Key information

Title: System and method for analysing an object
Application number: 20200190
Case type: National
Status: 11.07.2022 P.g.a. manglende svar. Søker har ikke begjært gjenopptakelse
Filed: 14.02.2020
Effective date: 14.02.2020
Publicly available: 16.08.2021
Applicant: Optonor AS (NO)
Inventor: Eiolf Vikhagen (NO)
Agent: DEHNS NORDIC AS (NO)

Abstract and drawing

Disclaimer: This text has been machine-scanned and may contain errors – please refer to "Publications" for legally binding content.

The invention relates to a system and method of analysing an object. The method comprises exciting the object at a vibration frequency so as to induce at least one wave, having the vibration frequency, on an excitation surface of the object; propagate the at least one wave into an analysis surface of the object; measuring vibration on a measurement surface of the object, the measurement surface being spatially separated from the excitation surface of the object by the analysis surface of the object; processing the vibration data to determine a change in at least one wave property of the at least one wave; and determining, based on the change in the at least one wave property of the at least one wave, at least one defect existing in the analysis surface of the object.

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Date	Doc. No.	Process	Case number	In/Out	Journal description	To/from
01.12.2022	11-01	Saksbehandling	20200190	UT	Finally shelved	DEHNS NORDIC AS
16.08.2022	10-01	Saksbehandling	20200190	UT	Henlagt manglede svar ENG	DEHNS NORDIC AS
11.03.2022	09-02	Saksbehandling	20200190	UT	PT report 02:22:26
11.03.2022	09-01	Saksbehandling	20200190	UT	Substantive examination	DEHNS NORDIC AS
03.01.2022	08-01	Saksbehandling	20200190	UT	PT Varsel om betaling av første årsavgift (3317) (PT20200190)
25.11.2021	02-01	Endring av fullmektig	2021/17179	UT	GH Forespørsel	DEHNS NORDIC AS
24.11.2021	01-02	Endring av fullmektig	2021/17179	INN	157569 2021-11-19 - Executed General Power of Attorney (NO)	DEHNS NORDIC AS
24.11.2021	01-01	Endring av fullmektig	2021/17179	INN	Generell henvendelse	DEHNS NORDIC AS
18.02.2021	07-02	Saksbehandling	20200190	INN	P26650NO00 Reply to Office Action	ONSAGERS AS
18.02.2021	07-01	Saksbehandling	20200190	INN	Korrespondanse (Hovedbrev inn)	ONSAGERS AS
11.02.2021	06-02	Saksbehandling	20200190	INN	Copies request Feb 11, 2021 P26650NO00	ONSAGERS AS
11.02.2021	06-01	Saksbehandling	20200190	INN	Korrespondanse (Hovedbrev inn)	ONSAGERS AS
28.08.2020	05-02	Saksbehandling	20200190	UT	PT report 04:32:37
28.08.2020	05-01	Saksbehandling	20200190	UT	Realitet patent	ONSAGERS AS
04.03.2020	04-03	Saksbehandling	20200190	INN	Fullmakt og erklæring	ONSAGERS AS
04.03.2020	04-02	Saksbehandling	20200190	INN	Hovedbrev	ONSAGERS AS
04.03.2020	04-01	Saksbehandling	20200190	INN	Korrespondanse (Hovedbrev inn)	ONSAGERS AS
18.02.2020	03-01	Saksbehandling	20200190	UT	Formal Examination 1	ONSAGERS AS
18.02.2020	02-01	Saksbehandling	20200190	UT	Infobrev til oppfinner	ONSAGERS AS
14.02.2020	01-03	Saksbehandling	20200190	INN	Patenttegninger	ONSAGERS AS
14.02.2020	01-02	Saksbehandling	20200190	INN	Beskrivelse	ONSAGERS AS
14.02.2020	01-01	Saksbehandling	20200190	INN	Søknadsskjema Patent	ONSAGERS AS

Description, claims and drawings

Disclaimer: This text has been machine-scanned and may contain errors – please refer to "Publications" for legally binding content.

Description

System and method for analysing an object

Background

This invention relates to methods and systems for analysing an object using vibrations to determine a defect existing in a surface between an excitation surface of the object and a measurement surface of the object.

It is known to use laser light to analyse objects, such as for the non-destructive testing of machine parts—for example, electronic speckle pattern interferometry (ESPI), electronic shearography, and laser Doppler vibrometry (LDV).

The applicant's earlier patent applications WO 2006/001712 and WO 2014/088424 describe various techniques for using optical interferometry to analyse objects that are subjected to a static deflection or that are caused to vibrate. WO2019/229473 discloses a system to excite an object at a vibration frequency to induce a wave on the surface of the object and use an optical interferometer to determine vibrational amplitude and phase of on a measurement surface of the object relative to a reference phase. A processing system uses a spatial derivative filter to the vibration phase data, and the resulting spatial-derivate-of-phase data is processed to determine a property of the object in the measurement surface. These methods are very useful when defects existing in the object is within the measurement surface, i.e. within view of the optical interferometer. However, parts of the object are often covered with an opaque material, in which case defects below the opaque material cannot be detected using the prior art methods.

The present inventor has realised, however, that it is possible to apply the known measurement technology to also identify defects existing in an area outside the measurement surface.

Thus in a first aspect, the invention provides a method of analysing an object, comprising:

exciting the object at a vibration frequency so as to induce at least one wave, having the vibration frequency, on an excitation surface of the object;

propagate the at least one wave into an analysis surface of the object; measuring vibration on a measurement surface of the object, the measurement surface being spatially separated from the excitation surface of the object by the analysis surface of the object;

processing the vibration data to determine a change in at least one wave property of the at least one wave; and

determining, based on the change in the at least one wave property of the at least one wave, at least one defect existing in the analysis surface of the object.

From a further aspect, the invention provides a system for analysing an object, comprising:

an exciter adapted to exciting the object at a vibration frequency so as to induce at least one wave, having the vibration frequency, on an excitation surface of the object, such that the at least one wave is propagated into an analysis surface of the object;

a vibration measuring device adapted to measuring vibration on a measurement surface of the object, the measurement surface being spatially separated from the excitation surface of the object by the analysis surface of the object;

a processing device adapted to determine a change in at least one property of the at least one wave; and

determining, based on the change in the at least one wave property of the at least one wave, at least one defect existing in the analysis surface of the object.

The object may be any single or compound object, such as a composite panel or polymer gas bottle, vehicle body panel, an aircraft structure, a turbine blade, an oil pipeline, a bolt, a musical instrument, etc. The method may be used to identify faults or imperfections in the object. The object may be a composite structure, such as a polymer and/or metal composite structure. The object may be a metallic structure, whose thickness may vary due to corrosion. The analysis may be used to identify corrosion, de-laminations, de-bonds, impact damage, material cracks, flaws or other weaknesses, or to detect loose components e.g. in bolted or riveted structures.

The object may be excited in any appropriate way. The system may comprise means (e.g., an exciter) for exciting the object, preferably at the vibration frequency, so as to induce the stationary or travelling wave on the surface of the object—e.g., by an acoustic signal or by direct mechanical excitation. The excitation may create a plurality of travelling or standing waves on the surface of the object, which may have a common wavelength or different wavelengths. The plurality of travelling or standing waves may be excited simultaneously or sequentially. The object may be excited by an exciter, such as an electro-mechanical actuator—e.g., a piezoelectric transducer. The exciter may be in contact with the object, or may be coupled to the object through a fluid medium such as air. For a substantially planar object, the object may be excited in an in-plane direction or in an out-of-plane direction. The vibration frequency may be an audible frequency, an infrasonic frequency, or an ultrasonic frequency. The exciter could vibrate the surface at a plurality of frequencies, e.g., using white noise; however, single-frequency excitation at the vibration frequency may be preferred at least in some embodiments. The exciter may be external to the object, or it may be part of the object—e.g., being embedded in the object. The may be a plurality of excitation sources, e.g., at different locations on or adjacent the object. The vibration frequency preferably induces a harmonic vibration.

In one embodiment, the excitation surface may comprise a single point or a plurality of points. The plurality of points may be arranged in a line, or a two-dimensional geometrical shape. The plurality of points may be phased-controlled in relation to one another creating a phased array of excitation points. Exemplary twodimensional shapes include, but are not limited to squares, rectangles, rhombuses, parallelograms, trapezoids, triangles, and all other kinds of regular and irregular polygons. The plurality of waves may be introduced having different shapes and/or propagation directions. The plurality of waves may be collimated, diverging or converging. Collimated, diverging or converging wave front may be created using the phased array of excitation points.

The surface of the object may be continuous or discontinuous. It may be planar, curved, bent or shaped in any way. The wave, or a plurality of waves, may be induced on part or all of the surface. It will be appreciated that, while the vibration at the surface of the object is used for measurement purposes, in practice it is not just the surface that moves—the object beneath the surface will also be involved in the vibration. In some cases, the entire object may vibrate.

In one embodiment, the change in the at least one wave property of the at least one wave may comprise a reduced wave amplitude or no detectable wave.

In one embodiment, the change in the at least one wave property of the at least one wave may comprise a non-spherical or non-planar wave-front.

In one embodiment, the change in the at least one wave property may comprise a second wave having a second propagation direction different from a propagation direction of the induced wave.

In one embodiment, the method may further comprise:

exciting a calibration object at the vibration frequency so as to induce at least one wave, having the vibration frequency, on an excitation surface of the calibration object;

propagate the at least one wave into an analysis surface of the calibration object;

measuring vibration data on a measurement surface of the calibration object, the measurement surface being spatially separated from the excitation surface of the calibration object by the analysis surface of the calibration object;

processing the vibration data to determine a calibrated wave propagation for the calibration object; and

wherein the change in the at least one wave property of the at least one wave comprises a wave propagation differing from the calibrated wave propagation.

In one embodiment, the object may be excited so as to induce a travelling wave.

In one embodiment, the excitation and measurement may be performed at a plurality of frequencies.

In one embodiment, the excitation and measurement may be performed using inplane excitation, out-of-plane excitation or a combination of both.

In one embodiment, the measuring of vibration data may comprise measuring an amplitude and a phase. In other embodiments, the measuring of vibration data may comprise measuring either amplitude or phase.

In one embodiment, the measuring of vibration data comprises using electronic speckle pattern interferometry (ESPI), electronic shearography, or scanning laser Doppler vibrometry (LDV) to determine the vibration data.

In one embodiment at least a part of the analysis surface of the object is covered by an opaque material.

The vibration data may be acquired for any number of points over the measurement surface e.g., tens, hundreds, thousands or millions of points. The points may be uniformly spaced, in one or two dimensions, over the surface of the object, or over an image plane of an optical-interference-based measurement apparatus. For example, the points may correspond to pixels in an imaging sensor. The vibration data may be stored in a digital memory of the processing system.

The processing system may take any suitable form. It may comprise one or more processors, FPGAs, ASICs, DSPs, discrete electronic components, etc. It may comprise volatile and/or non-volatile memory. The processing steps disclosed herein may be implemented entirely in hardware (e.g., using physical logic gates), or entirely in software, or a combination of the two. The processing system may be in one unit or it may be distributed—e.g., over a network. It may comprise hardware and/or software

Features of any aspect or embodiment described herein may, wherever appropriate, be applied to any other aspect or embodiment described herein. Where reference is made to different embodiments or sets of embodiments, it should be understood that these are not necessarily distinct but may overlap.

Brief description of the drawings

Certain preferred embodiments of the invention will now be described, by way of example only, with reference to the accompanying drawings, in which:

Figure 1 is a schematic view of an interferometric analysis system embodying the invention;

Figure 2 is a schematic illustration of an analysis system of the present invention;

Figure 3 is schematic illustration of an analysis system of the present invention;

Figure 4 is an exemplary flowchart for a method of the present invention; and

Figure 5 is an exemplary result of an interferometric analysis of the present invention.

Description of the invention

Figure 1 shows an interferometric analysis system 1 for analysing an object 2. The system 1 uses vibration-analysis ESPI.

A surface of the object 2 is made to vibrate at a driving frequency by a ceramic piezoelectric exciter 3 which is coupled to the object 2. The exciter is controlled by a processing system 4, to which it is coupled. Alternatively, the object 2 could be excited by an air-coupled transducer, or using an excitation unit embedded in the structure under evaluation (e.g., a piezo unit integrated in the structure during production of the structure), or in any other appropriate way.

The measurement device in the case of vibration-analysis ESPI comprises a plurality of devices. A laser 5 emits light towards the object 2. The light passes a beam-splitter 6, which diverts a reference-beam portion through a fibre optic cable 7 to a beam-combiner 8. The beam-combiner 8 combines the reference beam with laser light reflected off the surface of the object 2. A camera 9 captures the interference pattern between the two light paths. Exemplary light beams are represented by dashed lines in Figure 1.

Video data from the camera 9 is passed to the processing system 4, which processes the data in one or more of the ways described below. The processing system 4 is connected to a display screen 10 for outputting a graphical representation of the processed data to a human user.

In other embodiments, the system 1 may comprise a projection system for projecting graphical output from the processing system 4 back onto the surface of the object 2, as described in the applicant’s earlier application WO2017/085457, the entire contents of which are hereby incorporated by reference.

In other embodiments, the system may be configured to use shearography, instead of ESPI. In this measurement device, the beam-splitter 6, fibre optic cable 7 and beam-combiner 8 will be dispensed with. Instead, a beam-splitter, a reference mirror, and a shearing mirror will be provided in front of the camera 9, so that light from the object 2 interferes with a spatially-offset copy of the same light.

Some or all of these components of the system 1 may be contained in a common housing (not shown). In some embodiments, the processing system 4 and/or display screen 10 may be remote from other components of the system 1—e.g. the processing may be performed by a networked server, which could be located in a different room or building from the object 2.

The processing system 4 uses an appropriate algorithm to calculate vibration amplitude data and/or vibration phase data, for points on the surface of the object 2, from the image data output by the camera 9. In the case of ESPI, this data describes the vibration of the object 2 directly (i.e., based on the changes in axial distance between the object 2 and the camera 9), whereas in the case of shearography the data relates to a gradient (spatial derivative) in the shearing direction, because shearography captures differences in distance between a point on the surface and a neighboring point, rather than measuring changes in distance for each point independently as in ESPI. The details of the calculations are described in applicant’s earlier application WO2019/229473, the entire contents of which a re hereby incorporated by reference.

In one arrangement, a heterodyning approach may be used, whereby both the object vibration and the reference wave are excited by a system signal generator. In other embodiments, fringe analysis, such as Fourier analysis, may be performed.

In one arrangement the analysis system 1 may use scanning laser Doppler vibrometry (LDV) as the measurement device to determine the vibration data.

Figure 1 furthermore shows that at least a part of the analysis surface of the object 2 is covered by an opaque material 11. Defects below the opaque material is out of view of the optical interferometer, and a new methodology is applied to determine that such defects exists as will be disclosed with reference to Figure 2. This methodology is not only applicable when parts of the object 2 is below an opaque material, but is suitable in any situations where the field of view/measurement surface of the measurement device is spatially separated from the analysis area.

Figure 2 shows a schematic illustration of a system for analysing the object 2. The exciter 3 excites the object 2 at a vibration frequency so as to induce at least one wave, having the vibration frequency, on an excitation surface 12 of the object, such that the at least one wave is propagated into an analysis surface 13 of the object. The processing system 4 controls the exciters 2, and may use an appropriate algorithm to calculate excitation amplitude data and/or excitation phase data. A vibration measuring device, such as those discussed above, measures vibration on a measurement surface 14 of the object, the measurement surface 14 being spatially separated from the excitation surface 12 of the object by the analysis surface 13 of the object 2. Figure 2 shows for ease of understanding that the analysis surface 13 may be in-line between the excitation surface 12 and the measurement surface 14.

However, the analysis surface 13 may be any surface of the object 2 influenced by the propagation of the at least one wave, either directly or in-directly, e.g. in form of reflected waves from edges or other structural elements of the object 2

Figure 3 shows another schematic illustration of the system for analysing the object 2. An exemplary wave propagation is illustrated for an object 2 having a defect 15 that is not in-line between the excitation surface 12 and the measurement surface 14. Vibrations measured on the measurement surface 14 includes both vibrations from undisturbed waves 17 and reflected waves 16 from the defect 15.

Now with additional reference to Figure 4 showing an exemplary flow chart of method of analysing the object 2.

In a first step, the object 2 is excited at a vibration frequency so as to induce at least one wave, having the vibration frequency, on the excitation surface 12 of the object 2. The excitation surface may comprise a single point or a plurality of points as shown in Figure 3. The plurality of points may be arranged in a line, or a twodimensional geometrical shape. Exemplary two-dimensional shapes include, but are not limited to squares, rectangles, rhombuses, parallelograms, trapezoids, triangles, and all other kinds of regular and irregular polygons. The plurality of waves may be introduced having different shapes and/or propagation directions, such as Rayleigh-, Lamb- or Love waves. The plurality of waves may be collimated, diverging or converging. In an advantageous embodiment, the object 2 is excited so as to induce travelling waves. Hence, as a second step, the at least one wave propagate into the analysis surface 13 of the object 2.

In the next step, vibrations are measured on a measurement surface 14 of the object 2. The measurement surface 14 is spatially separated from the excitation surface 12 of the object 2 by the analysis surface 13 of the object. The analysis surface 13 is typically covered by an opaque material or is out of view of the measurement device performing the vibration measurements. The excitations and measurements may be performed at a single frequency or a plurality of frequencies. Furthermore, the excitations and measurements may be performed using in-plane excitation, out-ofplane excitation or a combination of both.

In the next step, the vibration data from the vibration measurements are processed to determine a change in at least one wave property of the at least one wave. A change in the at least one wave property may indicate that the at least one wave has been affected by defects in the analysis surface 13 through which the at least one wave has propagated. One such change in the at least one wave property is that the measured vibration data show a wave having a reduced wave amplitude compared with the induced wave. It is also possible that the measured vibration data show that there is no detectable wave, i.e. the induced wave has been attenuated to a nondetectable level due to the defects in the analysis surface. Another change in the at least one wave property is that the vibration data show a wave that has a nonspherical or non-planar wave-front, contrary to what would have been expected from an object without defects in the analysis surface 13. Another change in the at least one wave property is that the vibration data show a second wave having a second propagation direction different from the propagation direction of the induced wave. That is, the second wave may be a wave reflected from defects in the analysis surface 13.

The analysis surface may not be homogenous and isotropic. The analysis surface 13 may comprise flanges, edges, through holes, etc. creating complex wave-shapes at the measurement surface 14. In those cases, resulting waves may be registered for a similar object without defects, i.e. a calibration object, and the measured vibration data for the object 2 under test, may be compared with registered waves.

In one embodiment this may be performed by first exciting a calibration object at the vibration frequency so as to induce the at least one wave, having the vibration frequency, on an excitation surface of the calibration object. The at least one wave propagates into an analysis surface of the calibration object. The vibration data is measured on a measurement surface of the calibration object, the measurement surface being spatially separated from the excitation surface of the calibration object by the analysis surface of the calibration object. The measurement surface, the excitation surface and the analysis surface of the calibration object should be identical to the objects under test. As discussed above, the processor processes the vibration data to determine a calibrated wave propagation for the calibration object. Then, in the step of determining a change in the at least one wave property of the at least one wave, for the object 2 under test, determining a change in the at least one wave property of the at least one wave comprises comparing the measured wave propagation with the calibrated wave propagation. When they differ, it may be determined that there is a defect in the analysis surface 13 of the object 2.

If no changes in the at least one wave property of the at least one wave is detected, it is determined that no defects exist in the analysis surface.

Figure 5 shows an exemplary result of an interferometric analysis of an object according to the present invention. The figure shows a composite container excited at vibration frequency on an excitation surface 12 such that at least one wave has been propagated into the composite container. The surface container has a damaged area, or defect, 18. As mentioned in the prior art section, this defect can be detected directly using the methodology disclosed in WO2019/229473. However, composite containers are usually partially covered by a protecting opaque material, such as hard plastic. If the defect 18 was covered by the opaque material it would not be possible to find the defect using prior art methods. However, as described above, the defect 18 causes changes in the wave property in measurement surface areas 19 that may not be covered by the opaque material. The determination of changes in the wave property in the measurement surfaces 19 determines that at least one defect 18 exists in the analysis surface of the object. In this case, the analysis surface of the object may be any part of the surface covered by the opaque material.

It will be appreciated by those skilled in the art that the invention has been illustrated by describing various specific embodiments thereof, but is not limited to these embodiments; many variations and modifications are possible, within the scope of the accompanying claims.

Claims

CLAIMS

1. A method of analysing an object, comprising:

exciting the object at a vibration frequency so as to induce at least one wave, having the vibration frequency, on an excitation surface of the object;

processing the vibration data to determine a change in at least one wave property of the at least one wave; and

determining, based on the change in the at least one wave property of the at least one wave, at least one defect existing in the analysis surface of the object.

2. The method of claim 1, wherein the change in the at least one wave property of the at least one wave comprises a reduced wave amplitude or no detectable wave.

3. The method of any of the preceding claims, wherein the change in the at least one wave property of the at least one wave comprises a non-spherical or nonplanar wave-front.

4. The method of any of the preceding claims, wherein the change in the at least one wave property is a second wave having a second propagation direction different from a propagation direction of the induced wave.

5. The method of claim 1, wherein the method further comprising:

exciting a calibration object at the vibration frequency so as to induce at least one wave, having the vibration frequency, on an excitation surface of the calibration object;

propagate the at least one wave into an analysis surface of the calibration object;

processing the vibration data to determine a calibrated wave propagation for the calibration object; and

wherein the change in the at least one wave property of the at least one wave comprises a wave propagation differing from the calibrated wave propagation.

6. The method of any of claims 1 to 4, wherein the method further comprising exciting the object so as to induce a travelling wave.

7. The method of any of the preceding claims, wherein the excitation surface comprises a single point or a plurality of points.

8. The method of claim 7, wherein the plurality of points is arranged in a line, or a two-dimensional geometrical shape.

9. The method of any of the preceding claims, wherein the method further comprises introducing a plurality of waves having different shapes and/or propagation directions.

10. The method of claim 9, wherein the plurality of waves is collimated, diverging or converging.

11. The method of any of the preceding claims, wherein the excitation and measurement are performed at a plurality of frequencies.

12. The method of any of the preceding claims, wherein the excitation and measurement are performed using in-plane excitation, out-of-plane excitation or a combination of both.

13. The method of any of the preceding claims, wherein the measuring vibration data comprises measuring an amplitude and a phase.

14. The method of any of the preceding claims, comprising using electronic speckle pattern interferometry (ESPI), electronic shearography, or scanning laser Doppler vibrometry (LDV) to determine the vibration data.

15. The method of any of the preceding claims, wherein at least a part of the analysis surface of the object is covered by an opaque material.

16. A system for analysing an object, comprising:

a processing device adapted to determine a change in at least one property of the at least one wave; and

determining, based on the change in the at least one wave property of the at least one wave, at least one defect existing in the analysis surface of the object.

17. The system of claim 16, wherein at least a part of the analysis surface of the object is covered by an opaque material.

Drawings

Priority

No priority

Patent classes

IPC classes

G01N 21/88

G01N 21/62

G01N 21/17

G01B 11/16

CPC classes

G01N 21/8806

G01N 21/62

G01N 21/17

G01B 11/16

Citations

WO 2019229473 A1 (A1)

WO 2006001842 A2 (A2)

US 2004003662 A1 (A1)

US 2018340858 A1 (A1)

US 4928527 A (A)

US 2016282308 A1 (A1)

US 2013036820 A1 (A1)

DE 102015114855 A1 (A1)

Applicants, owners and inventors

Applicants

Optonor AS

Jarleveien 12

7041 TRONDHEIM

NO (TRONDHEIM Municipality, Trøndelag county)

Org. number: 916168306

Inventors

Eiolf Vikhagen

Jarleveien 12

7041 TRONDHEIM

NO (TRONDHEIM Municipality, Trøndelag county)

Agent

DEHNS NORDIC AS

Gaustadalléen 21

0349 OSLO

NO (OSLO Municipality, Oslo county)

Org. number: 925704261

Reference: -

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