• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to the real-time measurement of relative position data and / or geometric dimensions of a moving body (1) by a lighting unit (2) and a detector unit (4), wherein the moving body (1) is guided relative to the two guided. From the illumination unit (2), light beams (3) are sent in the direction of the detector unit (4); the moving body (1) protrudes between the illumination unit (2) and the detector unit (4) in the volume flooded by the light beams (3) so that the shadow boundary of the shadow thrown thereby by the moving body (4) passes over the detector unit (4) , The detector unit (4) comprises a planar optical position detector (4.1) which is designed as a planar optical waveguide which contains photoluminescent particles and from which signals are read out whose intensity is determined by a plurality of small-area photoelectric sensors (4.1.1) is correlated with the intensity of the light (4.1.1) in the waveguide mode at the location of the sensor.
    公开号:AT511200A4
    申请号:T1534/2011
    申请日:2011-10-20
    公开日:2012-10-15
    发明作者:Robert Dr Koeppe
    申请人:Isiqiri Interface Tech Gmbh；
    IPC主号:
    专利说明:

    J 454
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    description
    The invention relates to the true time measurement of relative position data and / or geometric dimensions of a moving body using optical measuring means, a particularly advantageous application · concerns the monitoring of changes in a wheel of a railway vehicle while driving.
    By DE 11 59 173 B is already proposed in 1962 rail vehicles to record relative movement between the frame and bogie or wheelset while driving. For recording, a pin is moved along with the parts moving relative to the frame, which pin writes on a paper surface which is uniformly stretched relative to the frame.
    According to US 3864093 A, the lateral offset of a wheel of a rail vehicle with respect to the rail is already measured while driving, is illuminated by the vehicle exclusively on the lower part of the rail and the light reflected therefrom by photodiodes as optical sensors, which also on the vehicle are attached is detected. A side edge of the rail shadows a portion of the reflected light from a portion of the sensors. From the position of the shadow edge on the sensors, the lateral wheel offset can be calculated. As a light source, for example, a laser can be used.
    According to US 4040738 A, the position of a rail vehicle relative to a rail is measured by a laser light beam focused as well as possible at a first angle to a surface of the rail lights and by the light spot through a directed from a different angle to the first angle thereon camera through a lens and a photocell array is formed, is imaged. Since the light spot must lie on the plane defined by connecting lines of the lens center with the individual points of the laser beam, the position of the image
    Page 1 ·································································································································································································································································· the position of the light spot relative to the camera can be calculated.
    According to FR 267 48 09 Al and JP 10332323 A, this principle is applied somewhat more widely. Instead of a laser beam with ideally point-shaped cross-sectional area either a laser beam with the cross-sectional area shape of a straight line or with the cross-sectional shape of several, lying along a straight line points is used. The image of the light surface caused by the laser beam on a rail taken by a camera from a defined position enables the distance of the rail to the camera and the calculation of a part of the outline of the cross-sectional area of the rail.
    According to EP 07 07 196 Bl, the above-discussed on laser light sources and photocells based detection means are mounted on the bogie of a rail vehicle. In addition, the movement of the bogie relative to the frame of the rail vehicle is preferably detected by mechanical sensors.
    According to EP 1 324 005 A2, the geometry of the running surface of a wheel of a rail vehicle is measured by the wheel slowly rolling over a measuring rail and being illuminated by a collimated laser beam. The image of the illuminated area is recorded by a camera and evaluated by a computer including the data at which point of the measuring rail the wheel is applied in each case.
    According to US 7715026 B2, a part of the edge line of a cross-sectional area of a stationary wheel of a rail vehicle is measured by pivoting an operating laser range finder over it and continuously recording and evaluating data, which position, direction and distance of the laser range finder and the distance between
    Page 2 • # Φ • · 1 * * * • • • • • • • • • • • • • J J J J J J J J J J J und und und und und J J J J J J J J J J J J ,
    According to EP 2 343 496 A1, a device is proposed, which is arranged on a rail vehicle at the level of the wheels and, as discussed above, has a lighting device and a camera, which are aligned at different angles on a rail, according to the principle discussed above - to measure these. The device is enclosed by a housing into which compressed air is passed through a hose. In the area of the required window of the housing, the compressed air flows out of the housing, thus preventing contamination from reaching the windows from the outside.
    In WO 2010/006348 Al a detector surface is described for the application as a control surface for a data processing system, which detects the fact of the impingement of a light pulse on her and the location coordinates of the point of impact on her. The detector surface is constructed as a planar optical waveguide. At spaced apart locations small-area photoelectric sensors are attached to the planar optical waveguide, at which light arriving via the optical waveguide is coupled out and causes an electrical signal. Parallel to the optical waveguide extends to this a layer with photoluminescent properties. Light in the appropriate wave spectrum, which strikes the layer arrangement, is converted at the photoluminescent layer into longer-wave light, which propagates in the waveguide and thereby reaches the photoelectric sensors. As the distance to the point of coupling into the waveguide increases, the intensity of the light conducted in the waveguide decreases. As a result, it is possible to calculate back from the signal strengths measured at several photoelectric sensors by a kind of triangulation to the location of the incident light incidence. By calculating this back to determine the point of impact of a light pulse
    Page 3 J 454 ··························································································································································································································· many times finer than the pitch of the distances between the individual photoelectric sensors.
    In view of this prior art, the inventor has taken on the task to improve the continuous measurement of position and geometry data of an object in operative movement. It should be possible to make more measurements per unit of time, the volume of data obtained in the measurement should still be easily transferable to the data processing system and the necessary devices should be robust and inexpensive. The invention should also be advantageous to be able to continuously record position and geometry data of a wheel of a railway vehicle in operative driving.
    To solve the problem, it is proposed to provide a light source which shines both on the object to be measured and just past this. As seen from the light source behind the monitored range of motion, a planar optical position detector is arranged, over which runs the shadow boundary of the shadow cast by the object to be measured. The planar optical position detector is - as the detector surface according to the above-described WO 2010/006348 Al - formed as a planar optical waveguide with integrated fotoluminescent Zentem, wherein the optical waveguide spaced relatively small-area photoelectric sensors are mounted, at which light is coupled out of the waveguide mode and causes an electrical signal. The electrical signals are evaluated in a connected data processing system. Changes in the shadow boundary on the planar optical position detector cause signal changes to a plurality of photoelectric sensors. From the amplitude of these signal changes is inferred by the data processing system on the change of the shadow boundary on the areal position detector and from this further to a change in the Po-
    Page 4 •••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••• of the object to be measured.
    The main advantages of this arrangement are: The measuring principle based on luminescence waveguide permits extremely rapid measurements and very rapid readout of the data obtained. This also makes it possible to detect very short-term or repetitive movements or dimensional changes that repeate at high frequency. By filtering out DC components from the individual detector signals, contamination of the transparent cover of the planar optical position detector or of the transparent cover of the light source can easily be prevented from falsifying the measurement result. The planar optical position detector is very cost per unit area compared to other optical position detectors. Therefore, the measuring principle of the invention allows large-scale applications that were previously not realized for economic reasons. - With the proposed planar optical position detector some space problems that occur with other position detectors are well avoidable:
    The proposed position detector is typically present as a flexible plastic film. He does not need to be arranged in a plane, but it can also be applied to a curved surface.
    The proposed position detector can easily be designed so large area that even for the image (or "monitoring") of a large imaging surface no lenses are required, which are required in conventional detectors, the coming of the large imaged surface light on the to focus much smaller detector area. Thus, the detector arrangement according to the invention can be very
    Page 5 • * • 44 44 44 • • 4 4 • 4 4 444 • 4 • 4 • 4 • 4 • 4 • 44 4 J 454 are designed to be much flatter than detector assemblies according to the state of the art Technology. Despite high possible spatial resolution, only a relatively small number of photoelectric sensors read data into a data processing system. Compared to the reading of the more common optical position detectors in which the number of distinguishable faces equal to the number of photoelectric sensors to be read,. Thus, the data transmission to the data processing system in terms of equipment costs easier and it is much faster feasible. - The system components used are relatively inexpensive and robust.
    Further details and advantageous developments are explained in more detail with reference to a schematic diagram:
    Fig. 1: shows a stylized side-sectional partial view of the essential parts for understanding the invention in an exemplary inventive measuring arrangement.
    In the example according to FIG. 1, the moving body to be measured is a wheel 1 which, as indicated by directional arrows, can be rotated about its axis as well as in a direction normal thereto. On a - not shown - body relative to which relative movement of the wheel 1 is to be detected, a lighting unit 2 and a detector unit 4 are attached.
    The wheel 1 could typically be a wheel of a rail vehicle. The purpose of the measurement would then be to determine deflections of the wheel relative to the rail vehicle or the bogie in the vertical direction and changes in shape of the tread of the wheel in real time and to document in a data processing system. Lighting unit 2 and detector unit 4 would be
    Page 6 • * • ft •• ft * • • ft ft ft • ft • ft • ft • ft • ft • ft * ft * J 454 then at the frame of the Rail vehicle or on the bogie on which the wheel is held attached.
    From the illumination unit 2, light beams 3 are sent to the detector unit 4. The light beams 3 are as well as possible collimated with respect to each other (ie aligned parallel to one another) or aligned as well as possible starting from a common real or virtual punctiform light source.
    With regard to the direction of the light beams 3, the object to be measured, in the example illustrated a wheel 1, is arranged between the illumination unit 2 and the detector unit 4. This wheel 1 protrudes into the volume flooded by the light beams 3, so that it casts a shadow whose edge line extends over the detector unit 4. When the wheel 1 is linearly moved normal to the direction of the light beams 3, or when its peripheral surface protruding upon rotation into the light-flooded volume is deformed, the shadow boundary on the detector unit 4 is shifted. Shifting the shadow boundary causes 4 signals in the detector unit.
    The core of the illumination unit 2 is a light source 2.1, which is best realized by a light-emitting semiconductor diode and a downstream lens. Thus, the light beams 3 can be best collimated to each other. Two further possibilities, which offer a semiconductor-based light source, make the arrangement very well insensitive to ambient light influences. First, one can limit the selectivity of the position detector 4 to the wavelength of the light used and provide the light with much higher intensity than light of this wavelength occurs in ambient light. Second, you can apply the intensity of the light with a modulation frequency, so it can rise and fall periodically with high frequency and of the output signals of the position detector 4 by appropriate filtering only
    Page 7
    Allow signals for further processing, which also have this modulation frequency.
    Of course, it is advisable to cover the light source 2.1 including the downstream lens by a transparent to the emitted light disk 2.4 outwards to protect them from dirt and mechanical damage. In the preferred embodiment outlined, the light source and the transparent pane 2.4 are enclosed by a housing 2.2 which is open on one side to the light exit side, and air is pumped into the housing 2.3 through a line 2.3, which escapes from the housing 2.3 through the opening from the light exit side. This ensures that the transparent pane 2.4 less dirty or may not even dirty in dusty or foggy environments.
    Likewise, to prevent contamination, the detector unit 4 preferably has a housing 4.2, which has to the side at which light must be able to penetrate, has an opening through which air flows, including the air through a line 4.3 elsewhere in the housing 4.2 is brought into it. Likewise, the sensitive Kernstückt the detector unit 4, namely that of the planar optical position detector 4.1 to the housing opening through a transparent disc 4.4 to be protected from mechanical damage and contamination. So that light scattering caused by contamination of the disk 4.4 does not affect the measurement result too much, the disk 4.4 should be arranged as close as possible to the planar optical position detector 4.1, preferably even abut it.
    The planar optical position detector 4.1 is a planar optical waveguide which contains photoluminescent particles and which has on one side a plurality of distributed, small-area photoelectric sensors 4.1.1, which are able to extract light from the waveguide mode and
    Page 8 J 454 99 9 ··· * # 99 ♦ · «9 9» 9 9 • · 9 · 9 9 9 9 9 § * · 9 * 9 · # 9 9 · 99 ··· 99 99 · 99 99 99 9, so that an electrical signal is generated in dependence on the intensity of the light coupled out at the respective point.
    The principle of operation of such a planar optical position detector, which is known per se, should be briefly repeated. By means of the photoluminescent particles, for example dye molecules or semiconductor nanoparticles, light incident from the outside is converted into scattered light having a longer wavelength. This light is largely coupled into the waveguide and spreads out in it. For several reasons, the light intensity in the waveguide decreases with increasing distance from the point at which the luminescence has taken place, and thus also the electrical signal generated at the respective photoelectric sensors. By a plurality of photoelectric sensors are arranged at a distance from one another on the optical waveguide can be deduced from the ratio of the measured signal strengths at the individual photoelectric sensors with mathematical methods that can be automated by data on the impact position of the light beam triggering the luminescence, wherein the achievable spatial resolution is often finer than the distance between the adjacent photoelectric sensors. Photodiodes based on silicon, whose active cross-sectional area is, for example, 0.36 mm 2, are usually used as photoelectric sensors. Depending on the desired spatial resolution may be between adjacent photoelectric sensors 15 to 150 mm distance.
    Among other things, because despite high spatial resolution of the position detection in a measurement per monitored area only from a relatively small number of photoelectric sensors 4.1.1 an analog signal value must be read, the described planar optical position detector 4.1 can be read extremely quickly and it can be extremely many Position measurements per unit time are made, typically 100,000 measurements per second. This is like having an extreme slow-motion
    Page 9 an extremely high temporal resolution of the observation is possible.
    The signals generated by the photoelectric sensors of the planar optical position detector 4.1 are read into a data processing system (not shown) and evaluated. Under the assumption that the above-described shadow boundary divides the detection area into two surface areas illuminated differently by the illumination unit 2, wherein one area area is homogeneously illuminated on its own and the other area area is not illuminated at all Data processing system by a kind of interpolation from the measurement results of the individual photoelectric sensors are calculated quickly the course of the shadow boundary on the detection surface. Thus, relative to the detector unit 4 in the plane normal to the direction of the light rays 3, the position of the individual points of the wheel 1 at which the light-shadow boundary is located on the wheel is defined.
    By observing the dynamics of signal changes to the individual photoelectric sensors 4.1.1 valuable information can be obtained, or false information can be suppressed:
    As already mentioned above, the intensity of the light beams 3 emitted by the illumination unit 2 can fluctuate at a specific frequency and the photoelectric sensors 4.1.1 can be followed by a frequency filter whose passband is set to this frequency. This can be well suppressed by ambient light interference effects.
    For example, the minimum time interval between successive measurements may be 1 ps (corresponding to a measurement frequency of 1 MHz) and the frequency with which the light beams 3 can be switched on and off may be 100 kHz (period
    Page 10 J 454 10 ps, 5 ps on and 5 ps off). With the measuring principle according to the invention that can be realized easily. Thus, within a period of the fluctuation of the light output, 5 measured values can be recorded in each case, which then correspond to the light intensity at the point of a detector. By subtracting the values measured while the light source is turned on from those measured while the light source is off then gives a very reliable measure of the actual light intensity caused by the light source.
    If the speed of the wheel 1 is also measured by the data processing system, it can be checked whether shifts of a part of the observed shadow boundary or also of the entire observed shadow boundary repeat in time with the rotation of the wheel 1 or an integral multiple time thereof. This is then a clear indication of points on the wheel 1, which differ from the other rotational symmetry.
    The example "Wheel of a rail vehicle" is the first appearance of such a measurement result as well as the one-time sudden shift of the entire observing shadow limit an indication of a defective location on a railway track. In conjunction with a tachograph can be found quickly with the measurement method, this defective location.
    A permanent shift of the shadow boundary without its shape has changed is an indication of a permanent relative displacement of the measured body. This can be done on the example of the rail vehicle by changing the elasticity of the suspension, which may indicate a corresponding material fatigue.
    A permanent change in shape of the shadow border is an indication that something has been removed or applied evenly. Using the example of the wheel of the rail vehicle, slower uniform removal over the circumference of the wheel would be typical.
    Page 11 J 454 »* · · · * * * * t t t t t t t..... T t t · · · · · · · · ··· · * · * · · »
    Permanent changes in brightness that do not follow the movements of the shadow boundary are a strong indication of contamination of one of the protective transparent panes 2.4 or 4.4.
    In a simple, inexpensive and sufficiently good design for many applications, the entire surface of the planar optical position detector 4.1 may be a single, continuous optical waveguide, to which photoelectric sensors 4.1.1 are attached in some places, both at the surface edges and at it can be arranged remotely located Flächenberei- chen.
    Especially in the case of complicated geometries to be measured or in the case of the need for particularly precise and rapid evaluation of the detector signals, it is advantageous if the surface of the optical position detector 4.1 is subdivided into a plurality of partial areas insulated from one another with respect to optical waveguides, each partial area being equipped with a plurality of photoelectric sensors 4.1.1 is. Since light signals which impinge on a single partial surface can thus not influence the sensor signals from the other partial surfaces, the evaluation of the overall result is simplified and less error-prone.
    In a preferred embodiment of the invention, a stencil 5, which projects into the volume flooded by the light rays 3 and together with the object 1 to be measured, is attached to that part on which lighting unit 2 and detector unit 4 are immovably mounted delimits a slot through which light beams 3 reach the detector unit 4. Compared to a construction without such a template 5, the illuminated area of the optical position detector 4.1 is better limited. When changing the shape or position of the object 1 to be measured, the relative change of the light spot on the surface of the optical position
    Page 12 J 454 ••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••••• φ φ • · ··· · | ΦΦ Φ * φ detector 4.1 higher and thus more clearly detectable. The template 5 may be formed, for example, by a sheet metal part whose the object 1 to be monitored facing edge of the local contour of the article 1 is approximately formed. Preferably, as indicated in FIG. 1, the template 5 can be mounted in an adjustable position relative to the illumination unit 2 and the detector unit 4, so that the gap to the object to be monitored is as narrow as possible, but no collision occurs.
    The measuring principle according to the invention is particularly usefully applicable to those devices which comprise relatively moving parts, wherein from a part of a relatively periodically moving to another moving other part with respect to its relative position or its geometry is to be measured. It is particularly valuable for monitoring those periodically recurring moving parts, which are so worn by operational stresses that they need to be serviced or replaced several times during the usual life of the device.
    Page 13
    权利要求:
    Claims (9)
    [1]
    J 454 ····················································································································································································································· 9. Device for real-time measurement of relative position data and / or geometric dimensions of a moving body (1) using optical measuring means, wherein a lighting unit (2) and a detector unit (4) from which output data can be transmitted to a data processing system, are immovably fixed to each other at a distance from each other, wherein the moving body (1) relative to illumination unit (2) and detector unit (4) is guided guided and is hit by a part of the illumination unit (2) emitted light beams (3), characterized in that - the light beams (3) are sent from the illumination unit (2) towards the detector unit (4), - the moving body (1) between the illumination unit f (2) and the detector unit (4) into that of the Lichtstr (3) flooded volume protrudes, - the shadow boundary of the moving body (4) thrown thereby shadow on the detector unit (4), - the detector unit (4) comprises a planar optical position detector (4.1), which is designed as a planar optical waveguide which contains photoluminescent particles and which has on one side a plurality of spaced-apart, small-area photoelectric sensors (4.1.1), which are able to extract light from the waveguide mode in the optical waveguide and to generate an electrical signal whose strength the intensity of the decoupled light correlates. Page 14 J 454

    • · · · · ··· · · · * ♦
    [2]
    2. Apparatus according to claim 1, characterized in that the moving body (1) is offset relative to the lighting unit (2) and detector unit (4) in a periodically repeating course of movement.
    [3]
    3. Apparatus according to claim 2, characterized in that the moving body (1) relative to illumination unit (2) and detector unit (4) rotates.
    [4]
    4. The device according to claim 3, characterized in that the moving body (1) is a wheel of a rail vehicle and that Beieuchtungseinheit (2) and detector unit (4) are attached to the frame of the rail vehicle or on a bogie of the rail vehicle.
    [5]
    5. Device according to one of claims 1 to 4, characterized in that the dimensions of the planar optical position detector (4.1) in the direction of the light beams (3) normal plane are equal to or greater than the cross-sectional area of the light beams ( 3) flooded volume.
    [6]
    6. Device according to one of claims 1 to 5, characterized in that relative to the illumination unit (2) and detector unit (4) stationary template (5) in the light rays (3) flooded volume protrudes and together with the object to be measured (1 ) delimits a slot through which light beams 3 reach the detector unit 4.
    [7]
    7. A method for the real time measurement of relative position data and / or geometric dimensions of a moving body (1) using optical measuring means, wherein a lighting unit (2) and a detector unit (4), from which output data are transmitted to a data processing system, in one Distance to each other are fixed immovably to each other, wherein the moving body (1) is moved relative to side lighting unit (2) and detector unit (4) and is hit by a part of the light beam (3) emitted by the lighting unit {2} in which the detector unit (4) comprises a planar optical position detector (4.1) which is designed as a planar optical waveguide which contains photoluminescent particles and which has a plurality of small-area photoelectric sensors (4.1.1) arranged at intervals on one side, which light from the waveguide mode in the optical waveguide it decouples generate electrical signals whose strength correlates with the intensity of the coupled-out light, wherein light beams (3) are sent from the illumination unit (2) in the direction of the detector unit (4), wherein the moving body (1) between the illumination unit ( 2) and the detector unit (4) projects into the volume flooded by the light beams (3) and wherein the shadow boundary of the shadow cast by the moving body (4) passes over the detector unit (4), characterized in that - the body (1 ) carries out periodically recurring similar movements and the data processing system detects the repetition frequency of the movements, - is checked by the data processing system, whether fluctuations in signal strengths of the photoelectric detectors (4.1.1) electrical signals are repeated in the same or integer many times higher repetition frequency.
    [8]
    8. The method according to claim 7, characterized in that by the data processing system by interpolation from the measured values of the individual photoelectric sensors (4.1.1) the course of the shadow boundary with respect to illumination with light beams (3) on the planar optical position Detector Page 16 J 454 ·· ···· # ··· ···················· Is calculated for the calculation of the boundary condition that the shadow boundary the surface of the planar optical position detector (4.1) with respect to illumination with light beams (3) in two different divides heavily illuminated areas, with one surface area is illuminated homogeneously by itself and the other surface area is not illuminated.
    [9]
    9. The method according to claim 7 or claim 8, characterized in that it is used to measure on a rail vehicle during the ferry operation position and geometry of a rolling on a rail wheel (1). Page 17
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    KR20140079489A|2014-06-26|
    WO2013056289A1|2013-04-25|
    JP2014532185A|2014-12-04|
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    法律状态:
    2019-06-15| MM01| Lapse because of not paying annual fees|Effective date: 20181020 |
    优先权:
    申请号 | 申请日 | 专利标题
    ATA1534/2011A|AT511200B1|2011-10-20|2011-10-20|REAL TIME MEASUREMENT OF RELATIVE POSITION DATA AND / OR GEOMETRIC MASSES OF A MOVING BODY USING OPTICAL MEASURING AGENTS|ATA1534/2011A| AT511200B1|2011-10-20|2011-10-20|REAL TIME MEASUREMENT OF RELATIVE POSITION DATA AND / OR GEOMETRIC MASSES OF A MOVING BODY USING OPTICAL MEASURING AGENTS|
    EP12787628.2A| EP2769175A1|2011-10-20|2012-09-24|Real-time measurement of relative position data and/or of geometrical dimensions of a moving body using optical measuring means|
    CN201280051647.6A| CN103890538A|2011-10-20|2012-09-24|Real-time measurement of relative position data and/or of geometrical dimensions of a moving body using optical measuring means|
    US14/351,997| US20140240719A1|2011-10-20|2012-09-24|Real-time measurement of relative position data and/or of geometrical dimensions of a moving body using optical measuring means|
    PCT/AT2012/050142| WO2013056289A1|2011-10-20|2012-09-24|Real-time measurement of relative position data and/or of geometrical dimensions of a moving body using optical measuring means|
    KR1020147013208A| KR20140079489A|2011-10-20|2012-09-24|Real-time measurement of relative position data and/or of geometrical dimensions of a moving body using optical measuring means|
    JP2014536062A| JP2014532185A|2011-10-20|2012-09-24|Real time measurement of relative position data and / or geometric dimensions of moving objects using optical measuring means|
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