Non-contact measurement of the thickness of a surface film using a superimposed ultrasonic standing wave

• Published in: Ultrasonics Vol. 110; p. 106291
• Main Authors: Kanja, J., Mills, R., Li, X., Brunskill, H., Hunter, A.K., Dwyer-Joyce, R.S.
• Format: Journal Article
• Language: English
• Published: Elsevier B.V 01.02.2021
• Subjects: Coating thickness; Continuous pulsing; Quarter wavelength; Superimposed standing wave; Surface layer thickness; Surface layer thickness; Coating thickness; Quarter wavelength; Superimposed standing wave; Continuous pulsing
• ISSN: 0041-624X; 1874-9968
• DOI: 10.1016/j.ultras.2020.106291

•Continuously repeating chirp wave that forms a standing wave within a component.•Surface layer resonant frequency identified from standing wave frequency response.•Reflected echoes reinforce the standing wave.•Simple and cheap instrumentation. Most methods used to measure the thickness of thin liquid or solid surface films and coatings need access to the coated surface. In this work reflected ultrasonic pulses were used to measure a coating thickness from a solid back face. Piezoelectric transducers on the solid back face emitted ultrasound waves and received the waves that bounced off the front face. The magnitude of the reflected wave was dependent on the film thickness at the front face. Most pulse-echo ultrasonic approaches use the time-of-flight through the surface layer to determine its thickness. However, as the film becomes thinner, the reflected echoes overlap and there is often an acoustic mismatch between the solid and the surface film that reduces the signal strength. In this work, we propose the use of an ultrasonic continuously repeated chirp longitudinal wave to amplify the effect of the surface film. Multiple reflections interfere within the solid to form a superimposed standing wave whose amplitude spectrum is highly dependent on the surface film thickness thus overcoming the acoustic mismatch problem. Two bare 10 MHz piezoelectric elements were bonded to a 10 mm thick aluminium solid in a pitch-catch arrangement such that one continuously sends repeating chirp ultrasound waves and the other acts as the receiver. The transmitter was set to send a repeating chirp wave of 4 ms duration corresponding to the bandwidth of the transducer in order to maximise signal amplitude. The incident and reflected waves constructively and destructively interfere to form a superimposed standing wave within the solid. The solid/surface film to solid/air boundary condition frequency spectra ratio showed the film resonant frequency modes as minima. Using this technique epoxy coatings ranging from 70 μm to 350 μm were measured and showed a good correlation with independent measurements using a surface profilometer.