Acoustic Emission Testing. Activity of AE Sources in Structural Loading AE Sources Non-metallic inclusions Cracks Frequency range 100 – 500kHz Activity.

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Acoustic Emission Testing

Activity of AE Sources in Structural Loading AE Sources Non-metallic inclusions Cracks Frequency range 100 – 500kHz Activity Primary activities Permanent changes in material (crack growth) Secondary activities E.g., crack surface rubbing Noise in AE testing Friction, impacts, …

Activity of AE Sources in Structural Loading Kaiser effect (CB) Insignificant flaws Felicity effect (EFG) Structural significant flaws

Sensing and Measuring

AE Signal Features

Amplitude, A, is the greatest measured voltage in a waveform and is measured in decibels (dB). This is an important parameter in acoustic emission inspection because it determines the detectability of the signal. Signals with amplitudes below the operator-defined, minimum threshold will not be recorded. Rise time, R, is the time interval between the first threshold crossing and the signal peak. This parameter is related to the propagation of the wave between the source of the acoustic emission event and the sensor. Therefore, rise time is used for qualification of signals and as a criterion for noise filter. Duration, D, is the time difference between the first and last threshold crossings. Duration can be used to identify different types of sources and to filter out noise. Like counts (N), this parameter relies upon the magnitude of the signal and the acoustics of the material. MARSE, E, sometimes referred to as energy counts, is the measure of the area under the envelope of the rectified linear voltage time signal from the transducer. This can be thought of as the relative signal amplitude and is useful because the energy of the emission can be determined. MARSE is also sensitive to the duration and amplitude of the signal, but does not use counts or user defined thresholds and operating frequencies. MARSE is regularly used in the measurements of acoustic emissions. Counts, N, refers to the number of pulses emitted by the measurement circuitry if the signal amplitude is greater than the threshold. Depending on the magnitude of the AE event and the characteristics of the material, one hit may produce one or many counts. While this is a relatively simple parameter to collect, it usually needs to be combined with amplitude and/or duration measurements to provide quality information about the shape of a signal.

AE Source Location Techniques

∆T approach

Good and Ambiguous Locations

Pencil Excitation

Lamb Wave Modes in Plates

Guard Sensor Concept

First Hit Zone Localization

AE Data Displays Planar source location display

AE Data Displays Linear location display

AE Data Displays Zone location display

AE Data Displays Activity display (AE rate versus time)

AE Data Displays Cumulative activity display

AE Data Displays Cumulative amplitude distribution

AE Data Displays Duration-amplitude cross plot

Conclusions Acoustic Emission is unlike most other nondestructive testing (NDT) techniques in two regards. The first difference pertains to the origin of the signal. Instead of supplying energy to the object under examination, AET simply listens for the energy released by the object. AE tests are often performed on structures while in operation, as this provides adequate loading for propagating defects and triggering acoustic emissions. The second difference is that AET deals with dynamic processes, or changes, in a material. This is particularly meaningful because only active features (e.g. crack growth) are highlighted. The ability to discern between developing and stagnant defects is significant. However, it is possible for flaws to go undetected altogether if the loading is not high enough to cause an acoustic event. Furthermore, AE testing usually provides an immediate indication relating to the strength or risk of failure of a component. Other advantages of AET include fast and complete volumetric inspection using multiple sensors, permanent sensor mounting for process control, and no need to disassemble and clean a specimen. Unfortunately, AE systems can only qualitatively gauge how much damage is contained in a structure. In order to obtain quantitative results about size, depth, and overall acceptability of a part, other NDT methods (often ultrasonic testing) are necessary. Another drawback of AE stems from loud service environments which contribute extraneous noise to the signals. For successful applications, signal discrimination and noise reduction are crucial.