. 8, the input / output surface of the reflecting prism 35 has the largest area, and the light transmitting objective lens 5 and the light receiving objective lens 7 combined in the objective lens unit 11.
The collimating telescope objective lens 22 is included in the entrance / exit surface of the reflecting prism 35. Therefore, as is apparent from FIG. 8, if the collimating telescope 21 collimates the center of the entrance / exit surface of the reflecting prism 35 (the collimating optical axis 33 is aligned with the central portion of the entrance / exit surface of the reflecting prism 35). The transmitting optical axis 31 and the receiving optical axis 32 are equally distributed in the left-right direction about the collimating optical axis 33, and always pass through predetermined positions in the input / output surface of the reflecting prism 35. While the embodiments of the present invention have been described above,
The present invention is not limited to the above embodiment. For example, in the embodiment, the light transmitting objective lens and the light receiving objective lens are arranged in the horizontal direction, but they may be arranged in the vertical direction. In addition, according to the surveying distance, weather conditions, use or non-use of the reflective prism, etc., a lens with optimal characteristics is combined as an objective lens unit, and an objective lens unit with different characteristics is selectively used according to the surveying situation. You may. When the diameter of the objective lens for transmitting and receiving light is increased, the distance between the focal points of these objective lenses becomes closer as the diameter of the objective lens increases, so that the diameter of these objective lenses increases. May be performed within a range where the light emitting element and the light receiving element can be arranged without using a prism having a wavelength selection characteristic. Further, in the embodiment, an arc-shaped notch for arranging the collimating telescope objective lens is formed in each of the light transmitting and receiving objective lenses, but the shape of the notch is circular. The shape is not limited to this, and may be another shape. For example, a plane orthogonal to a line connecting the centers of the light transmitting and light receiving objective lenses may be formed on each of the light transmitting and light receiving objective lenses. in this case,
Since it is only necessary to cut out the light transmitting and receiving objective lenses in a straight line so as to be orthogonal to their radial directions, the cost of the notch processing can be reduced. The control circuit, display, and the like for surveying used in the lightwave distance meter of the present invention can have the same configuration as that of the conventional one, so that the description thereof is omitted in the description of the above embodiment. . Further, these control circuits and displays may be built in the housing of the electro-optical distance meter or connected to the electro-optical distance meter as an external device. According to the lightwave distance meter according to the present invention configured as described above, the position collimated by the collimating telescope is set between the optical axis of the light transmitting lens system and the optical axis of the light receiving lens system. Although it is a low-cost, simple-structure compound-wave type optical distance meter located between the two, it is possible to easily perform surveying with a small collimation error. In addition, since the arrangement of the three objective lenses is very compact, the optical distance meter can be easily reduced in size. Further, if cutouts for disposing the objective lens of the collimating telescope are formed in the light transmitting objective lens and the light receiving objective lens, the area of these objective lenses can be widely and effectively used. It is possible to secure a sufficient amount of light required for surveying, and to solve the problem that the distance that can be measured becomes extremely short.
【図面の簡単な説明】
【図1】本発明の光波距離計の一実施例の概略正面図で
ある。
【図2】図1に示した光波距離計の概略平面図である。
【図3】図1に示した光波距離計の概略側面図である。
【図4】図2のA−A線矢視による概略断面図である。
【図5】図2のB−B線矢視による概略断面図である。
【図6】図3のC−C線矢視による概略断面図である。
【図7】本発明の光波距離計と反射プリズムとを組み合
わせて用いる場合の概略図である。
【図8】反射プリズムの入出射面に対する本発明の光波
距離計の送光用対物レンズ、受光用対物レンズおよび視
準望遠鏡用対物レンズの位置関係を示す概略図である。
【図9】従来の単眼式の光波距離計の概略図である。
【図10】従来の複眼式の光波距離計の概略平面図であ
る。
【図11】図10に示す複眼式光波距離計の概略側面図
である。
【符号の説明】
1 光波距離計
5 送光用対物レンズ
6 切り欠き
7 受光用対物レンズ
8 切り欠き
21 視準望遠鏡
22 視準望遠鏡用対物レンズ
31 送光光軸
32 受光光軸
33 視準光軸
35 反射プリズムBRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a schematic front view of one embodiment of a lightwave distance meter according to the present invention. FIG. 2 is a schematic plan view of the lightwave distance meter shown in FIG. FIG. 3 is a schematic side view of the lightwave distance meter shown in FIG. FIG. 4 is a schematic sectional view taken along line AA of FIG. 2; FIG. 5 is a schematic sectional view taken along line BB of FIG. 2; FIG. 6 is a schematic sectional view taken along line CC of FIG. 3; FIG. 7 is a schematic diagram of a case where the lightwave distance meter of the present invention and a reflecting prism are used in combination. FIG. 8 is a schematic diagram showing a positional relationship between a light transmitting objective lens, a light receiving objective lens, and a collimating telescope objective lens of the lightwave distance meter of the present invention with respect to an entrance / exit surface of a reflection prism. FIG. 9 is a schematic diagram of a conventional monocular lightwave distance meter. FIG. 10 is a schematic plan view of a conventional compound eye type light wave distance meter. 11 is a schematic side view of the compound eye type optical wave distance meter shown in FIG. [Description of Signs] 1 Lightwave distance meter 5 Transmitting objective lens 6 Notch 7 Receiving objective lens 8 Notch 21 Collimating telescope 22 Collimating telescope objective lens 31 Transmitting optical axis 32 Receiving optical axis 33 Collimating light Axis 35 Reflecting prism
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 実開 昭59−144482(JP,U) (58)調査した分野(Int.Cl.7,DB名) G01C 3/00 - 3/32 G01C 15/00 - 15/14 G01S 7/48 - 7/51 G01S 17/00 - 17/95 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References Japanese Utility Model Sho 59-144482 (JP, U) (58) Fields investigated (Int. Cl. 7 , DB name) G01C 3/00-3/32 G01C 15 / 00-15/14 G01S 7/48-7/51 G01S 17/00-17/95
Claims (1)
ンズ系および受光レンズ系と、 その光軸が上記送光および上記受光レンズ系の光軸と平
行になるように配置された視準望遠鏡とを備え、 上記送光レンズ系の対物レンズの外周縁上の点と上記受
光レンズ系の対物レンズの外周縁上の点とを結ぶ線分の
うち最大の長さが、測量点に配置される反射プリズムの
円形状入出射面の直径とほぼ等しい光波距離計におい
て、 上記視準望遠鏡の対物レンズを上記送光レンズ系の対物
レンズと上記受光レンズ系の対物レンズとの間に配置
し、かつそれぞれのレンズの光軸が同一平面内に含まれ
るように構成し、上記送光レンズ系の対物レンズおよび上記受光レンズ系
の対物レンズには、上記視準望遠鏡の対物レンズを配置
するための切り欠きをそれぞれ形成 したことを特徴とす
る光波距離計。(57) Claims 1. A light-sending lens system and a light-receiving lens system arranged so that their optical axes are parallel to each other, and the optical axes of the light-sending and light-receiving lens systems are the optical axes of the light-sending and light-receiving lens systems. And a collimating telescope arranged so as to be parallel to a line segment connecting a point on the outer peripheral edge of the objective lens of the light transmitting lens system and a point on the outer peripheral edge of the objective lens of the light receiving lens system. In the optical distance meter, the maximum length of which is substantially equal to the diameter of the circular entrance / exit surface of the reflection prism disposed at the surveying point, the objective lens of the collimating telescope and the objective lens of the light transmission lens system and the light reception lens system is arranged between the objective lens and configured as an optical axis of each lens is included in the same plane, the objective lens and the light receiving lens system of the light transmitting lens system
The objective lens of the collimating telescope is placed on the objective lens
An electro-optical distance meter characterized by forming cutouts for each .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP33324894A JP3515622B2 (en) | 1994-12-15 | 1994-12-15 | Lightwave rangefinder |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP33324894A JP3515622B2 (en) | 1994-12-15 | 1994-12-15 | Lightwave rangefinder |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH08166238A JPH08166238A (en) | 1996-06-25 |
| JP3515622B2 true JP3515622B2 (en) | 2004-04-05 |
Family
ID=18263988
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP33324894A Expired - Fee Related JP3515622B2 (en) | 1994-12-15 | 1994-12-15 | Lightwave rangefinder |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3515622B2 (en) |
-
1994
- 1994-12-15 JP JP33324894A patent/JP3515622B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH08166238A (en) | 1996-06-25 |
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