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声镊中的势阱模型。

Potential-well model in acoustic tweezers.

机构信息

Department of Biomedical Engineering and Environmental Sciences, National Tsing Hua University, Hsinchu, Taiwan.

出版信息

IEEE Trans Ultrason Ferroelectr Freq Control. 2010 Jun;57(6):1451-9. doi: 10.1109/TUFFC.2010.1564.

Abstract

Standing-wave acoustic tweezers are popularly used for non-invasive and non-contact particle manipulation. Because of their good penetration in biological tissue, they also show promising prospects for in vivo applications. According to the concept of an optical vortex, we propose an acoustics-vortex- based trapping model of acoustic tweezers. A four-element 1-MHz planar transducer was used to generate 1-MHz sine waves at 1 MPa, with adjacent elements being driven with a pi/2-rad phase difference. Each element was a square with a side length of 5.08 mm, with kerfs initially set at 0.51 mm. An acoustic vortex constituting the spiral motion of an acoustic wave around the beam axis was created, with an axial null. Applying Gor'kov's theory in the Rayleigh regime yielded the potential energy and radiation force for use in subsequent analysis. In the transverse direction, the vortex structure behaved as a series of potential wells that tended to drive a suspended particle toward the beam axis. They were highly fragmented in the near field that is very close to the transducer where there was spiral interference, and well-constructed in the far field. We found that the significant trapping effect was only present between these two regions in the transverse direction--particles were free to move along the beam axis, and a repulsive force was observed in the outer acoustic vortex. Because the steepness of the potential gradient near an axial null dominates the trapping effect, the far field of the acoustic vortex is inappropriate for trapping. Particles too close to the transducer are not sufficiently trapped because of the fragmented potential pattern. We suggest that the ideal distance from the transducer for trapping particles is in front of one-fourth of the Rayleigh distance, based on the superposition of the wavefronts. The maximum trapping force acting on a 13-mum polystyrene sphere in the produced acoustic vortex was 50.0 pN, and it was possible to trap approximately 10(6) particles within a plane; the maximum repulsive force was 24.5 pN, and this was reduced to less than 13 pN by smoothing the outer gradient. Most stiff and dense particles can be used in this model. The presence of transverse trapping and the long working distance make the model useful for 2-D manipulation, particularly in in vivo applications. This paper details the trapping properties in the acoustic vortex and describes methods for improving the design of the transducer. The results obtained support the feasibility of the potential-well model of acoustic tweezers.

摘要

驻波式声镊被广泛用于非侵入式和非接触式的粒子操控。由于其在生物组织中有很好的穿透性,因此在体内应用方面也具有广阔的前景。根据光学涡旋的概念,我们提出了一种基于声镊的声涡旋捕获模型。使用四元 1-MHz 平面换能器在 1 MPa 下产生 1-MHz 的正弦波,相邻元件之间的相位差为π/2。每个元件都是边长为 5.08mm 的正方形,初始开槽宽度为 0.51mm。通过创建一个构成声束轴周围声波螺旋运动的声涡旋,产生一个轴向零点。应用戈尔科夫在瑞利区的理论,得到了用于后续分析的势能和辐射力。在横向方向上,涡旋结构表现为一系列的势阱,这些势阱倾向于将悬浮粒子驱向束轴。在非常接近换能器的近场中,涡旋结构是高度碎片化的,存在螺旋干扰,而在远场中则是构造良好的。我们发现,只有在横向的这两个区域之间才存在显著的捕获效应,粒子可以沿着束轴自由移动,并且在外声涡旋中观察到一个排斥力。由于轴向零点附近的势梯度陡度主导着捕获效应,因此声涡旋的远场不适合捕获。由于势分布碎片化,太靠近换能器的粒子不能被充分捕获。我们建议,基于波前的叠加,从换能器捕获粒子的理想距离是在瑞利距离的四分之一之前。在产生的声涡旋中,作用在 13μm 聚苯乙烯球上的最大捕获力为 50.0pN,可以在一个平面内捕获大约 10^6 个粒子;最大排斥力为 24.5pN,通过平滑外部梯度可以将其减小到小于 13pN。该模型可以使用大多数刚性和密集的粒子。横向捕获和长工作距离使该模型适用于 2-D 操作,特别是在体内应用中。本文详细描述了声涡旋中的捕获特性,并描述了改进换能器设计的方法。所得到的结果支持声镊势阱模型的可行性。

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