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JP3459287B2 - Three-dimensional coordinate measuring method and three-dimensional coordinate measuring device for measuring three-dimensional coordinates by removing unnecessary light - Google Patents
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JP3459287B2 - Three-dimensional coordinate measuring method and three-dimensional coordinate measuring device for measuring three-dimensional coordinates by removing unnecessary light - Google Patents

Three-dimensional coordinate measuring method and three-dimensional coordinate measuring device for measuring three-dimensional coordinates by removing unnecessary light

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Publication number
JP3459287B2
JP3459287B2 JP00058494A JP58494A JP3459287B2 JP 3459287 B2 JP3459287 B2 JP 3459287B2 JP 00058494 A JP00058494 A JP 00058494A JP 58494 A JP58494 A JP 58494A JP 3459287 B2 JP3459287 B2 JP 3459287B2
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Japan
Prior art keywords
light
light receiving
signal
plane
reflected
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JP00058494A
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JPH07208990A (en
Inventor
菊雄 志村
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株式会社ソキア
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Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は三次元座標測定装置及び
三次元座標測定方法に関し、特に、複数の返光手段と複
数の平面光を用い、幾何学的に測定点との距離を求めて
三次元座標の値を算出するものに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a three-dimensional coordinate measuring device and a three-dimensional coordinate measuring method, and more particularly, to geometrically obtain a distance from a measuring point by using a plurality of returning means and a plurality of plane lights. The present invention relates to a device for calculating values of three-dimensional coordinates.

【0002】[0002]

【従来の技術】一般に、測定点の三次元の位置を測定す
るためには、基準点に測距儀及び測角儀を置き、該測定
点の高度角と基準方向との水平角を測角儀で測定し、更
に測距儀と反射板を使用して射出光と反射光との位相差
から基準点と測定点との距離を求めていた。
2. Description of the Related Art Generally, in order to measure the three-dimensional position of a measuring point, a rangefinder and a rangefinder are placed at a reference point, and the horizontal angle between the altitude angle and the reference direction of the measuring point is measured. The distance between the reference point and the measurement point was calculated from the phase difference between the emitted light and the reflected light by using a rangefinder and a reflector.

【0003】しかしながら近年では、光の位相差を測定
して距離を求めるのではなく、複数の平面光を複数の反
射手段で反射させ、受光素子が反射光を受光したときの
平面光の方向が基準方向と成す角度を測定し、前記角度
を変数とする方程式を連立させ、これを解いて測定点の
三次元座標の値を求めている。これを簡単に説明するた
めに、図4に測定方法の原理を示す。
However, in recent years, instead of measuring the phase difference of light to obtain the distance, a plurality of plane lights are reflected by a plurality of reflecting means, and the direction of the plane light when the light receiving element receives the reflected light is changed. The angle formed with the reference direction is measured, the equations having the angle as a variable are made simultaneous, and the equations are solved to obtain the value of the three-dimensional coordinate of the measurement point. In order to explain this simply, FIG. 4 shows the principle of the measuring method.

【0004】図4(a)を参照して、aは測定装置本体で
あり、互いに交叉する2つの平面光b1、b2を照射する
照射手段cを備えている。前記複数の平面光はスタッフ
dの備える2つの返光手段e1、e2で返光され、前記測
定装置本体aが備える受光手段に入射する。
Referring to FIG. 4 (a), reference numeral a denotes a measuring device main body, which is provided with an irradiation means c for irradiating two plane lights b1 and b2 intersecting each other. The plurality of plane lights are returned by the two light returning means e1 and e2 included in the stuff d, and enter the light receiving means included in the measuring apparatus main body a.

【0005】前記測定装置本体aは、基準位置Pに配置
されており、測定中心Oを原点として、既知点等がある
基準方向の水平成分をX軸にとり、これと水平面内で直
角な方向をY軸にとり、X−Y平面と垂直な方向をZ軸
にとって座標軸を定めている。
The measuring apparatus main body a is arranged at a reference position P, and a horizontal component in a reference direction having a known point or the like is taken as an origin with the measurement center O as an origin, and a direction perpendicular to the horizontal component in a horizontal plane. With respect to the Y-axis, the coordinate axis is defined with the direction perpendicular to the XY plane as the Z-axis.

【0006】なお、ここでは測定原理を簡単にするため
に、前記スタッフdは測定点Q上に鉛直に立てられてお
り、前記2つの返光手段e1、e2は前記スタッフdの該
鉛直線上に配置されているものとする。又、座標原点O
は、前記互いに交叉する2つの平面光b1、b2の張る平
面内にあるものとする。
Here, in order to simplify the measurement principle, the stuff d is erected vertically on the measuring point Q, and the two returning means e1 and e2 are on the vertical line of the stuff d. It is supposed to be arranged. Also, the coordinate origin O
Is in the plane defined by the two plane lights b1 and b2 intersecting with each other.

【0007】前記照射手段cが基準方向であるX軸方向
を向いているとき、即ち前記照射手段cと基準方向との
成す角度がゼロであるときの、前記2つの平面光b1、
b2の張る平面の方程式をそれぞれ、 k・x+m・y+n・z = 0 …… (1) p・x+q・y+r・z = 0 …… (2) とする。なお、前記2つの平面光は互いに交叉するの
で、(1)式で表される平面の法線ベクトル(k,m,
n)と(2)式で表される平面の法線ベクトル(p,q,
r)とは相異なるものである。
The two plane lights b1 when the irradiating means c faces the X-axis direction which is the reference direction, that is, when the angle formed by the irradiating means c and the reference direction is zero.
The equations of the plane spanned by b2 are respectively defined as k · x + m · y + n · z = 0 (1) p · x + q · y + r · z = 0 (2). Since the two plane lights intersect each other, the plane normal vector (k, m,
n) and the plane normal vector (p, q,
It is different from r).

【0008】前記2つの平面光b1、b2は、測定装置本
体aの備える回転手段で図4(a)上では時計回りと反対
方向に、Z軸を一の回転軸として回転移動させられる。
The two plane lights b1 and b2 are rotationally moved in the counterclockwise direction in FIG. 4 (a) with the Z axis as one axis of rotation by the rotating means provided in the measuring apparatus main body a.

【0009】前記平面光b1が基準方向から角度θ1回転
移動して前記返光手段e1に入射したときの該平面光b1
の張る平面の方程式を、 k’・x+m’・y+n’・z = 0 …… (4) で表すと、該平面の法線ベクトル(k’,m’,n’)
は、(1)式で表される元の平面の法線ベクトル(k,
m,n)と次の関係がある。
The plane light b1 when the plane light b1 is rotated by an angle θ1 from the reference direction and is incident on the light returning means e1.
When the equation of the plane spanned by is expressed by k ′ · x + m ′ · y + n ′ · z = 0 (4), the normal vector (k ′, m ′, n ′) of the plane is expressed.
Is the normal vector (k,
m, n) has the following relationship.

【0010】[0010]

【数1】 [Equation 1]

【0011】又、前記平面光b2が基準方向から角度θ2
回転移動して前記返光手段e1に入射したときの該平面
光b2の張る平面の方程式を、 p’・x+q’・y+r’・z = 0 …… (7) で表すと、該平面の法線ベクトル(p’,q’,r’)
は、(2)式で表される元の平面の法線ベクトル(p,
q,r)と次の関係がある。
The plane light b2 has an angle θ2 from the reference direction.
When the equation of the plane spanned by the plane light b2 when it is rotationally moved and is incident on the light returning means e1 is expressed by p ′ · x + q ′ · y + r ′ · z = 0 (7), the law of the plane is obtained. Line vector (p ', q', r ')
Is the normal vector of the original plane (p,
q, r) has the following relationship.

【0012】[0012]

【数2】 [Equation 2]

【0013】ところで、前記返光手段e1は、(4)式の
平面と(7)式の平面とのいずれの平面にも含まれるの
で、両平面の交線である直線s上に位置することにな
る。又、2つの平面光b1、b2は原点を含むものとした
ので、該直線sは原点Oを通り、その方程式は x/A = y/B = z/C ……(11) で表すことができる。そして、該直線sの方向余弦
(A,B,C)と、前記(4)式と(7)式の平面の法線ベ
クトル(k’,m’,n’)、(p’,q’,r’)と
には、 k’・A + m’・B +n’・C = 0 ……(12) p’・A + q’・B +r’・C = 0 ……(13) の関係があるので、前記2つの平面光b1、b2が返光手
段e1に入射したときに基準方向と成す角度θ1、θ2を
測定し、元の2つの平面の方程式(1)、(2)を順次(5)
式、(8)式、(12)式、(13)式を用いて変形すれば、
(11)式で表した直線sの方向余弦の値を得ることがで
きる。
By the way, since the returning means e1 is included in both the plane of the equation (4) and the plane of the equation (7), it should be located on the straight line s which is the intersection of the two planes. become. Since the two plane lights b1 and b2 include the origin, the straight line s passes through the origin O, and its equation can be expressed by x / A = y / B = z / C (11) it can. Then, the direction cosine (A, B, C) of the straight line s and the normal vectors (k ', m', n ') of the planes of the equations (4) and (7), (p', q '). , R ′) and the relation of k ′ · A + m ′ · B + n ′ · C = 0 (12) p ′ · A + q ′ · B + r ′ · C = 0 ... (13) Therefore, when the two plane lights b1 and b2 are incident on the light returning means e1, the angles θ1 and θ2 formed with the reference direction are measured, and the equations (1) and (2) of the two original planes are sequentially calculated. (5)
By using the equations (8), (12), and (13),
The value of the direction cosine of the straight line s expressed by the equation (11) can be obtained.

【0014】次に、前記平面光b1が基準方向から角度
φ1回転移動して前記返光手段e2に入射したときの該平
面光b1の張る平面の方程式を k”・x+m”・y+n”・z = 0 ……(21) で表すと、該平面の法線ベクトル(k”,m”,n”)
は、(1)式で表した元の平面の法線ベクトル(k,m,
n)と次の関係がある。
Next, the equation of the plane spanned by the plane light b1 when the plane light b1 moves by an angle φ1 from the reference direction and enters the light returning means e2 is k ".x + m" .y + n ".z. = 0 (21), the normal vector (k ″, m ″, n ″) of the plane
Is the normal vector (k, m,
n) has the following relationship.

【0015】[0015]

【数3】 [Equation 3]

【0016】又、前記平面光b2が基準方向から角度φ2
回転移動して前記返光手段e2に入射したときの該平面
光b2の張る平面の方程式を、 p”・x+q”・y+r”・z = 0 ……(23) で表すと、該平面の法線ベクトル(p”,q”,r”)
は、(2)式で表した元の平面の法線ベクトル(p,q,
r)と次の関係がある。
Further, the plane light b2 has an angle φ2 from the reference direction.
When the equation of the plane spanned by the plane light b2 when it is rotationally moved and is incident on the light returning means e2 is represented by p ″ · x + q ″ · y + r ″ · z = 0 (23), the law of the plane is obtained. Line vector (p ", q", r ")
Is the normal vector (p, q,
It has the following relationship with r).

【0017】[0017]

【数4】 [Equation 4]

【0018】従って、(11)式を導いたのと同様に、該
返光手段e2は、(21)式の平面と(23)式の平面の交
線である次式で表せる直線t上に位置する。
Therefore, similarly to the case where the formula (11) is derived, the light returning means e2 is on the straight line t which can be expressed by the following formula which is the intersection of the plane of the formula (21) and the plane of the formula (23). To position.

【0019】 x/D = y/E = z/F ……(25) 又、該直線tの方向余弦(C,E,F)と、(21)式と
(22)式の平面の法線ベクトル(k”,m”,n”)、
(p”,q”,r”)とは、 k”・D + m”・E +n”・F = 0 ……(26) p”・D + q”・E +r”・F = 0 ……(27) の関係がある。従って、(11)式で表した直線sの法
線ベクトルの各要素を得るのと同様に、元の2つの平面
の方程式(1)、(2)を、順次(22)式、(24)式、(2
6)式、(27)式を用いて変形すれば、(25)式で表し
た直線tの方向余弦の値を得ることができる。
X / D = y / E = z / F (25) Further, the direction cosine (C, E, F) of the straight line t and the equation (21)
The plane normal vector (k ″, m ″, n ″) of the equation (22),
(P ", q", r ") is k" .D + m ".E + n" .F = 0 ... (26) p ".D + q" .E + r ".F = 0 ... Therefore, there is a relation of (27), so that the equations (1) and (2) of the original two planes are sequentially calculated in the same manner as in obtaining each element of the normal vector of the straight line s expressed by the equation (11). Expression (22), Expression (24), (2
By modifying using equations (6) and (27), the value of the direction cosine of the straight line t represented by equation (25) can be obtained.

【0020】なお、ここでは返光手段e1と返光手段e2
とを結ぶ線分がX−Y平面に垂直であるので、直線sと
直線tの方向余弦のx軸要素の間で、 D = v・A ……(28) なるスカラー量vを導入すれば、y軸要素とz軸要素と
の間には次の関係が成立する。
Here, the light returning means e1 and the light returning means e2
Since the line segment connecting to and is perpendicular to the XY plane, if a scalar quantity v of D = v · A (28) is introduced between the x-axis element of the direction cosine of the line s and the line t. , Y-axis elements and z-axis elements have the following relationship.

【0021】 E = v・B 、 F ≠ v・C ……(29) なお、2つの平面光が必ず一定の順序でスタッフに入射
する様に、前記平面光b1と平面光b2をV字形に射出す
れば、スタッフ上の上方に位置する返光手段から順に返
光されるので、入射光がどの方程式に属するものである
かを特定することができる。そして、そのときの各平面
光が基準方向と成す角度θ1、θ2、φ1とφ2を測定すれ
ば、直線sの方程式(11)式と直線tの方程式(25)式
を得ることができる。
E = vB, F ≠ vC (29) It should be noted that the plane light b1 and the plane light b2 are V-shaped so that the two plane lights always enter the stuff in a fixed order. When the light is emitted, the light is returned in order from the light returning means located above the staff, so that it is possible to specify which equation the incident light belongs to. Then, by measuring the angles θ1, θ2, φ1 and φ2 formed by the respective plane lights at that time, the equation (11) of the straight line s and the equation (25) of the straight line t can be obtained.

【0022】前記2つの直線s、tと前記2つの返光手
段e1、e2の位置関係を図4(b)に示す。図4(b)を参
照して、Q’は前記測定点QからX−Y平面に降ろした
垂線の足であり、前記返光手段e1とe2とは予め定めら
れた長さh1を隔てて両方ともこの垂線上に位置してい
る。
The positional relationship between the two straight lines s and t and the two light returning means e1 and e2 is shown in FIG. 4 (b). Referring to FIG. 4 (b), Q'is a leg of a perpendicular line drawn from the measurement point Q to the XY plane, and the light returning means e1 and e2 are separated by a predetermined length h1. Both are located on this perpendicular.

【0023】前記原点Oと前記垂線の足Q’とを結ぶ線
分をu、その長さをLとすると、長さL及びh1と、直
線sと線分uの成す角度α及び直線tと線分uの成す角
度βとの間には次の関係が成り立つ。
When the line segment connecting the origin O and the perpendicular foot Q'is u and its length is L, the lengths L and h1 and the angle α formed by the line s and the line segment u and the line t are defined. The following relation holds with the angle β formed by the line segment u.

【0024】 L・tan(α) − L・tan(β) = h1 ……(31) 従って、線分uの長さLは、 L = h1/(tan(α)−tan(β)) ……(32) と表すことができる。ここで、ベクトル(x,y,z)
の大きさを、‖(x,y,z)‖で表すものとすると、
(32)式のtan(α)とtan(β)は、それぞれ、 tan(α) = ‖(A,B,C)‖/‖(A,B,0 )‖ ……(33) tan(β) = ‖(D,E,F)‖/‖(E,F,0 )‖ ……(34) で表せるので、前記2つの直線s、tの方向余弦、(1
1)式と(25)式から、角度αと角度βを測定しなくて
もその値を求めることができ、(32)、(33)、(34)
式から、線分uの長さLを得ることができる。
L · tan (α) −L · tan (β) = h1 (31) Therefore, the length L of the line segment u is L = h1 / (tan (α) −tan (β)) ... It can be expressed as (32). Where the vector (x, y, z)
If the magnitude of is represented by ‖ (x, y, z) ‖,
Tan (α) and tan (β) in the equation (32) are respectively tan (α) = ‖ (A, B, C) ‖ / ‖ (A, B, 0) ‖ …… (33) tan (β ) = ‖ (D, E, F) ‖ / ‖ (E, F, 0) ‖ ... (34) Therefore, the direction cosine of the two straight lines s and t, (1
From equations (1) and (25), the values can be obtained without measuring the angle α and the angle β. (32), (33), (34)
From the formula, the length L of the line segment u can be obtained.

【0025】一方、測定点Qが基準方向であるX軸と成
す水平角、即ち、前記線分uがX軸と成す角度をγとお
くと、その正接は該線分uの方向余弦(A,B, 0)よ
り直ちに、 tan(γ) = A/B ……(35) として求めることができる。
On the other hand, if the horizontal angle formed by the measurement point Q with the X axis that is the reference direction, that is, the angle formed by the line segment u with the X axis is γ, the tangent is the direction cosine (A) of the line segment u. , B, 0), tan (γ) = A / B (35)

【0026】又、スタッフdの下端部に位置する測定点
Qとスタッフd上にある返光手段e2との長さをh2が予
め定められているものとすると、測定点Qの高度角ζの
正接は、 tan(ζ) = (L・tan(β)−h2)/L ……(41) により直ちに求めるられる。
Assuming that the length h2 of the measuring point Q located at the lower end of the stuff d and the returning means e2 on the stuff d is predetermined, the altitude angle ζ of the measuring point Q is The tangent is immediately obtained by tan (ζ) = (L · tan (β) −h2) / L (41).

【0027】以上により、測定点Qの三次元座標(x,
y,z)は、 x = L・cos(γ) ……(45) y = L・sin(γ) ……(46) z = L・tan(ζ) ……(47) で求めることができる。
From the above, the three-dimensional coordinates (x,
y, z) can be obtained by x = L · cos (γ) …… (45) y = L · sin (γ) …… (46) z = L · tan (ζ) …… (47) .

【0028】以上概説した様に、2つの平面光b1とb2
が2つの返光手段により返光されたときの角度θ1、θ
2、φ1、及びφ2を測定すれば、位相差測定等により直
接測定点との水平距離を測定したり、測角儀等により直
接水平角γや高度角ζを測定しなくても、測定点までの
水平距離や水平角及び高度角の正接を算出することがで
き、これらの値により測定点Qの三次元座標の値を求め
ることができる。
As outlined above, two plane lights b1 and b2
Angles θ1 and θ when the light is returned by the two light returning means
If 2, φ1 and φ2 are measured, the horizontal distance from the measuring point can be directly measured by phase difference measurement, etc., and even if the horizontal angle γ and altitude angle ζ are not directly measured by a gyroscope, etc. It is possible to calculate the horizontal distance and the tangent of the horizontal angle and the altitude angle, and the values of the three-dimensional coordinates of the measurement point Q can be obtained from these values.

【0029】[0029]

【発明が解決しようとする課題】しかしながら、前記測
定点Qの周囲に窓ガラス等の光学的な反射面を有する建
造物が存在する場合があり、前記測定装置本体から照射
された各平面光が返光手段で返光された反射光だけでは
なく、窓ガラス等により反射された発生した反射光をも
受光してしまい、かかる場合には三次元座標測定を行う
ことができなくなってしまう。
However, there may be a building having an optical reflection surface such as a window glass around the measuring point Q, and each plane light emitted from the measuring apparatus main body is Not only the reflected light returned by the light returning means but also the generated reflected light reflected by the window glass or the like is received, and in such a case, three-dimensional coordinate measurement cannot be performed.

【0030】[0030]

【課題を解決するための手段】上記課題を解決するため
に、請求項1記載の発明は、互いに交叉する複数の平面
光を照射する照射手段とその反射光を受光して信号を出
力する複数の受光手段とを備えた測定装置本体と、複数
の返光手段を備えたスタッフとから成る三次元座標測定
システムを用いる三次元座標測定方法であって、測定点
上に前記スタッフを配置し、前記複数の平面光を一の回
転軸を中心に回転移動させて前記スタッフの備える複数
の返光手段に照射し、各々の返光手段により返光された
反射光を前記受光手段により受光し、前記受光手段が受
光したときの各平面光の回転角度と各々の返光手段がス
タッフ上の配置された位置とにより測定点の三次元座標
を求める三次元座標測定方法において、前記複数の返光
手段にコーナープリズムを用い、前記複数の平面光の回
転移動に伴い、前記受光手段で受光する反射光が移動す
る方向を検出し、該検出した方向が前記平面光の回転移
動方向と同方向か逆方向かによって、受光手段で受光し
た反射光がコーナープリズムにより返光された反射光な
のかコーナープリズム以外の反射面により反射された反
射光なのかを判別し、コーナープリズムにより返光され
反射光が受光手段に入射したときの前記回転角度のみ
に基いて測定点の三次元座標の値を算出することを特徴
とし、請求項2記載の発明は、請求項1記載の三次元座
標測定法方において前記受光手段は第1受光部と第2受
光部とを有し、それぞれが前記一の回転軸を中心に周設
して成り、前記第1受光部と前記第2受光部が反射光を
受光した順番を検出し、その順番に基づいて前記受光手
段で受光した反射光が移動する方向を検出することを特
徴とし、請求項3記載の発明は、請求項1又は請求項2
記載の三次元座標測定方法に用いられる三次元座標測定
装置であって、前記受光手段は、反射光を受光して第1
検出信号を出力する第1受光部と、反射光を受光して第
2受光信号を出力する第2受光部から成り、前記第1受
光部と第2受光部は前記一の回転軸を中心にして前記回
転手段の回転方向と同じ方向に配置され、前記測定装置
本体は、前記第1受光信号から前記第2受光信号を差し
引いた差信号を出力する減算手段と、前記第1受光信号
と前記第2受光信号を加えた和信号を出力する加算手段
と、第1閾値を基準として、該第1閾値よりも大きい場
合をハイ状態とし、小さい場合をロー状態として前記差
信号を2値化した2値化差信号を出力する差信号比較器
と、第1閾値よりも大きい第2閾値を基準として、該第
2閾値よりも大きい場合をハイ状態とし、小さい場合を
ロー状態として前記和信号を2値化した2値化和信号を
出力する和信号比較器と、前記2値化差信号と前記2値
化和信号とを受信して、前記2値化和信号がハイ状態で
あって前記2値化差信号がロー状態からハイ状態に変わ
ったときにパルス信号を出力するパルス回路と、前記パ
ルス信号を受信したときの前記回転手段の回転角度を記
憶する角度記憶手段を備え、前記角度記憶手段に記憶さ
れた角度に基いて測定点の三次元座標を算出する演算装
置を備えたことを特徴とする。
In order to solve the above-mentioned problems, the invention according to claim 1 irradiates a plurality of plane lights intersecting with each other with a plane light and a plurality of light receiving means for receiving the reflected light and outputting a signal. A three-dimensional coordinate measuring method using a three-dimensional coordinate measuring system comprising a measuring device main body having a light receiving means and a staff having a plurality of light returning means, wherein the staff is arranged on a measuring point, wherein the plurality of planar light by rotational movement around a first rotation axis by irradiating a plurality of Kaehikari means provided in the said staff were Kaehikari by each Kaehikari means
Three-dimensional calculation of the three-dimensional coordinates of the measurement point by receiving the reflected light by the light receiving means and the rotation angle of each plane light when the light receiving means receives the light and the position where each light returning means is arranged on the staff In the coordinate measuring method, a corner prism is used for the plurality of light returning means, and the reflected light received by the light receiving means moves along with the rotational movement of the plurality of plane lights .
Direction of the plane light is detected.
Depending on whether it is the same direction as the moving direction or the opposite direction,
The reflected light returned by the corner prism.
The anti-reflection reflected by a reflecting surface other than a corner prism
It is characterized in that the value of the three-dimensional coordinate of the measurement point is calculated based on only the rotation angle when the reflected light returned by the corner prism is incident on the light receiving means by determining whether it is incident light or not. According to a second aspect of the present invention, in the three-dimensional coordinate measuring method according to the first aspect, the light receiving means has a first light receiving portion and a second light receiving portion, each of which surrounds the one rotation axis. And detecting the order in which the first light receiving portion and the second light receiving portion receive reflected light, and based on the order,
The invention according to claim 3 is characterized in that the direction in which the reflected light received by the step moves is detected.
A three-dimensional coordinate measuring device used in the three-dimensional coordinate measuring method described above, wherein the light receiving means receives the reflected light and receives the first light.
A first light receiving unit for outputting a detection signal, comprises a second light receiving section for outputting a second light receiving signal by receiving the reflected light, the first light receiving portion and the second light receiving portion is centered on the axis rotation of the one Is arranged in the same direction as the rotating direction of the rotating means, and the measuring device main body outputs subtraction means for subtracting the second light receiving signal from the first light receiving signal, the first light receiving signal and the subtracting means. The adding means for outputting a sum signal to which the second light receiving signal is added, and the first threshold value as a reference, the difference signal is binarized by setting it to a high state when larger than the first threshold value and a low state when smaller than the first threshold value. Based on a difference signal comparator that outputs a binarized difference signal and a second threshold value that is larger than the first threshold value, the sum signal is defined as a high state when it is larger than the second threshold value and a low state when it is smaller than the second threshold value. Sum signal ratio that outputs the binarized sum signal And a binarized difference signal and the binarized sum signal, and the binarized sum signal is in a high state and the binarized difference signal changes from a low state to a high state. A pulse circuit for outputting a pulse signal, and an angle storage means for storing a rotation angle of the rotation means when the pulse signal is received, and a three-dimensional measurement point based on the angle stored in the angle storage means. It is characterized by comprising an arithmetic device for calculating coordinates.

【0031】[0031]

【作用】スタッフの備える各返光手段をコーナープリズ
ムとしたので、測定装置本体が照射し、回転移動させる
平面光の移動方向と、該平面光がコーナープリズムで返
光されて成る反射光との移動方向とは互いに逆方向とな
る。一方、平面光が窓ガラス等の反射面で反射された場
合には、該反射光の移動方向と平面光の移動方向とは同
じ方向になるので、受光手段が受光した反射光の移動方
向を測定装置本体が照射した平面光の移動方向と比較す
ることでいずれの反射光を受光したかを区別することが
できる。これにより、測定に不要な反射光を受光して生
じた信号を除去することができる。
Since each of the light returning means provided in the staff is a corner prism, the direction of movement of the plane light that is irradiated by the measuring apparatus main body and is rotationally moved, and the reflected light obtained by returning the plane light by the corner prism. The directions of movement are opposite to each other. On the other hand, when the planar light is reflected by the reflecting surface such as window glass, since in the same direction as the moving direction of the moving direction and the plane light reflected light, the movement direction of the reflected light receiving means has received It is possible to distinguish which reflected light is received by comparing with the moving direction of the plane light emitted by the measuring device body. This makes it possible to remove a signal generated by receiving reflected light unnecessary for measurement.

【0032】又、特に受光手段に第1受光部と第2受光
部とを設けこれを平面光の回転する一の回転軸を中心と
して回転方向と同じ方向に配置しておけば、コーナープ
リズムにより反射された光は先ず第2受光部に入射し、
次いで第1受光部に入射するが、窓ガラス等の反射面に
より反射された光は、先ず第1受光部に入射し、次いで
第2受光部に入射する。従って、第1受光部が入射光を
受光して出力した第1受光信号から第2受光部が入射光
を受光して出力した第2受光信号を減算した差信号は、
コーナープリズムから返光された反射光による場合に
は、41のように凹−凸になり、窓ガラス等の反射面が
反射した反射光による場合には41’のように凸−凹に
なる。
In particular, if the light receiving means is provided with the first light receiving portion and the second light receiving portion and arranged in the same direction as the rotation direction about one rotation axis of the plane light, the corner prism can The reflected light first enters the second light receiving portion,
Next, the light is incident on the first light receiving portion, and the light reflected by the reflecting surface such as the window glass first enters the first light receiving portion and then enters the second light receiving portion. Therefore, the difference signal obtained by subtracting the second light receiving signal output by receiving the incident light by the second light receiving unit from the first light receiving signal output by receiving the incident light by the first light receiving unit is
In the case of reflected light returned from the corner prism, it becomes concave-convex like 41, and in the case of reflected light reflected by a reflecting surface such as a window glass, it becomes convex-concave like 41 '.

【0033】一方、第1受光信号と第2受光信号とを加
算した和信号はコーナープリズムで返光された反射光が
入射した場合と、反射面で反射された反射光が入射した
場合と同じ波形になるが、前記差信号と和信号とを2値
化して2値化差信号と2値化和信号にする際に、差信号
を2値化する閾値よりも和信号を2値化する閾値を大き
くしておけば、2値化和信号と2値化差信号の立ち上が
る順序は、コーナープリズムが返光した反射光による場
合には2値化和信号の方が早く、反射面で反射された
光による場合には2値化差信号の方が早くなる。
On the other hand, the sum signal obtained by adding the first received light signal and the second received light signal is the same as when the reflected light returned by the corner prism is incident and when the reflected light reflected by the reflecting surface is incident. Although it has a waveform, when the difference signal and the sum signal are binarized into a binarized difference signal and a binarized sum signal, the sum signal is binarized rather than a threshold value for binarizing the difference signal. If the threshold value is increased, the rising order of the binarized sum signal and the binarized difference signal will be faster for the binarized sum signal and reflected by the reflecting surface when the reflected light returned by the corner prism is used. Anti
I found the following binary difference signal becomes faster in the case of morphism light.

【0034】そこで、2値化和信号が先にハイ状態にな
っており、2値化差信号がロー状態からハイ状態に変わ
ったときにのみパルスを出力するパルス回路を用いれ
ば、コーナープリズムが返光した反射光が入射したとき
にのみパルス出力が得られるので、これにより、窓ガラ
ス等の反射面で反射された反射光により発生する信号を
除去することができる。
Therefore, if the binarization sum signal is first in the high state and the binarization difference signal outputs a pulse only when the binarization difference signal changes from the low state to the high state, the corner prism is Since the pulse output is obtained only when the returned reflected light is incident, the signal generated by the reflected light reflected by the reflecting surface such as the window glass can be removed.

【0035】[0035]

【実施例】図1は本三次元座標測定方法の一手順を示す
フローチャートであり、処理開始後、照射手段側ルーチ
ン1と受光手段側ルーチン2とで並行して処理を進め
る。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a flow chart showing one procedure of the present three-dimensional coordinate measuring method. After the processing is started, the irradiation means side routine 1 and the light receiving means side routine 2 proceed in parallel.

【0036】照射手段側ルーチン1はステップS1で回
転手段や照射手段への電力供給を開始する等の初期化を
行いS2に処理を移行させる。
The irradiation means side routine 1 performs initialization such as starting power supply to the rotating means and the irradiation means in step S1 and shifts the processing to S2.

【0037】S2は回転照射ステップであり、測定装置
本体の備える照射手段から、互いに交叉する複数の平面
光を該測定装置本体の備える回転手段によって一の回転
軸線を中心に回転させつつ測定装置外部に照射し、該回
転照射ステップS2は、前記平面光を360°回転させ
たらステップS3に処理を移行させる。
S2 is a rotary irradiation step, in which a plurality of plane lights intersecting with each other from the irradiation means provided in the measuring apparatus main body are rotated about one rotation axis by the rotating means provided in the measuring apparatus main body, In step S2, the plane light is rotated by 360 °, and the process proceeds to step S3.

【0038】一方、測定点上にはスタッフが配置されて
おり、該スタッフ上の予め定められた位置には複数の返
光手段3が配置されている。そして、該スタッフに前記
複数の平面光が照射されると前記複数の返光手段3が平
面光を返光して測定装置本体の備える受光手段に入射さ
せる。
On the other hand, a staff is arranged on the measurement point, and a plurality of light returning means 3 are arranged at predetermined positions on the staff. When the staff is irradiated with the plurality of plane lights, the plurality of light returning means 3 returns the plane light and makes it incident on the light receiving means provided in the measuring apparatus main body.

【0039】S3は回転回数が規定回数に達したか否か
を判断する判断ステップであり、回転回数が規定回数未
満であれば回転照射ステップS2に処理を戻し、規定回
数に達していた場合には処理を終了させる。
S3 is a judgment step for judging whether or not the number of rotations has reached a prescribed number. If the number of rotations is less than the prescribed number, the process is returned to the rotary irradiation step S2, and if the prescribed number is reached, Terminates the process.

【0040】前記受光手段側ルーチン2は前記照射手段
側ルーチン1の処理の開始と同時に初期化ステップT1
から処理を開始する。該初期化ステップT1では、記憶
装置内の諸変数の初期化の他、前記平面光の回転移動す
る方向を回転方向変数Rに記憶させておき、処理をT2
に移行させる。
The light receiving means side routine 2 is initialized at the same time as the start of the processing of the irradiation means side routine 1 at the initialization step T1.
To start the process. In the initialization step T1, in addition to the initialization of various variables in the storage device, the direction in which the plane light is rotationally moved is stored in the rotation direction variable R, and the processing is performed in T2.
Move to.

【0041】T2は受光ステップであり、測定装置本体
の備える受光手段が、何らかの反射光を受光するまで待
機している。そして、何らかの反射光を受光した場合に
は、平面光が基準方向から回転移動した角度を一旦記憶
バッファM内に記憶させ、処理をT3に移行させる。
T2 is a light receiving step, which waits until the light receiving means provided in the measuring apparatus main body receives any reflected light. When any reflected light is received, the angle at which the plane light is rotationally moved from the reference direction is temporarily stored in the storage buffer M, and the process proceeds to T3.

【0042】T3は反射光移動方向検出ステップであ
り、反射光の移動方向を検出し、反射光移動方向変数G
に検出した方向を記憶させてT4に処理を移行させる。
[0042] T3 is a reflective light movement direction detection step, detecting a moving direction of the reflected light, the reflected light traveling direction variable G
The detected direction is stored in and the processing is shifted to T4.

【0043】T4は反射光判別ステップである。前記
光には平面光が前記コーナープリズム3で返光された
ものと、窓ガラス等の反射面で反射されたものとがある
ので、回転方向変数Rに記憶された平面光が回転移動す
る方向と、前記反射光移動方向変数Gに記憶された反射
光の移動方向を比較して、記憶バッファM内に記憶され
た角度を角度変数に記憶させるか否かを判断する。
T4 is a reflected light discrimination step. Anti
The morphism light to that plane light is Kaehikari by the corner prism 3, since there is to that reflected by the reflecting surface such as a window glass, a direction planar light stored in the rotation direction variable R is rotated and moved When the comparing the moving direction of the reflected light travel direction variable G to the stored reflected <br/> light, it determines whether to store the angular stored in the storage buffer M to the angle variable.

【0044】ここで、前記回転照射ステップS2で照射
された平面光が、窓ガラス等の反射面で反射された場合
に受光手段に入射する反射光の移動方向と、返光手段で
あるコーナープリズムで返光された場合に受光手段に入
射する反射光の移動方向との相違を図2に示す。
Here, when the plane light irradiated in the rotating irradiation step S2 is reflected by a reflection surface such as a window glass, the moving direction of the reflected light entering the light receiving means and the corner prism which is the light returning means. FIG. 2 shows the difference from the moving direction of the reflected light which is incident on the light receiving means when it is returned by.

【0045】図2を参照して、(a)は測定装置本体の備
える照射手段から照射された平面光が返光手段であるコ
ーナープリズム3で返光された場合を示す図である。コ
ーナープリズム3には平面光11aが入射して11bで示
す光が返光されており、前記平面光11aは矢印16で
示す図面右方向の12aの位置に移動するものとする
と、前記コーナープリズム3で返光される光は11bの
位置から矢印17で示す図面左方向の12bの位置に移
動する。この様に、コーナープリズム3に入射する光は
図面の右方向に移動するが、コーナープリズム3で返光
される反射光は図面の左方向に移動する等、両者の移動
方向は相異なるものとなる。
Referring to FIG. 2, (a) is a diagram showing a case where the plane light emitted from the irradiation means provided in the main body of the measuring apparatus is returned by the corner prism 3 which is the light returning means. If the plane light 11a is incident on the corner prism 3 and the light 11b is returned, and the plane light 11a is moved to a position 12a in the right direction of the drawing shown by an arrow 16, the corner prism 3 will be described. The light returned by moves from the position 11b to the position 12b in the left direction of the drawing indicated by the arrow 17. Thus, the light incident on the corner prism 3 moves to the right in the drawing, but the reflected light returned by the corner prism 3 moves to the left in the drawing. Become.

【0046】これに対し、窓ガラス等の反射面で平面光
が反射される場合を図2(b)で示す。平面光13aが窓
ガラス等の反射体5に入射して13bで示す光が反射さ
れており、前記平面光13aは矢印18で示す図面右方
向の14aの位置に移動するものとすると、前記反射体
5で反射された光は矢印19で示す図面右方向の14b
の位置に移動する。この様に反射体5に入射する光の移
動方向と該反射体5で反射された反射光の移動方向とは
等しくなる。
On the other hand, FIG. 2B shows the case where the plane light is reflected by the reflecting surface of the window glass or the like. If the plane light 13a is incident on the reflector 5 such as a window glass and the light 13b is reflected, and the plane light 13a moves to a position 14a in the right direction of the drawing shown by an arrow 18, the reflection The light reflected by the body 5 is indicated by arrow 19 in the right direction 14b in the drawing.
Move to position. In this way, the moving direction of the light incident on the reflector 5 and the moving direction of the reflected light reflected by the reflector 5 are equal.

【0047】この様に、前記回転方向変数Rには平面光
が回転移動する方向が記憶されており、反射光の移動方
向は反射光移動方向変数Gに記憶されているので、両変
数に記憶された内容を比較すれば、該反射光が窓ガラス
等の反射面で反射されたものかコーナープリズムで返光
されたものであるかを検出することができる。そして、
反射光がコーナープリズムで返光されたものである場合
には、処理はT5に移行して、記憶バッファM内に記憶
された角度を記憶変数内に格納する。一方、反射光がコ
ーナープリズム等で反射されたものであった場合には、
処理をT2に戻して再度反射光を受光するまで待機す
る。
[0047] Thus, the in the rotation direction variable R is stored in the direction in which the planar optical rotation movement, the moving direction of the reflected light is stored in the reflected beam moving direction variables G, stored in both variables the comparison is contents, the reflected light can be detected whether there are those Kaehikari by those or corner prisms reflected by the reflecting surface such as window glass. And
If the reflected light is the light returned by the corner prism, the process proceeds to T5 to store the angle stored in the storage buffer M in the storage variable. On the other hand, if the reflected light is reflected by a corner prism or the like,
The process is returned to T2, and the process waits until the reflected light is received again.

【0048】ところで、ステップT2からステップT5の
行う働きを電気回路で実現できれば処理速度が高速なの
で、測定時間の短縮等の面から好ましい。その様な電気
回路として、コーナープリズムから返光された反射光を
受光した場合にのみパルス出力を行って平面光が基準方
向から回転移動した角度を記憶させるトリガ回路の一例
を図3(a)に示す。
By the way, if the functions of steps T2 to T5 can be realized by an electric circuit, the processing speed is high, which is preferable from the viewpoint of shortening the measurement time. As such an electric circuit, an example of a trigger circuit that outputs a pulse only when the reflected light returned from the corner prism is received and stores the angle at which the plane light is rotationally moved from the reference direction is shown in FIG. Shown in.

【0049】図3(a)を参照して、21は測定装置本体
の備える受光手段であり、反射光を受光して第1検出信
号を出力する第1受光部22aと、第2検出信号を出力
する第2受光部22bから成っており、前記第1受光部
22aと第2受光部22bは一の回転軸を中心にして図示
するように配置され、照射手段が照射する複数の平面光
と共に方向23へ回転移動する。
Referring to FIG. 3 (a), reference numeral 21 denotes a light receiving means provided in the main body of the measuring apparatus, which receives a reflected light and outputs a first detection signal, and a second detection signal. It is composed of a second light receiving portion 22b for outputting, and the first light receiving portion 22a and the second light receiving portion 22b are arranged as shown in the figure with one rotation axis as a center, and together with a plurality of plane lights irradiated by the irradiation means. Rotate in direction 23.

【0050】前記第1受光部の出力する前記第1検出信
号は増幅器24aと検波器25aを経て加算手段26と減
算手段27に入力される。一方、前記第2検出信号は増
幅器24bと検波器25bを経て前記加算手段26と前記
減算手段27とに入力される。
The first detection signal output from the first light receiving section is input to the adding means 26 and the subtracting means 27 via the amplifier 24a and the detector 25a. On the other hand, the second detection signal is input to the adding means 26 and the subtracting means 27 via the amplifier 24b and the detector 25b.

【0051】前記加算手段26は、前記増幅器24aと
前記検波器25aを経て入力された前記第1検出信号
と、前記増幅器24bと前記検波器25bを経て入力され
た前記第2検出信号とを加算した和信号を和信号比較器
28に出力し、前記減算手段27は、前記増幅器24a
と前記検波器25aを経て入力された前記第1検出信号
から、前記増幅器24bと前記検波器25bを経て入力さ
れた第2検出信号を差し引いた差信号を差信号比較器2
9に出力する。
The adding means 26 adds the first detection signal input via the amplifier 24a and the detector 25a and the second detection signal input via the amplifier 24b and the detector 25b. And outputs the sum signal to the sum signal comparator 28, and the subtracting means 27 outputs the sum signal to the amplifier 24a.
And a difference signal obtained by subtracting the second detection signal input via the amplifier 24b and the detector 25b from the first detection signal input via the detector 25a.
Output to 9.

【0052】図3(b)はコーナープリズムで返光された
反射光が前記受光手段21に入射した場合に前記差信号
と前記和信号の波形を示した図である。コーナープリズ
ムで返光された反射光は照射手段が照射する複数の平面
光が回転移動する方向23とは逆向き方向31の方向に
移動するので、前記第1受光部22aよりも第2受光部
22bが先に反射光を受光する。従って、時間を横軸
に、信号強度を縦軸にとれば、前記差信号は曲線41で
示す特性となる。そして、差信号比較器29は、第1閾
値42を基準として、該第1閾値よりも大きい場合をハ
イ状態とし、小さい場合をロー状態として前記曲線41
の特性を有する差信号を2値化して、図3(c)の折線4
3で示す特性の2値化差信号をパルス回路30に出力す
る。
FIG. 3B shows the light returned by the corner prism.
FIG. 7 is a diagram showing waveforms of the difference signal and the sum signal when reflected light enters the light receiving means 21. Since the reflected light returned by the corner prism moves in a direction 31 opposite to the direction 23 in which the plurality of plane lights emitted by the irradiating means rotate, the second light receiving portion is more than the first light receiving portion 22a. 22b receives the reflected light first. Therefore, when the time is plotted on the horizontal axis and the signal strength is plotted on the vertical axis, the difference signal has the characteristic shown by the curve 41. The difference signal comparator 29 uses the first threshold value 42 as a reference, sets the high state when the value is larger than the first threshold value, and sets the low state when the value is smaller than the first threshold value 42.
The difference signal having the characteristic of is binarized, and the broken line 4 in FIG.
The binary difference signal having the characteristic indicated by 3 is output to the pulse circuit 30.

【0053】一方、加算手段26が出力する加算信号
は、図3(b)の曲線45で示す特性となる。そして、和
信号比較器28は、前記第1閾値42よりも大きい第2
閾値46を基準として、該第2閾値46よりも大きい場
合をハイ状態とし、小さい場合をロー状態として、前記
曲線45の特性を有する和信号を2値化して、図3(c)
の折線47で示す特性の2値化和信号をパルス回路30
に出力する。
On the other hand, the addition signal output from the addition means 26 has the characteristic shown by the curve 45 in FIG. 3 (b). Then, the sum signal comparator 28 outputs a second signal larger than the first threshold 42.
With reference to the threshold value 46, when the value is larger than the second threshold value 46, the high state is set, and when the value is smaller than the second threshold value 46, the low state is set, and the sum signal having the characteristic of the curve 45 is binarized.
The binarized sum signal having the characteristic indicated by the broken line 47 in FIG.
Output to.

【0054】そして、パルス回路30は入力された前記
2値化和信号がハイ状態であり、入力された前記2値化
差信号がロー状態からハイ状態に変わったときにパルス
信号を演算装置32に出力し、該演算装置32は、該パ
ルス入力があったときの平面光の回転角度を記憶手段3
3に記憶させれば、受光手段がコーナープリズムで返光
された反射光を受光したときの平面光が基準方向と成す
角度を検出することができる。
Then, the pulse circuit 30 outputs the pulse signal when the inputted binarization sum signal is in the high state and the inputted binarization difference signal changes from the low state to the high state. The arithmetic unit 32 outputs the rotation angle of the plane light when the pulse is input to the storage means 3.
If stored in 3, it is possible to detect the angle formed by the plane light with the reference direction when the light receiving means receives the reflected light returned by the corner prism.

【0055】一方、測定装置本体の備える照射手段が照
射した平面光が窓ガラス等の反射面で反射された場合に
は、反射光の移動方向は平面光が回転移動する方向と同
じになるので、第1受光部22aが第2受光部22bより
も先に反射光を受光する。この場合には、前記減算手段
27で作られる差信号は図3(d)の曲線41’で示す特
性となり、前記差信号比較器29が、第1閾値42を基
準として、該第1閾値よりも大きい場合をハイ状態と
し、小さい場合をロー状態として、前記曲線41’で示
す特性の差信号を2値化するので、図3(e)の折線4
3’で示す特性の2値化差信号がパルス回路30に出力
される。又、前記加算手段26は入力された信号を加算
し曲線45’で示す特性の和信号を和信号比較器28に
出力し、該和信号比較器28は、前記第1閾値42より
も大きい第2閾値46を基準として、該第2閾値46よ
りも大きい場合をハイ状態とし、小さい場合をロー状態
として前記曲線45’の特性の和信号を2値化して、図
3(e)の折線47’で示す特性の2値化和信号を前記パ
ルス回路30に出力する。
On the other hand, when the plane light emitted by the irradiation means provided in the main body of the measuring apparatus is reflected by the reflection surface such as the window glass, the moving direction of the reflected light becomes the same as the rotating direction of the plane light. The first light receiving portion 22a receives the reflected light before the second light receiving portion 22b. In this case, the difference signal generated by the subtraction means 27 has the characteristic shown by the curve 41 ′ in FIG. 3 (d), and the difference signal comparator 29 uses the first threshold 42 as a reference and outputs the difference from the first threshold. The difference signal having the characteristic indicated by the curve 41 ′ is binarized by setting the high state when it is large and the low state when it is small, so that the broken line 4 in FIG.
The binarized difference signal having the characteristic 3'is output to the pulse circuit 30. Further, the adding means 26 adds the input signals and outputs a sum signal having a characteristic indicated by a curve 45 ′ to a sum signal comparator 28, which sum signal comparator 28 is larger than the first threshold 42. When the threshold value is larger than the second threshold value 46, the sum signal of the characteristic of the curve 45 ′ is binarized by setting the high state when it is larger than the second threshold value 46 and the low state when it is smaller than the second threshold value 46, and the broken line 47 in FIG. The binarized sum signal having the characteristic indicated by 'is output to the pulse circuit 30.

【0056】そして、この場合には、2値化差信号4
3’がロー状態からハイ状態に変わるときは2値化和信
号47’はロー状態であり、パルス回路30はパルスを
出力しないので、前記演算手段32が平面光の回転角度
を記憶手段33に記憶させることはない。
In this case, the binarized difference signal 4
When 3'changes from the low state to the high state, the binarized sum signal 47 'is in the low state and the pulse circuit 30 does not output a pulse. Therefore, the arithmetic means 32 stores the rotation angle of the plane light in the storage means 33. There is nothing to remember.

【0057】この場合、第1および第2受光部の配置順
や、増巾器、検波器、減算手段、信号比較器などの極性
により、図3(b)、(d)に示す波形は変わるが、ど
ちらの場合でも選択的に動作させられることは言うまで
もない。
In this case, the waveforms shown in FIGS. 3 (b) and 3 (d) change depending on the arrangement order of the first and second light receiving portions and the polarities of the amplifier, detector, subtracting means, signal comparator and the like. However, it goes without saying that the operation can be selectively performed in either case.

【0058】この様に、照射手段の照射する平面光が回
転移動する方向と、受光手段が受光した反射光の移動方
向とを比較して、コーナープリズムから返光された反射
光か否かを検出して平面光が基準方向から回転移動した
角度を記憶しても、コーナープリズムから返光された
光を受光した場合に動作するトリガ回路の働きによ
り、コーナープリズムから返光された反射光を検出して
平面光が基準方向から回転移動した角度を記憶しても良
い。
[0058] Thus, the direction in which the plane light irradiation of the irradiation means is rotationally moved, the light receiving means is compared with the moving direction of the reflected light received, reflected <br/> light Kaehikari corner prisms detecting whether also store an angle planar light is rotated and moved from the reference direction, counterclockwise, which is Kaehikari corner prisms
By the action of the trigger circuit that operates when receiving a morphism light may store an angle planar light by detecting the reflected light Kaehikari corner prism is rotated and moved from the reference direction.

【0059】そして、前記平面光の回転移動した角度を
記憶した後は処理はT6に移行する。
Then, after storing the rotation angle of the plane light, the processing shifts to T6.

【0060】T6は角度の測定が終了したか否かを判断
する。前記角度変数の全てに角度が記憶されていなけれ
ば、測定は終了していないので処理をT2に戻し、前記
角度変数の全てに角度が記憶されていれば処理をT7に
移行させる。
At T6, it is determined whether or not the angle measurement is completed. If the angle is not stored in all the angle variables, the measurement has not been completed, so the process returns to T2. If the angle is stored in all the angle variables, the process proceeds to T7.

【0061】T7は三次元座標算出ステップであり、前
記複数の返光手段のスタッフ上の位置と前記角度変数に
記憶された移動手段の回転角度とにより測定点の三次元
座標の値を算出する。
T7 is a three-dimensional coordinate calculation step, in which the value of the three-dimensional coordinate of the measurement point is calculated from the positions of the plurality of light returning means on the staff and the rotation angle of the moving means stored in the angle variable. .

【0062】ところで、測定原理を簡単に説明するた
め、図4(a)では返光手段を2つ用い、該2つの返光手
段を測定点上に鉛直に配置したが、3つの返光手段をス
タッフに設け、該3つの返光手段をスタッフ上に一の平
面を張る様に配置すれば、スタッフを測定点上に鉛直に
立てる必要はなくなるが、この場合でも本三次元座標測
定法方及び三次元座標測定装置を用いることができるこ
とは言うまでもない。
By the way, in order to briefly explain the measurement principle, in FIG. 4A, two light returning means are used, and the two light returning means are arranged vertically on the measurement point. If the staff is provided and the three light-returning means are arranged so as to form a plane on the staff, it is not necessary to stand the staff vertically on the measurement point. It goes without saying that a three-dimensional coordinate measuring device can be used.

【0063】なお、該ステップT7では、三次元座標の
計算結果を表示装置33で表示して、処理をT8に移行
させる。
In step T7, the calculation result of the three-dimensional coordinates is displayed on the display device 33, and the process proceeds to T8.

【0064】T8では、予め定められた回数の測定が行
われたか否かを判断し、行われていなければ処理をT2
に戻し、行われた場合には、処理を終了させる。
At T8, it is determined whether or not a predetermined number of measurements have been performed, and if not, the process proceeds to T2.
If it is done, the process is terminated.

【0065】[0065]

【発明の効果】コーナープリズムで返光された反射
か、反射面で反射された反射光かを検出することができ
るので、窓ガラス等の反射体が多数存在する市街地にお
いても誤りなく三次元座標測定を行うことができる。
Effects of the Invention corner prisms have been either reflected light Kaehikari, since it is possible to detect whether the reflected light reflected by the reflecting surface, without error even in urban reflection body such as a window glass there are numerous three-dimensional Coordinate measurements can be made.

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

【図1】 本三次元座標測定方法の一実施例の処理手順FIG. 1 is a processing procedure of an embodiment of the present three-dimensional coordinate measuring method.

【図2】 コーナープリズムで返光された光と反射面で
反射された光の移動方向の相違を示す図
FIG. 2 is a diagram showing a difference in moving directions of light returned by a corner prism and light reflected by a reflecting surface.

【図3】 (a) 本三次元座標測定装置に用いられるト
リガ回路の一例 (b)〜(e)前記トリガ回路中の各ブロックの作る信号
波形を示す図
3A is a diagram showing an example of a trigger circuit used in the present three-dimensional coordinate measuring apparatus, and FIG. 3B is a diagram showing a signal waveform produced by each block in the trigger circuit.

【図4】 三次元座標測定の原理を示す図FIG. 4 is a diagram showing the principle of three-dimensional coordinate measurement.

【符号の説明】[Explanation of symbols]

a 測定装置本体 b1・b2 平面光
c 照射手段 d スタッフ e1・e2 返光手段 Q 測定点 3 コーナープリズム 5 反射体 21 受光手段 22a 第1受光部
22b 第2受光部 26 加算手段 27 減算手段 28 和信号比較器 29 差信号比較器 30 パルス回路 33 角度記憶手段
a Measuring device body b1, b2 plane light
c Irradiating means d Stuff e1, e2 Light returning means Q Measuring point 3 Corner prism 5 Reflector 21 Light receiving means 22a First light receiving section
22b Second light receiving section 26 Addition means 27 Subtraction means 28 Sum signal comparator 29 Difference signal comparator 30 Pulse circuit 33 Angle storage means

───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.7,DB名) G01C 15/00 G01C 15/06 ─────────────────────────────────────────────────── ─── Continued Front Page (58) Fields surveyed (Int.Cl. 7 , DB name) G01C 15/00 G01C 15/06

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 互いに交叉する複数の平面光を照射する
照射手段とその反射光を受光して信号を出力する複数の
受光手段とを備えた測定装置本体と、 複数の返光手段を備えたスタッフとから成る三次元座標
測定システムを用いる三次元座標測定方法であって、 測定点上に前記スタッフを配置し、 前記複数の平面光を一の回転軸を中心に回転移動させて
前記スタッフの備える複数の返光手段に照射し、 各々の返光手段により返光された反射光を前記受光手段
により受光し、 前記受光手段が受光したときの各平面光の回転角度と各
々の返光手段がスタッフ上の配置された位置とにより測
定点の三次元座標を求める三次元座標測定方法におい
て、 前記複数の返光手段にコーナープリズムを用い、 前記複数の平面光の回転移動に伴い、前記受光手段で受
光する反射光が移動する方向を検出し、該検出した方向
が前記平面光の回転移動方向と同方向か逆方向かによっ
て、受光手段で受光した反射光がコーナープリズムによ
り返光された反射光なのかコーナープリズム以外の反射
面により反射された反射光なのかを判別し、 コーナープリズムにより返光された反射光が受光手段に
入射したときの前記回転角度のみに基いて測定点の三次
元座標の値を算出する、 不要光を除去して三次元座標を測定する三次元座標測定
方法。
1. A measuring device main body comprising: an irradiation means for irradiating a plurality of plane lights intersecting with each other; and a plurality of light receiving means for receiving reflected light and outputting a signal, and a plurality of light returning means. A three-dimensional coordinate measuring method using a three-dimensional coordinate measuring system comprising a staff, wherein the staff is arranged on a measurement point, and the plurality of plane lights are rotatably moved around one rotation axis. a plurality of irradiating the Kaehikari means, the reflected light Kaehikari by each Kaehikari means received by said receiving means, each planar light rotation angle and each of Kaehikari means when said light receiving means has received with In the three-dimensional coordinate measuring method for obtaining the three-dimensional coordinates of the measurement point by the position arranged on the staff, a corner prism is used for the plurality of light returning means, and the light reception is accompanied by the rotational movement of the plurality of plane lights. hand Received in
The direction in which the reflected light that is emitted moves is detected, and the detected direction
Depending on whether the direction of rotation of the plane light is the same or opposite.
The corner prism to reflect the reflected light received by the light receiving means.
Is it reflected light that is reflected back? Reflection other than corner prism
It is determined whether it is the reflected light reflected by the surface and the three-dimensional coordinate value of the measurement point is calculated based only on the rotation angle when the reflected light returned by the corner prism enters the light receiving means. A three-dimensional coordinate measurement method that removes light and measures three-dimensional coordinates.
【請求項2】 前記複数の受光手段はそれぞれ第1受光
部と第2受光部とが前記一の回転軸を中心にして周設し
て成り、 前記第1受光部と前記第2受光部が反射光を受光した順
番を検出し、その順番に基づいて前記受光手段で受光し
た反射光が移動する方向を検出することを特徴とする請
求項1記載の三次元座標測定方法。
2. The plurality of light receiving means are each formed by arranging a first light receiving portion and a second light receiving portion around the one rotation axis as a center, and the first light receiving portion and the second light receiving portion are formed. The order in which the reflected light is received is detected, and the light is received by the light receiving means based on that order.
The three-dimensional coordinate measuring method according to claim 1, wherein the direction in which the reflected light moves is detected.
【請求項3】 前記受光手段は、反射光を受光して第1
検出信号を出力する第1受光部と、反射光を受光して第
2受光信号を出力する第2受光部から成り、 前記第1受光部と第2受光部は前記一の回転軸を中心に
して前記平面光の回転方向と同じ方向に配置され、 前記測定装置本体は、 前記第1受光信号から前記第2受光信号を差し引いた差
信号を出力する減算手段と、 前記第1受光信号と前記第2受光信号を加えた和信号を
出力する加算手段と、 第1閾値を基準として、該第1閾値よりも大きい場合を
ハイ状態とし、小さい場合をロー状態として前記差信号
を2値化した2値化差信号を出力する差信号比較器と、 第1閾値よりも大きい第2閾値を基準として、該第2閾
値よりも大きい場合をハイ状態とし、小さい場合をロー
状態として前記和信号を2値化した2値化和信号を出力
する和信号比較器と、 前記2値化差信号と前記2値化和信号とを受信して、前
記2値化和信号がハイ状態であって前記2値化差信号が
ロー状態からハイ状態に変わったときにパルス信号を出
力するパルス回路と、 前記パルス信号を受信したときの前記平面光の回転角度
を記憶する角度記憶手段を備え、 前記角度記憶手段に記憶された角度に基いて測定点の三
次元座標を算出する演算装置を備えたことを特徴とする
請求項1又は請求項2記載の三次元座標測定方法に用い
られる、 不要光を除去して三次元座標を測定する三次元座標測定
装置。
3. The light receiving means receives reflected light to receive the first light.
A first light receiving unit for outputting a detection signal, comprises a second light receiving section for outputting a second light receiving signal by receiving the reflected light, the first light receiving portion and the second light receiving portion is centered on the axis rotation of the one Is arranged in the same direction as the rotation direction of the plane light, and the measuring device body outputs subtraction means for subtracting the second light reception signal from the first light reception signal, the first light reception signal and the subtraction means. The adding means for outputting a sum signal to which the second received light signal is added, and the difference signal is binarized with the first threshold value as a reference, the case of being larger than the first threshold value as a high state, and the case of being smaller than the first threshold value as a low state. A difference signal comparator that outputs a binarized difference signal and a second threshold value that is larger than the first threshold value as a reference is set to a high state when it is larger than the second threshold value, and a low state when it is smaller than the second threshold value. A sum signal that outputs a binarized sum signal A comparator, and receiving the binarized difference signal and the binarized sum signal, the binarized sum signal is in a high state and the binarized difference signal is changed from a low state to a high state. When a pulse circuit that outputs a pulse signal and an angle storage unit that stores the rotation angle of the plane light when the pulse signal is received are provided, and a cubic of a measurement point based on the angle stored in the angle storage unit. A three-dimensional coordinate measuring device used for the three-dimensional coordinate measuring method according to claim 1 or 2, characterized in that the three-dimensional coordinate measuring device measures unnecessary three-dimensional coordinates by removing unnecessary light. .
JP00058494A 1994-01-07 1994-01-07 Three-dimensional coordinate measuring method and three-dimensional coordinate measuring device for measuring three-dimensional coordinates by removing unnecessary light Expired - Lifetime JP3459287B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP00058494A JP3459287B2 (en) 1994-01-07 1994-01-07 Three-dimensional coordinate measuring method and three-dimensional coordinate measuring device for measuring three-dimensional coordinates by removing unnecessary light

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP00058494A JP3459287B2 (en) 1994-01-07 1994-01-07 Three-dimensional coordinate measuring method and three-dimensional coordinate measuring device for measuring three-dimensional coordinates by removing unnecessary light

Publications (2)

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JPH07208990A JPH07208990A (en) 1995-08-11
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Cited By (1)

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CN108398104A (en) * 2018-02-01 2018-08-14 中国科学院国家天文台南京天文光学技术研究所 The photoelectricity dynamic angle measuring devices and its method of random error can be reduced

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KR100812127B1 (en) * 2007-11-16 2008-03-12 (주) 일신하이텍 Surveyor Position Lock
JP5422322B2 (en) * 2009-09-25 2014-02-19 公益財団法人鉄道総合技術研究所 Rail detection method and rail displacement measurement device in rail displacement measurement
JP7699022B2 (en) * 2021-09-24 2025-06-26 株式会社トプコン Surveying equipment, surveying method, and surveying program

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108398104A (en) * 2018-02-01 2018-08-14 中国科学院国家天文台南京天文光学技术研究所 The photoelectricity dynamic angle measuring devices and its method of random error can be reduced

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