Classifications

• • G—PHYSICS
  • G01—MEASURING; TESTING
  • G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
  • G01B11/00—Measuring arrangements characterised by the use of optical techniques
  • G01B11/24—Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
  • G01B11/25—Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures by projecting a pattern, e.g. one or more lines, moiré fringes on the object

Definitions

• the present invention relates to an opticocomputer method for 3D measurement of the complete or near-complete outer surface of a fringed projection object and use of a phase shift method and a corresponding measurement system.
• the surface characterization and the relief measurement by optical methods are realized thanks to different techniques among which the triangulation, the photogrammetry, the Moiré technique, the interferometry, the holography and the technique of "Speckle".
• photogrammetry is a widely used technique, but its use is often limited because of a certain complexity of the measurement process and its relatively high cost of implementation.
• This projection principle is a contactless optical method that is widely recognized as having a high potential for the measurement and characterization of a wide variety of objects.
• This method makes use of parallel or divergent luminous fringes projected onto the surface of an object by means of a conventional imaging system or a coherent light interference pattern and an image acquisition apparatus whose axis is distinct from that of the fringe projection system.
• the resulting phase distribution of the bright fringes of the image acquired contains information on the relief of the illuminated surface of the analyzed object. This phase distribution is processed by calculation to reconstruct the relief of the surface of the object.
• the Phase Shifting Method is a powerful method for reconstructing the phase distribution of a set of light fringes because of its high precision and accuracy. its speed of execution. It has been implemented with a piezoelectric transducer which makes it possible to obtain an offset of the light fringes, ie modulates their phase distribution. Another implementation consists in modulating the wavelength of a laser diode by driving its current, the diode being in a non-compensated interferometer to induce the phase shift of the light fringes. Another alternative for inducing this phase shift of the light fringes is to use a liquid crystal mask in the fringe projection system and to illuminate it in white light.
• phase shift calibration algorithms using four or five image acquisitions of the light fringes have been developed. These algorithms are very useful for identifying and compensating for measurement error sources such as non-constant phase shift, higher order harmonics in light fringes, and very low signal-to-noise ratios.
• Other phase shift calibration methods have been developed but they increase the amount of computation and therefore consume many more resources and processor time.
• the one with two distinct points of view and / or two distinct points of illumination can be associated with an algorithm of stripping of the phase and, this, in order to recover the absolute value and not modulo 2 ⁇ of the phase, ie the value of the phase without ambiguity.
• the PSM technique is robust, producing a very limited number of erroneous propagation effects.
• this automatically solves the problems associated with discontinuities of the light fringes which could taint the accuracy of the results or even prevent a correct phase measurement.
• the analysis algorithm is optimized in terms of time and memory consumption and is therefore easily executed on a personal computer for example.
• the present invention proposes to improve the PSM technique.
• the invention is based on a shape reconstruction system of an object by projection of light fringes using the phase shift method (FP-PSM system for "Fringe Projection - Phase Shifting Method") in which a set of illuminated fringes by illuminating a mask with light, which mask is a screen with opaque areas and light-transparent areas, which areas are distributed in a defined pattern, which pattern is produced by transmitting light through the mask wanted set of bright fringes and projected all these light fringes on the surface of an object to be treated.
• phase shift method FP-PSM system for "Fringe Projection - Phase Shifting Method”
• Images of the fringed object are acquired with a camera and repeats the acquisition operation several times by moving the set of light fringes in space and between each acquisition so that there is a phase shift of the distribution of the light fringes between each acquired image of the illuminated surface of the object.
• the acquired images are processed by calculation in a computer, in particular the phase shift of the distribution of the light fringes between each image makes it possible to recover the distributed variations of the height (the relief) of the illuminated surface of the object, visible variations according to the projection axis pair (axis of the light beam projected on the object, also called illumination axis) versus acquisition axis (axis of the image acquisition camera, also called shooting axis).
• the relief thus recovered is the partial relief of the illuminated surface of the object which includes all the visible details according to the pair projection and acquisition axes.
• the invention relates to the integration in the FP-PSM system of four fringe projection paths and four image acquisition paths of the surface of an object illuminated by the fringes according to a particular tetrahedral geometry.
• the projections of the fringes on the object are made according to four incidences from at least one device of illumination of the object by fringes associated (s) with possible means of switching and returning the luminous beam of fringes towards the object and whose illumination points are considered, an illumination point being a point from which emerges the light allowing the direct illumination of the surface of the object by fringes (each point of illumination is therefore along the corresponding incidence, that is to say along the projection axis), the illumination device as a physical entity that can correspond to the point of illumination or be physically shifted from the point of illumination and the illumination returned to the object or, more generally, the illumination device may be divided into several elements, one of which may correspond to the point of illumination as will be seen later.
• the four points of illumination are placed substantially at the vertices of a tetrahedron (at or near the vertices) at the center of which the object is located.
• the lines coming from the illumination points and passing through the center of the tetrahedron define the projection / illumination axes of the system (or "bearings" indicated above).
• the four illumination points are at a sufficient distance from the object so that each pair of illumination points illuminates the surface delimited by the contour seen according to the pseudonormal at said surface which pseudo-normal is the median of the two projection axes in the plane that they define together.
• the shooting there are four shooting points placed on the medians of the trihedrons formed by the triplets of projection axes or close to these medians, the straight lines from the shooting points and passing by the center of the tetrahedron thus define the axes of shooting.
• the four points of view are at a sufficient distance from the object so that the fields of view of each pair of points of view include the area defined as previously by the pair of two common neighboring projection axes. to the two axes of shooting of the pair of shooting points.
• each surface included in the contour defined above is visible by two points of view.
• the four points of illumination project luminous fringes on the object, each according to its axis of projection, but not necessarily the same set of luminous fringes.
• the invention relates first of all to an optico-computing method for 3D measurement of the external surface of an object in relief by projecting fringes on said object and using a phase shift method, the fringes being projected on the object by at least one illumination device, images of the fringed object being taken along several axes of shooting with at least one means of shooting, said images being transmitted to a computer equipment comprising a program relief calculation from the images.
• each projection axis being considered as a point of illumination disposed substantially at each of the four vertices of a virtual tetrahedron, the object being placed substantially in the center of said tetrahedron, and the shots are taken from four points of capture substantially along four axes of view, each of the axes of view being the median (from the center of the tetrahedron) of one of the four trihedrons formed by the four triplets of projection axes, the four points of view being at a distance from the object such that at each point of view, each image includes at least a part of each of the three surfaces of the object that can be illuminated by the three points of illumination of the triplet of projection axes defining by its median the axis of view of said point of view a set of images of each of the six il
• substantially mean that the points are on the corresponding axis or in its vicinity.
• the measurement of the external surface must be understood as meaning the measurement of the surface on which the fringes appear projected for the optical acquisition means, any transparent thicknesses at the surface that can not be taken into account since the illumination fringes through.
• the four illumination points come from at least one and up to four illumination devices by fringes, and in that said device is provided at the illumination points and / or the illuminations said means is redirected by at least one mirror and / or said means are physically movable,
• the four illumination points come from four independent illumination devices, said devices being arranged at the points of illumination or the illuminations being redirected towards the object,
• the illumination is redirected towards the object by at least one mirror
• the four illumination points come from three independent illumination devices,
• the four illumination points come from two independent illumination devices
• the four illumination points come from a single illumination device
• the four illumination points come from a single illumination device, and in that the illumination of said means is redirected along the corresponding projection axis by a set of mirrors,
• the mirror (s) are active, (the mirrors act as a four-output beam switch) the mirror (s) are controlled by the computer equipment,
• an illumination source a beam expander and a liquid crystal screen controlled by the computer equipment are used for each illumination device to form a fringe pattern
• a light source, a beam expander and a liquid crystal screen controlled by the computer equipment are used for each illumination device, in order going towards the object, to form a fringe pattern therein ,
• two independent and movable imaging means are used which can be moved for at least one of them
• the shooting axis can be moved by physical displacement of the corresponding shooting means
• the axis of shooting is movable by redirection by a set of mirrors
• the means of shooting is of the camera or camera type and makes it possible to capture images that can be transmitted to the computer equipment,
• the object is sequentially illuminated along the four projection axes, to acquire a set of images of each of the six surfaces that can be illuminated and defined by six pairs of illumination points,
• the invention relates secondly to a 3D measurement system of the outer surface of a raised object for implementing the method of any one of the preceding claims, which is characterized in that it comprises at least one illumination device of the object with fringes and a part of image acquisition and relief calculation in a computer equipment comprising a program from said images acquired by at least one means of shooting, the illumination device (s) allowing projection on the object of fringes according to four projection axes (final optical path of the fringes towards the object), the origin (real or virtual according to the structure of the illumination device (s)) ) of each projection axis being considered as a point of illumination disposed substantially at each of the four vertices of a virtual tetrahedron, the object being placed substantially in the center of said tetrahedron, and the images are taken at four points of capture substantially along four axes of view, each of the axes of view being the median (from the center of the tetrahedron) of one of the four trihedrons formed by the four triplets
• the illumination device comprises a light source, a beam expander and a liquid crystal screen controlled by the computer equipment to form a pattern of fringes.
• the initial pattern of the phase distribution of the luminous fringes is determined in a software manner and can be modified in particular (without any material modification in the preferred version) by a trained operator or software which determines the optimal pattern for a particular object.
• a trained operator or software which determines the optimal pattern for a particular object.
• the phase shift is controlled by the processeu r and induced by the mask in an extremely fast time which allows to proceed more r acquisitions of images in milliseconds.
• the speed of acquisition and processing places the system of the invention in the category of "real time" systems which allows its implementation on the production lines.
• this non-contact system is well adapted to hostile environments (dirt, vibrations) and does not require any absolute positioning of the object.
• FIG. 1 which is a known single-channel measurement system of the outer surface of an object
• Figure 2 which is an example of an algorithm for a two-channel system with an illumination point and two taps
• FIG. 3 which is an example of an algorithm for a two-channel system with two illumination points and a point of view (2PI / 1PV)
• FIG. 4 which shows schematically, relative to an object, the illumination points and the projection axes with regard to the means of illumination of the object by fringes as well as the axes of shooting on which are placed the points of view in the case of the tetrahedral multi-channel system of the invention
• FIG. 4 which shows schematically, relative to an object, the illumination points and the projection axes with regard to the means of illumination of the object by fringes as well as the axes of shooting on which are placed the points of view in the case of the tetrahedral multi-channel system of the invention
• FIG. 5 which shows the three-dimensional tetrahedral system with, in its simplest version, four liquid crystal screens placed at the four illumination points and from which emerge the luminous fringes projected along each projection / illumination axis and four cameras placed at four points of view.
• a set of light fringes distributed in the right section of a light beam (the "beam") according to a known initial pattern is generated.
• the distribution of the fringes can be modeled by a two-dimensional distribution of the phase of the luminous intensity or phase of the luminous fringes in the cross section of the beam.
• a mathematical function ⁇ then completely describes this phase distribution.
• All luminous fringes are projected onto the surface of an object whose relief is to be reconstructed.
• the set of luminous fringes forms on the surface illuminated by the object a distorted image of the initial pattern of all the luminous fringes.
• the variations of the height, ie the relief of the illuminated surface, cause this deformation of the initial pattern.
• the image thus formed on the surface is a distribution of the phase of the luminous fringes which results from the modulation of the distribution of the phase of the luminous fringes of the initial pattern by the relief of the illuminated surface.
• FIG. 1 A known single-channel system for reconstituting the partial relief of the illuminated surface by a fringe pattern is shown in FIG. 1 and comprises for the illumination device of the object 6 by fringes:
• a uniform light source 1 also called “source”
• source the most homogeneous possible (homogeneity of the distribution of the light power in the cross section of the emitted beam)
• beam expander 2 also called “expander” producing, here, a parallel beam 4
• liquid crystal screen 3 also called a "mask”
• a reflecting mirror 10 the illumination device thus making it possible to produce an illumination beam along an illumination axis 5, and for the acquisition and processing part:
• a CCD type 8 camera making it possible to acquire images of the object 6 illuminated by the fringes along a shooting axis 7, a computer equipment 9 (computer / microcomputer) comprising a processor capable of performing calculations according to algorithms on data including the images acquired by the camera, as well as driving the mask to set the fringe pattern.
• the light source generates the light necessary for illumination through the mask of the surface of the object whose system must reconstruct the relief of the illuminated surface.
• the beam expander gives a parallel section of the light beam with the dimensions required to properly illuminate the mask and the surface to be illuminated of the object.
• the position of the source 1 relative to the expander 2 determines the divergence or not of the light beam passing through the mask and illuminates the object.
• the dimensions of the illuminated surface are not necessarily limited to the dimensions of the mask and may be larger or smaller than the latter.
• a parallel illumination beam as shown in Figure 1, simplifies the calculations.
• the axis of the optical system consisting of the source, the expander and the mask which is also the axis of propagation of the light beam is oriented so that the surface of the object is illuminated directly (direct illumination), no other components are needed between the mask and the object. If, in a variant, this axis is initially oriented in a direction that does not pass through the object, then a mirror is placed between the mask and the object and oriented to redirect the initial light beam towards the object in order to properly illuminate the surface with the fringes (indirect illumination).
• the processor 9 controls the mask 3 to generate all the light fringes according to the desired pattern, controls the camera 8 and stores the images acquired by the camera and proceeds to the calculations necessary to determine the relief of the illuminated surface of the object for example 3D visual reconstruction on a screen.
• This system is said to be a single channel because it has only a couple or duet of point of illumination and point of view.
• a two-channel system comprises, for example, on the one hand, a uniform homogeneous light source possible, a beam expander, a liquid crystal display (the mask), an optical beam switch and several mirrors, and, on the other hand, two cameras and a processor.
• This type of two-channel system has one illumination point and two cameras and is symbolized 1PI / 2PV.
• the mirrors are distributed and distributed in space so that they can bend a light beam according to one or the other of two possible paths, each path being defined by a system of mirrors that illuminates the surface of the light. object along a projection axis specific to the path.
• the optical beam switch is driven by the computer and directs the light beam from the mask to one or the other of the mirror systems.
• the surface of the object is illuminated sequentially according to the two possible pairs of axes of projection and acquisition of the two-channel system.
• the processor proceeds to the reconstruction of two distinct partial reliefs and thanks to these two reliefs to the reconstruction of the almost complete relief of the illuminated surface of the object.
• the two partial reliefs reconstructed according to two, the choice, the four possible pairs of axes of projection and acquisition being distinct, it is possible to reconstruct without ambiguity the relief of the illuminated surface of the object through a stripping technique of the phase. This relief is then the quasi-integral relief of the illuminated surface of the object.
• the mask shapes the initial pattern of the distribution of the object. phase of bright fringes.
• the processor determines which pixels of the mask should be opaque or transparent to the light of the beam passing through it.
• the initial pattern is preferably formed in a parallel section of the same beam (non-diverging and non-converging straight beam).
• the illumination beam may be divergent, but this complicates the process because it is necessary to know the divergence to take it into account in order to correct the surface measurement calculations.
• the beam illuminates the surface of the object and is either reflected from the surface (opaque surface to beam light, reflection operation) or transmitted to the beam. through the object (object transparent to the light of the beam, operation in transmission).
• the transparent objects it is however necessary that a fringe pattern is deposited on a surface of the object and is visible
• the transparent objects are measurable in transmission provided that one of the two faces crossed between the P1 and / the PV does not distort the pattern of the fringes that has formed on the other, otherwise the information is no longer reliable because it is not possible to distinguish between the deformations of the one or the other face of the object.
• the images formed on the surface of the object and seen from both viewpoints of the two cameras are acquired and digitized by the two cameras that transmit them to the processor.
• the processor acquires several images of the illuminated surfaces of the object. Between each acquisition, the processor controls the mask so that the initial pattern of the phase distribution of the luminous fringes is shifted in space, ie the distribution of the phase undergoes a desired phase shift and is therefore known. .
• the processor can then proceed to the necessary calculations: it calculates the phase variations of the phase distribution of the light fringes and proceeds to the stripping of this phase thanks to the two points of view (that is to say that it determines the absolute value and not modulo 2 ⁇ ) which makes it possible to obtain the exact relief of the surface of the object, that is to say without ambiguity.
• the parts of the surface not visible by one channel are visible by the other which allows to reconstruct almost all the surface illuminated by the two incidences of illumination.
• FIG. 2 An example of an algorithm that can be used for such a 1 PI / 2PV two-channel system is given in FIG. 2.
• a two-channel system may alternatively have two illumination points and a camera. It is then symbolized 2PI / 1PV.
• An example of an algorithm that can be used for such a two-channel 2PI / 1PV system is given in FIG. 3.
• the system comprises, for example, on the one hand, for the device for illuminating the object with fringes, preferably:
• the illumination system may comprise other arrangements, in particular in number of sources, expanders, screens and switches whose type is adapted accordingly) and for the acquisition and processing part, preferably:
• the mirrors are distributed between four mirror systems and distributed in space so that they can bend a light beam according to one or the other of four possible angles, each incidence being defined by a system of mirrors that enables illuminate the surface of the object along a clean projection / illumination axis.
• the optical beam switch is driven by the computer and directs the light beam from the mask to one or the other of the mirror systems.
• the surface of the object is sequentially illuminated along the four possible projection / incidence axes of the tetrahedral multi-channel system of the invention.
• a projection / incidence axis is defined by the segment from the center of the last mirror of each possible path (which mirror reflects the light fringes directly onto the object to illuminate it with fringes) and the center of the illuminated surface.
• Each last mirror defines an illumination point.
• the four points of illumination are placed at the vertices of a tetrahedron (or near these vertices) at the center of which is the object to be illuminated. The edges coming from the points of illumination and passing through the center of the tetrahedron merge with the projection axes of the system.
• the four points of illumination are at a sufficient distance from the object so that each pair of illumination points illuminates the surface delimited by the contour seen according to the pseudo-normal to said surface, which pseudo-normal is the median of the two projection axes in the plane that they define together.
• Each of the four cameras (or mirror to a camera) is placed at a point on one of the four medians (from the center of the previously defined tetrahedron, with one camera per median) of the four trihedrons formed by the four triplets of projection axes or is placed close to one of these four medians.
• Each camera is thus placed at a point of view.
• the edges coming from the points of view and passing through the center of the tetrahedron define the axes of shooting of the system.
• the four points of view are at a sufficient distance from the object so that the fields of view of each pair of shooting points includes the area defined as previously by the pair of two adjacent projection axes common to both shooting axes of the pair of shooting points.
• FIG. 4 This arrangement is shown schematically in Figure 4 in which an object is placed in the center O of a tetrahedron whose four vertices PM, PI2, PI3 and PI4 form the four points of illumination. From these four points of illumination start along axes of projection / illumination PM-O, PI2-0, PI3-0 and PI4-0, the light beams bearing fringes and directed towards the center of the tetrahedron and, therefore, illuminating the object with fringes.
• the four illumination axes make it possible to define four trihedrons formed by triplets of projection axes (triplets of which there are four).
• the median of each trihedron is the support of a shooting axis and thus there are four shooting axes thus defined, PV1,2, PV2,3, PV3,4 and PV1,4.
• the processor proceeds to the reconstruction of the distinct partial reliefs defined by each pair of projection and shooting axes and thanks to these reliefs to the unambiguous reconstruction of the almost-complete relief of the various illuminated surfaces of the object. Thanks to the unambiguous and almost integral reconstruction of these illuminated surfaces, the processor proceeds to the unambiguous reconstruction of the quasi-integral relief of the complete outer surface of the illuminated object.
• the four projection axes make it possible to project fringes on the object but not necessarily the same set of luminous fringes for all the axes.
• a set of images of each of the six illuminated surfaces defined by the six pairs of illumination points is acquired. These images make it possible to recover the partial reliefs (seen according to the two pairs of axes projection and acquisition defined by two axes of projection and an axis of acquisition or, again, a projection axis and two axes of acquisition or, finally, a projection axis and a shooting axis and another axis of projection and another axis of shooting all four neighbors together) of each of the six illuminated surfaces of the object.
• quadsi quadsi-integral
• the invention allowing, when the complete illumination and visualization of the surface are possible, to find the completeness surface details.
• the luminous fringes used are "analog" in the sense that the transition between the minimum brightness and the maximum brightness is continuous, ie is a grayscale gradient and not an abrupt transition. which would be called “digital".
• a mask / liquid crystal screen that can be controlled in gray levels is used. This makes it possible to improve the accuracy of the reconstruction of the relief of the illuminated surface of the object.
• the pitch of the luminous fringes determines the accuracy / resolution of the relief measurement. The smaller this step, the better the measurement accuracy of the PSM method.
• This accuracy is however also determined by the quality of the other components of the system such as the step of the gray levels that the acquisition camera can distinguish and the resolution of the acquisition camera, namely the periodicity of its pixels .
• the quality of the image processing algorithm further determines the resolution and measurement accuracy of the PSM method.
• Each triplet of partial reliefs makes it possible to recover the quasi-integral surface of a hemisphere of the sphere, each hemisphere being illuminated by an illumination point because this point is sufficiently far away from the sphere for this purpose.
• This example of an object of the spherical type corresponds to an implementation intended more generally for the treatment of an object whose relief of the surface is a priori not known. This implementation requires a complex phasing and is relatively heavy.
• each illumination axis illuminates a defined area of the surface of the object being treated, which area generally intersects a portion of the area illuminated by each of the other three axes of illumination except exceptionally unfavorable geometry of the object treated. It is understood that it is desirable that it be so to leave no extent of the surface of the treated object not illuminated and therefore not treated.
• a first configuration called “trivial” includes four light sources, four beam expander, four LCD screens and four cameras.
• the accuracy of the measurement is the best because the projection of the patterns and the acquisition by the cameras are direct and therefore without deformations of the image fringed by components intermediate.
• this hardware configuration is relatively expensive.
• a second configuration comprises a light source, a beam widener, a liquid crystal screen placed immediately after the beam expander, a camera, three optical switches at an input and two outputs (1 X2) and three switches with two inputs and one output (2X1).
• the three switches 1 X2 are intended to switch the light emitted by the source to one of the four paths each leading to one of the four illumination points by placing a switch 1 X2 at each output of the switch 1 X2 whose input captures the light emitted by the source, the outputs of two downstream switches each feeding one of the paths leading to one of the four illumination points.
• the three 2X1 switches are intended to switch light from each point of view to the camera by placing a 2X1 switch so that it captures light from two paths coming from two shooting points and a 2X1 switch. so that it captures the light from the other two paths from the other two points of view and placing the third switch 2X1 so that it captures the light from the outputs of the two previous 2X1 switches and its output illuminates the camera.
• a set of mirrors (preferably "almost perfect") completes the configuration to guide the four paths bringing light to the four points of illumination and the four paths from the four points of view.
• switches 1 X2 and 2X1 are used which are a switch with one input and four outputs (1 X4) and a switch with four inputs and one output (4X1). ).
• the switch 1 X4 switches the light emitted by the source to one of the four paths each leading to one of the four illumination points and the switch 4X1 switches the light from each of the four paths from each of the four shooting points to the camera.
• a set of mirrors completes this configuration in order to orient the four paths leading the light to the four points of illumination and the four paths coming from the four points of view.
• a third hardware configuration is derived from the second configurations and has the same elements except that there are four liquid crystal screens instead of one, each screen being placed between one of the four illumination points and the object. treaty.
• the accuracy of the measurement is better than that of the second configurations due to the absence of deformation of the projected patterns, absence due to the elimination of the intermediate components between the liquid crystal displays and the suface of the treated object.
• the cost of this third hardware configuration is low but slightly higher than the cost of the second configurations.
• a fourth hardware configuration is derived from the second configurations and provides a compromise between cost and accuracy.
• This fourth configuration has the same elements as those of the second configurations but with four cameras each placed in one of the four points of view and only three switches 1 X2 or a switch 1 X4 which switch the light emitted by the source to one the four paths leading to the four points of illumination at a time.
• the accuracy of the measurement obtained is better than that of the second and third configurations because the acquisition by the cameras is di rect and therefore without deformations of the image fringed by intermediate components.
• the cost is a little higher than those of the second and third configurations but lower than that of the first configuration.
• a fifth hardware configuration is derived from the fourth configuration and also provides a compromise between cost and accuracy.
• This fifth configuration has the same elements as those of the fourth configuration but with four liquid crystal screens each placed between one of the four points of illumination and the surface of the object treated.
• the accuracy of the measurement obtained is better than that of the fourth configuration because the projection of the patterns and the acquisition by the cameras are direct and therefore without deformations of the image fringed by intermediate components.
• the cost is slightly higher than that of the fourth configuration but lower than that of the first configuration.
• Each control mode includes different phases of illuminations / acquisitions, some examples of which are provided below.
• a first modality consists of a complete control in which all the quadruplets defined by an illumination point and three points of view work and that, one after the other (an illumination and three sets of acquisitions).
• an illumination and three sets of acquisitions For each projection axis, three sets of acquired images are available for processing, one set per axis of view.
• the information obtained is as complete as possible, but the acquisition time is the least optimized and the use of computer resources is the heaviest.
• the acquisition time per quadruplet is the same as for a single-channel system (an illumination point, a point of view) but, on the other hand, the Processing time is longer because there is more information to process.
• the quadruplets may alternatively be defined by a point of view and three adjacent illumination points.
• three sets of acquired images are available for processing, one set per projection axis.
• quadruplets three points of illumination / a point of view forces the point of view to acquire all these points. images sequentially, each illumination point illuminating one after the other so as not to destroy the fringe patterns projected by each of the different points of illumination. This last mode of driving However, this is of little interest, especially as regards the acquisition time which is the longest for the tetrahedral multi-channel system of the invention (except colorimetric multiplexing).
• a second modality consists of a semi-complete piloting.
• This modality corresponds to the previous one except that some or all quadruplets are reduced to triplets (one point of illumination and only two adjacent points of view) and that only the quadruplets or triplets necessary for the recovery of the quasi-integral relief of the entire surface of the processed object work to avoid unnecessary redundant information.
• the acquisition time and the use of IT resources are improved.
• the degree of complexity of the relief of the surface of the object treated and the degree of complexity of the geometry of the same object determine the number of quadruplets and / or triplets necessary for the desired treatment.
• a third modality consists of an optimized control in which an illumination channel and a camera of an adjacent shooting axis operate at the same time, the different pairs or duets of illumination points / shooting point operating at one and the same time. after others.
• the duets illumination axis / shooting axis are chosen so that the information necessary for the treatment of the surface of the treated object is sufficient to cover the almost complete relief of this complete surface but is also reduced to minimum necessary for this.
• two duets have a point of illumination in common and that this is necessary for the good quasi-integral relief coverage of the illuminated surface, it is clear that these two duets must function at the same time, ie constitute again a triplet.
• three duets with a point of illumination in common they gather in a quadruplet. So the time acquisition is optimized and the use of computer resources also. This piloting procedure is only feasible if the relief and the geometry of the treated object are sufficiently simple.
• the FP-PSM method is the most suitable for the tetrahedral multi-channel system of the invention, other methods can be implemented with such a system for resolving the integral (or almost integral) relief of the outer surface of an object in three dimensions.
• the number of light sources, wideners and liquid crystal displays for generation of the fringes can be between one (as described above) and four, the system (s) switching of illumination beams by fringes and reflecting mirrors towards the object being provided accordingly. It may be the same for the number of cameras, between one and four, and with less than four cameras, means (s) switchable (s), displacement (s) camera (s) ...) to allow shooting from the four locations are provided to allow the geometric distribution described.
• the illumination beam switching system (s) may, in certain embodiments, be combined with the mirrors, the mirror acting as a beam switching means.
• many applications are possible, simple 3D visualization on 2 D screen, visualization in space by means of 3D visualization, control of a machine for photo-polymerization of 3D objects or a do machining machine ...
• the invention can be applied to color fringes, several illumination devices, each of one color specific, being implemented for colorimetric multiplexing, the color camera (s) and the computer equipment can differentiate the illumination fringes according to the color during simultaneous illuminations of the object from several illumination points .
• one or more calibration steps with standard objects can make it possible to take into account and correct various optical aberrations and / or slight shifts in the arrangement of the elements of the system during subsequent measurements on the objects to be measured.

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