Photoacoustic inspection of CFRP using an optical microphone

Air-coupled ultrasound (ACU) is already an established method for the non-destructive failure inspection of carbon fiber reinforced polymers (CFRP). In the through-transmission setup, plate-like structures are placed between the ultrasound (US) source and the receiver. The ultrasonic wave propagating through the material is observed; deteriorations inside the material such as defects alter the captured signal. Such defects can be delaminations, cracks, thickness changes or porosity. In the measurement setup chosen, conventional piezoelectric transducers and receivers are replaced by laser-based components. On the excitation side a nanosecond laser pulse, illuminating the plate surface, was used to induce ultrasonic waves (thermal regime) directly into the specimen. On the receiver side a laser-based optical microphone was tested. This membrane-free microphone detects the refractive index changes of the air, when the ultrasound propagates through the miniature Fabry-Pérot etalon. Using this new measurement setup, C-scans of CFRP plates were performed containing impact damage, delaminations and blind holes. In comparison to conventional aircoupled testing methods, our method is sensitive over a broader frequency range, has better signal-to-noise ratio (SNR) and a smaller acoustic aperture. This allows obtaining a more detailed image of a specimen including defects.

[1]  C. Grosse,et al.  Local Acoustic Resonance Spectroscopy: An Escalation Approach for Fast Non-Destructive Testing , 2018 .

[2]  F. Touchard,et al.  Impact damage assessment in biocomposites by micro-CT and innovative air-coupled detection of laser-generated ultrasound , 2019, Composite Structures.

[3]  B. Fischer,et al.  Listening to Ultrasound with a Laser , 2017 .

[4]  G. S. Taylor,et al.  Laser-generated ultrasound: its properties, mechanisms and multifarious applications , 1993 .

[5]  Balthasar Fischer,et al.  Optical microphone hears ultrasound , 2016, Nature Photonics.

[6]  Christian U. Grosse,et al.  Evolution of NDT Methods for Structures and Materials: Some Successes and Failures , 2013 .

[7]  David A. Hutchins,et al.  Quantitative measurements of laser‐generated acoustic waveforms , 1982 .

[8]  Gerhard Busse,et al.  MATERIAL CHARACTERIZATION AND NDE USING FOCUSED SLANTED TRANSMISSION MODE OF AIR-COUPLED ULTRASOUND , 2004 .

[9]  C. Grosse,et al.  Comparison of NDT Techniques to Evaluate CFRP - Results Obtained in a MAIzfp Round Robin Test , 2016 .

[10]  David A. Hutchins,et al.  Mechanisms of pulsed photoacoustic generation , 1986 .

[11]  H. Mooshofer,et al.  Advances in air-coupled ultrasonic testing combining an optical microphone with novel transmitter concepts , 2018 .

[12]  C. Grosse,et al.  Local Acoustic Resonance Spectroscopy , 2018 .

[13]  A G Bell The Production of Sound by Radiant Energy , 1881, Nature.

[14]  G. Busse,et al.  Air-Coupled Lamb and Rayleigh Waves for Remote NDE of Defects and Material Elastic Properties , 2010 .

[15]  Reisser,et al.  All-optical highly sensitive akinetic sensor for ultrasound detection and photoacoustic imaging , 2016 .

[16]  C. Grosse,et al.  Local Acoustic Resonance Spectroscopy (LARS) for Glass Fiber-Reinforced Polymer Applications , 2014 .

[17]  H. Tretout,et al.  Laser Ultrasonics : A Non Contacting NDT System , 1995 .