EP0142178B2 - Ultraschall-Wandler - Google Patents
Ultraschall-Wandler Download PDFInfo
- Publication number
- EP0142178B2 EP0142178B2 EP84201200A EP84201200A EP0142178B2 EP 0142178 B2 EP0142178 B2 EP 0142178B2 EP 84201200 A EP84201200 A EP 84201200A EP 84201200 A EP84201200 A EP 84201200A EP 0142178 B2 EP0142178 B2 EP 0142178B2
- Authority
- EP
- European Patent Office
- Prior art keywords
- piezoelectric material
- layer
- layers
- acoustic impedance
- medium
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 239000000463 material Substances 0.000 claims description 34
- 239000000758 substrate Substances 0.000 claims description 4
- 230000006978 adaptation Effects 0.000 description 14
- 230000035945 sensitivity Effects 0.000 description 8
- 238000013016 damping Methods 0.000 description 6
- 238000001228 spectrum Methods 0.000 description 3
- 238000012550 audit Methods 0.000 description 2
- 239000000919 ceramic Substances 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005284 excitation Effects 0.000 description 2
- HFGPZNIAWCZYJU-UHFFFAOYSA-N lead zirconate titanate Chemical compound [O-2].[O-2].[O-2].[O-2].[O-2].[Ti+4].[Zr+4].[Pb+2] HFGPZNIAWCZYJU-UHFFFAOYSA-N 0.000 description 2
- 238000002604 ultrasonography Methods 0.000 description 2
- 239000002033 PVDF binder Substances 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 238000002592 echocardiography Methods 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 229910052451 lead zirconate titanate Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 229920002981 polyvinylidene fluoride Polymers 0.000 description 1
- 238000004088 simulation Methods 0.000 description 1
- 230000026683 transduction Effects 0.000 description 1
- 238000010361 transduction Methods 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
- -1 vinylidène Chemical class 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G10—MUSICAL INSTRUMENTS; ACOUSTICS
- G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
- G10K11/00—Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
- G10K11/02—Mechanical acoustic impedances; Impedance matching, e.g. by horns; Acoustic resonators
Definitions
- the present invention relates to an ultrasonic transducer comprising a substrate constituting a rear medium, a layer of piezoelectric material and one or more adaptation layers, the values of the impedances of the layer of piezoelectric material, acoustic impedance adaptation layers and of the medium before propagation forming, considered in this order, a decreasing sequence.
- An ultrasonic transducer essentially consists, in a conventional manner, of a substrate constituting a rear absorption or reflection medium, a layer of piezoelectric material equipped with electrodes on its front and rear faces and at least one layer. acoustic impedance matching, placed in front of the piezoelectric material, between it and the propagation medium. Transducers of this type are notably described in the article "The effects of backing and matching on the performance of piezoelectric ceramic transducers" by G. Kossoff, published in the journal IEEE Transactions on sonics and ultrasonics, volume SU-13, March 1966 , pages 20 to 30. The implementation of one or more of these adaptation layers has the main effect of improving the sensitivity of the transducers and also contributes to increasing their bandwidth.
- the ultrasonic transducers used in ultrasound must combine two main qualities at the level of transduction: not only good sensitivity (because the increase in signal-to-noise ratio facilitates the processing of received signals) but also sufficient damping (because the brevity of the impulse response conditions the axial resolution).
- the object of the invention is to propose an ultrasonic transducer which easily reconciles the requirements of sensitivity and damping.
- the invention relates to an ultrasonic transducer as defined in the preamble to the description and further characterized in that the adaptation layers are placed in identical number on either side of the piezoelectric material, the layers located symmetrically two by two having the same acoustic impedance value and the same thickness, in that the rear medium has an acoustic impedance value substantially equal to that of the medium before propagation, and in that the thickness of the layer of piezoelectric material is equal to half the wavelength associated with the resonant frequency of the transducer, so that the structure is symmetrical with respect to the median plane of the layer of piezoelectric material.
- FIG. 1 shows an embodiment of a transducer according to the invention.
- the embodiment represented in FIG. 1 consists of an ultrasonic transducer with vibration in thickness mode, totally symmetrical, composed of a substrate 10 constituting the rear medium of the transducer, of a layer 20 of piezoelectric material of thickness equal to the half the wavelength associated with the resonant frequency of the transducer and covered on its front and rear faces with metal sheets 21 and 22 constituting first and second electrodes (connected in a known manner to a polarization circuit not shown which provides the excitation potential), and of two acoustic impedance adaptation layers 30, 40 known as quarter-wave interference layers and situated on the one hand between the rear medium and the piezoelectric material and on the other hand between this material and the medium before propagation 50.
- the values of the acoustic impedances form a decreasing sequence from that of the piezoelectric material and these impedance values as well as the thicknesses of the adaptation layers 30, 40 are symmetrical on either side of this material. From this symmetry of the structure, it follows that the deformations on the two faces of the piezoelectric material are identical (since these two faces are acoustically charged identically) and that, consequently, the deformation is zero in the median plane of this material. The part of the structure which is located on only one side of this median plane is therefore equivalent to an infinitely rigid rear medium, that is to say with zero deformation.
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
- Multimedia (AREA)
- Transducers For Ultrasonic Waves (AREA)
- Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
Claims (1)
- Ultraschall-Wandler mit einem Substrat (10), das ein hinteres Medium bildet, einer Schicht piezoelektrischen Materials (20) und einer oder mehreren Anpassungsschichten (30, 40), wobei die Impedanzwerte der piezoelektrischen Materialschicht (20), der Anpassungsschichten für die akustische Impedanz und des vorderen Fortpflanzungsmediums (50) in dieser Reihenfolge eine abfallende Reihe bilden, dadurch gekennzeichnet, daß die Anpassungsschichten (30, 40) in gleicher Anzahl auf beiden Seiten des piezoelektrischen Materials (20) angeordnet sind, wobei die je zwei und zwei symmetrisch angeordneten Schichten den gleichen akustischen Impedanzwert und die gleiche Dicke haben, daß das hintere Medium einen akustischen Impedanzwert im wesentlichen gleich dem des vorderen Fortpflanzungsmediums (50) hat, und daß die Dicke der piezoelektrischen Materialschicht (20) gleich der halben, der Wandler-Resonanzfrequenz zugeordneten Wellenlänge ist, derart, daß die Struktur in bezug auf die Mittelebene der piezoelektrischen Materialschicht symmetrisch ist.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR8313986A FR2551611B1 (fr) | 1983-08-31 | 1983-08-31 | Nouvelle structure de transducteur ultrasonore et appareil d'examen de milieux par echographie ultrasonore comprenant une telle structure |
FR8313986 | 1983-08-31 |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0142178A1 EP0142178A1 (de) | 1985-05-22 |
EP0142178B1 EP0142178B1 (de) | 1990-01-03 |
EP0142178B2 true EP0142178B2 (de) | 1994-01-12 |
Family
ID=9291921
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP84201200A Expired - Lifetime EP0142178B2 (de) | 1983-08-31 | 1984-08-20 | Ultraschall-Wandler |
Country Status (7)
Country | Link |
---|---|
US (1) | US4771205A (de) |
EP (1) | EP0142178B2 (de) |
JP (1) | JPH0640676B2 (de) |
CA (1) | CA1260603A (de) |
DE (1) | DE3480968D1 (de) |
FR (1) | FR2551611B1 (de) |
IL (1) | IL72791A (de) |
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US4211948A (en) * | 1978-11-08 | 1980-07-08 | General Electric Company | Front surface matched piezoelectric ultrasonic transducer array with wide field of view |
EP0015886A1 (de) * | 1979-03-13 | 1980-09-17 | Toray Industries, Inc. | Verbessertes elektro-akustisches Wandler-Element |
US4383194A (en) * | 1979-05-01 | 1983-05-10 | Toray Industries, Inc. | Electro-acoustic transducer element |
US4297607A (en) * | 1980-04-25 | 1981-10-27 | Panametrics, Inc. | Sealed, matched piezoelectric transducer |
US4434384A (en) * | 1980-12-08 | 1984-02-28 | Raytheon Company | Ultrasonic transducer and its method of manufacture |
JPS57170708U (de) * | 1981-04-20 | 1982-10-27 | ||
JPS5817358A (ja) * | 1981-07-23 | 1983-02-01 | Toshiba Corp | 超音波探触子 |
US4507582A (en) * | 1982-09-29 | 1985-03-26 | New York Institute Of Technology | Matching region for damped piezoelectric ultrasonic apparatus |
JPS59166139A (ja) * | 1983-03-10 | 1984-09-19 | 富士通株式会社 | 超音波トランスデュ−サ |
-
1983
- 1983-08-31 FR FR8313986A patent/FR2551611B1/fr not_active Expired
-
1984
- 1984-08-20 DE DE8484201200T patent/DE3480968D1/de not_active Expired - Lifetime
- 1984-08-20 EP EP84201200A patent/EP0142178B2/de not_active Expired - Lifetime
- 1984-08-24 US US06/644,161 patent/US4771205A/en not_active Expired - Fee Related
- 1984-08-28 IL IL72791A patent/IL72791A/xx not_active IP Right Cessation
- 1984-08-30 CA CA000462119A patent/CA1260603A/en not_active Expired
- 1984-08-31 JP JP59182519A patent/JPH0640676B2/ja not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
CA1260603A (en) | 1989-09-26 |
FR2551611A1 (fr) | 1985-03-08 |
JPH0640676B2 (ja) | 1994-05-25 |
DE3480968D1 (de) | 1990-02-08 |
EP0142178B1 (de) | 1990-01-03 |
EP0142178A1 (de) | 1985-05-22 |
IL72791A0 (en) | 1984-11-30 |
JPS6084099A (ja) | 1985-05-13 |
IL72791A (en) | 1988-08-31 |
FR2551611B1 (fr) | 1986-10-24 |
US4771205A (en) | 1988-09-13 |
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