U.S. patents available from 1976 to present.
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Noninvasive vibration measurement system and method for measuring amplitude of vibration of tissue in an object being investigated

Patent 4819649 Issued on April 11, 1989. Estimated Expiration Date: Icon_subject November 3, 2006. 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

Measurement method and system utilizing ultrasonic wave
Patent #: 4414850
Issued on: 11/15/1983
Inventor: Miwa ,   et al.

Method for measuring physical properties of material
Patent #: 4543827
Issued on: 10/01/1985
Inventor: Tominaga ,   et al.

Ultrasonic non-linear parameter measuring system
Patent #: 4610255
Issued on: 09/09/1986
Inventor: Shimura ,   et al.

System and method for measuring sound velocity of tissue in an object being investigated Patent #: 4653505
Issued on: 03/31/1987
Inventor: Iinuma

Inventors

Assignee

Application

No. 06/926452 filed on 11/03/1986

US Classes:

600/438, Used as an indicator of another parameter (e.g., temperature, pressure, viscosity)73/624, Having separate sonic transmitter and receiver73/625Having plural sonic type transmitter or receiver transducers

Examiners

Primary: Jaworski, Francis J.
Assistant: Manuel, George

Attorney, Agent or Firm

International Classes

G01N 29/04 (20060101)
A61B 8/08 (20060101)
A61B 5/12 (20060101)
G01N 29/11 (20060101)
G01S 15/00 (20060101)
G01S 15/50 (20060101)

Abstract

A system and method for measuring the acoustically induced vibrations within a living organism. The object is ensonified to set it into low frequency vibration. A continuous wave beam of ultrasonic energy is transmitted along one path and focused at the tissue to be investigated. A focused transducer receives the reflected beam along a second axis such that the intersection of the transmitted and received beams define a small, concentrated region positioned at the object under investigation. The received beam is phase modulated by the amplitude of vibration of the object producing sidebands whose amplitude can be ratioed to the amplitude of the high frequency peak to determine the absolute amplitude of the low frequency vibration.

Other References

  • Signals and Systems, by Poularikas et al., pp. 219-221, PWS Publisher, 1985
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