Damped acoustic transducers with piezoelectric drivers

• US 4,333,028 A
• Filed: 03/13/1981
• Issued: 06/01/1982
• Est. Priority Date: 04/21/1980
• Status: Expired due to Term

• Current Assignee: Milltronics, Ltd. (Titan Pacific Resources Ltd.)
• Original Assignee: Milltronics, Ltd. (Titan Pacific Resources Ltd.)
• Inventors: Panton, Stanley
• Primary Examiner(s): Budd, Mark O.
• Application Number:
  US06/243,490
• Time in Patent Office: 445 Days
• Field of Search: 310/322-324, 310/326, 310/327, 310/334, 310/335, 310/312, 179/110 A, 181/164-167
• US Class Current: 310/326
• CPC Class Codes: B06B 1/0618 of piezo- and non-piezoelectric elements, e.g. 'Tonpilz'
• CPC Class Codes: G10K 11/02 Mechanical acoustic impedances; Impedance matching, e.g. by horns; Acoustic resonators

Abstract

A tuned acoustic directional transducer for transmitting and receiving airborne sound, which provides enhanced efficiency and reduced cost without undue narrowing of bandwidth, makes use of an acoustic transducer element (2) coupled to a plate (10) having a higher order flexural mode resonance at approximately the desired frequency of operation, the plate being coupled to the air through low-hysteresis acoustic propagation material having an acoustic impedance much less than that of the plate and much greater than that of the air. The material is disposed so that in the desired direction of propagation there is no substantial reduction of sound intensity in the far field resulting from cancellation occasioned by interaction of sound radiated from adjacent antinodal zones. Preferably the thickness of the material is such that it acts as an efficient acoustic impedance matching transformer. Preferably, the transducer element is piezoelectric and coupled to the center of a circular plate to which the coupling material is applied in rings (16, 18, 20).

Claims

1. A broadly tuned directional transducer system comprising a plate having a radiating surface and a higher flexural mode resonance at substantially the operating frequency of the system, and a transducer element of much smaller effective area than the radiating surface of the plate and connected thereto for excitation or response to said higher flexural mode resonance, wherein at least alternate antinodal zones of the radiating surfaces of the plate are coupled to a gaseous propagation medium by coupling means formed of low-loss acoustic propagation material of much lower acoustic impedance than the plate and applied at least to said alternate antinodal zones of the radiating surface thereof in a thickness selected to differentiate at least one of the relative phase and the relative amplitude of the radiation from adjacent antinodal zones sufficiently to reduced substantially mutual cancellation, in the far field and in the desired direction of radiation, of sound radiated into said medium from adjacent antinodal zones of the plate.

2. A system according to claim 1, wherein the thickness of low-loss acoustic propagation material applied to said alternate zones is an odd number of quarter-wavelengths of sound in the material at the operating frequency of the system, and no such material is applied to the remaining zones.

3. A system according to claim 1, wherein the thickness of low-loss acoustic propagation material applied to said alternate zones differs from that applied to the remaining zones by an amount such that the sound reaching the far field from said alternate zones undergoes a phase shift, compared with that radiated from the remaining zones, sufficient substantially to reduce cancellation.

4. A system according to claim 1, 2 or 3, wherein the plate is axisymmetrically resonant and axisymmetrically coupled to the transducer element.

5. A system according to claim 1, 2, or 3 wherein the plate is a disc of uniform thickness, and both the plate and the transducer element are tuned to resonant frequencies close to the operating frequency of the system.

6. A system according to claim 1, 2 or 3, wherein the plate is a disc of uniform thickness and the ratio of plate diameter to thickness is between 25:

1 and 500;

1.

7. A system according to claim 3, wherein each antinodal zone of the plate is covered with said material to a thickness which differs by n/2f(1/C₀ -1/C₁) from that covering the next zone, where n is an odd integer, f is the frequency of operation of the system, C₀ is the velocity of sound in the gaseous medium, and C₁ is the velocity of sound in the material.

8. A system according to claim 3 or 7, wherein at least some of the antinodal zones of the plate are covered with low-loss, acoustic impedance matching material to a thickness equal to an odd number of quarter wavelengths of sound at the velocity of sound in said matching material.

9. A system according to claim 1, 2 or 3, wherein the low-loss acoustic propagation material is selected from closed-cell foamed synthetic plastics and unfoamed elastomers.

10. A system according to claim 1, 2 or 3, wherein the plate is a disc having at least three nodal rings.

11. A tuned directional acoustic transducer system comprising a plate exhibiting a high acoustic impedance and a flexural mode resonance at substantially the operating frequency of the system, a high impedance acoustic transducer element, a mechanical coupling between said transducer element and an antinodal zone of said plate so that flexural resonance of said plate occurs conjointly with mechanical deformation of the transducer element at the same frequency, one surface of said plate facing into a propagation medium and being covered at least in part with a low hysteresis acoustic propagation material having an acoustic impedance much lower than that of the plate and much higher than that of the gaseous medium, the thickness of said material in different antinodal zones varying such that acoustic waves radiated in antiphase from adjacent antinodal zones of the plate reach the far field in the gaseous medium substantially in phase with one another on a plane wavefront.

12. A system according to claim 11, wherein the plate is axisymmetrically resonant and axisymmetrically coupled to the transducer element.

13. A system according to claim 12, wherein the plate is disc shaped.

14. A system according to claim 13, wherein the plate is of uniform thickness, and both the plate and the transducer element are tuned to the same resonant frequency.

15. A system according to claim 11, wherein each antinodal zone of the plate is covered with said material to a thickness which differs by n/2f(1C₀ -1/C₁) from that covering the next zone, where n is an odd integer, f is the frequency of operation of the system, C₀ is the velocity of sound in the gaseous medium, and C₁ is the velocity of sound in the material.

16. A system according to claim 11, wherein at least some of the antinodal zones are covered with additional low-loss, low acoustic impedance matching material to a thickness equal to an odd number of quarter wavelengths of sound at the velocity of sound in said matching material.

17. A system according to claim 15 or 16, wherein the plate is disc shaped.

18. A system according to claim 15 or 16, wherein the material is selected from closed-cell foamed synthetic plastics and unfoamed elastomers.

19. A system according to claim 11, wherein the area of the radiating surface of the plate is very large compared to the effective surface area of the transducer element.

20. A broadly tuned directional transducer system comprising a radiating plate having a flexural mode resonance at substantially the operating frequency of the system, a transducer element of much smaller effective area than the plate and coupled thereto, and phase correcting means formed of layers of low-loss acoustic propagation material of much lower acoustic impedance than the plate and applied to selected portions of the radiating surface thereof such as to equalize the phase in the far field of sound radiated from different antinodal zones of the plate.

21. A transducer system according to claim 20, further comprising impedance matching means applied to the radiating surface of the plate including said phase correction means and comprising a layer of low-loss acoustic propagation material of lower acoustic impedance than said plate and of a thickness equal to an odd number of quarter wavelengths of sound of the operating frequency in said material.

22. A tuned directional acoustic transducer system comprising a plate exhibiting a high acoustic impedance and a higher order flexural mode resonance at substantially the operating frequency of the system, a high impedance acoustic transducer element, a mechanical coupling between said transducer element and an antinodal zone of said plate so that flexural resonance of said plate occurs conjointly with mechanical deformation of the transducer element at the same frequency, one surface of said plate facing into a propagation medium and being covered at least over alternate antinodal zones with a low hysteresis acoustic propagation material having an acoustic impedance much lower than that of the plate and much higher than that of the gaseous medium, the disposition of said material in respect of different antinodal zones of the plate being such that acoustic waves radiated from said one surface of the plate reach the far field in the gaseous medium without substantial mutual cancellation and on a plane wave front.

23. A system according to claim 22, wherein the plate is axisymmetrically resonant and axisymmetrically coupled to the transducer element.

24. A system according to claim 23, wherein the plate is disc shaped.

25. A broadly tuned directional transducer system comprising a radiating plate having a higher flexural mode resonance at substantially the operating frequency of the system, a transducer element of much smaller effective area than the plate and coupled thereto, and coupling means formed of low-loss acoustic propagation material of much lower acoustic impedance than the plate and applied to alternate antinodal zones of the radiating surface thereof such as to avoid substantial cancellation in the far field of sound radiated from said alternate antinodal zones of the plate by sound radiated from the remaining antinodal zones of the plate.