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Single-sided contact-free ultrasound inspection of aerospace composites

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Submitted on 12 Jun 2021

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Single-sided contact-free ultrasound inspection of

aerospace composites

Matthias Brauns, Fabian Lücking, Wolfgang Rohringer, Balthasar Fischer

To cite this version:

Matthias Brauns, Fabian Lücking, Wolfgang Rohringer, Balthasar Fischer. Single-sided contact-free

ultrasound inspection of aerospace composites. Forum Acusticum, Dec 2020, Lyon, France. pp.49-50,

�10.48465/fa.2020.0993�. �hal-03240355�

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Single-sided contact-free ultrasound inspection

of aerospace composites

Matthias Brauns

1,*

Fabian Lücking

1

Wolfgang Rohringer

1

Balthasar Fischer

1 1 XARION Laser Acoustics GmbH, Ghegastraße 3, 1030 Vienna, Austria

* Corresponding author (m.brauns@xarion.com)

ABSTRACT

In this paper, we present contact-free ultrasound measure-ments on an aerospace sample consisting of two carbon fi-ber-reinforced polymer (CFRP) sheets with a honeycomb core sandwiched between them. The sample mimics a core-plug repair, where part of the honeycomb structure is milled out and replaced. The reference defect is located in the film adhesive below the replacement plug.

We demonstrate the single-sided detection of this defect located several centimeters below the sample surface with a resolution high enough to resolve the honeycomb core structure. Spectral analysis of the data shows that the dif-ferent sample features cause resonances in difdif-ferent fre-quency ranges, which are covered in a single measurement due to the broadband excitation and detection of the ultra-sound waveform. The contact-free detection of defects far from the surface in a single-sided arrangement makes this technology relevant for ultrasound inspection of CFRP-based materials in aerospace.

1. INTRODUCTION

Ultrasonic inspection is used for a wide range of materials. Common ultrasound methods use liquid coupling for a high detection bandwidth and spatial resolution. However, liquid contact is in many cases impractical or impossible to implement [1]. Conventional laser ultrasound (LUS) testing is a non-contact inspection method [2], but heavily depends on sample surface reflectivity and roughness. In addition, accessibility is an issue due to the bulky optics.

We present experiments performed with Laser Excited Acoustics (LEA), a novel laser-based NDT approach inde-pendent from surface properties such as reflectivity and roughness. Similar to conventional LUS, an excitation la-ser generates a broadband ultrasonic waveform directly in the part. No laser beam is directed at the sample for the detection, but an optical microphone [3] detects the ultra-sound leaky wave radiated into the adjacent air by means of laser interferometry. Both the excitation laser and the optical microphone are fiber-coupled, allowing for a com-pact sensor head design. The wideband excitation and de-tection of ultrasound enables the use of advanced methods like defect detection using local resonances [4].

In this paper, we report on experiments, where LEA is used for the single-sided detection of deep-lying defects in honeycomb sandwich structures.

2. EXPERIMENTAL SETUP

LEA can be operated both as a through-transmission setup with excitation laser and optical microphone on opposite sides of the sample, as well as in a single-sided arrange-ment, where excitation laser and optical microphone are on the same side in a pitch-catch configuration (see Fig. 1). In this paper, the latter configuration was used to simulate a maintenance task, where two-sided access to the part is of-ten not possible.

The sample consists of two CFRP sheets with a honey-comb core structure sandwiched between them (see Fig. 2). This specially manufactured sample mimics a so-called ‘core-plug repair’ in a part of the wing structure of an airplane. Before laminating the CFRP top sheet, a part

Figure 1: The LEA setup can be configured for a) Through-transmission testing, where excitation laser and optical microphone are on opposite sides of the sample, and b) for single-sided testing, where both are integrated into one fiber-coupled sensor head.

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of the honeycomb core was milled out, and a laminate plate was glued to the bottom of the resulting hole. A new piece of honeycomb (the ‘core plug’) was glued to this laminate plate by a glue film, filling the milled-out volume. The ref-erence defect to be detected was a ring-shaped cut-out in this glue film, situated several centimeters away from the sample surface. Finally, the CFRP top sheet covered the honeycomb core including the core plug.

For the measurements performed in pitch-catch config-uration, the sensor head comprising the excitation laser and the optical microphone was attached to an x-y scanner unit, and the sample was placed such that the sensor head was hovering several millimeters above the sample surface. The sample surface was scanned point by point, with a la-ser pulse generating an ultrasound waveform in the sample and the optical microphone measuring a full A-scan at each position.

3. RESULTS

The resulting C-scan is shown in Fig. 3. In the C-scan, two main features become apparent. Firstly, the hexagonal honeycomb core structure is visible as a regular back-ground pattern over the whole scanning area. The pitch of approximately 4 mm between adjacent honeycomb cells is easily resolved. Secondly, on top of this regular back-ground pattern, also the ring-shaped cut-out becomes visi-ble.

In order to analyze the data in more detail, a fast Fourier transformation was applied to each A-scan. The resulting spectra for each measurement point contained frequency components within the whole detection bandwidth from 50 kHz to 2 MHz. In Fig. 2b), a C-scan with the acoustic en-ergy only within the frequency window from 130 to 150 kHz is plotted, making only the honeycomb core structure

visible. The C-scan in Fig. 2c) displays the acoustic energy between 775 and 820 kHz, revealing the cut-out defect, while the honeycomb pattern is not visible. This demon-strates that the different sample features cause resonances at different frequencies, which can be covered by LEA in a single measurement.

4. CONCLUSION

Using the contact-free LEA method, measurements were performed on honeycomb-core sandwich panels in a sin-gle-sided configuration. The sample exhibited a reference defect in the glue film below a honeycomb repair plug, several centimeters away from the sample surface. The re-sulting C-scans showed the regular honeycomb core struc-ture as well as the ring-shaped cut out in the glue film be-low the core plug. Spectral analysis of the data revealed that these features were contained in different frequency ranges. This underlines the advantage gained by the con-tact-free and broadband LEA inspection method.

5. REFERENCES

[1] B. Vanderheiden, C. Thomson et al. “Transition to high rate aerospace NDI processes”, AIP Conference Proceedings 1949, p. 020003, 2018.

[2] E. Cuevas Aguado, C. G. Ramos, and F. Lasagni, “Laser ultrasonic inspections of aero-nautical compo-nents validated by computed tomography” Proc. of 7th International Symposium on NDT in Aerospace, 2015.

[3] B. Fischer, F. Sarasini, et al. „Impact damage assess-ment in biocomposites by micro-CT and innovative air-coupled detection of laser-generated ultrasound“, Compos. Struct. 210, pp. 922–931, 2019.

[4] J. Rus and C. U. Grosse, “Local Ultrasonic Resonance Spectroscopy: A Demonstration on Plate Inspection.” J Nondestruct Eval 39, p. 31, 2020.

Figure 2: The sample mimics a core plug repair, where part of the honeycomb core is milled out and replaced by a core plug, a new piece of honeycomb structure, which is glued at the bottom by a glue film. The reference defect is a ring-shaped cut out. After preparing the core plug, the CFRP top sheet is laminated.

Figure 3: a) Single-sided C-scan of the sample, where the honeycomb core structure is visible as a regular pattern superimposed with the ring-shaped reference defect. In b) only the acoustic energy within a frequency window between 130 and 150 kHz is plotted, while in c) the fre-quency window is 775 to 820 kHz.

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