2004
DOI: 10.1016/j.mechrescom.2004.02.005
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Harmonic radiation from a liquid-filled spherical acoustic lens with an internal eccentric spherical source

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Cited by 3 publications
(2 citation statements)
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“…William 首先提出了偏心球模型并计算了偏心球源的 声辐射力 [25] , 随后 Roumeliotis 等发现由于引入偏心内球而引起的硬壁球形腔声 共振频率偏移 [26] . Hasheminejad 和 Azarpeyvand 对内置的偏心辐射源散射场做了 研究, 指出密封外壳的存在导致模态阻力和惯性振幅的明显增强 [27] . Zang 等建立 理论模型探究了位于零阶贝塞尔声束中双层偏心液滴中偏心球的位置对负向声 辐射力产生的影响, 指出当偏心球位于液体球心右侧时会产生负向声辐射力 [29] .…”
Section: 细胞的声操控是实现细胞筛选、分离的关键 声操控应用的基础是声辐射力unclassified
“…William 首先提出了偏心球模型并计算了偏心球源的 声辐射力 [25] , 随后 Roumeliotis 等发现由于引入偏心内球而引起的硬壁球形腔声 共振频率偏移 [26] . Hasheminejad 和 Azarpeyvand 对内置的偏心辐射源散射场做了 研究, 指出密封外壳的存在导致模态阻力和惯性振幅的明显增强 [27] . Zang 等建立 理论模型探究了位于零阶贝塞尔声束中双层偏心液滴中偏心球的位置对负向声 辐射力产生的影响, 指出当偏心球位于液体球心右侧时会产生负向声辐射力 [29] .…”
Section: 细胞的声操控是实现细胞筛选、分离的关键 声操控应用的基础是声辐射力unclassified
“…the pulsating, n = 0, and the oscillating, n = 1, sources) are of most practical interest as they are well known to best represent the common "expander" and "shaker" type acoustic transducers, respectively. 35 A FORTRAN code was constructed for treating boundary conditions, to determine the unknown modal coefficients, and to compute the modal impedance matrix, Z = SR −1 , and other relevant acoustic quantities as functions of the distance parameter, kr 0 , at selected nondimensional frequencies, ka = ωa/c. The computations were performed on personal computers with a truncation constant of n max = 100 to assure convergence in the high frequency range, and also in case of close proximity of the source to the thermoviscous sphere.…”
Section: Numerical Implementationmentioning
confidence: 99%