Title: Selective modal excitation using phase-shifted ultrasound radiation force Acoustical Society of America Meeting June 2006
1Selective modal excitation using phase-shifted
ultrasound radiation forceAcoustical Society
of America MeetingJune 2006
- Thomas M. Huber
- Physics Department, Gustavus Adolphus College
- Mostafa Fatemi, Randy Kinnick, James Greenleaf
- Ultrasound Research Laboratory, Mayo Clinic and
Foundation
2Introduction
- Overview of Ultrasound Stimulated Excitation
- Uses ultrasound radiation force for non-contact
modal excitation - Selective Excitation by Phase Shifted Pair of
Transducers - Results for hard-drive suspension
- Results for simple cantilever
- Results for MEMS mirror
- Conclusions
3Ultrasound Stimulated Radiation Force Excitation
- Vibro-AcoustographyDeveloped in 1998 at Mayo
Clinic Ultrasound Research Lab by Fatemi
Greenleaf - Difference frequency between two ultrasound
sources causes excitation of object. Detection
by acoustic re-emission - Technique has been used for imaging in water and
tissue - Recently, we have also used the ultrasound
radiation force for modal testing of organ reeds
and MEMS devices in air
4Ultrasound Stimulated Amplitude Modulated
Excitation
- Dual sideband, carrier suppressed amplitude
modulated signal centered, at 40 kHz - Difference frequency ?f between ultrasound
components produces radiation force that causes
vibration of object - Vibrations detected using a Polytec laser Doppler
vibrometer - Completely non-contact modal testing for
- both excitation and detection
-
5Selective Excitation using Phase-Shifted Pair of
Transducers
- Current Experiment Instead of using a single
transducer, use a pair of ultrasound transducers
to allow selective excitation of transverse or
torsional modes - If radiation force from both transducers are in
phase, selectively excites transverse modes while
suppressing torsional modes - If radiation force is out of phase, selectively
excites torsional modes while suppressing
transverse modes - Demonstrated for hard-drive suspensions, MEMS
mirror and cantilevers
6Phase-shifted selective excitation Detailed
Description
- Two 40 kHz transducers, each with dual sideband
suppressed carrier AM waveform - Modulation frequency swept from 50 5000 Hz
- Difference frequency Df leads to excitation from
100 Hz 10 kHz - Modulation phase difference of 90 degrees leads
to 180 degree phase difference in radiation force
7Photos of phase-shift excitation of hard-drive
suspension
8Phase-shifted selective excitation
- Adjust amplitudes of two ultrasound transducers
to give roughly equal response - The pair of 40 kHz transducers not exactly
matched (note different amplitudes near 5 kHz) - When both transducers turned on simultaneously
with same modulation phase - Enhanced Transverse Mode
- Suppressed Torsional Mode
9Phase-Shifted Selective Excitation of Suspension
- Driving in-phase excites transverse but
suppresses torsional mode (blue curve) - Driving out-of-phase (phase difference near 90
degrees) excites torsional while suppressing
transverse mode (red curve)
10Selective Excitation of Torsional/Transverse Modes
- The maximum amplitude for the transverse modes is
at angles near 0 degrees, with a minimum near 90
degrees -
- The maximum amplitude for torsional mode is at
angles near 90 degrees, with minimum near 0
degrees. - By shifting the phase by 90 degrees, the ratio of
the lowest transverse divided by torsional mode
can change from above 201 to smaller than 13. - Selective excitation via phase shifted ultrasound
has been demonstrated for several other types of
devices, including rectangular cantilevers and a
MEMS mirrors
11Phase-Shifted Selective Excitation of Simple
Cantilever
- Clamped-Free Brass Cantilever 3 cm by 0.8 cm
- Driving in-phase excites transverse modes but
suppresses torsional mode (Solid blue curve) - Driving out-of-phase excites torsional mode,
suppresses transverse modes (Dashed red curve) - Ratio of Fundamental divided by 1St Torsional
mode amplitudes varies by over two orders of
magnitude as modulation phase is shifted by 90
degrees
12Another 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 827 Hz
- Transverse mode (forward/back) 330 Hz
- (incidental not used for operation of mirror)
13Phase-Shifted Selective Excitation of MEMS Mirror
- Driving in-phase excites transverse and Z-Torsion
modes but suppresses X-torsional mode (blue
curve) - Driving with 90 degree phase shift excites
X-torsional mode while suppressing other modes
(red curve)
- By varying phase, the relative amplitude of the
modes can be adjusted
14Partial cancellation occurs even with
non-symmetric geometry
- Transducers 8 cm and 13 cm from 3mm square
mirror (?0.88 mm at 40 kHz)
- Oblique geometry one transducers not aimed
directly at mirror (sidelobe only)
15Conclusions
- Ultrasound excitation allows non-contact modal
testing - Using pair of phase-shifted transducers allows
selective excitation of torsional versus
transverse modes - Works for variety of devices
- Dimensions of objects can be smaller than
ultrasound wavelength - ?0.88 mm at 40 kHz
- Suspension pad 2 mm square, MEMS Mirror 3 mm
square - Partial cancellation can occur even for
non-uniform geometries or non-matched transducers - May be especially useful for devices with nearly
overlapping modes - Future areas of research
- Better understanding of radiation distribution
from diverging transducers - Understanding why maximum cancellation doesnt
always occur at 0 degrees and 90 degrees - Under development 600 kHz transducer pair with
high bandwidth and 2 mm focus diameter
16Acknowledgements
- This material is based upon work supported by the
National Science Foundation under Grant No.
0509993 - Any opinions, findings and conclusions or
recomendations expressed in this material are
those of the author(s) and do not necessarily
reflect the views of the National Science
Foundation (NSF)
Thank You