DE19859781A1 - Method for out-of-plane deformation or vibration analysis measurement using electronic speckle pattern interferometry based on use of microstructured refracting optical elements - Google Patents
Method for out-of-plane deformation or vibration analysis measurement using electronic speckle pattern interferometry based on use of microstructured refracting optical elementsInfo
- Publication number
- DE19859781A1 DE19859781A1 DE1998159781 DE19859781A DE19859781A1 DE 19859781 A1 DE19859781 A1 DE 19859781A1 DE 1998159781 DE1998159781 DE 1998159781 DE 19859781 A DE19859781 A DE 19859781A DE 19859781 A1 DE19859781 A1 DE 19859781A1
- Authority
- DE
- Germany
- Prior art keywords
- espi
- deformations
- vibrations
- plane
- measurement
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
- 238000000034 method Methods 0.000 title claims abstract description 34
- 230000003287 optical effect Effects 0.000 title claims abstract description 34
- 238000005259 measurement Methods 0.000 title claims description 25
- 238000005305 interferometry Methods 0.000 title claims description 6
- 238000004458 analytical method Methods 0.000 title description 3
- 238000012360 testing method Methods 0.000 claims description 9
- 230000000737 periodic effect Effects 0.000 claims description 6
- 238000011156 evaluation Methods 0.000 claims description 4
- 238000012545 processing Methods 0.000 claims description 2
- 229910052729 chemical element Inorganic materials 0.000 claims 1
- 230000005855 radiation Effects 0.000 description 5
- 230000001427 coherent effect Effects 0.000 description 2
- 241000589902 Leptospira Species 0.000 description 1
- 239000000835 fiber Substances 0.000 description 1
- 238000001093 holography Methods 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000004377 microelectronic Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
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
- G01B11/16—Measuring arrangements characterised by the use of optical techniques for measuring the deformation in a solid, e.g. optical strain gauge
- G01B11/161—Measuring arrangements characterised by the use of optical techniques for measuring the deformation in a solid, e.g. optical strain gauge by interferometric means
- G01B11/162—Measuring arrangements characterised by the use of optical techniques for measuring the deformation in a solid, e.g. optical strain gauge by interferometric means by speckle- or shearing interferometry
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B9/00—Measuring instruments characterised by the use of optical techniques
- G01B9/02—Interferometers
- G01B9/021—Interferometers using holographic techniques
- G01B9/023—Interferometers using holographic techniques for contour producing
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Length Measuring Devices By Optical Means (AREA)
Abstract
Description
Vorgestellt wird ein Verfahren zur Verformungs- oder Schwingungsmessung mittels elektroni scher Speckle-Pattern-Interferometrie (ESPI), das auf Verformungen oder Schwingungen or thogonal zur Ebene des Prüflings anspricht ("Out-of-Plane"-Verformungen bzw. -Schwin gungen). Hierzu wird der Prüfling mit der kohärenten Strahlung eines Lasers beleuchtet. Gleichzeitig wird eine Referenzoberfläche mit kohärenter Strahlung derselben Laserquelle be leuchtet. Die das Objekt und die Referenzoberfläche beleuchtenden Wellen werden an diesen diffus oder gerichtet reflektiert und bilden ESPI-Objekt- und Referenzwelle, welche von einem Kameraobjektiv aufgenommen werden. Zumindest eine ESPI-Welle (Abb. 1) oder beide ESPI- Wellen (Abb. 2) verlaufen schräg zur optischen Achse des Kameraobjektives. Ein speziell mi krostrukturiertes brechendes optisches Element, das als Strahlvereiniger wirkt, wird in den Strahlengang gebracht, um beide Wellen auf die optische Achse des Objektivs und zum Kame rasensor zu führen (Abb. 1 und Abb. 2). Beide ESPI-Wellen können eine glatte oder eine diffu se Wellenfront haben; beide Wellen können durch Teilung der Wellenfront oder der Amplitude der Laserstrahlung generiert werden; sie können von einem Spiegel oder einer diffus reflektie renden Oberfläche hervorgebracht werden.A method for deformation or vibration measurement using electronic speckle pattern interferometry (ESPI) is presented, which responds to deformations or vibrations orthogonal to the level of the test object ("out-of-plane" deformations or vibrations). For this purpose, the test object is illuminated with the coherent radiation from a laser. At the same time, a reference surface is illuminated with coherent radiation from the same laser source. The waves illuminating the object and the reference surface are reflected diffusely or directionally on them and form ESPI object and reference waves, which are recorded by a camera lens. At least one ESPI wave ( Fig. 1) or both ESPI waves ( Fig. 2) run at an angle to the optical axis of the camera lens. A specially micro-structured refractive optical element, which acts as a beam combiner, is brought into the beam path to guide both waves onto the optical axis of the lens and to the camera sensor ( Fig. 1 and Fig. 2). Both ESPI waves can have a smooth or a diffuse wavefront; both waves can be generated by dividing the wavefront or the amplitude of the laser radiation; they can be produced by a mirror or a diffusely reflecting surface.
Zumindest ein Teil der ESPI-Objektwelle oder ein Teil der ESPI-Referenzwelle breitet sich schräg zur optischen Achse der Kamera aus und bleibt ohne mikrostrukturiertes brechendes Element außerhalb des Blickfeldes des Kameraobjektives. Wenn das mikrostrukturierte Ele ment jedoch vor das Kameraobjektiv plaziert wird, so führt es beide Wellen auf die optische Achse des Kameraobjektives, welches die Abbildung auf den Kamerasensor durchführt.At least part of the ESPI object wave or part of the ESPI reference wave is spreading obliquely to the optical axis of the camera and remains without microstructured refractive Element outside the field of view of the camera lens. If the micro-structured Ele However, if it is placed in front of the camera lens, it leads both waves to the optical one Axis of the camera lens, which performs the imaging on the camera sensor.
Das von Objekt- und Referenzwelle gebildete Speckle-Interferenzmuster wird von einem Ka merasensor aufgenommen, der die Specklemuster vor und nach einer Verformung des Objekts festhält. Durch Auswertung dieser Specklemuster mittels Bildverarbeitung ist es möglich, die Out-of-Plane-Verformung oder -Schwingung des Prüflings zu berechnen. Hierfür wird der Prüfling im unverformten und im verformten Zustand (entsprechend zwei verschiedenen Zu ständen der Verformung bzw. Schwingung) mit mehreren Specklemustern verschiedener rela tiver Phasenlage der beiden interferierenden Wellen (Objekt- und Referenzwelle) aufgenommen und ausgewertet (Phasenschrittmethode). Eine andere Möglichkeit zur Auswertung ist die Be rechnung und Darstellung des Speckle-Korrelationsbildes zweier Specklemuster, die dem un verforrrtten und dem verformten Zustand des Objektes entsprechen. Ein solches Speckle- Korrelationsbild kann auch mittels einer photographischen Kamera hergestellt werden. Die geläufigen Verfahren von Out-of-Plane-ESPI unterscheiden sich hauptsächlich in der Art der Referenzwelle (ebene oder gestreute Welle), wie diese erzeugt wird (Wellenfront- oder Amplitudenteilung) und wie sie zum Kamerasensor geführt wird (durch die Kameralinse oder dahinter). Aufgrund des begrenzten Auflösungsvermögens der üblichen Kamerasensoren (hauptsächlich CCD-Sensoren) muß der Winkel zwischen der Objekt- und der Referenzwelle auf der Sensoroberfläche ausreichend klein sein, um ein auflösbares Interferenzmuster zu er zeugen. Abb. 3 zeigt ein Beispiel für eine ESPI-Anordnung zur Verformungs- und Schwin gungsanalyse entsprechend dem Stand der Technik, bei der eine diffuse Referenzwelle durch Wellenfrontteilung und mittels eines holographisch-optischen Elements erzeugt wird und durch das Objektiv auf den Sensor trifft [1, 2].The speckle interference pattern formed by the object and reference wave is recorded by a camera sensor, which records the speckle pattern before and after the object is deformed. By evaluating these speckle patterns using image processing, it is possible to calculate the out-of-plane deformation or vibration of the test specimen. For this purpose, the test specimen is recorded and evaluated in the undeformed and in the deformed state (corresponding to two different states of the deformation or vibration) with several speckle patterns of different relative phase positions of the two interfering waves (object and reference wave) (phase step method). Another possibility for evaluation is the calculation and representation of the speckle correlation image of two speckle patterns, which correspond to the undrawn and the deformed state of the object. Such a speckle correlation image can also be produced using a photographic camera. The common methods of out-of-plane ESPI differ mainly in the type of reference wave (plane or scattered wave), how it is generated (wavefront or amplitude division) and how it is guided to the camera sensor (through the camera lens or behind it) . Due to the limited resolution of the usual camera sensors (mainly CCD sensors), the angle between the object and the reference wave on the sensor surface must be small enough to produce a resolvable interference pattern. Fig. 3 shows an example of an ESPI arrangement for deformation and vibration analysis according to the prior art, in which a diffuse reference wave is generated by wavefront division and by means of a holographic-optical element and hits the sensor through the lens [1, 2].
Bei dem vorgestellten Verfahren kann das mikrostrukturierte brechende optische Element ent weder eine periodische oder eine nichtperiodische Struktur besitzen. In beiden Fällen muß das brechende optische Element mindestens zwei Gruppen von Mikrostrukturen aufweisen, um die ESPI-Objektwelle und die ESPI-Referenzwelle exakt auf der optischen Achse in das Kamera objektiv zu leiten. Das mikrostrukturierte brechende optische Element kann beispielsweise aus zwei Gruppen von periodisch angeordneten linearen Strukturen bestehen, von denen je eine mit der ESPI-Objektwelle oder mit der ESPI-Referenzwelle arbeitet, abhängig vom Einfallswinkel und von Periode, Profil und Brechungsindex des Materials des mikrostrukturierten Elements. In Abb. 1 und 2 sind mikrorefraktive Bereiche dargestellt, die als Strahlvereiniger dienen. Zum Beispiel können solche Bereiche aus zwei Gruppen von Mikroprismen bestehen.In the method presented, the microstructured refractive optical element can have either a periodic or a non-periodic structure. In both cases, the refractive optical element must have at least two groups of microstructures in order to objectively guide the ESPI object wave and the ESPI reference wave into the camera on the optical axis. The microstructured refractive optical element can, for example, consist of two groups of periodically arranged linear structures, one of which works with the ESPI object wave or with the ESPI reference wave, depending on the angle of incidence and on the period, profile and refractive index of the material of the microstructured element. Fig. 1 and 2 show microrefractive areas that serve as beam converters. For example, such areas can consist of two groups of microprisms.
Das vorgestellte Verfahren erlaubt es, ESPI-Anordnungen zu aufzubauen, die sehr kompakt sind (besonders wenn Halbleiterlaser oder diodengepumpte Nd : YAG-Laser verwendet wer den), einfach zu bedienen sind und praktisch keine Justierung benötigen. Solche neuartige An ordnungen können an Kompaktheit nur mit den in [1, 2] beschriebenen oder mit faseroptischen verglichen werden. Letztere benötigen ziemlich komplizierte und zeitaufwendige Prozeduren zur Justierung und sind nicht einfach zu bedienen.The method presented allows ESPI arrangements to be built which are very compact (especially when using semiconductor lasers or diode pumped Nd: YAG lasers den), are easy to use and require practically no adjustment. Such novel types Orders can only be compact with the ones described in [1, 2] or with fiber optics be compared. The latter require fairly complicated and time-consuming procedures for adjustment and are not easy to use.
Infolge des sehr einfachen optischen Aufbaus der vorgestellten ESPI-Anordnungen wird die Laserstrahlung sehr gut ausgenutzt. Daher ist es möglich, in einer hell beleuchteten Umgebung bei Beleuchtungsstärken zu arbeiten, wie sie für industrielle Arbeitsplätze empfohlen werden (einige hundert lux), oder sogar bei deutlich höheren Werten. Dazu kann in der Kamera ein geeigneter Interferenzfilter verwendet werden, der der Laserwellenlänge angepaßt ist, um den inkohärenten Strahlungsanteil auf dem Kamerasensor zu begrenzen.Due to the very simple optical structure of the ESPI arrangements presented, the Laser radiation used very well. Therefore, it is possible in a brightly lit environment work at illuminance levels that are recommended for industrial workplaces (a few hundred lux), or even at significantly higher values. You can do this in the camera suitable interference filter can be used, which is adapted to the laser wavelength by the limit incoherent radiation component on the camera sensor.
Die Einführung von mikrostrukturierten brechenden optischen Elementen, die als Strahlverei niger dienen, ermöglicht die Auswertung der Differenz von Verformungs- und Schwingungs mustern eines Musterobjekts und eines gleichartigen Prüflings. Dieses innovative ESPI- Verfahren kann beispielsweise als Schnelltest von Produkten und Komponenten in Produkti onslinien der Mikroelektronik-Industrie angewandt werden.The introduction of microstructured refractive optical elements that act as a beam serve niger, enables the evaluation of the difference between deformation and vibration sample a sample object and a similar test object. This innovative ESPI The method can be used, for example, as a quick test of products and components in product lines of the microelectronics industry.
1. V. Petrov, B. Lau, Electronic speckle pattern interferometry with a holographically genera
ted reference wave. Optical Engineering 35, pp. 2363-2370, (1996).
2. B. Lau, P. Kuschnir, U. Schmid, V. Petrov, Application of combined method of electronic
speckle pattern interferometry and holography to vibration analysis. 2nd Intern. Conf. on Vi
bration Measurements by Laser Techniques, Ancona, 23-25 September 1996, Proc. SPIE
2868, pp. 346-351, (1996).1. V. Petrov, B. Lau, Electronic speckle pattern interferometry with a holographically generated reference wave. Optical Engineering 35, pp. 2363-2370, (1996).
2. B. Lau, P. Kuschnir, U. Schmid, V. Petrov, Application of combined method of electronic speckle pattern interferometry and holography to vibration analysis. 2nd intern. Conf. on Vi bration Measurements by Laser Techniques, Ancona, 23-25 September 1996, Proc. SPIE 2868, pp. 346-351, (1996).
Claims (22)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE1998159781 DE19859781A1 (en) | 1998-12-23 | 1998-12-23 | Method for out-of-plane deformation or vibration analysis measurement using electronic speckle pattern interferometry based on use of microstructured refracting optical elements |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE1998159781 DE19859781A1 (en) | 1998-12-23 | 1998-12-23 | Method for out-of-plane deformation or vibration analysis measurement using electronic speckle pattern interferometry based on use of microstructured refracting optical elements |
Publications (1)
| Publication Number | Publication Date |
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| DE19859781A1 true DE19859781A1 (en) | 2000-06-29 |
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Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| DE1998159781 Withdrawn DE19859781A1 (en) | 1998-12-23 | 1998-12-23 | Method for out-of-plane deformation or vibration analysis measurement using electronic speckle pattern interferometry based on use of microstructured refracting optical elements |
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| DE (1) | DE19859781A1 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE10341714A1 (en) * | 2003-09-10 | 2005-05-25 | Nova Wave Light 01 Gmbh | Interferometer sensor e.g. for quality control of prefabricated parts, sensor and electronics are integrated in sensor housing with optics having special arrangement of polarization-optical components and four image sensors |
| EP2259009A1 (en) * | 2009-06-04 | 2010-12-08 | Gasera Ltd | Arrangement and method for measuring relative movement |
-
1998
- 1998-12-23 DE DE1998159781 patent/DE19859781A1/en not_active Withdrawn
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE10341714A1 (en) * | 2003-09-10 | 2005-05-25 | Nova Wave Light 01 Gmbh | Interferometer sensor e.g. for quality control of prefabricated parts, sensor and electronics are integrated in sensor housing with optics having special arrangement of polarization-optical components and four image sensors |
| EP2259009A1 (en) * | 2009-06-04 | 2010-12-08 | Gasera Ltd | Arrangement and method for measuring relative movement |
| CN101907713A (en) * | 2009-06-04 | 2010-12-08 | 伽泽拉有限公司 | Be used to measure the equipment and the method for relative motion |
| US8497996B2 (en) | 2009-06-04 | 2013-07-30 | Gasera Ltd | Arrangement and method for measuring relative movement |
| CN101907713B (en) * | 2009-06-04 | 2014-09-10 | 伽泽拉有限公司 | Arrangement and method for measuring relative movement |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| 8127 | New person/name/address of the applicant |
Owner name: LAU, BERNHARD, PROF. DR., 89275 ELCHINGEN, DE |
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| 8139 | Disposal/non-payment of the annual fee |