DYNAMIC ANALYSIS OF CMUTs IN DIFFERENT REGIMES OF OPERATION

Similar documents
Capacitive micromachined ultrasonic transducers

A Comparison Between Conventional and Collapse-Mode Capacitive Micromachined Ultrasonic Transducers in 10-MHz 1-D Arrays

Capacitive micromachined ultrasonic transducers

Capacitive micromachined ultrasonic transducers

BROADBAND CAPACITIVE MICROMACHINED ULTRASONIC TRANSDUCERS RANGING

High-frequency CMUT arrays for high-resolution medical imaging

VHDL-AMS Behavioural Modelling of a CMUT Element Samuel Frew University of British Columbia

Capacitive Micromachined Ultrasonic Transducers: Theory and Technology

Reconfigurable Arrays for Portable Ultrasound

Broadband Constant Beamwidth Beamforming MEMS Acoustical Sensors

MICROSONICS. Microsonics 39, rue des Granges Galand, Saint Avertin, France Phone : +(33) (0)

Diamond-Based Capacitive Micromachined Ultrasonic Transducers in Immersion

Two-Dimensional Capacitive Micromachined Ultrasonic Transducer (CMUT) Arrays for a Miniature Integrated Volumetric Ultrasonic Imaging System

886 ieee transactions on ultrasonics, ferroelectrics, and frequency control, vol. 51, no. 7, july 2004

Capacitive Micromachined Ultrasonic Transducers (CMUTs) for Photoacoustic Imaging

Evaluation of Wafer Bonded CMUTs with Rectangular Membranes Featuring High Fill Factor

A SHEAR WAVE TRANSDUCER ARRAY FOR REAL-TIME IMAGING. R.L. Baer and G.S. Kino. Edward L. Ginzton Laboratory Stanford University Stanford, CA 94305

Characterization of High Q Spherical Resonators

50 khz Capacitive Micromachined Ultrasonic Transducers for Generation of Highly Directional Sound with Parametric Arrays

Capacitive micromachined ultrasonic transducer (CMUT) arrays for medical imaging

Integrated Reconfigurable High-Voltage Transmitting Circuit for CMUTs

Micromachined ultrasonic transducers for air-coupled

Zero-Bias Resonant Sensor with an Oxide-Nitride Layer as Charge Trap

A Multichannel Pipeline Analog-to-Digital Converter for an Integrated 3-D Ultrasound Imaging System

Aging Aircraft NDE with Micromachined Ultrasonic Air Transducers

AN ULTRASOUND MODELING TOOL FOR CONTRAST AGENT IMAGING. Kangqiao Zhao, 2010, May

Noise from Pulsating Supercavities Prepared by:

CMUT as a Chemical Sensor for DMMP Detection

Broadband All-Optical Ultrasound Transducer

Ginzton Laboratory, W. W. Hansen Laboratories of Physics Stanford University, Stanford, CA 94305

Finite Element Modeling and Simulation of Ultrasonic Guided Wave Propagation using Frequency Response Analysis

Proceedings of Meetings on Acoustics

EWGAE 2010 Vienna, 8th to 10th September

Y. Huang, A. S. Ergun, E. Haeggstrom, and B. T. Khuri-Yakub E. L. Ginaon Laboratory, Stanford University Stanford, CA,

Recent developments in nonlinear ultrasonic NDE. Thomas Grimsley Ritec, Inc., Warwick, RI USA

Certificate of Accreditation

DYNAMICS OF NONLINEAR PLASMA-CIRCUIT INTERACTION *

Iterative Learning Control of a Marine Vibrator

Transmitting Performance Evaluation of ASICs for CMUT-Based Portable Ultrasound Scanners

Stresa, Italy, April 2007

Waves Q1. MockTime.com. (c) speed of propagation = 5 (d) period π/15 Ans: (c)

Ultrasound Physics. History: Ultrasound 2/13/2019. Ultrasound

High intensity and low frequency tube sound transmission loss measurements for automotive intake components

ULTRASONIC FIELD RECONSTRUCTION FROM OPTICAL INTERFEROMETRIC

Parameter Estimation Techniques for Ultrasound Phase Reconstruction. Fatemeh Vakhshiteh Sept. 16, 2010

Linear networks analysis

Texas A&M University Electrical Engineering Department ECEN 665. Laboratory #4: Analysis and Simulation of a CMOS Mixer

Acoustical cross-talk in row column addressed 2-D transducer arrays for ultrasound imaging

IN RECENT years, the ultrasound imaging has gained much

Lamb Wave Ultrasonic Stylus

THE invention of the printing press in the 15th century is

IREAP. MURI 2001 Review. John Rodgers, T. M. Firestone,V. L. Granatstein, M. Walter

LABORATORY #3 QUARTZ CRYSTAL OSCILLATOR DESIGN

Design of a Temperature-Compensated Crystal Oscillator Using the New Digital Trimming Method

This is a repository copy of Nonlinear Generation of Harmonic Content within High Intensity Ultrasound Signals using Granular Chains.

1. Introduction. 2. Concept. reflector. transduce r. node. Kraftmessung an verschiedenen Fluiden in akustischen Feldern

Analog Front End Low Noise Amplifier in 0.18-µm CMOS for Ultrasound Imaging Applications

SHORT PULSE CHARACTERIZATION OF NONLINEARITIES IN POWER ULTRASOUND TRANSDUCERS.

A High-frequency Transimpedance Amplifier for CMOS Integrated 2D CMUT Array towards 3D Ultrasound Imaging

Digital AudioAmplifiers: Methods for High-Fidelity Fully Digital Class D Systems

The Association of Loudspeaker Manufacturers & Acoustics International presents. Dr. David R. Burd

Simulation of a Capacitive Micromachined Ultrasonic Transducer with a Parylene Membrane and Graphene Electrodes

A MEMS Transducer for Ultrasonic Flaw Detection

Investigation of PDMS as coating on CMUTs for imaging

Nonlinear Effects in Active Phased Array System Performance

The Simulation for Ultrasonic Testing Based on Frequency-Phase Coded Excitation

COMPUTER PHANTOMS FOR SIMULATING ULTRASOUND B-MODE AND CFM IMAGES

Extension of X-parameters to Include Long-Term Dynamic Memory Effects

ISO INTERNATIONAL STANDARD. Non-destructive testing Acoustic emission inspection Secondary calibration of acoustic emission sensors

Resonator Factoring. Julius Smith and Nelson Lee

Optical generation of frequency stable mm-wave radiation using diode laser pumped Nd:YAG lasers

UNIT 2. Q.1) Describe the functioning of standard signal generator. Ans. Electronic Measurements & Instrumentation

Frequency f determined by the source of vibration; related to pitch of sound. Period T time taken for one complete vibrational cycle

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

FEM modeling of an entire 5-IDT CRF/DMS filter

Frequency Dependent Harmonic Powers in a Modified Uni-Traveling Carrier (MUTC) Photodetector

INTERNATIONAL STANDARD

Isolation Scanner. Advanced evaluation of wellbore integrity

INDIAN INSTITUTE OF TECHNOLOGY BOMBAY

A SAM BEARING BALL INSPECTION SYSTEM. C-H. Chou, P. Parent, and B. T. Khuri-Yakub

Measurement of the loss due to grooved bottom structure intended for use as a backing in Capacitive Micromachined Ultrasonic Transducers

Microphone Array Measurements for High-speed Train

Causes for Amplitude Compression AN 12

TOROIDAL ALFVÉN EIGENMODES

Dynamic Vibration Absorber

SELECTING RF AMPLIFIERS FOR IMPEDANCE CONTROLLED LLRF SYSTEMS - NONLINEAR EFFECTS AND SYSTEM IMPLICATIONS. Abstract

Sonic Distance Sensors

Frequency Agile Ferroelectric Filters, Power Dividers, and Couplers

CH85CH2202-0/85/ $1.00

ULTRASONIC GUIDED WAVES FOR AGING WIRE INSULATION ASSESSMENT

16.3 Standing Waves on a String.notebook February 16, 2018

Where DSP meets Measurement Science: A Sound Example. By Andrew Hurrell PhD

Theory and Applications of Frequency Domain Laser Ultrasonics

Detection of Lower Hybrid Waves on Alcator C-Mod with Phase Contrast Imaging Using Electro-Optic Modulators

PC1141 Physics I. Speed of Sound. Traveling waves of speed v, frequency f and wavelength λ are described by

A study of Vibration Analysis for Gearbox Casing Using Finite Element Analysis

EM/Circuit Co-simulation Vratislav Sokol

Capacitive Micromachined Ultrasonic Transducers for Therapeutic Ultrasound Applications

Multiple Audio Spots Design Based on Separating Emission of Carrier and Sideband Waves

From: James O'Loughlin, Diana Loree; Inventors, PL/WSR 01Nov94

Transcription:

DYNAMIC ANALYSIS OF CMUTs IN DIFFERENT REGIMES OF OPERATION Baris Bayram, Edward Hæggström, A. Sanli Ergun, Goksen G. Yaralioglu, and Butrus T. Khuri-Yakub Ginzton Laboratory, Stanford University, CA 2003 IEEE Ultrasonics Symposium, Honolulu, Hawaii This work is funded by Office of Naval Research

Outline Motivation FEM model of a single CMUT cell Dynamic FEM analysis Results Conclusion

Motivation Goal: Low voltage, high frequency CMUTs with more output power & less nonlinearity Method: Investigate different operation regimes for CMUTs: Conventional (no contact) (always in contact) Collapse-snapback (intermittent contact)

Different Operation Regimes

FEM model of a single CMUT cell Axisymmetric 2-D model Electrical Properties Structural Properties Fluid-structure Interface Acoustic Wave Equation Exact Absorbing Boundary (Grote et al) Basic Properties Collapse: 80 V Snapback: 50 V Resonance: 5 MHz

Dynamic FEM Analysis Commercially available software (ANSYS 7.1) Transient Analysis Coupled electrical & structural analysis Fluid medium Contact capability Exact absorbing boundary (Grote et al) Large Signal Characterization Pulse and sinusoidal (AC) excitation Displacement and pressure output Nonlinear distortion: 2 nd harmonic

Average Displacement ( m) Pressure (MPa) Results: Pulse Excitation -0.074-0.076 0.4 0.2 0-0.078-0.2-0.08 0 0.2 0.4 0.6 0.8 1-0.4 0 0.2 0.4 0.6 0.8 1-0.02 Conventional 0.05 Conventional -0.022 0-0.024 0 1 2 3 4 5 6 7 Time ( s) -0.05 0 1 2 3 4 5 6 Time ( s) V BIAS =70V, V PULSE =+5V, t PULSE =20ns Conventional Displacement (p-p) (Å) 39 70 Resonance freq. (MHz) 3.84 8.75

Results: Pulse Excitation operation V BIAS =65 V Pulse excitation: V PULSE =15V t PULSE =20ns Displacement (p-p): 200 Å, 13 Å/V Pressure (p-p): 2000 kpa, 133 kpa/v

Displacement (p-p) (A) Resonance Frequency (MHz) Results: Bias Voltage 70 60 50 40 10 8 6 4 30 Conventional 20 55 60 65 70 75 80 Bias Voltage(V) 2 Conventional 0 55 60 65 70 75 80 Bias Voltage(V) V PULSE =+5V, t PULSE =20ns operation: - Higher resonance frequency : contact radius effect - Larger displacement & output pressure

Results: AC Excitation operation V BIAS =70 V AC excitation: f EXC =1 MHz V P-P =30V 2 nd harmonic: -23 db Displacement (p-p): 200 Å, 7 Å/V Pressure (p-p): 36 kpa, 1.2 kpa/v

2nd order harmonic level (db) Average Displacement (p-p) (A) Results: AC Amplitude -14-16 -18-20 -22-24 -26 Conventional -28 10 15 20 25 30 AC Amplitude (p-p) (V) 240 220 200 180 160 140 120 100 Conventional 80 10 15 20 25 30 AC Amplitude (p-p) (V) V BIAS =65 V, f EXC =1 MHz operation: MORE LINEAR RESPONSE

Results: Collapse-snapback Collapse-snapback operation V BIAS =70 V AC excitation: f EXC =1 MHz V P-P =40 V 2 nd harmonic: -18 db 3 rd harmonic: -10 db Displacement (p-p): 1200 Å, 30 Å/V Pressure (p-p): 3600 kpa, 90 kpa/v

Results: Collapse-snapback Collapse-snapback operation V BIAS =65 V AC excitation: f EXC =5 MHz V P-P =60 V Displacement (p-p): 1600 Å, 26 Å/V Pressure (p-p): 9500 kpa, 158 kpa/v

Comparison of Operation Regimes Performance Conventional Collapse- Snapback V BIAS High Low Low V TOTAL <V COLLAPSE >V SNAPBACK >V COLLAPSE <V SNAPBACK Output Power Low Medium High Linearity Good Better Worse

Conclusion Investigated different regimes of operation using transient analysis in FEM operation: More linear Low voltage bias Higher frequency Collapse-snapback operation: Higher output pressure Future work: 3D analysis of CMUT arrays