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Publication numberUS3543059 A
Publication typeGrant
Publication dateNov 24, 1970
Filing dateOct 28, 1968
Priority dateOct 28, 1968
Publication numberUS 3543059 A, US 3543059A, US-A-3543059, US3543059 A, US3543059A
InventorsWesley L Angeloff
Original AssigneeUs Navy
Export CitationBiBTeX, EndNote, RefMan
External Links: USPTO, USPTO Assignment, Espacenet
Fluted cylinder for underwater transducer
US 3543059 A
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Description  (OCR text may contain errors)

NOV. 24, 1970 w. ANGELQFF 3,543,059

FLUTED CYLINDER FOR UNDERWATER TRANSDUCER Filed QCE. 28, 1968 FIG. 2

INVENTOR WESLEY L. ANGELOFF ATTORNEYS United States Patent O 3,543,059 FLUTED CYLINDER FOR UNDERWATER TRANSDUCER Wesley L. Angelolf, San Diego, Calif., assignor to the United States of America as represented by the Secretary of the Navy Filed Oct. 28, 1968, Ser. No. 771,224 Int. Cl. H02k 7/00 US. Cl. 310-8.7 4 Claims ABSTRACT OF THE DISCLOSURE STATEMENT OF GOVERNMENT INTEREST The invention described herein may be manufactured and used by or for the Government of the United States of America for governmental purposes without the payment of any royalties thereon or therefor.

BACKGROUND OF THE INVENTION Cylinders of electroacoustic material such as piezoelectric ceramic or magnetostrictive or electrostrictive metals are currently employed because, when freeflooded, they can be operated at any depth, inasmuch as the hydrostatic pressure is equalized at all parts of the cylinder. Unfortunately, the lowest natural resonant frequency of a cylinder is a function of the stiffness which in turn is a function of wall thickness and diameter of the cylinder and cannot be economically reduced below a fairly high value without increasing the diameter to unwieldy dimensions. Likewise, there is a definite limit to the minimum wall thickness to get compliance because of the inherent weakness of most ceramics.

SUMMARY OF THE INVENTION The objects of this invention are obtained by con structing the cylindrical transducer of staves of the electroacoustic material which staves are joined edge-to-edge to form the cylinder. The staves, or slats, are irregular in cross section, so that when they are joined edge-to-edge, the length of the circumferential path in the cylinder is greater than the mean circumferential diameter of the cylinder. It follows that the ratio of mean diameter to thickness is increased so that compliance and the natural frequency of resonance of the cylinder is correspondingly decreased.

OBJECTS OF THE INVENTION Accordingly, the principal object of this invention is to produce an improved cylindrical transducer which will operate efliciently at lower frequencies. A more specific object of this invention is to lower the mechanical resonant frequency of a cylindrical transducer.

Other objects and features of this invention will become apparent to those skilled in the art by referring to preferred embodiments described in the following specification and shown in the accompanying drawings.

DESCRIPTION OF THE DRAWINGS FIG. 1 is a perspective view of one cylindrical transducer of this invention.

Patented Nov. 24, 1970 ice FIG. 3 is an end view of a cast metal cylinder of this invention.

DESCRIPTION OF THE PREFERRED EMBODIMENTS The cylinder 10 shown in FIG. 1 is fabricated of staves 12. The staves 12 are relatively long, narrow slats of electroacoustic material and are joined edge-to-edge by adhesives or solder. If each stave is a piezoelectric ceramic, the soldered junctions 14 may contain connections 16 to the signal circuit. Preferably, the ceramic is of a barium titanate or lead zirconate titanate and preferably is polarized during manufacture by electrodes of opposed potential along opposite edges of the slats. Alternate electrodes in the cylinder are connected together and to external circuits. The external circuits may lead to either a transmitter or a receiver.

According to an important feature of this invention, the staves 12, in FIG. 1, are irregular in cross section, the irregularity comprising a radius of curvature, R which is less than the mean radius of, R the cylinder. The concaved sides of the slats can each be oriented toward the inside of the cylinder as suggested in FIGS. 1 or 3, or toward the outside of the cylinder as suggested in FIG. 2, or the concavity may alternate among these slats as shown in FIG. 4. It follows that the length of the circumferential path through the electroacoustic material is greater than in a cylinder of the same mean diameter with a smooth wall.

It can be shown that the natural mechanical resonant frequency, at which the cylinder will operate, is proportional to the stiffness or compliance of the cylinder which in turn is a function of the ratio of the diameter of the cylinder to the wall thickness of the cylinder, water loaded. That is, as the diameter, and the circumferential length of the cylinder wall are increased for a given wall thickness, the natural resonant frequency decreases. The order of magnitude of this ratio, found to be practical in sea operations, is about 30 to 1. If the diameter to wall thickness is still further increased, the end result approaches that of a paper-thin tube or wet noodle which of course is mechanically unfeasible. For most ceramics, at present in use in this art, the ratio of diameter to wall thickness should not substantially exceed 30 to 1.

Where greater ruggedness in the cylinder is required than can be provided by ceramic materials, metal may be used. Motion in the cylinder wall as a function of signal voltages may now be produced by magnetostriction. If the cylinder is of sheet nickel or other ferromagnetic metals, the signal can be inductively coupled to the cylinder, as suggested, for example, in the US. patent to Green, No. 3,177,382, issued Apr. 6, 1965. In fabricating such a transducer 22, FIG. 3, a single sheet of metal could be rolled with integral side-by-side flutes and the cylinder then closed with a single seam.

Still another technique of construction found to be satisfactory comprises casting the fluted cylinder. More specifically, metal can be vaporized in an electric arc and blown onto a form of the desired shape. As shown in FIG. 3, the metal layer 24 is sprayed on the split cylindrical form 22. The discrete metal particles of the layer 24 are quite small and densely packed, and can be laid down in layers which will have low eddy current losses, and yet can have a high coeflicient of expansion per unit of signal voltage. The voltage gradient preferably is applied by conductors wound around. the laminated coating.

What is claimed is:

1. A cylindrical transducer comprising:

a plurality of elongated slat-like staves of piezoelectric material, said staves being parallel, circularly artype-selected from the group consisting of barium ranged, and joined edge-to'edge to form a cylinder titanate, and lead zirconate titanate. having a predetermined mean radius, 3. In the cylindrical transducer defined in claim 1:

electrodes contacting each stave to functionally resaid staves comprising a sheet of magnetostrictive late signal voltages on the electrodes and physical 5 metal.

, distortion of the stave in a circumferential direc- 4. In the transducer defined in claim 1:

tion, the piezoelectric material of said staves being said cylinder comprising magnetostrictive metal cast so selected and polarized and the electrodes on each to the mentioned shape of said staves. stavebeing so .disposed that said physical distortion is principally expansion and contraction between 10 Refelfrellces Cited the side edges of said staves to cause radial displace- UNITED STATES PATENTS ment of the wall of said cylinder,

7 said staves being circular in cross-section between the gf ig 'f g'g'g joints, the radius of curvature of said cross section 2521136 9/1950 Thuras being uniform and less than said mean radius of 5 3302163 1/1967 A d the cylinder for increasing the length of the path n {ews 3 142 035 7/1964 Harris 3108.6 XR 1n the wall, circumferentially oi the cyllnder, beyond 2515446 7/1950, Gravley 310 9 6 XR the clrcumference corresponding to said predeter- 3,177,382 4/1965 Green 310 9'6 XR mined mean radius for lowering the natural me- :chanical resonant frequency of said cylinder, the 20 MILTON HIRSHFIELD Primary Examiner thickness, curvature and width of said staves being selected to stiffen the cylinder and prevent flexure in REYNOLDS: Assistant Exammel' the walls of the cylinder.

2. In the cylindrical transducer defined in claim 1:

said staves comprising piezoelectric ceramics of the a 3109.6, 26; 340-10

Patent Citations
Cited PatentFiling datePublication dateApplicantTitle
US2515446 *Jun 12, 1948Jul 18, 1950Brush Dev CoElectromechanical transducer
US2521136 *Apr 28, 1949Sep 5, 1950Of Commerce National BankHydrophone
US3043967 *Jan 13, 1960Jul 10, 1962Clearwaters Walter LElectrostrictive transducer
US3142035 *Feb 4, 1960Jul 21, 1964Harris Transducer CorpRing-shaped transducer
US3177382 *Jan 25, 1961Apr 6, 1965Green Charles EMosaic construction for electroacoustical cylindrical transducers
US3302163 *Aug 31, 1965Jan 31, 1967Andrews Jr Daniel EBroad band acoustic transducer
US3311352 *Mar 25, 1965Mar 28, 1967Bulova Watch Co IncMagnetostrictive transducers
Referenced by
Citing PatentFiling datePublication dateApplicantTitle
US3816774 *Jan 29, 1973Jun 11, 1974Victor Company Of JapanCurved piezoelectric elements
US4446544 *Nov 30, 1981May 1, 1984The United States Of America As Represented By The Secretary Of The NavySmall diameter, low frequency multimode hydrophone
US4941202 *Sep 13, 1982Jul 10, 1990Sanders Associates, Inc.Multiple segment flextensional transducer shell
US5225731 *Jun 13, 1991Jul 6, 1993Southwest Research InstituteSolid body piezoelectric bender transducer
US5900552 *Mar 28, 1997May 4, 1999Ohmeda Inc.Inwardly directed wave mode ultrasonic transducer, gas analyzer, and method of use and manufacture
Classifications
U.S. Classification310/358, 367/159, 367/168, 367/157, 310/337, 310/26, 310/369
International ClassificationG01S1/72
Cooperative ClassificationG01S1/72
European ClassificationG01S1/72