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Title: Selective modal excitation using phase-shifted ultrasound radiation force Acoustical Society of America Meeting June 2006


1
Selective 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

2
Introduction
  • 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

3
Ultrasound 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

4
Ultrasound 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

5
Selective 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

6
Phase-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

7
Photos of phase-shift excitation of hard-drive
suspension
8
Phase-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

9
Phase-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)

10
Selective 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

11
Phase-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

12
Another 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)

13
Phase-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

14
Partial 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)

15
Conclusions
  • 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

16
Acknowledgements
  • 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)

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