Non-contact mode excitation of small structures in air using ultrasound radiation force Acoustical Society of America Meeting: May 17, 2005 Thomas M. Huber,

Slides:



Advertisements
Similar presentations
Normal mode method in problems of liquid impact onto elastic wall A. Korobkin School of Mathematics University of East Anglia
Advertisements

Chapter 9b: Example of a Micromachined Device: The SA30 Crash Sensor from SensoNor Picture shows the interior chip assembly of SensoNor’s SA30 Crash Sensor.
Shaker training March 2011 Renard Klubnik Applications engineer The information contained in this document is the property of Meggitt Sensing Systems and.
Design and Simulation of a Novel MEMS Dual Axis Accelerometer Zijun He, Advisor: Prof. Xingguo Xiong Department of Electrical and Computer Engineering,
slide 1 Measuring Natural Frequency and Non-Linear Damping on Oscillating Micro Plates ICEM 13 Alexandroupolis, Greece July 1-5, 2007 Sandia is a multiprogram.
MEMS Tuning-Fork Gyroscope Group 8: Amanda Bristow Travis Barton Stephen Nary.
Resonance and Sound Decay: A Quantitative Study of Acoustic guitars Acoustical Society of America Meeting October 3, 2005 by Erika Galazen and Joni Nordberg.
Dr. Adnan Dawood Mohammed (Professor of Mechanical Engineering)
HIGH CYCLE FATIGUE DELAMINATION MEASUREMENT AND GROWTH PREDICTION
S M T L Surface Mechanics & Tribology Laboratory 3 rd Generation Device Design D S S S D D Driving/sensing setup allows for separate driving and sensing.
Slide 1 Assignment 3. Slide 2 PROBLEM 1 Calculate the maximum deflection in a beam clamped at the both ends as shown in Figure below where the thickness.
Imaging of flexural and torsional resonance modes of atomic force microscopy cantilevers using optical interferometry Michael Reinstaedtler, Ute Rabe,
GENERATING AND DETECTING OF ULTRASOUND
Ultrasound – Physics & Advances
Benoit BOLZON Nanobeam 2005 – Kyoto Active mechanical stabilisation LAViSta Laboratories in Annecy working on Vibration Stabilisation Catherine ADLOFF.
Sound II Physics 2415 Lecture 28 Michael Fowler, UVa.
Noncontact modal testing of hard-drive suspensions using ultrasound radiation force Acoustical Society of America Meeting: October 18, 2005 Thomas M. Huber.
Selective modal excitation using phase- shifted ultrasound radiation force Acoustical Society of America Meeting June 2006 Thomas M. Huber Physics Department,
GWADW, May 2012, Hawaii D. Friedrich ICRR, The University of Tokyo K. Agatsuma, S. Sakata, T. Mori, S. Kawamura QRPN Experiment with Suspended 20mg Mirrors.
LISA STUDIES AT THE UNIVERSITY OF COLORADO Michael J. Nickerson, Ellery B. Ames, John L. Hall, and Peter L. Bender JILA, University of Colorado and NIST,
George David Associate Professor Ultrasound Physics 04: Scanner ‘97.
Suspension Design Progression for Increasing Shock Performance Jacob Bjorstrom Sr. Product Design Eng. Hutchinson Technology September 22, 2004 DISKCON.
Abstract: A laser based ultrasonic technique for the inspection of thin plates and membranes is presented, in which Lamb waves are excited using a pulsed.
L 23 – Vibrations and Waves [3]  resonance   clocks – pendulum   springs   harmonic motion   mechanical waves   sound waves  golden rule for.
ACOUSTIC JOURNAL BEARING – A SEARCH FOR ADEQUATE CONFIGURATION Tadeusz Stolarski Rafal Gawarkiewicz Krzysztof Tesch ITC 2015, Tokyo, Japan Gdansk University.
Excitation of Vibrational Eigenstates of Coupled Microcantilevers Using Ultrasound Radiation Force ASME 2nd International Conference on Micro and Nanosystems.
Thomas M. Huber, Brian Collins
Resonance Chapter 4. Concert Talk Resonance: definition When a vibrating system is driven by a force at a frequency near the natural frequency of the.
Noncontact Modal Analysis of a Pipe Organ Reed using Airborne Ultrasound Stimulated Vibrometry May 25, 2004 Acoustical Society of America Meeting Thomas.
Chapter 10 Sinusoidally Driven Oscillations Question of Chapter 10 How do the characteristic frequencies generated in one object (say a piano string)
L 23 – Vibrations and Waves [3]  resonance   clocks – pendulum   springs   harmonic motion   mechanical waves   sound waves  golden rule for.
Ultrasound Physics Reflections & Attenuation ‘97.
An alternative spectrograph mount Bruce C. Bigelow University of Michigan Department of Physics 5/14/04.
AY-REU Project 7: Functional Model of a Cadaveric Human Middle Ear William Holden, Senior Chemical Engineering Margaret Welch, Pre-Junior Biomedical Engineering.
Cavity support scheme options Thomas Jones 1. Introduction Both cavities will be supported by the fundamental power coupler and a number of blade flexures.
G Z Test Mass Butterfly Modes and Alignment Amber Bullington, Stanford University Warren Johnson, Louisiana State University LIGO Livingston Detector.
Noncontact Modal Excitation of Small Structures Using Ultrasound Radiation Force Society for Experimental Mechanics Annual Meeting Springfield, MA June.
Charles University Prague Charles University Prague Institute of Particle and Nuclear Physics Absolute charge measurements using laser setup Pavel Bažant,
Advanced LIGO UK 1 IGRQA0003 LIGO-G K Modal testing facility for Advanced LIGO Caroline Cantley University of Glasgow Advanced LIGO SUS Workshop,
L 23 – Vibrations and Waves [3]  resonance   clocks – pendulum   springs   harmonic motion   mechanical waves   sound waves  golden rule for.
Piezoelectric Effect  Sound waves striking a PZ material produce an electrical signal  Can be used to detect sound (and echoes)!
Physics Section 12.3 Apply the properties of sound resonance Recall: A standing wave is the result of the superposition of a wave and its reflection from.
Hcal Geometry and Assembly Videoconference January 2008, 24th.
3M Drug Delivery Systems 3 Chris Blatchford & Gemma Nixon, 3M Drug Delivery Systems, Morley St, Loughborough, UK. Graham Hargrave, Tim Justham & Edward.
MEMS Tuning-Fork Gyroscope Group 8: Amanda Bristow Travis Barton Stephen Nary.
SPM Users Basic Training August 2010 Lecture VIII – AC Imaging Modes: ACAFM and MAC Imaging methods using oscillating cantilevers.
Date of download: 6/20/2016 Copyright © ASME. All rights reserved.
Engineering Design of Raon SC Cavities Myung Ook Hyun SCL Team Myung Ook Hyun SCL Team.
Date of download: 6/30/2016 Copyright © 2016 SPIE. All rights reserved. Trans-cis conformational change of the azo-dyes under light irradiation. (a) Equivalent.
Date of download: 7/1/2016 Copyright © 2016 SPIE. All rights reserved. Schematic view of the layered structure of the fabricated cantilever device. Figure.
1 Challenge the future A Study on Micro-Actuators for Atomic Force Microscopes Chonghe Zhong.
Imaging of propagating wave fronts resulting from ultrasonic pulses incident on heel bones using refracto-vibrometry Acoustical Society of America Meeting.
MECH 373 Instrumentation and Measurements
BNL-SLAC-Annecy TeleConference
Spatial distribution of acoustic radiation force modal excitation from focused ultrasonic transducers in air Acoustical Society of America Meeting Boston,
Reflections & Attenuation
Single-element transducers properties
Interacting with a Ferrocell®
Linseed oil + Styrene + Divinylbenzene
Status of Vibration Measurement Work at BNL
Modelling of Atomic Force Microscope(AFM)
Active Figure 18.4 The superposition of two identical waves y1 and y2 (blue and green) to yield a resultant wave (red). (a) When y1 and y2 are in phase,
Tapping mode AFM: simulation and experiment
Progress on 1.8m Telescope with 127-element Adaptive Optics at IOE
LATERALLY-DRIVEN DEFORMATION-ROBUST MEMS GYROSCOPES
Noninvasive measurement of aortic aneurysm sac tension with vibrometry
Regulation of Airway Ciliary Activity by Ca2+: Simultaneous Measurement of Beat Frequency and Intracellular Ca2+  Alison B. Lansley, Michael J. Sanderson 
The First Free-Vibration Mode of a Heat Exchanger Lid
Volume 106, Issue 11, Pages (June 2014)
Presentation transcript:

Non-contact mode excitation of small structures in air using ultrasound radiation force Acoustical Society of America Meeting: May 17, 2005 Thomas M. Huber, John Purdham Physics Department, Gustavus Adolphus College Mostafa Fatemi, Randy Kinnick, James Greenleaf Ultrasound Research Laboratory, Mayo Clinic and Foundation

Introduction  Background material on ultrasound stimulated excitation  Study of different devices  MEMS mirror  Hard Drive HGA Suspension  MEMS Gyroscope  Conclusions

Ultrasound Stimulated Vibrometry  Pair of ultrasound beams directed at object  One ultrasound transducer differed from other by audio-range frequency  Difference frequency between ultrasound beams produces radiation force that causes vibration of object  Vibrations were detected using a Polytec laser Doppler vibrometer  In some experiments, comparison of ultrasound excitation and mechanical shaker

Experiment Details Confocal ultrasound transducer used  600 kHz broadband (>100 kHz bandwidth)  30 mm focal length; 1 mm focus spot size  Confocal (concentric elements with different frequencies)  Mounted on 3-D translation stage  Inner disk fixed at 500 kHz  Outer ring sweeps 501 – 520 kHz  Difference frequency of 1 kHz – 20 kHz Caused excitation of object

Device Tested: 2-d MEMS Mirror  Manufactured by Applied MEMS  Mirror is 3mm on Side - Gold plated Silicon  Three vibrational modes  X Axis torsion mode: 60 Hz  Z Axis torsion mode: 829 Hz  Transverse mode (forward/back): 329 Hz (incidental – not used for operation of mirror)

Selective Ultrasound Excitation of MEMS Mirror  Ultrasound focus ellipse about 1x1.5 mm  Focus position can be moved horizontally or vertically  Changing transducer position allows selective excitation  Upper figure: All modes present when focus near center of mirror.  Red line shows excitation using mechanical shaker.  Middle: X-torsional mode increases when ultrasound focus near top of mirror.  Bottom: Z-Torsional mode increases when focus near right edge

Selective Ultrasound Excitation of MEMS Mirror  X-Torsional mode peaks when focus near top/bottom of mirror  Transverse mode decreases as transducer moved vertically (smaller fraction of beam on mirror)  Ratio of amplitudes of X-Torsional to Transverse modes changes by over factor of 10x as vertical position is varied

Hard Drive HGA Suspension  HGA (Head Gimbal Assembly) suspension holds heads as they fly over the disk  Leading manufacturer: Hutchinson Technology, in Hutchinson, MN  Length about 5-10 mm, max. width about 2 mm, thickness of μm  The suspensions are engineered to have specific vibrational modes.  Quality control involves measuring mode frequencies and deflection shapes (using mechanical shaker for excitation and vibrometer for measurement)

Ultrasound excitation of HGA Suspension  Goal: To determine whether vibrational modes of suspension can be excited using ultrasound radiation force  HGA Suspension was clamped and simply supported  Confocal ultrasound transducer used to excite modes from 1 kHz to 50 kHz  Vibrometer measured resonance frequencies and deflection shapes at several ultrasound focus positions  Brüel & Kjær mechanical shaker used for comparison

Photos of Setup

Results for focused ultrasound excitation: HGA Suspension  Interference between ultrasound frequencies between 501 – 520 kHz and 500 kHz  Ultrasound focus (ellipse of about 1mm by 1.5 mm) centered on suspension (red curve) and towards edge of suspension (blue curve) Demonstrates feasibility of noncontact excitation using ultrasound radiation force. Selective Excitation: For ultrasound focus towards the edge (blue curve), large increase in amplitude of torsional modes at 6, 10, 13 and 15 kHz relative to the transverse modes at 2, 7, and 16 kHz.

Mode shapes determined using ultrasound excitation 2.0 kHz 6.0 kHz 7.2 kHz 10.8 kHz (Click on each image for animation of deflection shape)

Results for MEMS Gyroscope  Analog Devices MEMS Gyroscope  Pair of Test Masses ¾ mm square separated by 1.5 mm  14 kHz resonance frequency Variation of Ultrasound Transducer Position Mechanical Shaker Can Produce Selective Excitation of Masses Shakes Entire Structure

Conclusions Ultrasound excitation shown to be feasible for modal analysis  Allows excitation of resonances from below 1 kHz to over 40 kHz  Parts such as MEMS mirror, gyroscope and HGA suspension  Completely non-contact for both excitation and measurement  Selective excitation of torsional/transverse modes  Selective excitation by moving ultrasound focus point  Similar selective excitation using phase shift between two transducers  Special thanks to  Hutchinson Technology  Applied MEMS  Analog Devices  Polytec Incorporated