TW201538925A - Non-contact measurement device and method for object space information and the method thereof for computing the path from capturing the image - Google Patents

Abstract

The present disclosure is a non-contact measurement device and method for object space information and the method thereof for computing the path from capturing the image, wherein the measurement device comprising: a camera capture a image of a measured object, a laser scanning device scan the measured object, a mobile platform which the camera and the laser scanning device are fixed on, a movable control unit drive the mobile platform to move within a three-dimesional, a central processing unit connected with the movable control unit, by way of the movable control unit, the central processing unit control the image capturing angle of the camera and the scanning angle of the laser scanning device, wherein the central processing unit provides actuation in executing an initial scan positioning and executing an image capturing path compensation.

Description

Non-contact object space information measuring device and method and calculation method of image taking path

The invention relates to an object space information measuring device and method, in particular to a non-contact object space information measuring device and method and a calculating method of an image taking path.

With the vigorous development of industry, the traditional two-dimensional detection method can not meet the complex object to be tested. Therefore, the three-dimensional measuring instrument is currently used on the market to measure the complex object to be tested. Generally, the three-dimensional measuring instrument can be divided into two types: contact type and non-contact type. The contact type three-dimensional measuring instrument directly measures the size by using the probe to contact the object to be tested, and the disadvantage of this method is that the speed is slow. There are also doubts about the surface of the object to be tested. In recent years, non-contact laser ranging scanning methods have been widely used in industrial automation. With the improvement of process capability, the accuracy and speed requirements of measurement have gradually increased. In order to greatly accelerate the speed of the whole measurement, in the laser ranging scanning method, a single laser spot is replaced by a camera combined with a laser structured light stripe, and the laser stripe is scanned to obtain a correct workpiece model. However, when the size of the object to be tested is large but requires a certain resolution and measurement accuracy, the range of the laser scanning measurement will be taken with high magnification. The field of view of the camera is reduced and reduced, and if the object is not in a straight line shape, it is impossible to scan the entire object in a single axial direction by driving the laser and the camera.

Generally speaking, the above problem can be achieved by manually teaching the scanning movement path of the mobile unit or inputting the 3D engineering CAD drawing of the known object to be tested, so that the mobile unit can complete the full scan measurement of the object, but the manual teaching is very time consuming and requires professional operation. However, most of the objects to be measured immediately do not necessarily have a three-dimensional engineering CAD drawing, and the space coordinate conversion correction of a certain program is required after inputting the drawing surface, so that the mobile unit conforms to the path formed by the engineering CAD drawing, The object to be tested needs to be fixed or designed to fix the posture and position of the workpiece. Otherwise, the coordinate of the CAD drawing of the engineering must be recalibrated once, which makes the work of laser scanning measurement or reconstruction of the shape of the space object difficult. .

The present disclosure provides a non-contact object space information measuring device and method and a method for calculating an image capturing path, which can scan a spatial information information of a three-dimensional object to be measured in time through a laser scanning device, and calculate a next laser scanning device and The camera scans the position and direction of the camera, and solves the problem that the complete scan path of the object to be tested must be established in advance, or the information of the model of the object to be tested is given, so as to avoid the problem of requiring a long time for the teaching process and the operation of the professional. In turn, the ability of the workpiece to measure and reconstruct the shape is greatly improved.

The present disclosure aims to provide a non-contact object space information measuring device and method and a method for calculating an image capturing path, which is to realize non-contact three-dimensional vision by using a two-dimensional camera visual measurement and laser scanning device technology. Measure. As shown in FIG. 1 , the first moving path of the laser scanning device is firstly transmitted through the camera and the central processing unit, and the mobile control unit is driven to extract the three-dimensional information of the object to be tested, and then the three-dimensional information is estimated. Laser sweep The moving path of the drawing device and the camera, and the next moving path of the laser scanning device and the camera are estimated along with the result of the timely estimation. If the three-dimensional curved surface of the object to be tested is turned or undulated, the laser scanning device and the camera will follow The surface of the object to be tested is yawed or turned to achieve three-dimensional object measurement.

The disclosure provides an embodiment of a non-contact object space information measuring device, comprising: a camera for acquiring an image of an object to be tested; a laser scanning device for scanning the object to be tested; Providing the camera and the laser scanning device fixed on the mobile platform; the mobile control unit is configured to control the mobile platform to move in a three-dimensional space; and the central processing unit is coupled to the mobile control unit, and The image capturing angle of the camera and the scanning angle of the laser scanning device are controlled via the movement control unit; wherein the central processing unit performs an initial scanning positioning and an image capturing path compensation.

Another embodiment provided by the present disclosure is a method for calculating a non-contact image taking path for driving a mobile platform, wherein a camera and a laser scanning device are fixed on the mobile platform, and the steps include: performing An initial scanning positioning step of obtaining a spindle direction θ _p of the object to be tested according to an image captured by the camera; and performing an image capturing path compensation step according to the laser scanning device Scanning the complex image of the object to be tested along the spindle direction θ _{p to} obtain a turn compensation angle Δθ _α in a first plane direction at a first time point and a depth yaw compensation angle Δθ in a second plane direction _And obtaining a corresponding spindle direction θ _p ' at a second time point, and when entering the second time point at the first time point, directing a scan line of the laser scanning device to the second time point The spindle direction θ _p ' is relatively opposed to establish an image capturing path.

Another embodiment of the present disclosure is a non-contact object space information measuring method for driving a mobile platform, wherein a camera and a laser scanning device are fixed on the mobile platform, and the steps thereof include: Performing an initial scan positioning step of obtaining a main axis direction θ _p of the object to be tested according to an image captured by the camera; performing an image path compensation step according to the laser scanning device Scanning the complex image of the object to be tested along the spindle direction θ _{p to} obtain a turn compensation angle Δθ _α in a first plane direction at a first time point and a depth yaw compensation angle Δθ in a second plane direction _And obtaining a corresponding spindle direction θ _p ' at a second time point, and when entering the second time point at the first time point, directing a scan line of the laser scanning device to the second time point relative to the major axis direction to be θ _p '; and performing the step of measuring the object to be measured, through this initial positioning step and scan imaging path compensation step, measuring the object to be measured Inch.

11‧‧‧ camera

12‧‧‧ Laser scanning device

13‧‧‧Central Processing Unit

14‧‧‧Mobile platform

15‧‧‧ objects to be tested

16‧‧‧Mobile Control Unit

17‧‧‧Laser scan line

21~22‧‧‧Steps 21~22

31~39‧‧‧Steps 31~39

Figure 1 Schematic diagram of a non-contact object space information measuring device.

Figure 2 Schematic diagram of the initial scan positioning step.

Figure 3 Schematic diagram of the image path compensation step.

Figure 4 A scan line of the laser scanning device is directed to the corresponding direction of the main axis at a second point in time to establish a schematic representation of the image taking path.

Figure 5A Schematic diagram of the midpoint of a single laser scan line.

Fig. 5B is a schematic diagram of calculating the Δθ _α turning compensation angle at the intermediate point of the continuous laser scanning line.

Figure 6A is a schematic diagram showing the difference in depth between the starting point ( x _s , z _s ) and the ending point ( x _e , z _e ).

In Fig. 6B , the depth yaw angle Δθ _{β of} the nth scan line and the n+th scan line is calculated from the difference in depth between the starting point ( x _s , z _s ) and the end point ( x _e , z _e ).

The thick arrow in Fig. 7A is a schematic diagram of the original moving direction of θ _p .

The thick arrow in Figure 7B is A schematic diagram of the movement direction after the correction of the turning compensation angle Δθ _α and the depth yaw angle Δθ _β .

In order to achieve the basic purpose of the present disclosure, the technical means and features will be described below by way of specific embodiments. The disclosed method can be divided into two main processes, which are divided into an initial scan positioning step and an image capture path compensation step to provide automatic scan measurement. The initial scanning positioning step is as shown in FIG. 2, and please refer to FIG. 1. In step 21, the camera 11 recognizes the position of the object for initial positioning, and first uses the camera 11 to image the working area. When the working area is not placed any In the case of an object, the image is taken as the basic image T1. When the object is placed in the work area, the image obtained by the camera 11 is the image T2. By subtracting the images T1 and T2, the position of the object placed in the image can be found. In step 22, the main axis direction θ _{p of the} object is identified, and the end point or boundary point of the image is transmitted. For example, the space moment method and the boundary detection method are used, and the second order space moments algorithm can be used to calculate the object. The centroid and the long axis direction are used to obtain the initial scanning direction θ _{p of the} scanned object, and θ _p is the main axis direction. Assuming that the object can be represented by an elliptical shape, the region R can be an ellipse representing the center at the origin, then R can be expressed as, R = {( x , y )| dx ² +2 exy + fy ² 1}, the coefficients d , e , f of the elliptic equation have the following relationship with the quadratic vector moments μ _xx , μ _yy and μ _xy : ; the direction of the spindle The angle between the major axis direction based principal inertia axis and a coordinate axis (X axis) of the object to be measured 15, the object to be measured of the object to be measured 15 of the main shaft of inertia of the boundary 15 took the longest distance between two points; wherein A is The area, ( x , y ) is the coordinates of the pixels in the captured position image. The centroid of the position image is captured for this. Please refer to FIG. 3, a schematic diagram of the compensation system taken as a step of the route, the display automatically scan measurement process, first, the drive control unit 16 according to the movement of a process the obtained θ _p main scanning direction starts, the main axis direction assuming the XY θ _p Plane movement, because the depth (Z) data of the laser scan can be obtained instantly, that is, the change value on the Z axis, and the data position on the nth scan line can be expressed as f _n ( x, y, z ), the single point depth value on the scan line is z _i , i =1~L, the depth data point is calculated from the starting point (i=1, 2,...), the starting point z _{s is the} largest depth change, and the depth data point is determined by the end point (i =L, L-1, L-2, L-3, ...) Calculate the maximum end point z _{e of the} depth change, and the corresponding XY plane coordinates are ( x _s , y _s ) and ( x _e , y _e ) However, it is necessary to judge whether the starting point and the ending point have significant changes according to the threshold value T _Z to define whether the object is placed within the scanning line range; if the depth value of the starting point or the ending point on the same scanning line ( z _s or z _e ) One cannot be detected or zero, indicating that the scan line is falling at the 90° turn of the object, so the scan spindle direction θ _p needs to be rotated +90° Or -90° (according to the user's definition of z _s and z _e ), then return to the process to continue the scan measurement along θ _p ; if the depth value of the start or end point on the same scan line is zero at the same time, it means that Complete a full scan of the object.

Please refer to Fig. 4, where the turning compensation angle Δθ _{α of the} main shaft direction θ _p on the XY plane, if the main axis θ _{p does} not fall on the direction of the object 15 to be tested, correct θ _p to guide the scan line back to the test The direction of the object 15. The intermediate point of the current scan line can be calculated:

The laser scanning line 17 is generated when scanned by the laser scanning device 12.

Please refer to FIG. 5A, which is a schematic diagram of the intermediate point of a single laser scanning line 17. After calculating the position of the intermediate point (x _m , y _m ) of each scanning line, refer to Figure 5B. The turning compensation angle Δθ _α can be calculated from the nth to the n+thth scanning lines. Wherein the x coordinate and the y coordinate lower subscript m refer to the middle point of each scan line, the right subscript n+k, n+k-1 refers to the n+kth scan line and the n+k- 1 scan line.

Referring to Figure 6A, each scan line can calculate its depth yaw angle Δθ _β on the XZ plane, using the depths of the starting point ( x _s , z _s ) and the end point ( x _e , z _e ). For the difference, please refer to FIG. 6B to calculate the depth yaw angle Δθ _{β of} the nth scan line and the n+kth scan line as the correction basis for the yaw angle of the next scan direction. Wherein the x coordinate and the z coordinate lower right standard e refer to the end point of each scanning line; the x coordinate and the z coordinate lower right standard s refer to the starting point of each scanning line; the n+k, 1 index in the lower subscript The n+kth scan line and the 1st scan line of each scan line. The main axis direction θ _p can correct the path of the instant scanning according to the obtained depth yaw angle Δθ _β of the XZ plane angular difference, and effectively follow the change, the trend and the degree of distortion of the surface of the object, and automatically complete the scanning of the whole object.

Please refer to Figure 7A. The thick arrow is θ _p for the original moving direction. Please refer to Figure 7B for the thick arrow. According to the turning compensation angle Δθ _α and the depth yaw angle Δθ _β , the corrected moving direction is corrected. According to the automatic scanning measurement process of the image path compensation step diagram according to FIG. 3, when the change of the depth value is less than a set threshold T _Z and one of them is equal to 0, the scanning operation is completed, and the scanning is stopped.

In addition, the device may be a mobile platform 14 or a robot arm having X, Y, Z and θ combined into multiple axes, but not limited thereto, for moving the camera 11 and the laser scanning device 12 to the central processing unit. 13 planned moving positions, so a turning compensation angle Δθ _α of the first plane direction (XY plane) of the above embodiment and a depth yaw compensation angle Δθ _{β of the} second plane direction (XZ plane) can be Change to a turn compensation angle Δθ _{α in the} first plane direction (XZ plane) and a depth yaw compensation angle Δθ _{β in the} second plane direction (XY plane), or change to the first plane direction (YZ plane) A turn compensation angle Δθ _α and a depth yaw compensation angle Δθ _{β in the} second plane direction (YX plane) are equal variations and modifications according to the scope of the present invention.

A non-contact object space information measuring device according to the present disclosure, as shown in FIG. 1, includes: a camera 11 for acquiring an image of an object 15 to be tested; and a laser scanning device 12 for scanning for testing The contour of the object 15; the mobile platform 14, the camera 11 and the laser scanning device 12 are fixed on the mobile platform 14; a mobile control unit 16 for controlling the movement of the mobile platform 14 in a three-dimensional space; and a central processing unit 13, the mobile control unit 16 is connected, and the imaging angle of the camera 11 and the scanning angle of the laser scanning device 12 are controlled via the movement control unit 16; wherein the central processing unit 13 performs an adaptive initial scanning positioning, and a Adaptive image acquisition path compensation. The central processing unit 13 includes a calculation unit that obtains a major axis direction of the object 15 to be tested according to the image of the object 15 to be tested, and performs an adaptive initial scan positioning, according to a depth obtained by the laser scanning device 12 scanning. Information, calculating a turning compensation angle Δθ _α and a depth yaw compensation angle Δθ _β ; and a coordinate conversion unit according to the turning compensation angle Δθ _{α of} the object 15 to be measured and the depth yaw compensation angle Δθ _β , The adaptive image path compensation is performed to be converted into a moving path and output to the mobile control unit 16.

The central processing unit 13 performs an adaptive initial scan positioning, and further includes: an initial scan positioning module. Referring to FIG. 3, the image of the object 15 to be measured captured by the camera 11 is obtained, and the object to be tested is obtained. The main axis direction θ _p , the initial scan positioning module acquires the first image of the camera 11 for one working area, and obtains the second image after the object 15 to be tested moves into the working area, and the first image and the first image 2 image subtraction to obtain a captured position image of the object 15 to be tested; the initial scan positioning module example obtains the centroid and length of the captured position image according to a second order spatial moments algorithm. In the axial direction, the main axis direction θ _{p is} established; the initial scanning positioning module drives the laser scanning device 12 to find a boundary point along the main axis direction θ _p , which is exemplified by the Sobel gradient boundary detection method.

The central processing unit 13 performs adaptive image capturing path compensation, and further includes: an image capturing path compensation module. Referring to FIG. 3, the image capturing the plurality of images of the object 15 to be tested by the laser scanning device 12 in the direction of the main axis is obtained. Obtaining a corresponding bending direction θ of a second time point according to a turning compensation angle Δθ _α in a first plane direction at a first time point and a depth yaw compensation angle Δθ _{β in} a second plane direction _{After p} enters a second time point at the first time point, a scan line of the laser scanning device 12 is directed to the corresponding spindle direction θ _p at the second time point to establish an image capturing path, and the initial scanning position is established. The spindle direction θ _p obtained in the module drives the movement control unit 16 to control the laser scanning device 12 to continuously generate scanning line scanning measurements along the main axis direction θ _p , and each scanning line finds the starting point and the ending point at which the depth value changes the most. The point depth value and the end point depth value of the same scanning line are greater than or equal to a threshold value T _z , and the turning processing is calculated by the central processing unit 13 every nth scanning line to the n+k scanning line. Compensating the angle Δθ _α and the depth yaw compensation angle Δθ _β , and then continuing the spindle direction θ _p obtained in the initial scanning positioning step, driving the movement control unit 16 to control the laser scanning device 12 along the main axis direction θ _p Continuously generating scan line scan measurement, the same point depth value and an end point depth value of the same scan line, if less than a threshold T _z , and when the depth value of the start depth value changes, or the depth value of the end depth value When there is a change of 0, the movement control unit 16 controls the laser scanning device 12 to rotate +90° or -90° in the scanning spindle direction θ _p , and then continues to drive the movement control unit 16 to control the laser scanning device 12 . Scanning line scan measurement is continuously generated along the main axis direction θ _p . If the same point depth value or an end depth value of the same scan line is less than a threshold value T _z , and the depth value of the starting depth value changes, or When the depth value change of the end point depth value is not 0, the movement control unit 16 stops scanning.

The method for calculating a non-contact imaging path is used to drive a mobile platform 14, wherein the camera 11 and the laser scanning device 12 are fixed on the mobile platform 14, and the steps include: performing an initial scanning positioning. step, as shown by the line image acquired by the camera 11 captured the object to be measured 15, and outputs the object to be measured 15 in the major axis direction as θ _p acquired FIG. 2; and performing a channel compensation image capturing step, as in the first As shown in FIG. 3, a plurality of images of the object 15 to be tested are scanned by the laser scanning device 12 along the main axis direction, and a turn compensation angle Δθ _α and a first plane direction are used according to a first time point. a depth yaw compensation angle Δθ _{β in the} second plane direction, after a corresponding spindle direction θ _p at a second time point, when entering the second time point at the first time point, the laser scanning device 12 is A scan line is directed to the corresponding major axis direction θ _p at the second point in time to establish an image capture path. The initial scan positioning step includes: obtaining a first image of the camera 11 for a working area, and then acquiring a second image after the object 15 to be moved into the working area, and subtracting the first image from the second image to obtain a test. The image of the captured position of the object 15; according to the second order spatial moments algorithm, the centroid and the long axis direction of the captured position image are obtained, and the spindle direction θ _{p is} established; the laser scanning device 12 is driven along the main axis The direction θ _p finds a boundary point, which is based on the Sobel gradient boundary detection method, and its mask system ,as well as .

The image capturing path compensating step, as shown in FIG. 3, performs automatic scanning measurement, and includes the step 31 of driving the movement control unit 16 to control the laser scanning device 12 by the spindle direction θ _p obtained in the initial scanning positioning step. The scan lines are continuously generated along the spindle direction θ _p for scanning measurement; in step 32, the start point and the end point coordinate with the largest change in depth value are found by each scan line; and in step 33, the start point depth value and the end point depth of the same scan line are determined. If the value is greater than or equal to a threshold value, each of the n-th scan line to a first scan line n + k, in step 34, is calculated by the central processing unit 13 to compensate the turning angle △ θ _α, step 35 and the depth of the partial The pendulum compensation angle Δθ _β , step 36 corrects the main axis direction θ _p according to the turning compensation angle Δθ _α and the depth yaw compensation angle Δθ _β , and then returns to step 31 to drive the movement control unit 16 to control the laser scanning device. 12, θ rear direction along the main axis of the correction _p 'is continuously generated scan line measurement; in step 33, with a point of the scan line depth value together with an end point when the value is less than a threshold depth, And when the depth value of the change in depth value change starting point depth value, or the end point depth value has one of 0, see step 37, the movement control unit 16 controls the laser scanning device 12, see step 38, θ _p in the major axis direction After rotating +90° or -90°, returning to step 31, continuing to drive the movement control unit 16 to control the laser scanning device 12, continuously generating scanning line scanning measurement along the main axis direction θ _p ; but in step 33, if the same a point depth value of the scan line, or an end point depth value is less than a threshold value, and when the depth value change of the start depth value is not 0, see step 37, or the depth value change of the end depth value is not 0, then The mobile control unit 16 stops driving the scan, see step 39.

The above description is only intended to describe the preferred embodiments or embodiments of the present invention, which are not intended to limit the scope of the invention. That is, the equivalent changes and modifications made in accordance with the scope of the patent application of the present invention or the scope of the invention are covered by the scope of the invention.

△θ _α ‧‧‧turn compensation angle

△θ _β ‧‧‧depth yaw compensation angle

θ _p ‧‧‧main axis direction

θ _p '‧‧‧corrected spindle direction

T _Z ‧‧‧ threshold

Z _S ‧‧‧ starting point depth value

Z _e ‧‧‧end point depth value

21~22‧‧‧Steps 21~22

31~39‧‧‧Steps 31~39

Claims (20)

A non-contact object space information measuring device comprises: a camera for acquiring an image of an object to be tested; a laser scanning device for scanning the object to be tested; and a mobile platform for providing the camera And the laser scanning device is fixed on the mobile platform; a mobile control unit controls the mobile platform to move in a three-dimensional space; and a central processing unit connects the mobile control unit and controls the mobile control unit The unit controls the image capturing angle of the camera and the scanning angle of the laser scanning device; wherein the central processing unit performs an initial scanning positioning and an image capturing path compensation. The measuring device of claim 1, wherein the central processing unit comprises: a calculating unit, obtaining a main axis direction θ _{p of} the object to be tested according to the image of the object to be tested, and according to The laser scanning device scans the obtained at least one depth information to obtain a turning compensation angle Δθ _α and a depth yaw compensation angle Δθ _β ; and a label conversion unit according to the turning compensation angle Δθ _α and the The depth yaw compensation angle Δθ _{β is} performed and output to the movement control unit. The measuring device of claim 1, wherein the central processing unit further comprises: an initial scanning positioning module for acquiring an image of a working area, The image is subtracted to obtain a position image of the object to be tested, and a spindle direction θ _{p is} obtained according to the centroid and the long axis direction of the captured position image. The measuring device of claim 3, wherein the two image systems of the working area are respectively acquired at different time points, and one of the two images includes the object to be tested. The measuring device of claim 3, wherein the initial scanning positioning module further drives the laser scanning device to find a boundary point along the main axis direction θ _p . The measuring device of claim 1, wherein the central processing unit further comprises: an image capturing path compensation module for obtaining a laser scanning device along a main axis The direction θ _p scans the plurality of images of the object to be tested, and obtains a maximum starting point and an end point of each of the image depth changes according to the depth information of the images to obtain a first plane direction of the first time point a turn compensation angle Δθ _α and a depth yaw compensation angle Δθ _{β in the} second plane direction, thereby obtaining a spindle direction θ _p ' at a second time point, and entering a second time at the first time point At the point, a scan line of the laser scanning device is directed to the main axis direction θ _p ' at the second time point. The measuring device according to claim 6, wherein the turning compensation angle Δθ _α is obtained based on a plurality of intermediate points of the starting point and the ending point. The measuring device according to claim 6, wherein the depth yaw compensation angle Δθ _β is obtained based on the starting point and the ending point. The measuring device of claim 6, wherein if the depth values of the starting points and the ending points are greater than or equal to a predetermined threshold, the turning compensation angle Δθ _{α is obtained} and the depth is offset. The pendulum compensation angle Δθ _β , if less than the threshold and one of them is 0, rotates the spindle direction θ _p by +90° or -90°, otherwise the scanning is stopped. The measuring device according to claim 2, wherein the main axis direction θ _{p is} an angle between a main inertia axis of the image of the object to be tested and a target axis, and the main inertia axis refers to the image. The longest distance between any two points on the boundary. A method for calculating a non-contact imaging path for driving a mobile platform, wherein a camera and a laser scanning device are fixed on the mobile platform, the step comprising: performing an initial scanning positioning step, according to The camera captures an image of the object to be measured, obtains a main axis direction θ _{p of} the object to be tested, and performs an image capturing path compensation step, according to the scanning by the laser scanning device along the main axis direction θ _p Measuring a plurality of images of the object, obtaining a turn compensation angle Δθ _α in a first plane direction at a first time point and a depth yaw compensation angle Δθ _{β in} a second plane direction, thereby obtaining a second time point The spindle direction θ _p ', when the first time point enters the second time point, directing a scan line of the laser scanning device to the main axis direction θ _p ' of the second time point to establish an image capturing path. The calculation method of claim 11, wherein the initial scanning and positioning step further comprises: acquiring two images of a working area, and subtracting the two images to obtain one of the objects to be tested; And obtaining the main axis direction θ _p according to the centroid and the long axis direction of the captured position image. The calculation method of claim 12, wherein the two image systems of the work area are respectively acquired at different time points, and one of the two images includes the object to be tested. The calculation method of claim 11, wherein the initial scan positioning step further drives the laser scanning device to find a boundary point along the main axis direction θ _p . The calculation method of claim 11, wherein the image capturing path compensation step further comprises: obtaining a point and an end point where the depth value of each of the plurality of images is the largest; determining the depth value of the starting point and the ending point, If it is greater than or equal to a predetermined threshold, the turning compensation angle Δθ _{α is} obtained according to the complex intermediate points of the starting point and the ending point, and the depth yaw compensation angle Δθ _{β is} obtained according to the starting point and the ending point, but If it is less than the threshold and one of them is 0, the main shaft direction θ _{p is} rotated by +90° or -90°, otherwise the scanning is stopped; according to the turning compensation angle Δθ _α and the depth yaw compensation angle △ θ _β , the main axis direction θ _p ' is obtained. A non-contact object space information measuring method is used for driving a mobile platform, wherein a camera and a laser scanning device are fixed on the mobile platform, and the step comprises: performing an initial scanning positioning step, according to the one object to be measured an image captured by the camera, to obtain a major axis direction of the object to be measured [theta] _p; imaging path for a compensation step, in accordance with the [theta] of the laser scanning apparatus in the main scanning direction _p test a plurality of images of the object, obtaining a turn compensation angle Δθ _α in a first plane direction at a first time point and a depth yaw compensation angle Δθ _{β in} a second plane direction, thereby obtaining a second time point a spindle direction θ _p ', when the first time point enters the second time point, directing a scan line of the laser scanning device to a spindle direction θ _p ' at the second time point; and performing the object to be tested And a measuring step of measuring the size of the object to be tested via the initial scanning positioning step and the image capturing path compensation step. The measurement method of claim 16, wherein the initial scanning and positioning step further comprises: acquiring two images of a working area, and subtracting the two images to obtain a position of the object to be tested. The image is obtained from the centroid and the long axis direction of the captured position image to obtain the spindle direction θ _p . The measurement method of claim 17, wherein the two image systems of the work area are respectively acquired at different time points, and one of the two images includes the object to be tested. The measuring method of claim 16, wherein the initial scanning positioning step further drives the laser scanning device to find a boundary point along the main axis direction θ _p . The measurement method of claim 16, wherein the image path compensation step further comprises: obtaining a point and an end point where the depth value of each of the plurality of images has the largest change; and determining a depth value of the start point and the end point. If greater than or equal to a predetermined threshold, the turn compensation angle Δθ _{α is} obtained according to the plurality of intermediate points of the start point and the end point, and the depth yaw compensation angle Δθ _{β is} obtained according to the start point and the end point, However, if it is less than the threshold and one of them is 0, the main shaft direction θ _{p is} rotated by +90° or -90°, otherwise the scanning is stopped; according to the turning compensation angle Δθ _α and the depth yaw compensation angle Δθ _β , the main axis direction θ _p ' is obtained.