冰层中相控阵超声波束传播特性的数值模拟

doi:10.7527/S1000-6893.2023.29289

Abstract

Abstract:

To solve the problems of small monitoring range， low detection sensitivity and limited detection of ice thickness， the mechanism of ultrasonic icing detection based on phased array is studied. Based on the synthesis principle of phased array ultrasonic beam， using COMSOL as a numerical calculation platform， a propagation model of phased array ultrasonic beam on aluminum plate covered with ice is constructed， and the propagation law of phased array ultrasonic beam in three-dimensional ice layer is studied. Compared with the other icing detection technologies， phased array ultrasonic icing detection offers a wider detection range. Compared with in-phase excitation， the energy of ultrasonic beam generated by phased array excitation is more concentrated. The displacement peak of the S₀ mode beam changes more significantly with ice thickness， ice width， and ice length. The displacement peak change rate of the S₀ mode beam increases with the excitation frequency， which can enhance the sensitivity of ice detection. When the excitation frequency exceeds a certain level， the peak displacement of the S₀ mode beam exhibits a turning point， which may lead to early saturation of ice thickness. Choosing an appropriate excitation frequency can simultaneously improve the sensitivity of icing detection and the upper limit of ice thickness detection. The propagation characteristics of phased array ultrasonic beam in ice layer are preliminarily verified， which provides theoretical reference for future engineering application of ultrasonic icing detection.

Key words: ice detection, ultrasonic beam, phased array, numerical simulation, S₀ mode

CLC Number:

V241

Hongjian ZHANG, Yanxin ZHANG, Jianjun XIONG, Zhao ZHAO, Lin RAN, Xian YI. Numerical simulation of phased array ultrasonic beam propagation characteristics in ice layer[J]. Acta Aeronautica et Astronautica Sinica, 2023, 44(S2): 729289-729289.

Figures/Tables 19

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冰层厚度/mm	单点激励位移峰值/nm	同相激励位移峰值/nm	相控阵激励位移峰值/nm
0.5	6.5	60.2	115
1	3.8	34.8	65.1

冰层宽度/mm	单点激励位移峰值/nm	同相激励位移峰值/nm	相控阵激励位移峰值/nm
10	8.4	76.2	143.1
20	6.8	60.6	111.4
30	5.3	49.1	88.7
40	4.3	40	70.2
50	3.4	31.1	56.1

冰层长度/mm	单点激励位移峰值/nm	同相激励位移峰值/nm	相控阵激励位移峰值/nm
10	5.6	51.5	98.9
20	5.5	48.3	88.2
30	5.3	49.1	88.7
40	5.4	49.7	89.2
50	5.4	49.9	89.7

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Numerical simulation of phased array ultrasonic beam propagation characteristics in ice layer

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