2019
DOI: 10.1016/j.apacoust.2019.04.016
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Underwater sound absorption characteristics of metamaterials with steel plate backing

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Cited by 38 publications
(12 citation statements)
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“…To evade detection by armaments, the stealth device is required to manage its reflective or emissive signatures in various ranges, including radar, [1][2][3][4] infrared (IR), [5][6][7][8][9][10][11][12][13][14][15] and sonar. [16][17][18] Regarding IR vigilance, thermal engineering against IR search and track systems (IRSTs), which measure the thermal emission signals of objects, have been investigated. [5][6][7][8][9][10][11][12][13][14][15] At the ambient temperature, thermal camouflage materials adapt their thermal signals to the background signals excitation, [28,29] leading to strong interference.…”
Section: Introductionmentioning
confidence: 99%
“…To evade detection by armaments, the stealth device is required to manage its reflective or emissive signatures in various ranges, including radar, [1][2][3][4] infrared (IR), [5][6][7][8][9][10][11][12][13][14][15] and sonar. [16][17][18] Regarding IR vigilance, thermal engineering against IR search and track systems (IRSTs), which measure the thermal emission signals of objects, have been investigated. [5][6][7][8][9][10][11][12][13][14][15] At the ambient temperature, thermal camouflage materials adapt their thermal signals to the background signals excitation, [28,29] leading to strong interference.…”
Section: Introductionmentioning
confidence: 99%
“…The outer space of the sound absorption layer was assumed as a water domain with semi-infinite space, possessing the ideal fluid condition of uniform, incompressible, nonviscous, and zero-flow velocity. The acoustic excitation was a small disturbance near the stable state of the fluid domain, and the wave equation of the fluid medium could be expressed as [ 38 , 39 ]: in which c represented the sound velocity of the fluid medium ( , K was the bulk modulus, and ρ 0 was the density), p denoted the sound pressure, and was the transpose of the gradient operator. Taking the integral of small incremental sound pressure over the fluid domain, the following equation could be obtained: where V f was the fluid domain, S sf was the interface of the fluid domain and the solid domain, S ff was the interface of the fluid domain and the fluid domain, and [n] was the outward unit normal vector of the surface.…”
Section: Methodsmentioning
confidence: 99%
“…Taking the integral of small incremental sound pressure over the fluid domain, the following equation could be obtained: where V f was the fluid domain, S sf was the interface of the fluid domain and the solid domain, S ff was the interface of the fluid domain and the fluid domain, and [n] was the outward unit normal vector of the surface. The equation utilized to represent the medium movement in the small amplitude linear acoustic fields was expressed as [ 39 ]: in which u represented the particle vibration velocity of the fluid medium. As the structure of the interior sound absorption layer displayed a periodic array, the sound absorption proprieties of the layer could be analyzed using a structural unit according to the Bloch’s theory.…”
Section: Methodsmentioning
confidence: 99%
“…In order to grasp the sound absorption effect of the structure, this paper adopts the sound absorption coefficient α [28] as the evaluation index of the structure, which is given as follows:…”
Section: Evaluation Indicatorsmentioning
confidence: 99%