|Publication number||USRE32062 E|
|Application number||US 06/529,224|
|Publication date||Jan 14, 1986|
|Filing date||Aug 29, 1983|
|Priority date||Jan 6, 1981|
|Publication number||06529224, 529224, US RE32062 E, US RE32062E, US-E-RE32062, USRE32062 E, USRE32062E|
|Inventors||Arthur J. Samodovitz|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (6), Referenced by (5), Classifications (7), Legal Events (3)|
|External Links: USPTO, USPTO Assignment, Espacenet|
Cross reference to related applications: none. Statement as to the rights to inventions made under Federally-sponsored research and development: none.
1. Field of the Invention
The invention relates to transducers, and more particularly to a plurality of alternately layered transducing elements and acoustical lenses for use in focussing acoustical waves at different colinear regions without any mechanical motion.
2. Description of the Prior Art
Ultrasound is used to examine inside a specimen and produce an image. An ordinary transducer is electrically pulsed, and in response it transmits an ultrasonic (mechanical) wave. The wave passes through an acoustic lens to focus at a particular location inside the specimen. That location is determined by the focal length of the lens. The wave interacts with the specimen producing echoes, some of which reflect back onto the lens and through to the transducer. The transducer then produces electrical signals, and those which correspond to the echoes of the field are used to make an image. A highly focussed wave yields good resolution but only over a small depth of field. The quality of resolution and depth of field are inversely related according to standard lens properties.
To focus over a large depth of field, two or more lenses of different focal lengths can be interchanged mechanically to yield two or more fields. The pulse-echo procedure would be repeated for each lens whereby the echoic electrical signals corresponding to the fields would be combined to effect a large depth of field. However, interchanging lenses takes too long and requires precise alignment. The invention provides a large depth of field without any mechanical motion.
It is a first object of the invention to provide a transducer assembly which can focuss over a large depth of field yet have good resolution.
It is a second object of the invention to provide a transducer assembly which need not move in the course of transmitting highly focussed acoustic waves over a large depth of field, and need not move in receiving echoes produced from the interaction of said waves with objects within the extended depth of field.
To satisfy these objects and others, there is provided a transducing assembly comprising a first converging, acoustic lens, a first transducing element located behind the first lens, a second, converging acoustic lens located behind the first transducing element, a second transducing element located behind the second acoustic lens, a backing material located behind the second transducing element to absorb rearwardly directed waves, and means to couple the first lens to the first transducing element, the first transducing element to the second lens, and the second lens to the second transducing element via coupling mediums, matching layers, filler materials, and direct contact between layers.
The invention focusses in the far field by transmitting and receiving with the first transducing element, and the invention focusses in the near field by transmitting and receiving with the second transducing element: the far field focussing is effected by the focussing power of the first lens, and the near field focussing is effected by the focussing power of the first lens in conjunction with the focussing power of the second lens.
FIG. 1 is a cross-sectional diagram of a simple transducer-lens assembly. The transducer lens, and specimen are interfaced through a coupling medium.
FIG. 2 is a cross-sectional diagram not drawn to scale of the first embodiment of the invention comprising a transducer-internal lens-transducer assembly, an external lens, and a coupling medium which interfaces said assembly, external lens, and the specimen.
FIG. 3(a) is a cross-sectional diagram, not drawn to scale, demonstrating the far field focussing ability of the preferred embodiment of the invention.
FIG. 3(b) is a cross-sectional diagram, not drawn to scale, demonstrating the near field focussing ability of the preferred embodiment of the invention.
The first embodiment of the invention comprises elements shown in FIG. 2: a transducer-internal lens-transducer assembly, an external lens, and a coupling medium which interfaces said assembly, external lens, and the specimen. Said assembly comprises eleven section: section 1 is material(s) to absorb and dissipate any ultrasound which impinges on it, section 2 is a thin electrode, section 3 is a piezoelectric material, section 4 is a thin electrode, section 5 is a material to fill the gap between the flat section 4 and the concave internal lens, and has the same acoustic impedance as the piezoelectric material of section 3 and the internal lens, section 6 is the converging lens, section 7 is the same as section 5, section 8 is the same as section 4, section 9 is the same as section 3, section 10 is the same as section 2, and section 11 is material(s) to match the acoustic impedance of the piezoelectric section 9 to that of water whereby ultrasound passes from said assembly to water with minimal losses and minimal reflections.
To focus in the far field, electrodes section 8 and 10 are electrically pulsed. In response, piezoelectric section 9 transmits a forward acoustic wave towards the specimen, and a backward acoustic wave towards the absorptive section 1. The backward wave travels from section 8 to section 1 with minimal reflections since sections 9, 7, 6, 5, and 3 have the same acoustic impedance, electrode sections 8,4, and 2 are thin, and section 1 absorbs and dissipates the wave. The forward wave passes through the electrode section 10, matching section 11, the coupling medium, the external lens, and the coupling medium and into the specimen. The wave focusses at a location determined by the focal length of the external lens as shown in FIG. 3, and that location is the far field. The forward wave interacts with the specimen producing echoes. Some of these echoes reflect back onto the external lens and proceed through sections 11 and 10, and to piezoelectric section 9. In response, piezoelectric section 9 generates an electrical signal between electrode sections 8 and 10 which is transmitted electrically to an electronic unit. The electronic unit processes the segment of this signal which corresponds to the far field. The echoes, reduced in power, proceed through piezoelectric section 9, and sections 8-2, and dissipate in section 1.
To focus in the near zone, electrode sections 2 and 4 are electrically pulsed. Piezoelectric section 3 transmits a forward acoustic wave towards the specimen, and a backward acoustic wave towards the absorptive section 1. The backward wave travels through electrode section 2 and is dissipated in section 1. The forward wave passes through sections 4-11, the coupling medium, the external lens, and the coupling medium, and into the specimen. The focal length (Ft) is determined by the focal length of the internal lens (Fi) in conjunction with that of the external lens (Fe):
and is shown in FIG. 3. The forward wave interacts with the specimen producing echoes. Some of these echoes reflect back onto the external lens and proceed through sections 11-4 and to the piezoelectric section 3. In response, piezoelectric section 3 generates an electrical signal between electrode sections 2 and 4 which is transmitted electrically to the electronic unit. The electronic unit processes the segment of this signal which corresponds to the near field. The echoes, reduced in power, proceed through piezoelectric section 3 and section 2, and dissipate in section 1. The electronic unit combines the processed electrical signals of both piezoelectric sections to produce a focussed image over a large depth of field.
As the forward wave of piezoelectric section 3, and resulting echoes pass through piezoelectric section 9, some mechanical energy is lost as they produce electrical energy. This loss is decreased if electrode sections 8 and 10 are open circuited.
The second embodiment of the invention is similar to the first except the acoustic impedance of the internal lens and surrounding two filler material sections is different from that of the piezoelectric materials, and a section to match them is required immediately before section 5 and immediately after section 7. The second embodiment of the invention is functionally equivalent to the first embodiment.
In any embodiment of the invention, the internal lens may be larger in diameter than the other sections of the transducer-lens-transducer assembly to avoid difraction at the perimeter of the lens. Also, the internal lens may be divergent which would cause the rear piezoelectric material to focus in the farthest field. In these latter embodiments, the diameter of the rear piezoelectric section should be smaller than the rest of the assembly so that the forward wave does not collide with the cylindrical surface of the assembly.
Any embodiment of the invention is expandable to focus in three (or more) fields. In the first embodiment, section 11 is removed and another unit similar to sections 5-11 is added onto section 10 connected at the new section 5. The forward wave from the added piezoelectric section focusses in the farthest field, that from the middle one focusses in the middle field, and that from the rear one focusses in the near field.
The preferred procedure for operating the first embodiment of the invention requires up to twice the time as a simple transducer-lens arrangement. To operate in less time, the first embodiment transmits once with piezoelectric section 9, and receives with piezoelectric sections 9 and 3. The electronic unit processes the segment of the electrical signal from section 9 that corresponds to the far field, and that from section 3 which corresponds to the near field. This procedure yields resolution in the far field as good as that of the preferred procedure, but resolution in the near field intermediate in quality between that of the preferred procedure and that of the simple one transducer-one lens system operating comparably outside its field.
Any embodiment of the invention may be operated to produce a B-scan. The operation begins with any said operational procedure. Then the invention is mechanically moved to focus and operate in an adjacent coplanar field. The invention is moved and operated again and again until a sufficiently large plane has been scanned.
|Cited Patent||Filing date||Publication date||Applicant||Title|
|US3913061 *||Apr 25, 1973||Oct 14, 1975||Stanford Research Inst||Focusing and deflecting system for acoustic imaging|
|US3995179 *||Dec 30, 1974||Nov 30, 1976||Texaco Inc.||Damping structure for ultrasonic piezoelectric transducer|
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|Citing Patent||Filing date||Publication date||Applicant||Title|
|US4967873 *||Jul 21, 1989||Nov 6, 1990||Olympus Optical Co., Ltd.||Acoustic lens apparatus|
|US5235553 *||Nov 22, 1991||Aug 10, 1993||Advanced Imaging Systems||Solid ultrasonic lens|
|US7204342 *||Apr 25, 2003||Apr 17, 2007||Postech Foundation||Sound focus speaker of gas-filled sound lens attachment type|
|US20050224282 *||Apr 25, 2003||Oct 13, 2005||Postech Foundation||Sound focus speaker of gas-filled sound lens attachment type|
|US20120223620 *||May 14, 2012||Sep 6, 2012||Avago Technologies Wireless Ip (Singapore) Pte. Ltd.||Multi-aperture acoustic horn|
|U.S. Classification||73/642, 181/176, 367/155, 367/150|
|Nov 28, 1986||FPAY||Fee payment|
Year of fee payment: 4
|Jan 15, 1991||REMI||Maintenance fee reminder mailed|
|Jun 16, 1991||LAPS||Lapse for failure to pay maintenance fees|