The nonlinear imaging technique of Potter et al (2014) has been successfully implemented and experimentally proven. On the sample used, the signal from the crack tip had been just visible using the (linear) FMC technique, but was much weaker than the notch and back wall signals (see Figure 2a – over).
On the other hand, in the nonlinear imaging technique the fatigue crack produced a significantly nonlinear response with nonlinear metric γ=22.5%. There was no nonlinear response form notch or back wall, so the clarity with which the crack was seen was much improved.
However, this result was only achieved after very many repeat trials with varying experimental parameters. Results were extremely sensitive to the choice of parameters, such as time delays and acquisition intervals, as well as assumed velocities and the exact probe position. The optimum parameters will vary on a case-by-case basis according to the material properties, specimen geometry, specimen condition, and random noise (Cheng et al, 2017). If non-optimum parameters were selected, we found that the nonlinear technique gave no detectable response above the linear methods.
Furthermore, the data acquisition for the method is very slow. The most time-intensive part is the need for a separate phased array firing for each image pixel.
Due to the extreme sensitivity to variables and the slow acquisition speed, it is not recommended that the technique be adopted for industrial application.
References
Cheng J, Potter J N, Croxford A J and Drinkwater B W, ‘Monitoring fatigue crack growth using nonlinear ultrasonic phased array imaging’, Smart Materials and Structures 26 (2017)
Potter J N, Croxford A J and Wilcox P D, ‘Nonlinear Ultrasonic Phased Array Imaging’, Physical Review Letters 113, 144301 (2014)
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