U.S. patents available from 1976 to present.
U.S. patent applications available from 2005 to present.

Tunable acoustic resonator for clinical ultrasonic transducers

Patent 5438554 Issued on August 1, 1995. Estimated Expiration Date: Icon_subject February 28, 2014. Estimated Expiration Date is calculated based on simple USPTO term provisions. It does not account for terminal disclaimers, term adjustments, failure to pay maintenance fees, or other factors which might affect the term of a patent.

Patent References

2589403

3093760

3378704

3401377

3462746

3590287

3718898

3833825

Multi-layer element consisting of piezoelectric ceramic laminations and method of making same
Patent #: 4087716
Issued on: 05/02/1978
Inventor: Heywang

Variable acoustic wave energy transfer-characteristic control device
Patent #: 4096756
Issued on: 06/27/1978
Inventor: Alphonse

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Inventors

Application

No. 203216 filed on 02/28/1994

US Classes:

367/140, SIGNAL TRANSDUCERS310/320, Piezoelectric slab having different resonant frequencies at different areas310/334, Acoustic wave type generator or receiver310/336, Nondestructive testing type367/153, Plural transducer array600/447, Electronic array scanning600/459Structure of transducer or probe assembly

Examiners

Primary: Eldred, J. Woodrow

Foreign Patent References

  • 0401027 EP 12/13/1990
  • 3430161A1 DE 02/13/1986
  • 45-23667 JP 08/13/1970
  • 60-208200 JP 10/13/1985
  • 2059716B GB 07/13/1983

International Class

H04R 017/00

Abstract

A tunable ultrasonic probe includes a body of a first piezoelectric material acoustically coupled in series with a body of a second piezoelectric material. The second piezoelectric material has a Curie temperature that is substantially different than that of the first piezoelectric material. Preferably, the first piezoelectric material is a conventional piezoelectric ceramic, such as lead zirconate titanate, while the second piezoelectric material is a relaxor ferroelectric ceramic, such as lead magnesium niobate. At an operating temperature of the probe, the first piezoelectric material has a fixed polarization. In contrast, the second piezoelectric material has a polarization that is variable relative to the fixed polarization of the first piezoelectric material. A preferred novel arrangement of electrodes electrically couples the bodies in parallel with one another. An oscillating voltage for exciting the acoustic signals in the probe is coupled with the electrodes. The polarization of the second piezoelectric material is variably controlled by a bias voltage coupled with the electrodes. In a preferred embodiment, the bias voltage has a reversible electrical polarity for selecting one resonant frequency from a plurality of resonant frequencies of the probe. In another preferred embodiment, the bias voltage source has a variable voltage level for selecting at least one of a plurality of resonant frequencies of the probe.

Other References

  • N. Kim, S. J. Jang, and T. R. Shrout; "Relaxor Based Fine Grain Piezoelectric Materials"; Proceedings of the 1990 IEEE International Symposium on Applications of Ferroelectrics; pp. 605-609, 1991
  • W. Y. Pan, W. Y. Gu, D. J. Taylor and L. E. Cross; "Large Piezoelectric Effect Induced by Direct Current Bias in PMN:PT Relaxor Ferroelectric Ceramics"; Japanese Journal of Applied Physics, vol. 28, No. 4, 1989, pp. 653-661
  • Thomas R. Shrout and Joseph Fielding, Jr.; "Relaxor Ferroelectric Materials"; 1990 Ultrasonic Symposium Proceedings, vol. 2, IEEE, 1990, pp. 711-720
  • Sixte de Fraguier, Jean-Francois Gelly, Leon Volnrerman and Olivier Lanuzel; "A Novel Acoustic Design for Dual Frequency Transducers Resulting in Separate Bandpass for Color Flow Mapping (CFM)"
  • Hiroshi Takeuchi, Hiroshi Masuzawa, and Yukio Ito; "Medical Ultrasonic Probe Using Electrostrictive/Polymer Composite"; 1989 Ultrasonic Symposium Proceedings; IEEE, pp. 705-708
  • D. J. Taylor, D. Damjanovic, A. S. Bhalla, and L. E. Cross; "Complex Piezoelectric, Elastic, and Dielectric Coefficient of La-Doped 0.93 Pb(Mg1/3 NB2/3)O3 :0.07 PbTiO3 under DC Bias", Ferroelectrics Letters, 1990, vol. 11, pp. 1-9
  • D. J. Taylor, D. Damjanovic, A. S. Bhalla, and L. E. Cross; "Electric Field Dependence of dh In Lead Magnesium Niobate Lead Titanate Ceramics"; Proceedings of the 1990 IEEE International Symposium on Application of Ferroelectric; pp. 341-345, 1991
  • Wallace Arden Smith and Bertram A. Auld; "Modeling 1-3 Composite Piezoelectrics: Thickness-Mode Oscillations"; IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control, vol. 38, No. 1, Jan., 1991, pp. 40-47
  • R. E. Newnham, D. P. Skinner and L. E. Cross; "Connectivity and Piezoelectric-Pyroelectric Composites"; Mat. Res. Bull. vol. 13, pp. 525-536
  • M. I. Haller and B. T. Khuri-Yakub; "Micromachined Acoustic Matching Layers"; SPIE, vol. 1733, 1992, pp. 72-77
  • M. I. Haller and B. T. Khuri-Yakub; "Micromachined Ultrasonic Materials"; 1991 IEEE Ultrasonics Symposium; pp. 403-405
  • Peder C. Pedersen, Oleh Tretiak, and Ping He; "Impedance-Matching Properties of an Inhomogeneous Matching Layer with Continuously Changing Acoustic Impedance"; 1982 Acoustical Society of America, vol. 72, No. 2, pp. 327-336
  • Erhard K. Sittig; "Transmission Parameters of Thickness-Driven Piezoelectirc Transducers Arranged in Multilayer Configurations"; IEEE Transactions on Sonics and Ultrasonics, vol. SU-14, No. 4, Oct., 1967, pp. 167-174
  • Karen Pendergraft and Ronald Piper; "An Exact Solution for a Reflection Coefficient in a medium having an Exponential Impedance profile"; 1993 Acoustical Society of America, vol. 94, No. 1, Jul., 1993, pp. 580-582
  • Wallace Arden Smith; "New Opportunities in Ultrasonic Transducers Emerging from Innovations in Piezoelectric Materials"; 1992 SPIE International Symposium, Jul. 1992, pp. 1-2
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