Acoustic Tweezers for the Life Sciences

Total Page:16

File Type:pdf, Size:1020Kb

Acoustic Tweezers for the Life Sciences REVIEW ARTICLE https://doi.org/10.1038/s41592-018-0222-9 Acoustic tweezers for the life sciences Adem Ozcelik 1, Joseph Rufo1, Feng Guo2, Yuyang Gu1, Peng Li2, James Lata2 and Tony Jun Huang 1,2* Acoustic tweezers are a versatile set of tools that use sound waves to manipulate bioparticles ranging from nanometer-sized extracellular vesicles to millimeter-sized multicellular organisms. Over the past several decades, the capabilities of acoustic tweezers have expanded from simplistic particle trapping to precise rotation and translation of cells and organisms in three dimensions. Recent advances have led to reconfigured acoustic tweezers that are capable of separating, enriching, and pat- terning bioparticles in complex solutions. Here, we review the history and fundamentals of acoustic-tweezer technology and summarize recent breakthroughs. ew discoveries are often preceded by technological progress. However, they are dependent on particle or cell polarizability and The development of cell theory, for example, is inextricably generally require low-conductivity media, which may disrupt cell Nlinked to advances in microscopy1. Just as early advances physiology. Optoelectronic tweezers are the dynamic counterpart in the ability to visualize cells resulted in the development of cell to electrode-based electrokinetic tweezers. Instead of electrodes, a theory, recent advances in the ability to manipulate single cells and light source and photoconductive substrate induce dielectrophore- biomolecules have contributed to breakthroughs in microbiology2, sis, thus enabling dynamic manipulation at relatively low optical- molecular biology3, biophysics4, and bioanalytical chemistry5. power intensities13. However, they are constrained by the same Acoustic tweezers are an emerging platform for the precise requirement for low-conductivity media, thus restricting their use manipulation of bioparticles across a broad size range. Acoustic in many biological applications. Hydrodynamic tweezers are per- tweezers spatially and temporally manipulate matter by using the haps the simplest approach for achieving particle manipulation, by interaction of sound waves with solids, liquids, and gases. The term using fluid flows to position particles within a microchannel17. They ‘acoustical tweezers’ was first coined to describe the linear transla- are capable of a variety of applications, including trapping, focusing, tion of latex spheres and frog eggs that were trapped in an acoustic and sorting, but their controllability is rather poor, and their ability field6. Since then, a substantial number of acoustic-tweezer configu- to manipulate nanoparticles is limited. rations have been developed for applications in science and engi- Acoustic tweezers are a versatile tool that can address many of neering. Many of these acoustic-tweezer devices are modeled after the limitations of other particle-manipulation techniques. Because their predecessor, optical tweezers. Optical tweezers, invented in acoustic waves with frequencies in the kilohertz-to-megahertz 1986 (ref. 7), were quickly adopted as an invaluable tool in biology, range can be easily generated19–21, acoustic tweezers can directly chemistry, and physics, and have been used to trap viruses, bacte- manipulate particles across a length scale spanning more than five ria, and cells8,9. Despite being a powerful tool for force spectroscopy orders of magnitude (10−7 to 10−2 m). In addition, the applied acous- and biomolecular manipulation, traditional optical tweezers require tic power (10−2–10 W/cm2) and frequencies (1 kHz to 500 MHz) complex optics, including high-powered lasers and high-numerical- are similar to those used in ultrasonic imaging (2–18 MHz, less aperture objectives, and they are potentially damaging to biological than 1 W/cm2)22, which has been safely used in diagnostic applica- samples10,11. To improve the accessibility and versatility of contact- tions21,23. Studies on the biocompatibility of acoustic tweezers have free particle-manipulation technology, alternatives to optical twee- shown that their operating parameters can be optimized to avoid zers have since been developed. damage in cells24,25 and small-animal models26. For example, red Additional platforms for contactless particle manipulation rely blood cells placed in an acoustic-tweezer device for up to 30 min on different mechanisms, including magnetic12, optoelectronic13, show no changes in cell viability25, and zebrafish embryos placed plasmonic14, electrokinetic15,16, and hydrodynamic forces17 (over- in an acoustic-tweezer device for the same duration do not exhibit view of the operating parameters and system requirements for these developmental impairments or changes in mortality rates26. The techniques in Table 1). Magnetic and optical tweezers provide the versatility and biocompatibility of acoustic tweezers should allow highest degree of spatial resolution; however, manipulating particles current challenges in biology and biomedicine to be addressed, such smaller than 100 nm is challenging with either technique. Plasmonic as the isolation and detection of circulating biomarkers for cancer tweezers are a variation of optical tweezers that make use of locally diagnostics27. These biomarkers range in size from nanometer-sized enhanced electromagnetic fields on nanostructured substrates. extracellular vesicles28 to micrometer-sized circulating tumor cells Plasmonic tweezers require lower laser power and are capable of (CTCs)29. Moreover, acoustic tweezers are capable of isolating both trapping nanometer-sized particles, but the large localized inten- extracellular vesicles30 and CTCs31, capabilities valuable for oncol- sities that help to trap particles can also lead to substantial heat- ogy laboratories. For cell-to-cell and cell-to-environment interac- ing of the surrounding fluid18. As a result, thermal management of tion studies, precise control over the physical position of cells, while these devices is necessary to prevent sample heating and convective preserving normal physiology, is necessary. Acoustic tweezers can flows. Electrokinetic tweezers, which use both electrophoretic and form flexible 2D32 and 3D33 cell arrays and have been used in inter- dielectrophoretic forces, apply an electric field to trap and manipu- cellular communication studies34. Furthermore, noninvasive tools late particles across the nanometer–to-millimeter size range15,16. for manipulating organisms are required to investigate internal 1Department of Mechanical Engineering and Materials Science, Duke University, Durham, NC, USA. 2Department of Engineering Science and Mechanics, Pennsylvania State University, University Park, PA, USA. *e-mail: [email protected] NatURE METHODS | VOL 15 | DECEMBER 2018 | 1021–1028 | www.nature.com/naturemethods 1021 REVIEW ARTICLE NATURE METHODS Table 1 | Summary of different particle-manipulation platforms Technique Size range Input powera Spatial resolution Labeling required Additional system requirements (W/cm2) Acoustic tweezers 100 nm–10 10−2–10 1–10 µ m No Acoustic source mm Optical tweezers7–9 100 nm–1 106–107 0.1–1 nm Required for smaller High-powered laser, high-numerical- mm particles aperture lens Magnetic tweezers12 1 µ m–10 µ m 1–10 tesla 1–10 nm Yes Permanent magnet, superparamagnetic beads Optoelectronic tweezers13 100 nm–10 10−2–10 1–10 µ m No Photoconductive substrate, µ m low-conductivity media Plasmonic tweezers14 10 nm–1 µ m 102–104 10–100 nm No Plasmonic substrate, heat sink Electrokinetic tweezers15,16 1 nm–1 mm 104–107 V/m 0.1–1 µ m Yes Prepatterned electrodes, Low-conductivity media Hydrodynamic tweezers17 100 nm–1 N/A 1–10 µ m No Multiple pressure regulators, mm flow-control algorithm a The minimum field strength is reported for magnetic and electrokinetic tweezers. processes, such as the neuronal activity in Caenorhabditis elegans35. surface39. 1D and 2D interference patterns can be achieved by using Acoustic tweezers have been used to manipulate and rotate C. ele- sets of two and four IDTs, respectively39,40 (Fig. 1b). Suspended par- gans36 as well as larger organisms, such as zebrafish embryos26, with ticles in a standing SAW field move to pressure nodes or antinodes no adverse effects. according to their physical properties41. In addition to 2D in-plane Although acoustic tweezers have been used in various biological manipulation, standing SAWs are used to achieve 3D manipulation studies, the versatility of acoustic tweezers has proven to be a double- by exploiting the modulation of acoustic parameters (for example, edged sword. Currently, many different acoustic-tweezer platforms phase shifts and amplitude modulation), thus enabling the trapping are available, each with advantages and shortcomings; however, for position to be changed in real time33. Owing to their compact size, researchers who are not technical experts in the field, identifying the SAW-based tweezers can be conveniently integrated with microflu- acoustic-tweezer technology best suited for a particular application idic systems enabling versatile lab-on-a-chip tools40. is difficult. For example, for manipulating nanometer-sized objects, Standing-wave tweezers are mainly used for separating and pat- should an acoustic-tweezer device based on surface acoustic waves terning different types of particles and cells. Whereas BAW-based (SAWs) or bulk acoustic waves (BAWs) be used? Which acoustic- standing-wave tweezers have the advantage of handling higher vol- tweezer platform is best for handling large volumes of biofluids?
Recommended publications
  • Three-Dimensional Manipulation of Single Cells Using Surface Acoustic Waves
    Three-dimensional manipulation of single cells using surface acoustic waves Feng Guoa,1, Zhangming Maoa,1, Yuchao Chena, Zhiwei Xieb, James P. Lataa, Peng Lia, Liqiang Rena, Jiayang Liua, Jian Yangb, Ming Daoc,2, Subra Sureshd,e,f,2, and Tony Jun Huanga,b,2 aDepartment of Engineering Science and Mechanics, The Pennsylvania State University, University Park, PA 16802; bDepartment of Biomedical Engineering, The Pennsylvania State University, University Park, PA 16802; cDepartment of Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139; dDepartment of Biomedical Engineering, Carnegie Mellon University, Pittsburgh, PA 15213; eComputational Biology Department, Carnegie Mellon University, Pittsburgh, PA 15213; and fDepartment of Materials Science and Engineering, Carnegie Mellon University, Pittsburgh, PA 15213 Contributed by Subra Suresh, December 17, 2015 (sent for review November 23, 2015; reviewed by Ares Rosakis and M. Taher A. Saif) The ability of surface acoustic waves to trap and manipulate involving sound waves have a power intensity that is ∼10 million micrometer-scale particles and biological cells has led to many times lower than that of optical tweezers. Therefore, acoustic applications involving “acoustic tweezers” in biology, chemistry, tweezers have minimal impact on cell viability and function. engineering, and medicine. Here, we present 3D acoustic twee- Moreover, acoustic tweezers operate at a power intensity and zers, which use surface acoustic waves to create 3D trapping frequency similar to the widely used medical ultrasound method nodes for the capture and manipulation of microparticles and cells that is well known as a safe technique for sensitive clinical ap- along three mutually orthogonal axes. In this method, we use plications such as imaging of a fetus in the mother’s womb.
    [Show full text]
  • Acoustical and Optical Radiation Pressures and the Development of Single Beam Acoustical Tweezers Jean-Louis Thomas, Régis Marchiano, Diego Baresch
    Acoustical and optical radiation pressures and the development of single beam acoustical tweezers Jean-Louis Thomas, Régis Marchiano, Diego Baresch To cite this version: Jean-Louis Thomas, Régis Marchiano, Diego Baresch. Acoustical and optical radiation pressures and the development of single beam acoustical tweezers. Journal of Quantitative Spectroscopy and Radiative Transfer, Elsevier, 2017, 195, pp.55-65. 10.1016/j.jqsrt.2017.01.012. hal-01438774 HAL Id: hal-01438774 https://hal.archives-ouvertes.fr/hal-01438774 Submitted on 18 Jan 2017 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Acoustical and optical radiation pressures and the development of single beam acoustical tweezers Jean-Louis Thomasa,∗, R´egisMarchianob, Diego Barescha,b aSorbonne Universit´es,UPMC Univ Paris 06, CNRS UMR 7588, Institut des NanoSciences de Paris, 4 place Jussieu, Paris, France bSorbonne Universit´es,UPMC Univ Paris 06, CNRS UMR 7190, Institut Jean le Rond d'Alembert, 4 place Jussieu, Paris, France Abstract Studies on radiation pressure in acoustics and optics have enriched one an- other and have a long common history. Acoustic radiation pressure is used for metrology, levitation, particle trapping and actuation. However, the dexter- ity and selectivity of single-beam optical tweezers are still to be matched with acoustical devices.
    [Show full text]
  • 3D Acoustic Tweezers-Based Bio-Fabrication
    The Pennsylvania State University The Graduate School College of Engineering 3D ACOUSTIC TWEEZERS-BASED BIO-FABRICATION A Thesis in Engineering Science and Mechanics by Kejie Chen © 2016 Kejie Chen Submitted in Partial Fulfillment of the Requirements for the degree of Master of Science May 2016 ii The thesis of Kejie Chen was reviewed and approved* by the following: Tony J. Huang Professor of Engineering Science and Mechanics Thesis Advisor Joseph L. Rose Paul Morrow Professor of Engineering Science and Mechanics Bernhard R. Tittmann Schell Professor of Engineering Science and Mechanics Judith A. Todd Professor of Engineering Science and Mechanics P.B. Breneman Department Head *Signatures are on file in The Graduate School. iii ABSTRACT The ability to create 3D in vivo-like tissue models raises new possibility in studying complex physiology and pathophysiological process in vitro, and enabling the development of new therapy strategies for underlying diseases. Recent observations showed that gene expression in 3D cell assembles was much closer to clinical expression profile than those in 2D cases, which generated hope in manufacturing artificial 3D tissue for therapy test platforms with a better prediction of clinical effects. In this work, we developed a 3D acoustic tweezers-based method for rapid fabrication of multicellular cell spheroids and spheroid-based co-culture models. Our 3D acoustic tweezers method used drag force from acoustic microstreaming to levitate cells in vertical direction, and used acoustic radiation force from Gov’kov potential field to aggregate cells in horizontal plane. After optimizing the device geometry and input power, we demonstrated the rapid and high- throughput characteristics of our method by continuously fabricating more than 150 size- controllable spheroids and transferring them to Petri dishes every 30 minutes.
    [Show full text]
  • Axial Acoustic Radiation Force on Rigid Oblate and Prolate Spheroids in Bessel Vortex Beams of Progressive, Standing and Quasi-Standing Waves
    Axial acoustic radiation force on rigid oblate and prolate spheroids in Bessel vortex beams of progressive, standing and quasi-standing waves F.G. Mitri A B S T R A C T The analysis using the partial-wave series expansion (PWSE) method in spherical coordinates is extended to evaluate the acoustic radiation force experienced by rigid oblate and prolate spheroids centered on the axis of wave propagation of high-order Bessel vortex beams composed of progressive, standing and quasi-standing waves, respectively. A coupled system of linear equations is derived after applying the Neumann boundary condition for an immovable surface in a non-viscous fluid, and solved numerically by matrix inversion after performing a single numerical integration procedure. The system of linear equations depends on the partial-wave index n and the order of the Bessel vortex beam m using truncated but converging PWSEs in the least-squares sense. Numerical results for the radiation force function, which is the radiation force per unit energy density and unit cross-sectional surface, are computed with particular emphasis on the amplitude ratio describing the transition from the progressive to the pure standing waves cases, the aspect ratio (i.e., the ratio of the major axis over the minor axis of the spheroid), the half-cone angle and order of the Bessel vortex beam, as well as the dimensionless size parameter. A generalized expression for the radiation force function is derived for cases encompassing the progressive, standing and quasi-standing waves of Bessel vortex beams. This expression can be reduced to other types of beams/waves such as the zeroth-order Bessel non-vortex beam or the infinite plane wave case by appropriate selection of the beam parameters.
    [Show full text]
  • Generation of Acoustic Self-Bending and Bottle Beams by Phase Engineering
    ARTICLE Received 14 Oct 2013 | Accepted 5 Jun 2014 | Published 3 Jul 2014 DOI: 10.1038/ncomms5316 Generation of acoustic self-bending and bottle beams by phase engineering Peng Zhang1,*, Tongcang Li1,*, Jie Zhu1,*, Xuefeng Zhu1, Sui Yang1,2, Yuan Wang1, Xiaobo Yin1,2 & Xiang Zhang1,2 Directing acoustic waves along curved paths is critical for applications such as ultrasound imaging, surgery and acoustic cloaking. Metamaterials can direct waves by spatially varying the material properties through which the wave propagates. However, this approach is not always feasible, particularly for acoustic applications. Here we demonstrate the generation of acoustic bottle beams in homogeneous space without using metamaterials. Instead, the sound energy flows through a three-dimensional curved shell in air leaving a close-to-zero pressure region in the middle, exhibiting the capability of circumventing obstacles. By designing the initial phase, we develop a general recipe for creating self-bending wave packets, which can set acoustic beams propagating along arbitrary prescribed convex trajectories. The measured acoustic pulling force experienced by a rigid ball placed inside such a beam confirms the pressure field of the bottle. The demonstrated acoustic bottle and self-bending beams have potential applications in medical ultrasound imaging, therapeutic ultrasound, as well as acoustic levitations and isolations. 1 National Science Foundation Nanoscale Science and Engineering Center, 3112 Etcheverry Hall, University of California, Berkeley, California 94720, USA. 2 Materials Sciences Division, Lawrence Berkeley National Laboratory, 1 Cyclotron Road, Berkeley, California 94720, USA. * These authors contributed equally to this work. Correspondence and requests for materials should be addressed to X.Z.
    [Show full text]
  • The Pennsylvania State University
    The Pennsylvania State University The Graduate School College of Engineering ACOUSTIC TWEEZERS: MANIPULATING CELLS IN MICROFLUIDICS A Dissertation in Engineering Science and Mechanics by Xiaoyun Ding 2013 Xiaoyun Ding Submitted in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy August 2013 The dissertation of Xiaoyun Ding was reviewed and approved* by the following: Tony Jun Huang Professor of Engineering Science and Mechanics Dissertation Advisor Chair of Committee Bernhard R. Tittmann Schell Professor of Engineering Science and Mechanics Corina S. Drapaca Assistant Professor of Engineering Science and Mechanics Qiming Zhang Distinguished Professor of Electrical Engineering Judith A. Todd Professor P. B. Breneman Head of the Department of Engineering Science and Mechanics *Signatures are on file in the Graduate School iii ABSTRACT Techniques that can noninvasively and dexterously manipulate cells and other bioparticles (such as organisms, DNAs, proteins, and viruses) in a compact system are invaluable for many applications in life sciences and medicine. Historically, optical tweezers have been the primary tool used in the scientific community for bioparticle manipulation. Despite the remarkable capability and success, optical tweezers have notable limitations, such as complex and bulky instrumentation, high equipment costs, and potential damage to cells. To overcome the limitations of optical tweezers and other particle manipulation methods, we have developed a series of acoustic-based, on-chip devices called acoustic tweezers that can manipulate cells and other bioparticles using sound waves. The power density required by our acoustic device is 10,000,000 times less than that of optical tweezers, which renders the technique noninvasive and amenable to miniaturization.
    [Show full text]
  • Three Dimensional Acoustic Tweezers with Vortex Streaming ✉ Junfei Li 1,3, Alexandru Crivoi2,3, Xiuyuan Peng1, Lu Shen 2, Yunjiao Pu1, Zheng Fan 2 & ✉ Steven A
    ARTICLE https://doi.org/10.1038/s42005-021-00617-0 OPEN Three dimensional acoustic tweezers with vortex streaming ✉ Junfei Li 1,3, Alexandru Crivoi2,3, Xiuyuan Peng1, Lu Shen 2, Yunjiao Pu1, Zheng Fan 2 & ✉ Steven A. Cummer1 Acoustic tweezers use ultrasound for contact-free manipulation of particles from millimeter to sub-micrometer scale. Particle trapping is usually associated with either radiation forces or acoustic streaming fields. Acoustic tweezers based on single-beam focused acoustic vortices have attracted considerable attention due to their selective trapping capability, but have proven difficult to use for three-dimensional (3D) trapping without a complex transducer 1234567890():,; array and significant constraints on the trapped particle properties. Here we demonstrate a 3D acoustic tweezer in fluids that uses a single transducer and combines the radiation force for trapping in two dimensions with the streaming force to provide levitation in the third dimension. The idea is demonstrated in both simulation and experiments operating at 500 kHz, and the achieved levitation force reaches three orders of magnitude larger than for previous 3D trapping. This hybrid acoustic tweezer that integrates acoustic streaming adds an additional twist to the approach and expands the range of particles that can be manipulated. 1 Department of Electrical and Computer Engineering, Duke University, Durham, NC, USA. 2 School of Mechanical and Aerospace Engineering, Nanyang ✉ Technological University, Singapore, Singapore. 3These authors contributed equally: Junfei Li, Alexandru Crivoi. email: [email protected]; [email protected]. edu COMMUNICATIONS PHYSICS | (2021) 4:113 | https://doi.org/10.1038/s42005-021-00617-0 | www.nature.com/commsphys 1 ARTICLE COMMUNICATIONS PHYSICS | https://doi.org/10.1038/s42005-021-00617-0 recise and contact-free manipulation of physical and bio- Here we propose a hybrid 3D single beam acoustic tweezer by logical objects is highly desirable in a wide range of fields combining the radiation force and acoustic streaming.
    [Show full text]
  • Acoustic Radiation Force on a Rigid Cylinder in a Focused Gaussian Beam. Journal of Sound and Vibration, 332(9), 2338-2349
    Azarpeyvand, M., & Azarpeyvand, M. (2013). Acoustic radiation force on a rigid cylinder in a focused Gaussian beam. Journal of Sound and Vibration, 332(9), 2338-2349. https://doi.org/10.1016/j.jsv.2012.11.002 Peer reviewed version Link to published version (if available): 10.1016/j.jsv.2012.11.002 Link to publication record in Explore Bristol Research PDF-document University of Bristol - Explore Bristol Research General rights This document is made available in accordance with publisher policies. Please cite only the published version using the reference above. Full terms of use are available: http://www.bristol.ac.uk/red/research-policy/pure/user-guides/ebr-terms/ Acoustic radiation force on a rigid cylinder in a focused Gaussian beam Mahdi Azarpeyvand1 Engineering department, University of Cambridge Trumpington street, Cambridge CB2 1PZ, UK. Mohammad Azarpeyvand Department of materials engineering, Isfahan University of Technology, Isfahan, Iran. ABSTRACT- The acoustic radiation force resulting from a 2D focused Gaussian beam incident on cylindrical objects in an inviscid fluid is investigated analytically. The incident and the reflected sound fields are expressed in terms of cylindrical wave functions and a weighting parameter, describing the beam shape and its location relative to the particle. Our main interest here is to study the possibility of using Gaussian beams for axial and lateral handling of rigid cylindrical particles by exerting attractive forces, towards the beam source and axis, respectively. Results have been presented for Gaussian beams with different waist sizes and wavelengths and it has been shown that the interaction of a focused Gaussian beam with a rigid cylinder can result in attractive axial and lateral forces under specific operational conditions.
    [Show full text]
  • Tornado-Inspired Acoustic Vortex Tweezer for Trapping and Manipulating Microbubbles
    Tornado-inspired acoustic vortex tweezer for trapping and manipulating microbubbles Wei-Chen Loa, Ching-Hsiang Fanb,c, Yi-Ju Hoa, Chia-Wei Lina, and Chih-Kuang Yeha,d,1 aDepartment of Biomedical Engineering and Environmental Sciences, National Tsing Hua University, Hsinchu, 30013 Taiwan; bDepartment of Biomedical Engineering, National Cheng Kung University, Tainan, 701 Taiwan; cMedical Device Innovation Center, National Cheng Kung University, Tainan, 701 Taiwan; and dInstitute of Nuclear Engineering and Sciences, National Tsing Hua University, Hsinchu, 30013 Taiwan Edited by Robert Langer, Massachusetts Institute of Technology, Cambridge, MA, and approved December 9, 2020 (received for review November 17, 2020) Spatially concentrating and manipulating biotherapeutic agents tweezers are standing-wave tweezers (17–19), single-beam within the circulatory system is a longstanding challenge in acoustic tweezers (20–22), and acoustic-streaming tweezers medical applications due to the high velocity of blood flow, which (23–25). Standing-wave tweezers spatially form periodic pressure greatly limits drug leakage and retention of the drug in the targeted nodes to produce acoustic radiation forces that can be used to region. To circumvent the disadvantages of current methods for control the positions of particles (19). Unfortunately, a complex systemic drug delivery, we propose tornado-inspired acoustic vortex setup is needed because the trapped objects need to be located tweezer (AVT) that generates net forces for noninvasive intravascu- between one or more pairs of ultrasound transducers. Single- lar trapping of lipid-shelled gaseous microbubbles (MBs). MBs are beam acoustic tweezers can produce a trapping effect to ma- used in a diverse range of medical applications, including as ultra- nipulate particles and cells under the conditions of Mie regime in sound contrast agents, for permeabilizing vessels, and as drug/gene a single-transducer setup (21, 26).
    [Show full text]
  • Comparing Acoustic and Optical Forces for Biomedical Research
    Comparing acoustic and optical forces for biomedical research Kishan Dholakia1;2;y, Bruce W. Drinkwater3;y and Monika Ritsch-Marte4;y 1SUPA, School of Physics and Astronomy, University of St Andrews, UK. 2 Department of Physics, College of Science, Yonsei University, Seoul, South Korea. 3 Faculty of Engineering, University of Bristol, Bristol, UK. 4 Institute of Biomedical Physics, Medical University of Innsbruck, Innsbruck, Austria. ye-mail: [email protected]; [email protected]; [email protected] 1 Abstract The application of acoustic and optical waves to exert non-contact forces on microscopic and mesoscopic objects has grown considerably in importance in the past few decades. Different phys- ical principles govern the acoustic and optical forces, leading to diverse biomedical applications. Biocompatibility is crucial, and useful optical and acoustic forces can be applied in devices that maintain local heating to acceptable levels. Current acoustic and optical devices work on com- plementary length scales, with both modalities having useful capabilities at the scale of the cell. Optical devices also cover sub-cellular scales and acoustic devices super-cellular scales. This com- plementarity has led to the emergence of multi-mode manipulation, often with integrated imaging. In this Technical Review, we provide an overview of optical and acoustic forces, before comparing and contrasting the use of these modalities, or combinations thereof, in terms of sample manipula- tion and suitability for biomedical studies. We conclude with our perspective on the applications in which we expect to see notable developments in the near future. KEY POINTS • Acoustic and optical forces are governed by different physical principles, but both enable the application of non-contact forces to biomedically important objects such as cells and microorganisms.
    [Show full text]
  • Acoustic Radiation Force Based Ultrasound Elasticity Imaging for Biomedical Applications
    sensors Review Acoustic Radiation Force Based Ultrasound Elasticity Imaging for Biomedical Applications Lulu Wang 1,2 ID 1 Department of Biomedical Engineering, School of Instrument Science and Opto-electronics Engineering, Hefei University of Technology, Hefei 230009, China; [email protected] 2 Institute of Biomedical Technologies, Auckland University of Technology, Auckland 1142, New Zealand Received: 13 May 2018; Accepted: 11 July 2018; Published: 12 July 2018 Abstract: Pathological changes in biological tissue are related to the changes in mechanical properties of biological tissue. Conventional medical screening tools such as ultrasound, magnetic resonance imaging or computed tomography have failed to produce the elastic properties of biological tissues directly. Ultrasound elasticity imaging (UEI) has been proposed as a promising imaging tool to map the elastic parameters of soft tissues for the clinical diagnosis of various diseases include prostate, liver, breast, and thyroid gland. Existing UEI-based approaches can be classified into three groups: internal physiologic excitation, external excitation, and acoustic radiation force (ARF) excitation methods. Among these methods, ARF has become one of the most popular techniques for the clinical diagnosis and treatment of disease. This paper provides comprehensive information on the recently developed ARF-based UEI techniques and instruments for biomedical applications. The mechanical properties of soft tissue, ARF and displacement estimation methods, working principle and implementation instruments for each ARF-based UEI method are discussed. Keywords: ultrasound elasticity imaging; acoustic radiation force; ultrasonic imaging; tissue stiffness; mechanical properties 1. Introduction Changes in mechanical properties of tissues also alter pathological state [1]. Previous studies have demonstrated that fibroadenoma tissues and carcinomas are much harder than normal tissues [2].
    [Show full text]
  • NCRP Composite Glossary
    NCRP Composite Glossary [updated July 2011] A absolute risk: Expression of excess risk due to exposure as the arithmetic difference between the risk among those exposed and that obtained in the absence of exposure. The resultant risk coefficient is normalized to a population base of 10,000 people and is expressed as the number of excess cases per 10,000 persons per gray per year at risk [i.e., (104 PY Gy)–1]. Absolute risk coefficients project can be modeled as a function of time since exposure (or attained age). [159] absorbed dose (D): The energy imparted to matter by ionizing radiation per unit mass of irradiated material at the point of interest. The SI unit is J kg–1 with the special name gray (Gy). The special unit previously used was rad. 1 Gy = 100 rad (see mean absorbed dose). [163] absorbed dose ( D): The energy imparted to matter by ionizing radiation per unit of irradiated material at the point of interest. Absorbed dose is the quotient of d∈ by dm, where d∈ is the mean energy imparted by ionizing radiation to matter in a volume element and dm is the mass of matter in that volume element: D = d∈/dm. The SI unit of absorbed dose is joule per kilogram (J kg –1), and its special name is gray (Gy). The special unit previously used was rad. 1 Gy = 100 rad (see mean absorbed dose). [158] absorbed dose (D): Quotient of d∈ by dm, where d∈ is the mean energy imparted by ionizing radiation to matter in a volume element and dm is the mass of matter in that volume element: D = d∈/dm.
    [Show full text]