• 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 present invention is directed to a holographic interferometer for measuring the deformation of an object or mechanical structure by exposing one or more hologram plates to a light source and a reference beam. In particular, the invention is directed to a method and apparatus for moving the hologram plate during and between exposures to thereby obtain exposures on different portions of the hologram plate. Each of these different exposures is taken in a short time interval in response to light reflected by the object from the light source as well as light from the reference beam. The image on the hologram plates is then reconstructed in a manner generally known in the art to determine the deformation of the object or mechanical structure. In order to obtain these exposures on different portions of the hologram plates, a screen having one or more apertures is positioned in front of the hologram plates to restrict the size of the short time interval exposures on the hologram plates. The hologram plates are continuously rotated prior to and during the exposures about an axis of rotation which is located perpendicularly to the surface of the hologram plates and is positioned so that some portion of the hologram plates is always located behind the aperture in the screen. In order to obtain a suitable direction of the interference lines, the reference beam, the aperture in the screen, the object and the axis of rotation of the hologram plates are positioned in the same plane. In the preferred embodiment, two different hologram plates are rotated together behind the screen. During reconstruction, these different hologram plates are positioned adjacent one another so that the surfaces of the forward hologram plate exposed by the first exposure pulse cover the surfaces of the rearward hologram plate exposed by the second exposure pulse, or vice versa. As a result, the interference lines in the hologram image correspond to the object or mechanical structure which is being measured for deformation.
    公开号:SU818503A3
    申请号:SU782575949
    申请日:1978-02-02
    公开日:1981-03-30
    发明作者:Абрамсон Нильс
    申请人:Abramson Nils；
    IPC主号:
    专利说明:

    The invention relates to holographic interferometry and can be used to measure the deformation of mechanical structures in a holographic non-destructive testing method.
    Known methods of holographic interferometry, which consist in registering a hologram before and after the formation of deformations by double exposure. An important condition in this case is the stability of the holographic installation. When the hologram is restored, a three-beam image is formed ._ Covered with interference fringes, which are used to judge the changes that have occurred with the object [1].
    Closest to the proposed one is a method of holographic interferometry, which consists in recording the holograms corresponding to different states of the object on different recording plates and restoring the holographic inter-25 Ferogram.
    The advantage of this method is that even after disassembling the experimental equipment, various combinations of loads can be studied by combining different holograms. The effect of the general movement of an object can eliminate-. and, thus, it is possible to study small deformations, despite the presence of significant displacements of the entire object, to obtain maximum information, you can change the interference pattern, and you can also simulate various deformations (forward and backward) [2]. However, ordinary holography is highly sensitive to displacements and vibration. One solution to this problem is to reduce the exposure time to the extent that the displacement during exposure does not exceed the permissible (no more than 0.25). For this purpose, pulsed ruby lasers with a pulse duration of 20 ns and an interval between pulses of the order of 1 ms are used, which makes it possible to reproduce even high-speed objects. However, when measuring deformation by means of double pulses, the result of the movement of the object during the time between two pulses to the interference pattern from the deformation of the object is additional. interference fringes arising from the displacement of the object. This can lead to the impossibility of performing measurements, since interference fringes from the movement of the object under study can completely hide information about the deformation of the object. Therefore, it is desirable that the holographic information from exposure to a double pulse be fixed on two different holographic plates. The implementation of the known method requires compliance with the strict installation stability conditions. And strict compliance with the restoration of the original recording conditions.
    The purpose of the invention is to increase the sensitivity of the method and the ability to determine the direction of movement of the object.
    This goal is achieved in that in the method of holographic interferometry, which consists in recording holograms corresponding to different states of the object on different recording plates and restoring the holographic interferogram, recording plates are moved between exposures at a speed t
    y ------- t-8s <n os where i t _ about -
    In order not to have a special starting impulse to start the movement of the plates and to avoid the action of large acceleration forces on the hologram plates, the plates are constantly rotating before, during, and after exposure. In this case, the rotation axis of the hologram plates is perpendicular to the surface of the plate and so that part of the plate is always located behind the slot on the screen (a screen with a slot is set to limit the exposed areas on the recording plate). Example.
    Exposure time, t, ns Interval between pulses, T, ms Minimum distance between interference fringes on the recording plate, d, Maximum angle between laser beams illuminating the recording plate, 2 rev, deg Distance between exposed areas on the plate Maximum permissible movement of the plate during exposure Maximum permissible speed of movement of the plate, λ 2sir »oC radiation wavelength; exposure time, .poluugol between the object and the reference beams, so that the hologram recording was performed on different parts of the recording plate, and when reconstructing the image recording plate are displaced relative to each other so that the recording from the first platen coincides with za- 1 pisyo from the second exposure and the obtained bands judge the movement and deformation of the investigated object.
    The method is as follows.
    By changing the displacement of the plates, the interference lines arising from the movement of the object are eliminated so that only strips from the deformation of the object remain. By measuring the magnitude and direction of displacement of the holograms, the magnitude of the th direction is calculated. tensions and deformation of the object. Using specially gradient of the calculated displacement of the object makes the corresponding slope of the interference fringes, which may schityvat- 1 Xia with sufficient accuracy, 'instead of the derivative of the density bands. Thus, for example, the stresses arising from the bending of an object are calculated, and a region subject to maximum load is easily found. In addition, additional combinations of the hologram recordings are performed by additional displacement of the plates when the laser generates more than two pulses.
    0.6328 -10 ' 6 h , 1 -_____ V ~ t-8s <not'24 · 1Ο- 9 8..Ο, 3Θ3' M '8.6 / s
    The distance from the exposed area on the plate to the axis of rotation, R, 4
    Rotation speed,, 2054
    P = r o .---- 106.// LIN t-8s <noc-24 · R i · 60
    In this case, therefore, the maximum possible number of revolutions is reached of the order of 2000 rpm./min, while the gap between the exposed areas is
    V .. t
    8.6 · 0/5 · 10 ' 3
    When the gap between the exposed areas on the recording plate is 2.23 mm, the slot in the screen should also be of appropriate width, and the two exposed areas can occupy the maximum area of the plate without interrupting each other.
    When it is desirable to have a large exposed area, first of all, the influence of the angle 2 06 can be reduced by such a direction of the reference beam relative to the object beam at which the resulting interference fringes are located substantially parallel to the direction of movement of the plate, i.e., perpendicular to the radius. This is achieved if 0 the reference beam, the slot, the object and the axis of rotation of the plate lie in the same t plane. When the reference 3 beams are in this plane, in addition, while maintaining the angle between the reference and the object beams small, the angle giving the appearance of bands perpendicular to the direction of rotation of the plate, '* is determined only by the angle of sight of the object. The practically minimum value of this angle can be sin 2 <x, = = 0.1 (i.e., the object has dimensions 0.1x x 0.1 m at a distance of about 1 m). At 15 sin 2ot = 0.1, instead of 2 ot »45®, a maximum rotation speed of 7523 rpm and a minimum width (0) of 15.77 mm are achieved.
    When such a gap width is 20 • sufficient or. when it is desirable to have a shorter interval (T) between pulses, for example, at a high speed of rotation of the object, the slot in the screen can be replaced by several slots, each having a width D and the distance between them is 0. The slots should be of a significant degree parallel to each other to a friend and, as far as possible, perpendicular to the movement of the recording plate ..;
    The invention improves the sensitivity of the method and makes it possible to determine the direction of movement of the object. The advantage yav- 35 also wish to set up the possibility of measuring movement of the object of several tens of times larger than in the known methods. The invention allows holographic reproduction of high-speed objects.
    权利要求:
    Claims (2)
    [1]
    The invention relates to holographic interLerometry and can be used to measure the deformation of mechanical structures in the holographic non-invasive confer method. Methods are known for holographic and interlerometry, which consist in recording a hologram before and after deformation by the method of double exposure. An important condition for this is the stability of the holographic installation. When a hologram is restored, a three-beam image is formed, covered with interference fringes, which are used to judge the changes that have occurred with the object. The closest to the present is the method of holographic interferometry, which consists in recording holograms corresponding to different states of the object for different recordings. plates and restoration of a holographic interogram. The advantage of this method is that even after disassembling the experimental equipment, various combinations of loads can be studied by combining different holograms. The effect of the general movement of an object can eliminate -, c, and thus it is possible to study small deformations, despite the presence of significant displacements of the entire object, to obtain maximum information, the interference pattern can be changed, and various deformations (forward and backward) can be simulated (2J However, conventional holography is highly sensitive to displacement and vibration. One solution to this problem is to reduce the exposure time to the extent that the displacement during exposure time does not exceed the allowable (not more than its value is 0.25). For this purpose, pulsed ruby lasers with a pulse duration of 20 n are used, and the interval between pulses is of the order of 1 ms, which makes it possible to reproduce even fast-acting objects. However, when measuring the deformation by means of double pulses, the movement of an object between two The impulses to the interference pattern from the deformation of the object are additional interference fringes arising from the displacement of the object. This can lead to the impossibility of performing measurements, since the interference bands from the movement of the object under study can completely hide the information about the deformation of the object. Therefore, it is desirable that the holographic information from exposure to a double pulse is recorded on two different holographic plates. The implementation of a known method requires strict compliance with the conditions of stable installation. And strict compliance with the restoration of the original recording conditions. The purpose of the invention is to increase the sensitivity of the method and the possibility of determining the direction of movement of an object. . The goal is achieved by the fact that in the method of holographic interferometry that holograms corresponding to different states of the object are recorded onto different recording plates and the holographic interferogram is restored, the recording plates are moved between exposures with a speed of V t-Ssin L Where 7. radiation wavelength; t is the exposure time, about the half-angle between the object and reference beams, so that the holograms are recorded at different sites of the recording plates, and when the image is restored, the recording plates are shifted relative to each other so that the recording from the first exposure coincides with And from the second exposure, and on the resulting lanes, the movement and deformation of the object under study is judged. The method is recommended as follows. By changing the displacement of the plates, the interference lines arising due to the movement of the object are eliminated so that only the bands from the deformation of the object remain. Measuring the magnitude and direction of displacement of the holograms, calculate the magnitude and direction of displacement and deformation of the object. By means of a specially calculated displacement, the gradient of the movement of the object is made corresponding to the slope of the interference fringes, which can be obtained with sufficient accuracy, and not derived from the density of the fringes. TiaKHM, for example, calculates the stresses arising from the bending of an object, and easily find the area subject to maximum load. In addition, other combinations of hologram recording are performed by additional displacement of the plates; the laser generates more than two pulses. . In order not to have a special starting impulse to start the movement of the plates and to avoid the effect of large acceleration forces on the hologram plates, the plates are continuously scaled before, during, and after exposure. At the same time, the axis of rotation of the hologram plates is perpendicular to the surface of the plate and so that a part of the plate is always located behind the E slot of the screen (a slotted screen is installed to limit the exposed areas on the recording plate). Example. Exposure time, t, not 24 Interval between pulses, T, KC0, Minimum distance between interference fringes on the recording plate, d, Maximum angle between laser beams illuminating the recording plate, 2 wasps, grad 45 Distance between the exposed areas on the plate Maximum permissible plate movement during exposure The maximum permissible speed of plate movement. 0.6328-10 V t-85in ", ° 24 - (.- 0.383 Distance from the exposed area on the plate to the axis of rotation, R, 4 Speed of rotation. 10b. // LIN t-8s not-24-R In this In this case, therefore, the maximum possible number of revolutions is reached on the order of 2000 rpm, while the gap between the exposed areas is equal to V .. T 8.6 0/5 10 9.3 mm. When the gap between the exposed areas on the recording plate is 2 , 23 mm, the slot in the screen should also be of appropriate width, and the two exposed areas can occupy the maximum area of the plate, not the interruption of others When it is desirable to have a large exposed area, first of all, the influence of the angle 2 06 can be reduced by directing the reference beam relative to the object, in which the resulting interference bands are located substantially parallel to the direction of movement of the plate, i.e. perpendicular This is achieved when the reference beam, the slot, the object and the axis of rotation of the plate lie on the plane. When the reference beam is located in this plane and, moreover, while keeping the angle between the reference and the subject beams small, the angle that gives rise to bands perpendicular to the direction of rotation of the plate is determined only by the angle of sight of the object. Practically the minimum value of this angle can be stn2oc 0.1 (i.e., the object has rjoura 0, X 0.1 m at a distance of about 1 m). Tg si.t) 2ai 0.1, instead of 2 OL 45, maximum speed of rotation, is 7523 rpm, and the minimum width (0), equal to .15.77 mm, is reached. When such a situation is sufficient or when there are more than a SHORT interval (T) with pulses, for example, an object at a HIGH speed of rotation, the slot in the screen can be replaced with OiiTb, each with a wide &amp; is equal to &amp;; dorozno dolokna (in the pumping station, pen pyra p &amp; no. "but to each other in how much the sao are perpendicular to the movement of the reversal plate;) at the side of the plate ..; ,; ..; ;. :. ,.;:., The invention allows the sensitivity of the method to be poked and gives the opportunity to feel the movement of the object. Prefixing with 4 in the eFs is also possible and the first &lt; &amp; &amp; &amp; &n; &n; &p; (about ten dozen times more than in his weight; t} s, ways. The invention allows for a graphical reproducing the most active objects. Claims of holographic interlerometry, which consist in recording holograms corresponding to different states of an object on different recording plates and restoring a holographic interloragram, characterized in that, in order to increase the sensitivity of the method and the possibility of determining of the object's movement, the recording of the plate is moved between exposures with the speed V .. (. where I is the radiation wavelength; t is the exposure time; 0 is the half-angle between the Object and reference beams, TaicBM, so that holograms are recorded in different parts of the reshstr 1 and 1X plates, and when the 9EO-ENERGENCES are restored, the recording plates should be relatively different from each other so that the record from the first exposure coincided with the recording from the second exposure and, according to the hard lines, we check wow object. Sources of information taken into account in the examination 1. R. Hopier n / C. Optical headband. M., Mir, 1973, p. 473-49.
    [2]
    2. Abramson Nils Sandwich Hologram Jnterferoraetry: a New Dimension In Holographtc Comparison. - Appiied Optics, 1974, vol. 13.9, p.2012025 (prototype).
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    同族专利:
    公开号 | 公开日
    CA1095296A|1981-02-10|
    FR2379845A1|1978-09-01|
    JPS5397454A|1978-08-25|
    SE408735B|1979-07-02|
    GB1583415A|1981-01-28|
    DE2804289A1|1978-08-10|
    SE7701188L|1978-08-04|
    US4205917A|1980-06-03|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US3627916A|1966-09-21|1971-12-14|Fritz Bestenreiner|Apparatus for recording and reproducing holograms of moving subjects|
    US3606517A|1969-02-14|1971-09-20|Hughes Aircraft Co|Holographic motion picture system|
    US3802758A|1973-05-21|1974-04-09|Us Air Force|Dual hologram plate holder|FR2385079B1|1977-03-23|1981-12-11|Thomson Csf|
    SE460874B|1986-05-20|1989-11-27|Ingegerd Dirtoft|PROCEDURE METHOD FOR CONTROL OF ANY CONDUCTIVE, UNEXPECTED FORM CHANGES IN A MANUFACTURED PRODUCT|
    US4704666A|1986-08-15|1987-11-03|Davis Charles S|Artificial light source utilizing a holographic optical element to control radiant light|
    SE459456B|1988-05-02|1989-07-03|Ingegerd Dirtoft|FIXTURE INTENDED FOR EXTREMELY SHAKE-FREE LAYOUT|
    US8170322B2|2006-03-22|2012-05-01|Jadak Llc|Optical imaging system and method using a reflective background|
    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    SE7701188A|SE408735B|1977-02-03|1977-02-03|PROCEDURE FOR USING INTERFEROMETRIC INFORMATION FROM TWO DIFFERENT HOLOGRAMS EXPOSED IN SHORT TIME SPACES|
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