Ecole Centrale de Lille, IEMN, 59650 Villeneuve d'Ascq Cedex, France
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HIGHLIGHTSA time-domain model of an air-coupled, non-contact, ultrasonic setup, is proposed.The receiver size and the attenuation in air are modelled.The prediction error is evaluated experimentally and is smaller than 1%.The experimental recovery of the system's electric response is proposed.Different planar and quasi planar (i.e. focussing) transducers can be modelled.This paper presents a time-domain model for the prediction of an acoustic field in an air-coupled, non-contact, ultrasonic setup, which includes an air-coupled Emitter, the Propagation space and an air-coupled Receiver (EPR). The model takes into account the finite size of the aperture receiver, attenuation in air, and the electric response of the emitter-receiver set Symbol. The attenuation is characterized by a causal time-domain Green's function, allowing the wideband attenuation of a lossy medium obeying the power law Symbol to be included. The electrical response is recovered experimentally using a procedure which includes the deconvolution of air absorption effects. The model is implemented numerically using a discrete representation approach. In order to study the influence of receiver size and attenuation, five different computational approaches are proposed; each of these is evaluated quantitatively, by comparing the predicted acoustic field with the experimentally measured signal. The prediction error is studied in both the near and far fields, for three typical field features: the system's impulse response, the on-axis field distribution, and the directivity pattern, for the case of air-coupled transducers operating at two different central frequencies, namely 50 kHz and 350 kHz, with a 10 mm diameter wideband receiver. It is shown that when the attenuation in air, the receiver size, and the accurately recovered electric response Symbol, are correctly taken into account, the model allows the system's impulse response to be accurately predicted, with on-axis errors ranging between 0.2% in the far field and 1% in the near field. In the near-field area and within the far field −3 dB beam spread width, the error is generally greater than on the axis, but globally remains smaller than 1%. Inclusion of the size of the receiver dimension in the model appears to be crucial to the accuracy of the near field predictions, and an approximate criterion is proposed for the evaluation of the influence of receiver. The procedure used to recover the electric response Symbol is also presented in detail. The results obtained from this study are used to formulate various recommendations related to EPR modelling.