publication year: 2017icu2017/20171205... · 12/5/2017 · suk wang yoon, ph.d. president,...

Publication Year: 2017

Copyright © 2017 ICU Honolulu and Acoustical Society of Korea

2017 ICU Honolulu, University of Hawaii at Manoa, and the Acoustical Society ofKorea shall not be liable for personal injury or damage to property or damage caused by the use, manipulation, negligence or other methods of materials, products, guidelines or ideas contained herein.

ISBN 979-11-5610-347-9 (95500)

Aloha! Greetings from Hawai’i!We are pleased to invite you to the International Congress on Ultrasonics (ICU), which will be held in Honolulu Hawaii on December 18 - 20, 2017. This Congress brings together multidisciplinary subjects on all aspects of Ultrasonics and will lead us into the future of “Eco-sound.”

The allure of Hawai`i is well known. However, few understand how deeply Aloha can energize our lives and renew our spirit. Come and join in the discussion on what’s being accomplished in our respective specialties. Relax your body but reinvigorate your mind as we all learn what role we can play in shaping our society.

Our Congress success will rely on how well the Aloha spirit will make an extraordinary experience for all who attend.

We welcome you in Waikiki, a paradise of “Green Sound.”

Suk Wang YoonPresidentInternational Congress on Ultrasonics (ICU) /General Chair2017 ICU Honolulu

About the International Congress on UltrasonicsThe International Congress on Ultrasonics (ICU) was constituted in 2005 as the result of the merger of two existing international Congresses: The World Congress on Ultrasonics (WCU) and Ultrasonics International (UI). The ICU is currently an international affiliated member of the International Commission for Acoustics (ICA), the parent organization of many national and regional acoustical societies.

The history of the ICU, as the merger of the two previous Congresses on ultrasound, is relatively short. However, the history of the two Congresses integrating ICU, is much longer: the UI started in the 1960s and the WCU started in 1993. UI, the first international congress devoted to ultrasound, was linked to the journal “Ultrasonics” created by the group Butterworth-Heinemann in England and later acquired by the well-known publisher Elsevier. The WCU was created in 1993, as an independent world congress, by a group of ultrasound scientists from several countries. The third WCU was held in Lyngby, Denmark jointly with the UI. This meeting was a first attempt towards a merger of WCU and UI. Finally, the last WCU meeting, again jointly with UI, was held in Beijing, China in 2005. This meeting marked the starting point of the definitive merger of both Congresses into the present ICU.

In fact, the first 2007 ICU Vienna was held at the Vienna University of Technology, Austria, the second 2009 ICU Santiago in Chile, the third 2011 ICU in Gdansk, Poland, and the fourth 2013 ICU was held in Singapore. In 2015 the fifth ICU was held in Metz, France. The sixth ICU will be held in Honolulu, Hawaii, U.S.A for December 18 –20, 2017.

About the Hosting Organizations

The Acoustical Society of Korea

Since the Acoustical Society of Korea (ASK) was formed in 1981, it has been healthily grown in membership and in stature. The present ASK membership is over 3,000 members in academia and industries, who work as leaders in Acoustics in the world as well as in Korea.

Important roles of ASK have been to publish the Journal of Acoustical Society of Korea (JASK) bimonthly, and to hold two annual meetings in May and November. The JASK is accredited as a Korea Citation Index Journal by Korea National Research Foundation. Papers are published in the 12 technical categories: Acoustic Signal Processing, Acoustic Communication, Electroacoustics, Psychological and Music Acoustics, New Media Research, Underwater Acoustics, Physical Acoustics, Bioacoustics, Ultrasonics, Architectural Acoustics, Structural Acoustics, and Linguistics.

The ASK annually holds underwater acoustics conference, acoustic signal processing conference, and architectural sound workshops, and also grants hearing-aid expert certification system. The Society recognizes distinguished achievement in acoustics by a series of awards: Emile Grand Award, Emile Technical Award, Best Paper Award, B&K Student Award, and ASK President Citation.

University of Hawaii at Manoa

Nestled in idyllic Mānoa Valley in Honolulu, Hawai‘i, the University of Hawai‘i at Mānoa (UHM) is a leading center for higher learning throughout the Pacific Rim.

UHM is one of the 115 “R1: Research Universities”, considered the top tier in the nation, and one of a handful of land-, sea- and space-grant institutions. It is a global leader in earth and environmental sciences, consistently ranked among the top 15 universities internationally, ahead of some of the world’s most prestigious schools. Our researchers provide world class expertise to local leaders on important issues including sustainability, climate, food systems, and Hawai‘i’s unique health issues.

Currently, the University has an enrollment of over 18,000, and more specifically, the College of Engineering (CoE) supports more than 1500 active students. Since classes began over a century ago in 1908, engineering has played an integral role in the institution’s curriculum. It remains so today. The College offers BS, MS, and PhD degrees in three major areas of intensive study including Civil Engineering, Electrical Engineering, and Mechanical Engineering. It also offers a BS in Computer Engineering.

As College’s vision states, “The College of Engineering is dedicated to world-class education and research, producing the entrepreneurial and innovative human and intellectual capital required to be competitive in an ever-increasing technological and global society. Through our graduates and our research, we provide people and discoveries to transform lives and to support vibrant, knowledge-based economies. We are inspired by the principles of sustainability and resilience, flavored by our unique island environment.”, the UHM CoE will maintain its unique identity!

2017 ICU Honolulu Committees

Executive Committee

Suk Wang Yoon, Ph.D.President, International Congress on Ultrasonics (ICU)General Chair, 2017 ICU HonoluluProfessor of PhysicsSungKyunKwan UniversityRepublic of Korea

Song K. Choi, Ph.D.Secretary General, 2017 ICU HonoluluAssistant Dean, College of EngineeringUniversity of Hawaii, ManoaU.S.A.

Kendall H. KidoCoordinator, 2017 ICU HonoluluU.S.A.

Hwi Suk KangDepartment of PhysicsSungKyunKwan UniversityRepublic of Korea

Wan-Gu KimDepartment of PhysicsSungKyunKwan UniversityRepublic of Korea

Changgun Song Department of PhysicsSungKyunKwan UniversityRepublic of Korea

Technical CommitteeCo-ChairThomas J. Matula, Ph.D.DirectorCenter for Industrial and Medical Ultrasound (CIMU)Applied Physics LaboratoryUniversity of WashingtonSeattle, WA 98105, U.S.A.

Representative of EuropeBadreddine Assouar, Ph.D.Research ScientistInstitut Jean LamourUniversité de LorraineVandoeuvre-lès-Nancy, France

Hideyuki Nomura, Ph.D.Associate ProfessorDepartment of Communication Engineering and Informatics University of Electro-CommunicationsTokyo, Japan

Co-ChairYoshiaki Watanabe, Ph.D.Professor, Deptartment of Biomedical InformationFaculty of Life and Medical SciencesDoshisha UniversityKyoto, Japan

Kang Il Lee, Ph.D.ProfessorDepartment of PhysicsKangwon National UniversityChuncheon, Republic of Korea

Jin Ho Chang, Ph.D.Associate Professor,Department of Electric Engineering / Biomedical Engineering,Sogang UniversitySeoul, Republic of Korea

International Organizing CommitteeLeonard Bond, U.S.A.Younho Cho, KoreaLarry Crum, U.S.A.Marc Dechamps, FranceNico Declercq, BelgiumJürg Dual, SwitzerlandArthur G. Every, South AfricaLuis Gaete-Garreton, ChileVitalyi Gusev, FranceSigrun Hirsekorn, GermanyHiroshi Kanai, Japan

Pascal Laugier, FrancePeter A. Lewin, U.S.A.Bogumil Linde, PolandKentaro Nakamura, JapanMichiel Postema, NorwayStefan Radel, AustriaEnrique Riera, SpainWolfgang Sachse, U.S.A.Xiuming Wang, ChinaJens E. Wilhjelm, Denmark

Session Organizers and Chairs

I. Akiyama, JapanB. Assouar, FranceJ. Allen, U.S.A.K. Baik, KoreaF. Balle, GermanyN. Boechler, U.S.A.L. J. Bond, U.S.A.J. H. Chang, KoreaP. Chitnis, U.S.A.Y. Cho, KoreaJ. W. Choi, KoreaJ. Christensen, SpainC. C. Coussios, UKL. A. Crum, U.S.A.N. F. Declercq, FranceC. L. De Korte, NetherlandsB. Djafari-Rouhani, FranceA. Every, South AfricaA. Feeney, UKL. Gaete-Garreton, ChileM. R. Haberman, U.S.A.C.-C Huang, TaiwanH. Hasegawa, JapanB. Helfield, CanadaH. Hu, ChinaN. Hu, ChinaJ. Y. Hwang, KoreaY. Y. Kim, KoreaK. Kim, U.S.A.V. A. Khokhlova, RussiaV. Laude, France

L. Le, U.S.A.K. I. Lee, KoreaB. Liang, ChinaT. J. Matula, U.S.A.O. Matsuda, JapanA. Maznev, U.S.A.A. Merkel, SpainF. Muenzel, GermanyH. Nagata, JapanH. Nomura, JapanK. Nakamura, JapanY. Ohara, JapanY. Pennec, FranceI. Park, KoreaZ. Su, Hong KongO. A. Sapozhnikov, RussiaS.-I. Sakamoto, JapanK. M. Tant, UKV. Tournat, FranceS.-I. Umemura, JapanM. Versluis, NetherlandsJ. Wang, ChinaX. Wang, ChinaY.-S. Wang, ChinaO. B. Wright, JapanY. Watanabe, JapanK. A. Wear, U.S.A.X. Xie, ChinaA. C. Yu, CanadaC. Yang, U.S.A.X. Zou, China

AcknowledgementsWe would like express our special thanks and gratitude to our session organizers, plenary lecturers and invited speakers as well as to the conference participants whose continued support has allowed us the opportunity to hold the International Congress on Ultrasonics here in Honolulu, Hawaii, U.S.A.

The online service DC/ConfOrg for 2017 ICU Honolulu has been made possible with the help of Didier Cassereau. We appreciate his dedicated service.

Plenary Lectures

1. “The Best Short Range Active Sonar System on this Planet:the Ultrasonic Sonar of Dolphins”Plenary Speaker: W. AuEmeritus Research ProfessorHawai`i Institute of Marine BiologyUniversity of Hawai`i at ManoaU.S.A.

2. “Optimal Sound Absorbing Structures”Plenary Speaker: P. ShengDr William M W Mong Chair Professor of NanoscienceDepartment of PhysicsHong Kong University of Science and TechnologyChina

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Abstract book 2017 ICU Honolulu 1

Table of ContentsAuthor speaker is underlined.

Invited paper is marked ∗.

Monday 18 December 2017

Plenary Lecture 1Room: 306

Time: 10:00

Chair: S. W. Yoon

10:00 The best sonar system on this planet: the ultrasonic sonar of dolphins∗ 23W. Au

Acoustic FluidicsRoom: 304A

Time: 8:00

Chair: V. A. Khokhlova

8:00 Spreading of Water Drop On a Vibrating Surface 23N. Candia Muñoz, L. Gaete-Garretón, Y. Vargas-Hernández and J. Meneses-Dı́az

8:15 Measurement and Simulation of Acoustic Radiation Force from Focused Ultra-sound Beam Acting on a Spherical Scatterer in Water

24

M. M. Karzova, A. V. Nikolaeva, S. A. Tsysar, V. A. Khokhlova and O. A. Sapozhnikov

8:30 Elucidating the Mechanism of Paracetamol Sonocrystallization for Product Pu-rity Enhancement

24

C. Forbes, T. T. Nguyen, R. L. Leary and C. J. Price

8:45 Recent Advances and Opportunities of Mechanical Metamaterials 25E. G. Karpov and L. A. Danso

Bubbles and Cavitation 1Room: 308B

Time: 8:00

Chair: T. J. Matula, M. Versluis

8:00 Lipid Intermolecular Forces and Microbubble Resonance∗ 25M. Borden

8:25 High-Precision Acoustic Measurements of the Nonlinear Dilatational Elasticityof Phospholipid-Coated Monodisperse Microbubbles∗

25

T. Segers, E. Gaud, M. Versluis and P. Frinking

8:50 Propagation of ultrasound through a microbubble population: Effect of ultra-sound pressure, frequency, microbubble concentration and lipid shell properties∗

26

A. Jafarisojahrood, Q. Li, H. Haghi, R. Karshafian, T. M. Porter and M. C. Kolios

Optomechanical Structures and Opto-acousticsRoom: 307B

Time: 8:00

Chair: J. Wang

8:00 Proposal for optical beam-steering with optomechanical antennas on a siliconchip∗

26

R. Van Laer, C. J. Sarabalis and A. H. Safavi-Naeini

2 2017 ICU Honolulu Abstract book

8:25 Non-reciprocal and chiral acoustics in optomechanical systems∗ 27G. Bahl

8:50 Dissipative optomechanical cooling of a glass-fiber nanospike coupled to a bottleresonator

27

R. Pennetta, S. Xie, R. Zeltner and P. S. J. Russell

9:05 Doubly-resonant nanostructure for enhanced acousto-optical modulation 27V. Laude, A. Belkhir, M. Addouche, S. Benchabane, A. Khelif and F. I. Baida

9:20 Propagation of Elastic Waves along 1D Phononic Crystal Nanowalls 28Y. Pennec, A. Gueddida, E. Alonso-Redondo, E. H. El Boudouti, S. Yang, G. Fytas and B.Djafari-Rouhani

Underwater Network Communications and DetectionRoom: 305B

Time: 8:00

Chair: J. W. Choi

8:00 Range measurement of active underwater source using Doppler frequency esti-mation

28

W.-J. Park, K.-M. Kim, M.-S. Han and J.-Y. Choi

8:15 Long-range Underwater Acoustic Communications in the East Sea of Korea 29H. Kim, S. Kim, K.-H. Choi and J. W. Choi

8:30 Optimal deployment of vector sensor nodes based on Performance Surface ofunderwater acoustic communication

29

S. Kim and J. W. Choi

8:45 Analysis of Passive Time-reversal Communication Performance in Shallow Wa-ter with Underwater Sound Channel Axis

30

K.-H. Choi, S. Kim and J. W. Choi

9:00 Acoustical Inversion Method using Cepstrum Analysis of Underwater Ship Noise 30C. S. Park, G.-D. Kim, G.-T. Yim and H. Ahn

Acoustic Nondestructive Evaluation and Technology 1Room: 305B

Time: 11:00

Chair: L. J. Bond

11:00 Development of a Numerical Test Bed for Ultrasonic Inspection of Highly Re-inforced Concrete∗

30

M. T. Baquera and L. J. Bond

11:25 Quality-factor and frequency shifts of suspended Ge membranes 31L. Zhou, G. Colston, O. Trushkevych, M. Myronov, D. Leadley and R. S. Edwards

11:40 Enhanced surface defect detection using focused electromagnetic acoustic trans-ducers (EMATs)

31

C. B. Thring, S. Hill, W. E. Somerset, A. Feeney and R. S. Edwards

11:55 FEM Study of Grain Size Evaluation in Polycrystalline Materials 32Z. Youxuan, N. Hu and J. Qu

12:10 Laser-induced ultrasound imaging for evaluation of temperature fields in paratel-lurite optical crystal

32

V. P. Zarubin, K. B. Yushkov, A. I. Chizhikov, V. Y. Molchanov, S. A. Tretiakov, A. I.Kolesnikov, E. B. Cherepetskaya and A. A. Karabutov


12:25 Experimental Evaluation of Impact Damage in an Adhesive Bonding Using Non-linear Ultrasonic Method

33

G. Shui and Y.-S. Wang

12:40 Ultrasonic NDT and In-situ Acoustic Flow Control of Residual Stress 33C. Xu

Acoustic Phononic Crystals 1Room: 304A

Time: 11:00

Chair: Y. Pennec

11:00 Non-hermitian valley states in artificial acoustic meta-crystals∗ 33J. Christensen

11:25 Acoustic Topological States 34C. He, M.-H. Lu and Y.-F. Chen

11:40 Some Novel Effects of Phononic Crystals for Surface Acoustic Waves 34S.-Y. Yu, X.-C. Sun, X.-P. Liu, M.-H. Lu and Y.-F. Chen

Acoustics and CellsRoom: 309

Time: 11:00

Chair: A. C. Yu

11:00 High-frequency ultrasound microbeam techniques: from cell manipulation tophyenotyping∗

34

J. Y. Hwang

11:25 Simple evaluation method of acoustic trapping performance by tracking motionof trapped microparticle

35

C. Yoon and H.G. Lim

11:40 Enhancement of Reactive Oxygen Species Generation by Using Cavitation Bub-bles for Sonodynamic Treatment

35

S. Nishitaka, D. Mashiko, R. Iwasaki, S. Yoshizawa and S.-I. Umemura

11:55 Cetuximab coated albumin nanobubbles for enhanced cell killing and apoptosisof oral squamous carcinoma cells

36

A. Watanabe, H. Sheng, K. Narihira, S. Kondo, T. Kikuta and K. Tachibana

12:10 Dynamics of Acoustic Droplet Vaporization Induced Sonoporation on Single cell 36Y. Feng

BAW and SAW Resonators and ApplicationsRoom: 307B

Time: 11:00

Chair: V. Laude

11:00 Recent Progress on Quartz Crystal Resonators for Frequency Control Applica-tions∗

36

M.-C. Chao and J. Wang

11:25 Optimal Orientations of Quartz Crystals for Bulk Acoustic Wave Resonatorswith the Consideration of Thermal Properties

37

J. Wang, L. Zhang, L. Xie, H. Huang, M. Ma, J. Du, M.-C. Chao, S. Shen and R. Wu

11:40 Acoustofluidic Multibody Simulations of Hydrodynamically and AcousticallyInteracting Particles Beyond the Rayleigh Limit

37

T. Baasch and J. Dual


11:55 Enhanced ferroelectric, and piezoelectric properties in La modified BiFeO3-PbTiO3 Multiferroic Ceramics prepared by tape casting

38

S. Shen, J. Chen and J. Cheng

12:10 Theoretical and experimental study of c-axis-tilted ScAlN / sapphire for SAWdevices with high electromechanical coupling

38

S. Tokuda, S. Takayanagi, M. Matsukawa and T. Yanagitani

Engineering Applications of Power UltrasonicsRoom: 308A

Time: 11:00

Chair: F. Balle

11:00 Ultrasonic Joining of Hybrid Materials and Structures for Engineering Applica-tions∗

38

F. Balle

11:25 Ultrasonic Complex Vibration Welding Systems Using Two- dimensional Vibra-tion Stress -Ultrasonic welding using various welding tips -

39

J. Tsujino

11:40 Study of Ultrasonic-Assisted Ozone Treatment on Oil Recovery Wastewaterfrom Polymer Flooding

39

W. Song, S. Yu, L. Zhang and W. Wang

11:55 Dynamic Characteristics of Flexural Ultrasonic Transducers 40A. Feeney, L. Kang, G. Rowlands and S. Dixon

Ultrasound Signal and Image ProcessingRoom: 308B

Time: 11:00

Chair: J. H. Chang

11:00 Simultaneous Enhancement of B-Mode Axial and Lateral Resolution using AxialDeconvolution

40

Á. Makra, G. Csány, K. Szalai and M. Gyöngy

11:15 Development of skin thickness measurement algorithm for HIFU treatment guid-ance

41

E.-J. Shin, J. Lee and J. H. Chang

11:30 Reconstruction of wavespeed maps using seismic full waveform inversion 41E. Bachmann and J. Tromp

11:45 Evaluation of Blood Flow Dynamics in Normal and Myocardial Infarction HeartsUsing Echodynamography

41

S. Oktamuliani, K. Hasegawa and Y. Saijo

12:00 Two-dimensional Blood Flow Vectors Obtained with a Single Sector Probe 42M. Maeda, R. Nagaoka, S. Yaegashi, H. Ikeda and Y. Saijo

12:15 Effects of flow velocities on the pressure wave using a blood vessel mimickingtube

42

F. Iwase, S.-Y. Shimada and M. Matsukawa


Acoustic and Elastic Metamaterials 1Room: 304A

Time: 13:00

Chair: B. Assouar

13:00 Discovery of Transmodal Fabry-Perot Resonance for Elastic Wave Mode Con-version∗

43

Y. Y. Kim, J. M. Kweun and X. Yang

13:25 Elastic waves in tunable acoustic metamaterials by active control 43Y.-Z. Wang and Y.-S. Wang

13:40 Elastic wave lens and mirror concepts for enhanced energy harvesting 43S. Tol, L. Degertekin and A. Erturk

13:55 Stress wave mitigation and filtering via origami-based metamaterials 44H. Yasuda and J. Yang

14:10 Elastic Metamaterial for Vibration Shielding at Broad Low Frequencies 44J. H. Oh, S. Qi, Y. Y. Kim and B. Assouar

Acoustic Modeling of Sound Fields in Complex EnvironmentsRoom: 307B

Time: 13:00

Chair: N. F. Declercq

13:00 Ultrasonic nondestructive evaluation of complex media - case studies∗ 44N. F. Declercq, L. Chehami, P. Pomarède, F. Meraghni, E. Ahmed Mohammed and O.Ez-Zahraouy

13:25 Ultrasound field simulation in crystal-based acousto-optic devices 45S. N. Mantsevich, V. I. Balakshy, K. B. Yushkov and V. Y. Molchanov

13:40 Grain Shape Dependent Coherent Wave Attenuation in Heterogeneous Media 45M. Ryzy, T. Grabec and I. A. Veres

13:55 Additively Manufactured Acoustic Diffuser Structures for Ultrasonic Applica-tions

46

L. Claes, H. Zeipert, P. Koppa, T. Tröster and B. Henning

14:10 Experiments and Simulations of the Standing Wave Acoustic Field Produced byTwo Transducers Mounted in Contraposition

46

H. Dong, L. Jia, Y. Guan and J. Zhao

Advances in Biomedical UltrasoundRoom: 309

Time: 13:00

Chair: J. Allen, C.-C. Huang

13:00 3D Blood vessel mapping for small animal using high frequency ultrafast DopplerImaging∗

47

C.-C. Huang

13:25 Estimation of the linear displacement and rotation movement of the extensordigitorum communis tendon based on ultrafast high frequency ultrasound imag-ing

47

C.-C. Huang, M.-Y. Wang and P.-Y. Chen

13:40 Instantaneous Frequency and Phase of Coupled Microbubble Oscillations 48J. Allen and R. Hayashi


13:55 A Stippling Algorithm to Generate Equivalent Point Scatterer Distributionsfrom Ultrasound Images

48

K. Füzesi, Á. Makra and M. Gyöngy

14:10 A Low-Cost Portable Ultrasound System for Skin Diagnosis 48G. Csány, K. Szalai, K. Füzesi and M. Gyöngy

14:25 A smart-phone Based Portable Ultrasound Imaging system for Point-Of-Careapplications

49

S. Yeo, J. H. Kim, M. Kim, S. Kye, Y. Lee and T.-K. Song

Guided Waves and Their Applications in NDE 1Room: 305B

Time: 13:00

Chair: N. Hu, Z. Su

13:00 In-situ Health Monitoring of Space Structures Under Hypervelocity Impact:Hybrid Use of Passive Acoustic Emission and Active Nonlinear Guided Waves∗

49

Z. Su

13:25 Guided wave propagation characteristics in two layers cylindrical porousmedium -containing half-space structure

49

H. Qingbang

13:40 An improved two-stage rapid reconstruction scheme for Lamb wave tomography 50Y. Liu, S. Qin, X. Liu and N. Hu

13:55 A High-sensitivity and Fast-response Nanocomposites-inspired Sensor forAcousto-ultrasonics-based Structural Health Monitoring

50

Y. Liao, F. Duan, L. Zhou and Z. Su

14:10 Optical Visualization of Leaky Lamb Wave and Its Application in Nondestruc-tive Testing

51

Z. An, Z. Hu, J. Mao, G. Lian and X. Wang

14:25 Flow Imaging of Metallic Melts through a Multimode Waveguide 51R. Nauber, M. Kalibatas and J. Czarske

14:40 Modelling Guided Waves in Layered Media Materials Using the State-vectorFormalism and Legendre Polynomial Method

51

Y. Lu, J. Gao, G. R. Song, B. Wu and C. F. He

Ultrasound Elasticity Imaging and Biomedical Applications 1Room: 308B

Time: 13:00

Chair: K. Kim

13:00 Advances in Optical Coherence Elastography∗ 52Z. Chen

13:25 Elastography of ocular tissues using acoustic radiation force and optical meth-ods∗

52

S. Aglyamov

13:50 New Multi-Physics Strategies to Induce Shear Waves in Soft Tissues for Me-chanical Assessment of Tissue Properties∗

52

G. Cloutier, P. Grasland-Mongrain, F. Lesage and S. Catheline

14:15 Shear Wave Propagation Imaging by Color Doppler Shear Wave Elastography 53Y. Yamakoshi, M. Yamazaki and K. Taniuchi

14:30 The Role of Shear Waves in the Generation of the Radiation Force on an ElasticSphere in a Liquid by a Quasi-Gaussian Acoustic Beam

53

O. A. Sapozhnikov, A. V. Nikolaeva and M. R. Bailey


Ultrasound in Industrial Processing and Material EngineeringRoom: 308A

Time: 13:00

Chair: L. Gaete-Garretón, H. Nagata

13:00 High-Power Piezoelectric Characteristics of Bi-based Lead- free PiezoelectricCeramics

54

H. Nagata

13:15 Atomization Threshold in a Layer of Distilled Water under Vertical Vibrations 54L. Gaete-Garretón, Y. Vargas-Hernández, J. Meneses-Dı́az and B. B. Lagos-Farfán

13:30 Experimental Study of Aging Oil Viscosity Reduction Caused by Ultrasound 55J. Qiao, W. Song, W. Wang, X. Yuan and L. Li

13:45 Experimental study of ultrasound-assisted cyanide leaching of gold 55X. Yu, S. Yu, X. Yuan, W. Wang and W. Song

14:00 Ultrasonic metal welding changing the shape of vibration locus by ultrasoniccomplex vibration source

55

Y. Tamada, T. Asami and H. Miura

14:15 Development of ultrasonic complex vibration source using square prism rod withdiagonal slits

56

T. Asami and H. Miura

14:30 Closed Loop Control of Cavitation - A Sonomechatronic Approach 56J. Twiefel and K.-A. Saalbach

Authors’ WorkshopRoom: 304ATime: 15:00Chair: A. Every, F. Muenzel

Tuesday 19 December 2017

Plenary Lecture 2Room: 306

Time: 10:00

Chair: B. Assouar

10:00 Optimal Sound Absorbing Structures∗ 57P. Sheng


Time: 8:00

Chair: B. Assouar

8:00 Acoustic Topological States in Topological Phononic Crystals∗ 57Y.-F. Chen, C. He, M.-H. Lu and X. Ni

8:25 Tunable Manipulation of Lamb Waves in Fluid-Solid Phononic Slabs 58Y.-F. Wang, Y.-S. Wang and V. Laude

8:40 Reprogrammable phononic metamaterial 58O. Bilal, A. Foehr and C. Daraio


8:55 Bifurcation of avoided crossings in the dispersion of sound and light in locallyresonant media

58

A. Maznev

9:10 Scattering Properties and Fano Resonances in a Pillared Metasurface 59Y. Pennec, Y. Jin and B. Djafari-Rouhani

Applications of Nonlinear Acoustics to Measurements and ImagingRoom: 307A

Time: 8:00

Chair: H. Nomura, Y. Ohara

8:00 Nonlinear ultrasonic phased array for closed crack imaging∗ 59Y. Ohara

8:25 Application of Parametric Ultrasound to Low-frequency Acoustic Imaging∗ 59H. Nomura

8:50 Harmonic Imaging of Multiple Defects in Solid Material by Aerial UltrasonicBeam

60

Y. Mukaiyama, A. Osumi and Y. Ito

9:05 Non-contact Harmonic Measurement of Elastic Modulus and Surface Propertiesof Mortar Having Fire Damage

60

T. Saito, A. Osumi and Y. Ito

9:20 A Novel Sensitivity Matrix Construction Method FOR Ultrasonic Tomography 60N. Li, K. Xu and J. Jiao


Time: 8:00

Chair: C. C. Coussios, M. Versluis

8:00 Acoustic cavitation from nanocups∗ 61J. Kwan, G. Lajoinie, N. De Jong, E. Stride, M. Versluis and C. C. Coussios

8:25 Non-spherical bubble oscillations drive the ultrasound-mediated release fromtargeted microbubbles∗

61

M. Versluis

8:50 Multibubble Sonoluminescence and Bubble Dynamics in Glycerol-water Mix-tures

62

P.-K. Choi and M. Ban

9:05 Water-Molecular Emission from Acoustic Bubbles under Electric Fields 62H.-B. Lee and P.-K. Choi

Life at the Intersection of Light and SoundRoom: 309

Time: 8:00

Chair: X. Wang, C. Yang

8:00 Photoacoustic tissue characterization toward potential in vivo biopsy∗ 62X. Wang

8:25 Fast Time Reversal Ultrasound Encoded Optical Focusing for Deep Brain Op-togenetic Activation∗

63

C. Yang

8:50 Transcranial transmission of shock waves by a Laser-generated Carbon NanoTube transducer

63

M. Lee, D.-G. Paeng, K. Ha and M. J. Choi


9:05 Three-dimensional Photoacoustic and Ultrasound Combined Microscope forImaging of Skin Micro Vasculature

64

Y. Saijo, R. Nagaoka, H. Iwazaki, T. Omuro, T. Ida, S. Yoshizawa and S.-I. Umemura

9:20 Identification of prostate cancer in ex vivo human prostates by photoacousticphysio-chemical analysis

64

Y. Chen, Y. Qin, J. Pan, S. Huang, C. Xu, D. Wu, T. Feng, J. Yuan, X. Wang, G. Xu andQ. Cheng

9:35 Carbon Nanotubes as Potential Candidate for Photoacoustic Imaging ContrastAgent

65

S. Siregar, R. Nagaoka and Y. Saijo

Linear and Nonlinear Granular Metamaterials and DevicesRoom: 305BTime: 8:00Chair: V. Gusev, V. Tournat

8:00 Recent Progress in the Characterization of Nonlinear Phenomena in MicroscaleGranular Media via Laser Ultrasonics∗

65

N. Boechler

8:25 Polydispersed Granular Chains: From Long-lived Chaotic Anderson-like Local-ization to Energy Equipartition

66

V. Achilleos, G. Theocharis and C. Skokos

8:40 Vibrational Dynamics of a Two-dimensional Micro-granular Crystal Studied viaLaser-induced Transient Gratings

66

A. Vega-Flick, R. A. Duncan, S. P. Wallen, N. Boechler, C. Stelling, M. Retsch, J.-J.Alvarado-Gil, K. A. Nelson and A. Maznev

8:55 Strongly nonlinear hysteretic propagation of torsional waves in a granular chain 66A. Cebrecos, P. Béquin, G. Theocharis, V. E. Gusev and V. Tournat

9:10 Tuning the Vibrational Response of Microscale Granular Crystals via Manipu-lation of Nanoscale Contact Features

67

M. Abi Ghanem, A. Khanolkar, J. Eliason, A. Maznev, N. Vogel and N. Boechler

Novel Sensors and ActuatorsRoom: 307B

Time: 8:00

Chair: K. Baik

8:00 Densely packed semi-random spherical array transducer to su-ppress gratinglobe levels in real-time photoacoustic imaging

67

S.-I. Umemura, R. Nagaoka, S. Yoshizawa and Y. Saijo

8:15 The Effect of Ti-6Al-4V Microstructure on the Performance of Ultrasonic SoftTissue Cutting Tips

68

M. Wilkie and M. Lucas

8:30 Ultrasonically assisted cutting blades for large bone surgeries 68D. Richards and M. Lucas

8:45 Focusing of ultrasound using flat piston transducer and Fresnel Zone Plate forMedical Imaging

69

K. Baik, S. Kim, Y. T. Kim, I. Doh, J. Hyun and H. J. Lee

9:00 Kerfless Phased Array Using Sol-Gel Composite Spraying Technique 69M. Tanabe, M. Kobaysahi, K. Nakatsuma and M. Nishimoto

9:15 Wide-band Design of Diaphragm pMUT based on Induction of Strain in FilmThickness Direction by Aspect Ratio Control

69

Y. Ishiguro, N. Tagawa and T. Okubo


Ultrasound in AirRoom: 308A

Time: 8:00

Chair: K. Nakamura

8:00 Ultrasonic Characterization of Noodle Dough for the Development of Air-coupled Ultrasound On-line Quality Control During Production

70

R.-M. Guillermic, S. O. Kerhervé, H. Wang, A. Strybulevych, D. W. Hatcher, M. G. Scanlonand J. H. Page

8:15 Directivity of a circular transverse vibrating plate type aerial ultrasonic sourcewith a truncated cone shaped reflective plate

70

H. Yoshino, T. Asami and H. Miura

8:30 Analysis of Vertical Sound Image Control with Parametric Loudspeakers 71S. Aoki, K. Shimizu and K. Itou

8:45 Divergence control of ultrasonic sound waves generated by a parametric speaker 71Y. Matsui, M. Oi, G. Cheng, X. Wu and H. Furuhashi


Time: 11:00

Chair: Y.-S. Wang

11:00 Effect of diffraction modes on acoustic bandgap formation in two-dimensionalphononic crystal in water

72

H. S. Kang, W.-G. Kim, S. W. Yoon and K. I. Lee

11:15 Guided Elastic Waves in Nanoscaled 1D Piezoelectric Phononic Crystals 72A. Chen, D.-J. Yan and Y.-S. Wang

11:30 Ceramic Phononic Crystals with MHz-range Frequency Band Gaps 72M. Koller, A. Kruisova, H. Seiner, P. Sedlák, M. Landa, B. Roman-Manso, P. Miranzo, M.Belmonte and T. Grabec


Time: 11:00

Chair: O. A. Sapozhnikov

11:00 Application of Improved Orthogonal Polynomial Expansion Method in Calcu-lating Dispersion Curves on Layered Semi-infinite Structure

73

G. R. Song, M. K. Liu, Y. Lu, B. Wu and C. F. He

11:15 Acoustic Delay-Lines Based on Wedge Waves 73C.-H. Yang and P.-H. Tung

11:30 Non-Contact Monitoring of Fatigue Damage in Metallic Plates Using Laser-Generated Zero-Group Velocity Lamb Waves

73

G. Yan, S. Raetz, N. Chigarev, V. E. Gusev and V. Tournat

11:45 Phased Waveguide Array for Ultrasonic Imaging in Aggressive Liquids 74S. A. Tsysar, S. A. Petrosyan, V. D. Svet and O. A. Sapozhnikov

12:00 Characterization of Micro-crack Evolution Using Nonlinear Lamb Waves 74C. Ma, W. Zhu, Y. Xiang, M. Deng and H. Zhang

12:15 Guided Wave Inspection for Rail Foot Using Piezoelectric Probe 75R. Lin, Y. Wen, Y. Ma and H. Ma


12:30 Finite Element Modeling of Microcrack Detection in Plate by Nonlinear LambWaves

75

Y. Liu, S. Ma and H. Zhang

High-frame Rate Ultrasound Imaging and ApplicationsRoom: 308A

Time: 11:00

Chair: C. L. De Korte, H. Hasegawa

11:00 High frame-rate carotid ultrasound imaging∗ 76H. H. Hansen, S. Fekkes, A. E. Saris, P. Van Lochem and C. L. De Korte

11:25 Vector Projectile Imaging (VPI): Dynamic Flow Visualization Using High FrameRate Ultrasound∗

76

A. C. Yu

11:50 Adaptive Beamformer with Phase Coherence Weighting Applied to UltrafastUltrasound∗

76

H. Hasegawa and M. Mozumi

12:15 Computationally Efficient Super Resolution Ultrasound Imaging Based on Mul-tiple Transmission/Reception with Different Carrier Frequencies

77

J. Zhu and N. Tagawa

12:30 3-D Electromechanical activation mapping of the heart in canines and humansin vivo

77

J. Grondin, D. Wang, N. Trayanova and E. Konofagou

Picosecond Laser Ultrasonics 1Room: 307B

Time: 11:00

Chair: O. B. Wright

11:00 Theoretical models supporting some recent experiments in picosecond laser ul-trasonics∗

78

V. E. Gusev

11:25 Time-domain Brillouin scattering assisted by diffraction gratings∗ 78O. Matsuda, T. Pezeril, I. Chaban, K. Fujita and V. E. Gusev

11:50 Longitudinal sound velocities, elastic anisotropy and phase transition of highlypressurized H2O ice evaluated by picosecond acoustic interferometry

79

M. Kuriakose, S. Raetz, Q.-M. Hu, S. M. Nikitin, N. Chigarev, V. Tournat, A. Bulou, A.Lomonosov, P. Djemia, V. E. Gusev and A. Zerr

12:05 Temperature Dependence of Polycrystalline Aluminum Thin Film Elastic Con-stants by In-Situ Brillouin Light Scattering and Picosecond Ultrasonics

79

P. Djemia, L. Belliard, F. Challali, N. Girodon-Boulandet and D. Faurie

12:20 Probing the van der Waals coupling of 2D materials by using Terahertz Ultra-sonics

80

P.-J. Wang, V. E. Gusev, J.-K. Sheu and C.-K. Sun

Reservoir Acoustics and Borehole Acoustic Logging 1Room: 306

Time: 11:00

Chair: X. Wang, H. Hu

11:00 Advances in borehole acoustic reflection imaging∗ 80X. M. Tang


11:25 An Inversion Scheme for The Shear Speed from The Sholte Wave Excited by ADipole Source during Logging While Drilling in A Slow Formation

81

H. Hu, C. Zhang and X. Zheng

11:40 Numerical Simulations of a Slim-hole Piezoelectric Dipole Transmitter forAcoustic Logging

81

Y. Zhou, Y. Dai, D. Chen and Q. Zhang

11:55 Indirect Collar Waves in Acoustic Logging While Drilling 81X. He, X. Wang, H. Chen and X. Zhang

12:10 A Broadband Sonic Logging Monopole Transducer 82Y. Dai, Y. Zhou, H. He, Z. Wang and X. Wang

12:25 Step by step inversion of anisotropy parameters using cross dipole logging data 82H. Chen, H. He, X. He and X. Wang

Safety of UltrasoundRoom: 308B

Time: 11:00

Chair: Y. Watanabe

11:00 Effect on Rabbit Heart Exposure to Ultrasound with Long Pulse Duration∗ 82I. Akiyama, W. Takano, K. Rifu, N. Takayama, H. Sasanuma and N. Taniguchi

11:25 The promotion of muscle synthesis of skeltal muscle cell exposed to ultrasound 83W. Takano, M. Furuya, C. Okamoto, H. Ichikawa and I. Akiyama

11:40 The Effect of Ultrasound with Acoustic Radiation Force Impulse on the Lung:A Preliminary Study in Rabbits

83

H. Sasanuma, N. Takayama, K. Rifu, W. Takano, Y. Ishiguro, N. Taniguchi, A. KawaraiLefor and I. Akiyama

11:55 Proteomic analysis of developmental effect on medaka embryo exposed by ul-trasound

84

E. Matsumoto, K. Kawanabe, K. Yoshida, I. Akiyama, M. Hirose, M. Ikegawa and Y. Watan-abe

Ultrasonic Bone CharacterizationRoom: 309

Time: 11:00

Chair: K. I. Lee, K. A. Wear

11:00 Using Quantitative Ultrasound to Probe Material, Mechanical, and Microarchi-tectural Properties of Trabecular Bone∗

84

K. A. Wear

11:25 Application of Sparse Radon Transform in Quantitative Bone Ultrasound∗ 84L. H. Le, T. N. Tran, K.-C. T. Nguyen and M. D. Sacchi

11:50 Dispersion Response of Ultrasonic Guided Modes to the Variation of Geometryand Material Properties in Cortical Bone Characterization by Semi-AnalyticalFinite-Element Modeling

85

T. N. Tran, L. H. Le, M. D. Sacchi and V.-H. Nguyen

12:05 Structural Dependence of Piezoelectric Signal in Cancellous Bone at an Ultra-sound Frequency

85

A. Hosokawa

12:20 Induced electric potential in bone by low intensity ultrasound irradiation 86S. Mori, M. Kuraoka, T. Makino, Y. Sakata and M. Matsukawa


12:35 Finite Element Resonant Ultrasound Spectroscopy to Measure Elastic Proper-ties of Small Animal Cortical Bone∗

86

K. Xu, P. Dargent, P. Laugier and Q. Grimal

Ultrasonic Motors, Actuators, and SensorsRoom: 307A

Time: 11:00

Chair: A. Feeney

11:00 Focus control of a liquid crystal lens using ultrasound vibration 87D. Koyama, Y. Shimizu, Y. Harada, M. Fukui, A. Emoto, K. Nakamura and M. Matsukawa

11:15 Effect of thermal annealing on mechanical quality factors of poly phenylenesulfide under high-amplitude ultrasonic vibration

87

J. Wu, Y. Mizuno and K. Nakamura

11:30 Two-Dimensional Flexural Ultrasonic Phased Array for Flow Measurement 87L. Kang, A. Feeney, R. Su, D. Lines, A. Jäger, H. Wang, Y. Arnaudov, S. N. Ramadas, M.Kupnik and S. Dixon

11:45 Directional Control of Ultrasonic Sensor Using Parabolic Radiation-type Reflec-tor

88

T. Ueda, J. Neguchi, T. Ohgo, T. Orita and K. Saeki

12:00 Towards New Imaging Methods for Ultrasonic Nondestructive Testing - Part I 88D. Braconnier, N. Laroche, E. Carcreff and J. Lorenz

12:15 Towards New Imaging Methods for Ultrasonic Nondestructive Testing - Part II 88D. Braconnier, N. Laroche, E. Carcreff and J. Lorenz


Time: 13:00

Chair: Y. Y. Kim

13:00 Dynamic non-reciprocity in piezo-phononic media 89A. Merkel, M. Willatzen and J. Christensen

13:15 Breaking acoustic reciprocity using deformation mechanism 89T. Devaux, A. Cebrecos, O. Richoux, V. Pagneux and V. Tournat

13:30 Simulation of gigahertz plate waves in elastic metamaterials 90M. Tomoda, K. Fujita, K. Inagaki, O. Matsuda, O. B. Wright and V. E. Gusev

13:45 Gradient metamaterial matching layer for ultrasonic transducers 90J. Zhu


Time: 13:00

Chair: Y. Cho, I. Park

13:00 Effect of microstructural evolution on acoustic nonlinear response of ultrasonicwaves in solid media∗

90

Y. Cho and W. Li

13:25 Leakage noises in valves 91A. Rondeau, E. Lafargue and F. Cartier

13:40 Validation of the first prototype high temperature ultrasonic sensor for gascomposition measurement

91

O. Gatsa, E. Rosenkrantz, D. Fourmentel, C. Destouches, P. Combette and J.-Y. Ferrandis


13:55 Low Frequency Ultrasonic Collimated Beam Generation from PiezoelectricTransducers

92

V. K. Chillara, C. Pantea and D. Sinha

14:10 Development of High Speed Inversion Technique for the Characterization of Full-Field Material Properties Based on Quantitative Laser Ultrasound VisualizationSystem

92

S.-P. Tseng and C.-H. Yang

14:25 Imaging the Adhesion Quality of a 255nm Tungsten Thin Film With a SiliconSubstrate Using Picosecond Ultrasonics

92

A. Abbas, X. Tridon and J. Michelon

14:40 Development of Acoustical Microscopy System with Ultra High Resolution forMicro/Nano Structure Inspection

93

I. Park, T. Park and D. Kwak

Guided Waves in Physical AcousticsRoom: 308A

Time: 13:00

Chair: N. Boechler, A. Maznev

13:00 Elastic Waves in Magnetogranular Metamaterials∗ 93G. Theocharis

13:25 Acoustic waves in Freestanding Silicon Structures and Applications to ThermalEngineering and Optomechanics∗

93

J. Maire, D. Navarro-Urrios, M. Sledzinska, B. Graczykowski, E. Chávez Angel, F. Alzina,R. Anufriev, M. Nomura and C. M. Sotomayor-Torres

13:50 Continuum Elasticity Modeling of Long-wavelength Acoustic Vibrations ofQuasi-2D Structures and Micro-tubules

94

A. G. Every, D. Liu and D. Tomanek

14:05 Mechanical Anisotropy of Plant Cell Walls Studied by Laser Generated GuidedAcoustic Waves

94

M. Abi Ghanem, L. Khoryati, N. Boechler and T. Dehoux

14:20 Ritz-Rayleigh Approach: Numerical Calculation of Guided- Wave Properties 95T. Grabec, P. Sedlák, H. Seiner and M. Landa

14:35 How to Induce Dynamic Fracture by Focusing Flexural Waves 95V. Van Gemmeren, B. Zybach and J. Dual

Thermo-acousticsRoom: 307B

Time: 13:00

Chair: S.-I. Sakamoto, X. Xie

13:00 Fundamental study on the effect of the change in the cross- sectional area onthe straight-tube-type thermoacoustic prime mover∗

96

S.-I. Sakamoto, T. Wada and T. Saito

13:25 Investigation on Acoustic Radiation Characteristics of an Open-Air Traveling-Wave Thermoacoustic Generator

96

X. Xie, S. Yang, F. Liu and Q. Li

13:40 Optimizations of an Open-air Traveling-wave Thermoacoustic Generator 96F. Liu, X. Xie, S. Yang and Q. Li

13:55 Effect of temperature distribution of the stack on heat flow in standing-wavethermoacoustic-system

97

M. Sugimoto, S.-I. Sakamoto and Y. Watanabe


14:10 Effect of acoustic impedance on a thermoacoustic system using a Heat PhaseAdjuster

97

H. Morishita, S.-I. Sakamoto, K. Shiraki and Y. Watanabe

Ultrasonic Cavitation for TherapyRoom: 308B

Time: 13:00

Chair: C. C. Coussios, S.-I. Umemura

13:00 Cavitation generating and utilizing exposure sequence for focused ultrasoundtreatment∗

98

S.-I. Umemura and S. Yoshizawa

13:25 Cavitation-Enhanced Drug Delivery to Tumours using Sub-Micron CavitationNuclei and Passive Acoustic Mapping∗

98

C. C. Coussios, C. Coviello, C. Mannaris, P. Katti and R. Carlisle

13:50 Triplet Pulse Sequence for Cavitation Bubble Imaging in High-Intensity FocusedUltrasound Treatment

98

R. Iwasaki, R. Nagaoka, S. Yoshizawa and S.-I. Umemura

14:05 Effect of focal shape control on stone erosion rate using cavitation bubbles 99T. Yura, M. Lafond, S. Yoshizawa and S.-I. Umemura

14:20 Comparison of spatial distribution characteristics of shock wave pressure fieldand cavitation bubble cloud

99

G. Kang, O. Kwon, J.S. Huh and M. J. Choi

Ultrasound Elasticity Imaging and Biomedical Applications 2Room: 309

Time: 13:00

Chair: K. Kim

13:00 Towards the Goal of High Resolution, Low Noise, Low Variance Shear WaveElastography∗

100

S. McAleavey

13:25 Ultrasound Strain Elastography to Detect Placenta Diseases∗ 100C. H. Yap, S. N. Saw, J. Y. R. Low, C. N. Z. Mattar, A. Biswas and L. Chen

13:50 Ultrasound-based carotid elastography for detection of vulnerable atheroscle-rotic plaques validated by magnetic resonance imaging

101

J. Luo

14:05 Ultra-high Frequency Shear wave elastogrpahy for Human Finger Tendon 101C.-C. Huang and Y.-Y. Hsiao

Memorial Session for Leif BjørnøRoom: 304A

Time: 15:00

Chair: L. A. Crum

15:00 The underwater sounds of precipitation∗ 101L. A. Crum

15:25 Nonlinear Problems in the Generation, Propagation and Measurement of HighIntensity Ultrasonic Waves in Air∗

102

J. A. Gallego-Juárez, E. Riera and L. Gaete-Garretón

15:50 Leif Bjørnø and International Ultrasonics Conferences∗ 102W. Sachse


16:15 Professor Leif Bjørnø - Recollection∗ 102

B. Linde and A. Śliwiński

Poster SessionRoom: 306

Time: 15:00

Chair: K. I. Lee, H. Nomura, J. H. Chang

Biomedical Ultrasound

000043 Acoustic Impedance Imaging Conversion From B mode (Detection of early agingalteration in human facial skin)

103

Y. Ogura, T. Kondo, T. W. Chean, S. Yoshida, K. Kobayashi, N. Hozumi and O. Yuki

000077 Ultrasound heating induced in the presence of magnetic nanoparticles 103A. Jozefczak, K. Kaczmarek, T. Hornowski and R. Bielas

000137 Implementation of backend processing system for real-time intravascular ultra-sound imaging

103

J.-W. Park and J. H. Chang

000145 Design of PZT and PVDF-based dual-layer transducers for intravascular ultra-sound tissue harmonic imaging

104

S. Park, J. Lee and J. H. Chang

000146 Prediction and Measurement of Temperature Rise Induced by High IntensityFocused Ultrasound in Tissue-Mimicking Phantoms

104

K. I. Lee, H. S. Kang and S. W. Yoon

000156 Multi-angular vector flow imaging (mVFI) for accurate, reliable vector Dopplerestimation

105

J. H. Jeong, S. Yeo, C. Yoon and T.-K. Song

000176 Transcranial passive acoustic mapping with thin tube phantom using CT-basedskull aberration correction: a preliminary study

105

C. Jin, C. W. Jin and J. Park

000232 Lens design simulation and fabrication of Carbon Nano Tube transducer fortranscranial applications

106

C. Lee, D.-G. Paeng and K. Ha

000253 Difference of Acoustic Emission Eignal between Transcranial and Skull-lessBrain while Blood-Brain Barrier Dsruption in a Rat Brain

106

Y. Hur, M. Han, J. Yang, C. Jin and J. Park

000256 Transmit Sequence Optimization for Motion Corrected 3D Diverging WaveCompounding: A Simulation Study

107

Y. Chen, J. D’Hooge and J. Luo

000286 Characteristics of high intensity and high frequency ultrasonic transducers usinghydrothermal epitaxial piezoelectric films

107

M. Ishikawa, Y. Uchida, T. Shiraishi, M. Tabaru, H. Funakubo and M. Kurosawa

000301 A Preliminary Study To Investigate The Accuracy Of Ultrasound To AssessAlveolar Bone Level

107

K.-C. T. Nguyen, L. H. Le, N. R. Kaipatur, E. H. Lou and M. W. Major

000321 Focused Ultrasound Ablation of Liver Tumor: Model Development and Simula-tion

108

S. Maxim and T. W. Sheu


000324 Visualization Experiment of Frequency Dependent Attenuation of Tissue byMulti-Spectral Phase-Contrast Imaging

108

S. Ishikura, N. Tagawa, M. Yoshizawa and T. Irie

Emerging Fields

000092 Side-Lobe Suppression for Air-Coupled Ultrasonic Sensors Attached on the BackSide of Automobile Bumpers

109

K. Ibata, R. Hara, T. Kimura, Y. Nishioka, N. Yoneda and S. Inoue

000210 T-shaped configuration of multi-frequency acoustic camera and visualization inair

109

M. Fujii and K. Nakamura

Industrial Ultrasound

000008 An Ultrasonic Vibration System Used in Friction Stir Welding 110B. Fu, W. Zhang and G. Zhou

000020 HiFFUTs for High Temperature Ultrasound 110A. Feeney, L. Kang and S. Dixon

000074 An ultrasonic motor using transmission line and a spring washer driven by aLangevin transducer

110

T. Ishii, M. Mochizuki and T. Shimizu

000168 Material Parameter Identification of a Piezoelectric Disc with Triple-Ring-Electrodes for Increased Sensitivity

111

B. Jurgelucks, N. Feldmann, L. Claes, A. Walther and B. Henning

000228 Impregnation of liquid droplet in non-contact by aerial ultrasonic waves 111R. Nakayama, T. Asami and H. Miura

000270 Measurement of the flexoelectric coefficient for bulk barium titanate under one-dimension shock wave

111

T. Hu

000292 Measuring Liquid-level Utilizing Wedge Wave 112I. Matsuya, Y. Honma and I. Ihara

000298 Influence of Acoustic Cavitation Bubbles on Tough Hydrophone in High-intensity Acoustic Fields Generated by 22 kHz Sonoreactor

112

N. Okada, M. Shiiba, S. Yamauchi, T. Sato and S. Takeuchi

Physical Acoustics

000027 Effect of Frequency on Generation of Ultrafine Bubble by Ultrasonic Irradiation 113Y. Asakura, H. Matsushima and K. Yasuda

000050 Development of magnetostrictive FeCo film coated surface acoustic wave basedmagnetic field sensor

113

W. Wang, Y. Jia, X. Liu, Y. Liang and S. He

000061 Image Analysis of Hydrodynamic-Acoustic-Cavitation 114L. Bai, P. Wu and W. Lin

000062 Surface Oscillations and Fragmentation of Bubbles in an Acoustic Field 114P. Wu, L. Bai, W. Lin, D. Xu and C. Li

000063 Image Analysis of Hydrodynamic-Acoustic-Cavitation 114P. Wu, L. Bai, W. Lin, D. Xu and C. Li


000075 Thermal Tuning on the Band Gaps with Temperature Sensitive Materials inPhononic Crystals

115

Y. Li

000078 Research on A Surface Acoustic Wave Based PM2.5 Monitor 115J. Liu, W. Hao and S. He

000090 Attenuation Characteristics of Acoustic Waves in Boiler Flue gas ContainingSolid Particles

115

G. Jiang and W. Xu

000100 Performance evaluation of array transducer for underwater acoustic camera 116C.-S. Park and S. Cho

000107 Study on characteristics of the suspension of the particle in thermoacousticsystems

116

S. Yang, X. Xie, F. Liu and Q. Li

000130 Experimental realization of nonreciprocal topological insulators based onangular-momentum-biased resonator array

116

Y. F. Zhu, Y. G. Peng, J. Yang, X. Y. Zou, B. Liang, X. F. Zhu and J. C. Cheng

000131 Long-Term Monitoring of Underwater Sound near the Eastern Coast of Koreausing a Four-Element Planar Hydrophone Array

117

S.-H. Byun, S.-M. Kim, I.-Y. Che and Y. Kim

000158 Development of ultrasound measurement system to measure acoustic propertiesof the piston core sediments laboratory condition

117

B.-N. Kim, S. K. Jung, B.-C. Kum, B. K. Choi, E. Kim and S. H. Kim

000159 Broadband ultrasound backscattering of cylindrical target in water 117B. K. Choi, B.-N. Kim, E. Kim, S. H. Kim and M. S. Sim

000161 Surface Wave Propagation on Single Crystals: Measurement and FEM Analysis 118H.-B. Kim, H. S. Park, H.-S. Lee, H.-S. Lee and Y. H. Kim

000178 Acoustic Energy Harvesting based on Metastructures 118B. Assouar, S. Qi and Y. Li

000192 Asymptotic Behaviour of 1D Sonic Crystal Band Structure with Applicationsin Optimization

118

M. I. Pop, N. Cretu and A. Boer

000222 Characterization of grain boundary cracks by evaluating the integral responseof surface acoustic waves

119

R. Galos, S. Zamiri, P. Burgholzer, T. Berer and I. A. Veres

000268 Planar acoustics lenses with helical-structured metamaterials 119S. Liu, H. Lv, W. Zhang, J. Zhang and L. Yang

000295 Frequency characteristics of thickness-shear mode BAW resonator consisting ofc-axis parallel oriented ZnO film for liquid viscosity measurement

120

I. Rikuya, S. Takayanagi, M. Matsukawa and T. Yanagitani

000304 Study of shear mode acoustic wave devices with c-axis parallel oriented ZnOfilm to measure the liquid loading properties

120

K. Mori, S. Takayanagi, M. Matsukawa and T. Yanagitani

000309 Sound Blocking using A Series of Scaled Composite Structures 121S. Park and J. Kim

000310 Single Sensor Acoustic Tracking using Asymmetric Impedance MetamaterialSurface

121

C. Kim, K. Song and J. Kim


000313 Numerical investigation of the nonlinear dynamics of dense polydisperse cloudsof interacting microbubbles

121

H. Haghi, A. Jafarisojahrood and M. C. Kolios

Wednesday 20 December 2017

Acoustic and Elastic Metamaterials 4Room: 304ATime: 8:00Chair: J. Christensen, A. Merkel

8:00 Manipulating Sound Wave Radiation by Zero-index Metamaterials 122X. Liu, J. Liu, Y. Mao and E. Ding

8:15 Sub-wavelength acoustic microscope based on extraordinary transmission in azero-mass metamaterial

122

T. Devaux, J. J. Park, E. Bok, S. H. Lee and O. B. Wright

8:30 A multi-scale insight into the dynamic behavior of acoustic metamaterials 123K. Chrzaszcz, V. G. Kouznetsova, J. P. Hoefnagels and M. G. Geers

8:45 Acoustic invisibility based on transparent anisotropic metamaterials 123B. Li and W. Kan

9:00 Band gap and double negative properties of star-structured sonic metamaterial 123W. Yuren, C. Meng, J. Heng, L. Yu and X. Wenshuai


Time: 8:00

Chair: K. M. Tant

8:00 Induced phonons by pulse laser technique to improve Brillouin scattering mea-surement

123

A. Perino, M. Matsukawa and Y. Shibagaki

8:15 Non-contact Detection of A Foreign Material Inside Soft Material by Using AHigh-intensity Aerial Ultrasonic Wave and Optical Equipment

124

L. Jin, A. Osumi and Y. Ito

8:30 Material Property Mapping using Ultrasonic Travel-time Tomography for Im-proved Imaging in Heterogeneous Media

124

K. M. Tant and A. J. Mulholland

8:45 In-situ characterization of phase transitions by ultrasonic methods 125J. Nejezchlebova, H. Seiner, P. Sedlák, M. Janovská, P. Stoklasová, M. Landa and T. Grabec

9:00 Investigating Ultrasound Interaction Behaviors with Defects in Infrared ImagingNDE

125

X. Han and Q. Yu

9:15 Resonant Ultrasonic Activation of Damage: A Shortcut to Efficient NDE andDiagnostic Imaging

125

I. Solodov


High-frequency Ultrasound and Cell ImagingRoom: 309

Time: 8:00

Chair: J. Y. Hwang

8:00 High Frequency Ultrasound Transducers for High Definition Imaging∗ 126H. H. Kim

8:25 The New Intracellular Delivery Platform using High Frequency Ultrasound∗ 126S. Yoon

8:50 4D High-Frequency Ultrasound Imaging of Small Animal Embryonic Heart toSupport Computational Flow Simulation Studies

127

C. H. Yap, S. Ho, G. X. Y. Tan, T. J. Foo and N. Phan-Thien

9:05 High Resolution Facial Skin Imaging with Three-dimensional Ultrasound Mi-croscope

127

S. Yokoshiki, M. Maeda and Y. Saijo

9:20 The optimized high frequency intravascular ultrasound transducer design forvisualizing bioresorbable scaffold∗

128

J. Park

Picosecond Laser Ultrasonics 2Room: 307B

Time: 8:00

Chair: O. Matsuda

8:00 Gigahertz Ultrasonics in Metamaterials∗ 128O. B. Wright

8:25 Picosecond Acoustic Computed Tomography in a Microscopic Fibre 128S. Mezil, P. H. Otsuka, M. Tomoda, O. Matsuda and O. B. Wright

8:40 Imaging subsurface features in a micro-scale slab using laser ultrasonics at GHzfrequencies

129

P. H. Otsuka, K. Miyoshi, S. Mezil, M. Tomoda, O. Matsuda and O. B. Wright

8:55 GHz frequency S1 Lamb mode resonator 129D. M. Photiadis, M. K. Zalalutdinov, S. G. Carter, A. S. Bracker, M. Kim, C. S. Kim, D.G. Gammon and B. H. Houston

9:10 Imaging of Buried Microstructures by Nonlinear Picosecond Laser Ultrasonics 130B. Perrin, E. Péronne, L. Belliard and L. Becerra

9:25 Single Nanowire acting as Acoustic Resonator and Emitter 130L. Belliard, C. Jean, T. W. Cornelius, O. Thomas, Y. Pennec, M. Cassinelli, M. EugeniaToimil-Molares and B. Perrin

9:40 Guide wave excitation and detection in a single nanowire 131A. Nagakubo, T. Taniguchi, H. Ogi and T. Ono

Reservoir Acoustics and Borehole Acoustic Logging 2Room: 306

Time: 8:00

Chair: H. Hu, X. Wang

8:00 A Pilot Test of Ultrasonic Viscosity Reduction of Heavy Crude Oil in Oilfield 131D. Xu, C. Li, J. Deng, W. Lin and L. Bai

8:15 Scalable Time Series Feature Engineering Framework to Understand MultiphaseFlow using Acoustic Signals

131

M. K. Mudunuru, V. K. Chillara, S. Karra and D. Sinha


8:30 A Spectral Gamma Ray Logging Tool with 57mm Outer Diameter for DeepMineral Resources Prospecting

132

D. Xu, W. Ma and X. Wang

Acoustic Metasurfaces and Topological MetamaterialsRoom: 307B

Time: 10:00

Chair: B. Assouar

10:00 Wavefront Manipulations via Acoustic Metasurfaces∗ 132Y. Li, B. Liang, J. C. Cheng, L. Zhang and Y. Jing

10:25 Topologically protected acoustic helical edge states and interface states in acous-tic networks∗

133

Y. X. Shen, Y. G. Peng and X. F. Zhu

10:50 Broadband Coherent Perfect Absorption of Acoustic Waves with Bubble Meta-Screens

133

M. Lanoy, R.-M. Guillermic, A. Strybulevych and J. H. Page

11:05 Optical holographic imaging of three-dimensional complex ultrasonic field 133Q. Cheng, X. Zheng, Y. Li, M. Qian, Q. Zhan and X. Wang


Time: 10:00

Chair: Y. Pennec

10:00 Optimization Design and Experimental Evidence of Light-Weighted LatticeStructures with Wide Bandgaps∗

134

Y.-S. Wang, H.-W. Dong, Y.-F. Wang, C.-L. Yang and C. Zhang

10:25 Strong Coupling of Phononic Cavity Modes in 1D Corrugated Nanobeam 134Y. Pennec, A. Korovin and B. Djafari-Rouhani

10:40 Loss Compensation in Time-Dependent Elastic Metamaterials 134D. Torrent, W. Parnell and A. Norris

10:55 A high-quality narrow passband filter for elastic SV waves via aligned parallelseparated thin polymethylmethacrylate plates

135

J. Zhang, Y. Liu, W. Yan and N. Hu


Time: 10:00

Chair: B. Helfield, T. J. Matula

10:00 Cavitation biophysics: single-cell observations of sonoporation episodes∗ 135A. C. Yu

10:25 Biophysics of Sonoporation∗ 136B. Helfield

10:50 Inactivation of Planktonic Escherichia Coli by High Intensity Focused Ultra-sound Pulses∗

136

T. J. Matula, A. A. Brayman, B. E. Macconaghy, Y.-N. Wang, K. T. Chan, W. L. Monsky,V. P. Chernikov, S. V. Buravkov and V. A. Kohklova

11:15 Ultrasonic treatment for marine growth and its verification through sea-trial 136J. Lee and J. Park



Time: 10:00

Chair: A. Feeney

10:00 Residual stress estimation using acoustoelastic effect of surface acoustic wave 137J. Jun, Y.-D. Shim, K.-Y. Jhang, J. You and C. H. Lim

10:15 Development of Defect Sizing Algorithm for Surface Micro-Defect Using theLeaky Rayleigh Wave

137

Y. T. Yeom, Y. S. Lim, H. J. Kim, S. J. Song, S. D. Kwon and S. W. Yoo

10:30 Interrogation of Lamb Wave Interaction with Disbond in Adhesively BondedJoint

138

M. Liu and F. Cui

10:45 Characterisation and Modelling of Surface Wave EMATs for Optimal Coil De-sign

138

C. B. Thring, S. Hill, A. Feeney, S. Dixon and R. S. Edwards

11:00 Tungsten Thin Film Thickness Cartography With Nanometric Resolution UsingPicosecond Ultrasonics

139

A. Abbas, X. Tridon and J. Michelon

11:15 Fabrication and Characterization of Fluoropolymer-Based Spherically FocusedAir-Coupled Ultrasonic Transducer

139

L. Tong, Y. Xiang, M. Deng, J. Pan, Y. Chen and Q. Cheng

11:30 Facile Measurements of Single-Crystal Elastic Constant Tensor Properties fromPolycrystalline Samples

139

X. Du

Ultrasonic Transducers for Imaging and TherapyRoom: 309

Time: 10:00

Chair: V. A. Khokhlova, O. A. Sapozhnikov

10:00 Image-guided Transcranial Focused Ultrasound Using Dual-mode Arrays 140E. S. Ebb

10:15 Reconstruction of Nonlinear Ultrasound Field of an Annular Therapeutic Arraywith Electronic Focus Steering Based on Acoustic Holograms of Its IndividualElements

140

V. A. Khokhlova, P. Yuldashev, P. Rosnitskiy, O. A. Sapozhnikov, E. Dumont, M. Hoogen-boom, M. Den Brok, J. Futterer and G. Adema

10:30 Shape Optimization of Lens Focused Piezoelectric Transducers 141G. P. Thomas, J.-Y. Chapelon and C. Lafon

10:45 The Effect of Driving Conditions on the Performance of an Ultrasonic BoneBiopsy Needle

141

R. Cleary and M. Lucas

11:00 Imaging of Scatterer Distribution Structure of Living Tissue based on EmpiricalBayesian Learning with Consideration of Statistical Properties

142

J. Zhu and N. Tagawa


Abstracts

Mon 10:00 306 Plenary Lecture 1

The best sonar system on this planet: the ultrasonic sonar of dolphins – (000328)

W. AuHawaii Institute of Marine Biology, P.O. Box 1346, Kaneohe, 96744, USA

Corresponding author E-mail: [email protected]

Dolphins have very sophisticated short-range sonar thatsurpasses all technological sonar in its capabilities to per-form complex target discrimination and recognition tasks.The system that the U.S. Navy has for detecting minesburied under ocean sediment is one that uses Atlanticbottlenose dolphins. However, close examination of thedolphin sonar system will reveal that the dolphin acoustic”hardware” is fairly ordinary and not very special. Thetransmitted signals have peak-to-peak amplitudes as highas 225 - 228 dB re 1 µPa which translate to an rms valueof approximately 210 - 213 dB. The transmit beamwidthis fairly broad at about 10o in both the horizontal andvertical planes and the receiving beamwidth is slightlybroader by several degrees. The auditory filters are notvery narrow with Q values of about 8.4. Despite thesefairly ordinary features of the acoustic system, these an-imals still demonstrate very unusual and astonishing ca-pabilities. The dolphin biosonar system will be discussed

from the perspective of a technological sonar system start-ing with how the broadband signal is generated with itscharacteristics dependent on the intensity of the signal andhow this signal propagates through the head forming abeam and making a transiting from the near field into thefar field. The presentation will also discuss the receptionof echoes including receiving sensitivity, directivity, andinternal filtering process, and a signal processing section.Some of the capabilities of the dolphin sonar system willbe presented and the reasons for their keen sonar capabil-ities such as discriminating and recognizing different fishspecies, differences in wall thickness of metal cylinders anddifferences in the composition of metallic targets will bediscussed. Important features of their sonar include thebroadband click-like signals used, adaptive sonar searchcapabilities and large dynamic range of its auditory sys-tem.

Mon 8:00 304A Acoustic Fluidics

Spreading of Water Drop On a Vibrating Surface – (Contributed, 000007)

N. Candia Muñoza, L. Gaete-Garretónb, Y. Vargas-Hernándezb and J. Meneses-Dı́azcaUniversidad de Santiago de Chile, Av Ecuadore 3493, Estacion Central, Santiago, Chile, 9170124 Santiago, Chile; bUniversidad de

Santiago de Chile, Av Ecuador 3493, Estacion Central, Santiago, Chile, 9170124 Santiago, Chile; cUNIVERSIDAD DE SANTIAGO

DE CHILE, Av Ecuador 3493, estacion central, santiago, 9170124 Santiago, Chile


Since of illuminating work of Faraday the knowledge ofthe behavior of a liquid on a vibrating surface is growingconstantly, however, too many aspects of the problem con-tinued open until today. In the present time, the effects ofa vibrating surface in a liquid can be classified in at leastthree branches: liquid in a layer, liquid in fountains anddrops of liquids.One of the more interesting aspects of vibrations and liq-uids is its wettability; it is related to surface energiescomprising solid-vapor, solid-liquid and liquid-vapor inter-faces. Many industry and technology applications, such asprint, paint, inject, lubrication, surface engineering, etc.,have a great interest to enhance the wettability. One wayto enhance the wettability of a liquid on a surface is addinga chemical surfactant, particles or another chemical mix-ture to a solution or suspension. This technique has thedisadvantage that sometimes changes the chemical com-position of the samples, which very often is not desired.

One previous experimental work has shown that the ap-plication of vertical vibrations on a solid surface increasesits wettability. The wettability study from a point of viewmore complete than the former, working at a greater fre-quency range and studying the transient stage during thedrop spreading until it reaches an equilibrium position isconsidered in this paper. In particular, the time of appari-tion of capillary waves is considered. In our opinion, thispoint of view allows a better understanding of the com-plex phenomena involved in the wettability studies. Inaddition, it was developed a new algorithm to calculatecontact angle of a water drop placed on a set of vibratingsurfaces driven by piezoelectric transducers of own design.The study of kinetic of the radius and contact angle willcarry out through the image analysis captured by a fastcamera.

[email protected] [email protected]



Measurement and Simulation of Acoustic Radiation Force from Focused Ultrasound Beam Acting ona Spherical Scatterer in Water – (Contributed, 000197)

M. M. Karzovaa, A. V. Nikolaevaa, S. A. Tsysara, V. A. Khokhlovaa and O. A. Sapozhnikova,baPhysics Faculty, Moscow State University, Leninskie Gory, 119991 Moscow, Russian Federation; bApplied Physics Laboratory, Uni-

versity of Washington, 1013 NE 40th Street, Seattle, WA 98105, USA


Acoustic radiation force (ARF) has been successfully usedin a recently developed therapeutic technology for kid-ney stone propulsion. To plan the treatment and predictthe outcome of the procedure, calibration of ARF has tobe performed for stones of different dimensions and loca-tions. However, such calibration remains a problem. Here,a method for measuring ARF acting on a mm-sized spher-ical object positioned on the axis of a focused ultrasoundbeam was proposed and tested. The method is based onthe balance between different forces acting on the objectand initiation of its movement when the value of ARFcrosses a certain threshold. Spherical scatterers made fromnylon, steel, and glass were used as targets; their diam-eters varied from 2 to 8 mm. Single-element 1.072 MHztransducer (100 mm aperture and 70 mm focal length) waspositioned in water at the bottom of the tank and used togenerate a focused ultrasound beam in vertical direction.

Scatterers were positioned at different distances along thebeam axis. For each scatterer, the beam power was grad-ually changed until the scatterer started to move. At thisthreshold power of the source, the value of ARF was deter-mined as a difference between the gravity and buoyancyforces acting on the scatterer. At other source power out-puts, the value of ARF was linearly scaled. ARF was alsocalculated from pressure distributions reconstructed fromacoustic hologram of the source and physical parameters ofthe scatterers. Experimental and theoretical results werefound in a good agreement. It was shown that dependingon the scatterer parameters, the maximum ARF occurredbefore or after the focus, while the most effective pushingwas observed at distances where the beam was slightlywider than the scatterer. Work supported by the stipendof the President of Russia (SP-2621.2016.4).


Elucidating the Mechanism of Paracetamol Sonocrystallization for Product Purity Enhancement –(Contributed, 000287)

C. Forbesa, T. T. Nguyenb, R. L. Learyc and C. J. PricebaEPSRC Centre for Continuous Manufactuing and Crystallisation, University of Strathclyde, Technology and Innovation Centre, 99

George Street, G1 1RD Glasgow, UK; bDepartment of Chemical and Process Engineering, University of Strathclyde, James Weir

Building, 75 Montrose Street, G1 1XJ Glasgow, UK; cCentre for Ultrasonic Engineering, University of Strathclyde, 204 George Street,

G1 1XW Glasgow, UK


Pharmaceutical revenue exceeds $1 trillion per year, withraw material and manufacturing costs accounting for 22%of the total. Product manufacture and purification is typ-ically achieved via solution based crystallization. This ap-proach can give rise to loss of raw material to waste due toincomplete utilisation of the solute in the crystallisationprocess - exacerbated by retardation of crystal growth dueto poisoning of the growth surface by isomers of the de-sired crystal form.In this paper we describe the effect of ultrasound on thecrystallization of paracetamol undertaken in organic sol-vents in a temperature controlled XUB25 ultrasonic bath(Grant Instruments). Sonomechanical activity within thesolvent arsing in the XUB25 ultrasonic bath was char-acterised by measurement of acoustic intensity using aNH4000 PVDF needle hydrophone. Application of ultra-sound was found to increase the nucleation temperature ofthe crystallization, modify the size and morphology of theresultant product and importantly improve product yield.

A number of phenomena arise from the application of ul-trasound, including cavitation, acoustic streaming and en-hanced mixing of the solution. In order to further explorethese phenomena in the context of paracetamol crystal-lization, we explore the acoustic properties and cavitationthreshold in organic solvents, namely isoamyl alcohol andethanol. The necessary acoustic properties of the solventsare used to construct acoustic field models for comparisonin an effort to link prediction and measurement of cavita-tion with crystallization outcomes.The ultimate goal is to elucidate the mechanisms ofsonocrystallization via acoustic cavitation and streaming,with a focus on nucleation and impurity incorporation dur-ing crystal growth. The adoption of acoustic simulationand field characterisation techniques is required to designprocesses and equipment to implement sonocrystallizationin pharmaceutical manufacturing. The industrial driver isto improve the product quality, reduce waste and improveaccess to medicines.




Recent Advances and Opportunities of Mechanical Metamaterials – (Contributed, 000315)

E. G. Karpov and L. A. DansoUniversity of Illinois at Chicago, Department of Civil and Materials Engineering, 842 W Taylor St, M/C 246, Chicago, 60607, USA


Mechanical metamaterials represent a novel interestingclass or structural composites that manifest behaviors be-yond the scope of traditional materials mechanics. Thoseinclude negative elastic moduli [1-3] and basic symmetriesbreaking, such as reciprocity of mechanical deformation.The ongoing research aims to understand relationships be-tween a desired property, which often corresponds to anexotic domain in the overall design space, and the mate-rial’s internal structure. Some recent studies use multi-stabilities at the unit cell level to deploy a load-inducedpolymorphic phase transformation in an entire material

sample. When properly designed, this phase transforma-tion can lead to a contraction of the sample in the direc-tion of an increasing load, a manifest of the negative ex-tensibility phenomenon. Other studies suggest that prop-erly designed highly nonlocal periodic lattices can providemetamaterials featuring reversal of the Saint-Venant edgeeffect. In this presentation, we overview recent develop-ments in the analysis and design of these interesting mate-rial systems, and outline their opportunities for nonlinearacoustics and structural health monitoring.

Mon 8:00 308B Bubbles and Cavitation 1

Lipid Intermolecular Forces and Microbubble Resonance – (Invited, 000150)

M. BordenUniversity of Colorado, 1111 Enigneering Drive, Boulder, 80309-0427, USA


An intermolecular forces model for the lipid shell will beintroduced that provides calculation of the shell elasticitydirectly from first-principle intermolecular pair potentials.Additionally, a new laser acoustics technique will be pre-sented that allows measurement of microbubble shell elas-ticity and viscosity for very small-amplitude oscillations.Results from experiments on microbubbles with differentlipid shell compositions and at different temperatures willbe discussed. As predicted by the model, a significantincrease in surface elasticity at room temperature was ob-served for lipid acyl-chain lengths of 16 to 20 carbons. The

surface viscosity was found to be equivalent for these lipidshells. We also observed an anomalous decrease in elas-ticity and increase in viscosity when increasing the acylchain length from 20 to 22 carbons, indicating that mi-crostructural effects may be important for such small dis-placements. For DPPC shells, we observed a nearly lineardecrease in elasticity and viscosity with increasing temper-ature. Transient effects in viscoelasticity were observed forrapidly heated microbubbles. The talk will conclude withinsights gleaned from the molecular model on resonanceeffects for larger amplitude oscillations.


High-Precision Acoustic Measurements of the Nonlinear Dilatational Elasticity of Phospholipid-CoatedMonodisperse Microbubbles – (Invited, 000190)

T. Segersa,b, E. Gauda, M. Versluisc,d,e and P. FrinkingaaBracco Suisse S.A., Route de la Galaise 31, 1228 Geneva, Switzerland; bUniversity of Twente, Drienerlolaan 5, 7522 NB Enschede,

Netherlands; cInstitute of Biomedical Engineering, Physics of Fluids group, University of Twente, P.O. Box 217, 7500 AE Enschede,

Netherlands; dMESA+ Institute for Nanotechnology, University of Twente, P.O. Box 217, 7500 AE Enschede, Netherlands; eMIRA

Institute for Biomedical Technology and Technical Medicine, University of Twente, P.O. Box 217, 7500 AE Enschede, Netherlands


The acoustic response of phospholipid coated ultrasoundcontrast agents (UCA) is dramatically affected by the sta-bilizing shell around the microbubbles. The elasticity ofthe microbubble shell increases the resonance frequency,and its nonlinear behavior promotes the generation of har-monic echoes that are currently exploited for contrast-enhanced ultrasound imaging. The harmonic scattering ofcontrast bubbles has been quite successfully modelled bythe rather ad-hoc assumptions in the model of Marmot-

tant et al., where the nonlinear behaviour was capturedin a linear elastic part around equilibrium, a rupturedpart for bubble expansion and a buckling part upon bub-ble compression. Here we present for the first time high-precision experimental data of acoustic measurements ofthe exact non-linear behavior of these bubbles. Microbub-ble viscoelastic shell properties were measured as a func-tion of the ambient pressure-controlled surface dilatation(pressures ranging from 70 to 140 kPa) through acoustic

[email protected] [email protected] [email protected]


attenuation spectra of monodisperse bubble suspensionsformed by flow-focusing. The bubble samples had meanradii ranging from 1.5 to 3.3 µm, with a typical PDI of5%, and the bubbles were coated by DPPC and DPPE-PEG5000 mixed at PEG molar fractions of 5.0, 7.5, and10.0%. Bubble size as a function of ambient pressure wasmeasured optically. The obtained dilatational elasticitywas found to be independent of the absolute microbub-ble size and PEG molar fraction. However, in contrastto the constant elasticity in the Marmottant model for

elastic oscillations, shell elasticity was found to be highlydependent on the surface dilation. The dilatational elas-ticity curve was integrated with respect to bubble areato find the dilatational interfacial tension of phospholipid-coated microbubbles. For compressed bubbles, it increasesduring decompression, first rapidly, and then more slowlyfrom zero to the surface tension of the surrounding aque-ous medium. This new insight will allow for more accuratemodeling of nonlinear bubble dynamics.


Propagation of ultrasound through a microbubble population: Effect of ultrasound pressure, frequency,microbubble concentration and lipid shell properties – (Invited, 000311)

A. Jafarisojahrooda, Q. Lib, H. Haghic, R. Karshafiand, T. M. Portere and M. C. KoliosfaRyerson University, 350 Victoria Street, Toronto, Canada M5B2K3; bBoston University, 110 Cummington St. ENG 319, Boston,

MA, Boston, Canada 02215; cRyerson University, 350 Victoria Street, Toronto, ON, Canada M5B2K3; dRyerson University, 110

Cummington St, Unit. 2103, Boston, Canada 02215; eBoston University, 110 Cummington St, Boston, Canada 02215; fRyerson

University, 350 Victoria Street, Toronto, AB, Canada M5B2K3


The existence of MBs in a medium increases the mediumattenuation and changes the sound speed; these changesare nonlinear and depend on the dynamics of the MBsexposed to the ultrasound (US). Knowledge of how atten-uation and sound speed vary as a function of US pres-sure, frequency and MB concentration can help to opti-mize US parameters in applications. Our recently devel-oped model is used to calculate changes in attenuationand sound speed as a function of frequency and pressure.The Marmattont model was modified to include the mul-tiple scattering of up to 200 MBs and was solved usingour novel approach for solving for MB-MB interactions.The MBs were randomly distributed within a cube; thelength of each edge of the cube was varied to achieve a de-sirable concentration (200 micron-1mm). At each acousticparameter, the attenuation and sound speed were calcu-lated for 20 random distributions of MBs, and the resultswere weighted by the number density of each MB sizes

in experiments. Attenuation and sound speed were mea-sured experimentally using transmission and reception ofbroadband pulses of center frequency of 2.25 MHz, andpressure amplitudes of 10-120kPa through monodispersesolutions (mean diameter ∼6 microns) with different con-centrations. The results of numerical simulations with-out MB interactions are in good agreement with the ex-perimental observations for small concentrations. As theconcentration increases, an agreement was only achievedwhen simulations included MB-MB interaction. For highconcentrations and low pressures the attenuation peak be-comes wider and does not have a distinct peak. As thepressure increases, multiple peaks appear in the attenu-ation vs. frequency diagrams. Results of this work sug-gest that MB shell characterization is more accurate ifexperiments are done in low concentrations (the optimumconcentration depends on size). For higher MB concen-trations, MB-MB interaction must be included.

Mon 8:00 307B Optomechanical Structures and Opto-acoustics

Proposal for optical beam-steering with optomechanical antennas on a silicon chip – (Invited, 000241)

R. Van Laer, C. J. Sarabalis and A. H. Safavi-NaeiniStanford University, 348 Via Pueblo Mall, Stanford, CA 94305, USA


Rapid and low-power control over the direction of light is amajor challenge in photonics and a key enabling technol-ogy for emerging free-space optical communication linksand sensors such as lidar. Current approaches based onbulky motorized components are limited by their high costand power consumption, while on-chip optical phased ar-rays face challenges in scaling and programmability. Inthis talk we propose a new chip-based approach to beam-steering using optomechanical antennas. We combine therecent progress in simultaneous control of optical and me-chanical waves with advances in on-chip optical phased

arrays to enable efficient and full two-dimensional beam-steering of monochromatic light. We present calculationsfor a silicon system made of nanoscale photonic-phononicwaveguides, predicting that thousands of resolvable spotscan be addressed with milliwatts of mechanical power. Us-ing mechanical waves as active gratings will allow us toquickly reconfigure the beam direction, beam shape andthe number of beams. By non-reciprocity it also will alsoenable us to distinguish between light that we send andreceive.



Mon 8:25 307B Optomechanical Structures and Opto-acoustics

Non-reciprocal and chiral acoustics in optomechanical systems – (Invited, 000327)

G. BahlUIUC, 1206 W. Green St., MEL 4413, Urbana, 61801-2906, USA


Time-reversal symmetry is a property shared by wavephenomena in linear stationary media. However, brokentime-reversal symmetry is required for synthesizing non-reciprocal devices like isolators, circulators, gyrators, andfor topological systems supporting chiral states. Magneticfields can of course enable nonreciprocal behavior for elec-tromagnetic waves, but this method does not convenientlytranslate to the chip-scale or to the acoustic domain, com-pelling us to search for nonmagnetic solutions.We have adopted a unique approach to address this chal-lenge through the use of co- localized interacting modesof light and sound in resonator systems. The acousto-op

publication year: 2017icu2017/20171205... · 12/5/2017 · suk wang yoon, ph.d. president,...

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