US2775749A - Mass-loaded ring vibrator - Google Patents

Mass-loaded ring vibrator Download PDF

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US2775749A
US2775749A US346293A US34629353A US2775749A US 2775749 A US2775749 A US 2775749A US 346293 A US346293 A US 346293A US 34629353 A US34629353 A US 34629353A US 2775749 A US2775749 A US 2775749A
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ring
vibrator
mass
protuberances
resonant frequency
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Sussman Harry
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B06GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06BMETHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B1/00Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
    • B06B1/02Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy

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  • FIG. 2 H. sussMAN MASS-LOADED RING VIBRATOR Filed April 1, 1953 FIG. 2
  • This invention concerns a mass-loaded ring vibrator.
  • the invention concerns a vibrator that can be used in the resonant range as a receiver or as a transmitter of airborne or underwater sound.
  • the resonant frequency of a ring vibrator is determined by the dimensions and the elastic properties of the ring.
  • the fundamental resonant frequency is proportional to the ratio of the stiffness to the mass and, therefore, to its average diameter. Increasing the radial thickness of the ring increases its mass but also increases its stiffness in approximately the same ratio so that its fundamental radial resonant frequency changes very little. As a result of this situation, rings which are resonant in the lower portion of the audio-frequency range are very large in diameter.
  • the resonant frequency of a magnetostrictive ring may be lowered by cutting a very large number of radial slots or tooth-shaped protuberances uniformly around the ring in such a manner that the mass of the ring is increased without any essential increase in its elasticity.
  • the mass of the ring is increased but the elasticity is not significantly changed.
  • the present invention marks an advance from the prior art by providing a massloaded ring having a relatively few radial protuberances that increase the mass and decrease the eifective stiffness of the ring.
  • the protuberances are preferably detachable from the ring.
  • the protuberances are of a preselected size and weight to regulate the resonant frequency of the ring. In this manner a structure of given size can be made to resonate at a much lower frequency than the fundamental resonance of an equivalent simple ring.
  • the resonant frequency can be changed by detaching one set of protuberances or by attaching a set of added weights.
  • the mass may be increased while the elasticity is decreased thereby achieving lower frequences for the same sized structure.
  • the vibrator improvement of this invention is adaptable to magnetostrictive laminations, piezoelectric rings, and electrostrictive rings.
  • the resonant frequency can be changed by a change in the number of and/ or the size of the protuberances.
  • An object of this invention is to provide a mass-loaded ring vibrator.
  • Another object is to provide a vibrator ring and means which increase the mass and decrease the efiective stiltness of the ring.
  • Another object is to provide a ring and means for varying the fundamental resonant frequency of the ring.
  • Another object is to provide a ring that can be made nited States Patent ice of piezoelectric, electrostrictive, or magnetostrictive material and means for increasing the mass and decreasing the effective stiffness of the ring and for varying the fundamental resonant frequency of the ring.
  • Fig. 1 is a cross-sectional view taken along line 11 of Fig. 2 of a preferred embodiment of the invention including a ring piezoelectric or electrostrictive material.
  • Fig. 2 is a perspective view of the preferred. embodiment shown in Fig. 1.
  • Fig. 3 is a fragmentary sectional view showing a modification of the invention including a ring of magnetostrictive material and an electrical coil therefor, and
  • Fig. 4 is a fragmentary sectional view of a modification of the invention shown in Fig. 1.
  • the active element shown in Fig.1 is either a piezoelectric ring 1 or a polarized electrostrictive barium titanate ring 1.
  • Six narrow metal protuberances 2 are evenly spaced and detachably fastened by screws 10 or the like to the inner surface of ring 1.
  • Ring 1 is excited into resonant vibration by an alternating current of the proper frequency. This current is fed into terminals 3 and 4, which are connected to an inner electrode 5 and an outer electrode 6.
  • Each of electrodes 5, 6 is a layer of silver-conducting paint baked to the inner and outer surfaces of ring 1.
  • the resonant frequency of the massloaded ring is lower than that of ring 1 alone because of the added mass of the protuberances 2 and the lower effective stiffness of the mass-loaded ring 1 due to some bending vibration, which is a result of the small number of added discrete masses.
  • the resonant frequency may be changed by sliding six additional keyed weights 7 onto the protuberances 2 and fastening these by means of screws 8.
  • electrical insulation and protection against corrosion are provided.
  • FIG. 3 there is shown a modification of this invention differing from the form shown in Figs. 1 and 2 in that it includes a magnetostrictive ring 111 and a toroidal coil 11.
  • Fig. 4 there is shown a modification of this invention wherein the protuberances 2 and the weights 7 are disposed on the outside of ring 1.
  • a relatively small number of protuberances 2 that are uniformly spaced, are attached on the inside and/ or outside of ring 1.
  • the protuberances 2 may be detachable, permanently fastened, or an integral part of the ring 1.
  • the ring 1 may be of magnetostrictive, piezoelectric, or polarized electrostrictive material such as barium titanate.
  • an alternating current in toroidal winding 11 excites the structure into vibration.
  • the magnetostrictive structure is used as a sound receiver, a voltage is generated in the toroidal winding as a result of the resonant vibration produced in the structure by sound waves.
  • the curved inner and outer surfaces of the ring 1 are covered with electrodes 5, 6 suitable for driving the structure as a generator or for collecting the generated electric charges when the unit acts as a sound receiver.
  • the embodiments described provide for changing the resonant frequency of the device by changing the attached Weights 7. If only a single resonant frequency is desired, this provision can be omitted. In that case, it is also possible to make the ring 1 and its protuberances 2 in one piece.
  • the number of weights 7, the method of attachment, and their location may be varied in several different ways.
  • a mass-loaded ring vibrator comprising a ring of transducing material adapted for reversibly converting energy which is quantitatively characterized by flux density into energy of mechanical vibration, and a small number of separate narrow radial protuberances detachably fastened to said ring.
  • a mass-loaded ring vibrator comprising a ring, said ring being made of piezoelectric mate rial, and a pair of electrodes formed' one on the inside and one on the outside of said ring, and a small number of separate narrow radial protuberances fastened to said ring.
  • a mass-loaded ring vibrator comprising a ring, said ring being made of electrostrictive material, a pair of electrodes formed one on the inside and one on the outside of said ring, and a small number of Separate narrow radial protuberances fastened to said ring.
  • a mass-loaded ring vibrator comprising a ring, said ring being made of magnetostrictive material, a toroidal winding on said ring, and a small num- Pierce Oct. 11, 1932 Thuras Sept. 5, 1950

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  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Transducers For Ultrasonic Waves (AREA)

Description

Dec. 25, 1956 H. sussMAN MASS-LOADED RING VIBRATOR Filed April 1, 1953 FIG. 2
INVENTOR HARRY SUSSMAN BY 5 mro nnav 2,775,749 MASS-LOADED RING VIBRATOR Harry Sussman, Waterford, Conn.
Application April 1, 1953, Serial No. 346,293
13 Claims. (Cl. 340-8) (Granted under Title 35, U. S. Code (1952), see. 266) The invention described herein may be manufactured and used by or for the Government of the United States of American for governmental purposes without the payment of any royalties thereon or therefor.
This invention concerns a mass-loaded ring vibrator. In particular the invention concerns a vibrator that can be used in the resonant range as a receiver or as a transmitter of airborne or underwater sound.
The resonant frequency of a ring vibrator is determined by the dimensions and the elastic properties of the ring. The fundamental resonant frequency is proportional to the ratio of the stiffness to the mass and, therefore, to its average diameter. Increasing the radial thickness of the ring increases its mass but also increases its stiffness in approximately the same ratio so that its fundamental radial resonant frequency changes very little. As a result of this situation, rings which are resonant in the lower portion of the audio-frequency range are very large in diameter.
In the prior art it is known that the resonant frequency of a magnetostrictive ring may be lowered by cutting a very large number of radial slots or tooth-shaped protuberances uniformly around the ring in such a manner that the mass of the ring is increased without any essential increase in its elasticity. By resort to the above expedient the mass of the ring is increased but the elasticity is not significantly changed.
The present invention marks an advance from the prior art by providing a massloaded ring having a relatively few radial protuberances that increase the mass and decrease the eifective stiffness of the ring. The protuberances are preferably detachable from the ring. The protuberances are of a preselected size and weight to regulate the resonant frequency of the ring. In this manner a structure of given size can be made to resonate at a much lower frequency than the fundamental resonance of an equivalent simple ring. The resonant frequency can be changed by detaching one set of protuberances or by attaching a set of added weights.
In the vibrator of this invention the mass may be increased while the elasticity is decreased thereby achieving lower frequences for the same sized structure. Whereas the aforementioned prior art is limited to magnetostrictive laminations, the vibrator improvement of this invention is adaptable to magnetostrictive laminations, piezoelectric rings, and electrostrictive rings. In the prior art only a single resonant frequency is achieved by a given resonator, but in the vibrator of this invention the resonant frequency can be changed by a change in the number of and/ or the size of the protuberances.
An object of this invention is to provide a mass-loaded ring vibrator.
Another object is to provide a vibrator ring and means which increase the mass and decrease the efiective stiltness of the ring.
Another object is to provide a ring and means for varying the fundamental resonant frequency of the ring.
Another object is to provide a ring that can be made nited States Patent ice of piezoelectric, electrostrictive, or magnetostrictive material and means for increasing the mass and decreasing the effective stiffness of the ring and for varying the fundamental resonant frequency of the ring.
Other objects and many of the attendant advantages of this invention will be readily appreciated as the same becomes better understood by reference to the following detailed description when considered in connection with the accompanying drawings wherein:
Fig. 1 is a cross-sectional view taken along line 11 of Fig. 2 of a preferred embodiment of the invention including a ring piezoelectric or electrostrictive material.
Fig. 2 is a perspective view of the preferred. embodiment shown in Fig. 1.
Fig. 3 is a fragmentary sectional view showing a modification of the invention including a ring of magnetostrictive material and an electrical coil therefor, and
Fig. 4 is a fragmentary sectional view of a modification of the invention shown in Fig. 1.
The active element shown in Fig.1 is either a piezoelectric ring 1 or a polarized electrostrictive barium titanate ring 1. Six narrow metal protuberances 2 are evenly spaced and detachably fastened by screws 10 or the like to the inner surface of ring 1. Ring 1 is excited into resonant vibration by an alternating current of the proper frequency. This current is fed into terminals 3 and 4, which are connected to an inner electrode 5 and an outer electrode 6. Each of electrodes 5, 6 is a layer of silver-conducting paint baked to the inner and outer surfaces of ring 1. The resonant frequency of the massloaded ring is lower than that of ring 1 alone because of the added mass of the protuberances 2 and the lower effective stiffness of the mass-loaded ring 1 due to some bending vibration, which is a result of the small number of added discrete masses. The resonant frequency may be changed by sliding six additional keyed weights 7 onto the protuberances 2 and fastening these by means of screws 8. For use under Water, electrical insulation and protection against corrosion (not shown) are provided.
In Fig. 3 there is shown a modification of this invention differing from the form shown in Figs. 1 and 2 in that it includes a magnetostrictive ring 111 and a toroidal coil 11.
In Fig. 4 there is shown a modification of this invention wherein the protuberances 2 and the weights 7 are disposed on the outside of ring 1.
In this invention, a relatively small number of protuberances 2 that are uniformly spaced, are attached on the inside and/ or outside of ring 1. The protuberances 2 may be detachable, permanently fastened, or an integral part of the ring 1. The ring 1 may be of magnetostrictive, piezoelectric, or polarized electrostrictive material such as barium titanate. In the case of the magneto strictive ring In acting as a sound transmitter, an alternating current in toroidal winding 11 excites the structure into vibration. When the magnetostrictive structure is used as a sound receiver, a voltage is generated in the toroidal winding as a result of the resonant vibration produced in the structure by sound waves. For the piezoelectric and the electrostrictive materials, the curved inner and outer surfaces of the ring 1 are covered with electrodes 5, 6 suitable for driving the structure as a generator or for collecting the generated electric charges when the unit acts as a sound receiver.
The embodiments described provide for changing the resonant frequency of the device by changing the attached Weights 7. If only a single resonant frequency is desired, this provision can be omitted. In that case, it is also possible to make the ring 1 and its protuberances 2 in one piece. The number of weights 7, the method of attachment, and their location may be varied in several different ways.
Obviously many modifications and variations of the present invention are possible in the light of the above teachings. It is therefore to be understood that within the scope of the appended claims the invention may be practiced otherwise than as specifically described.
I claim: 7
1. A mass-loaded ring vibrator, said vibrator comprising a ring of transducing material adapted for reversibly converting energy which is quantitatively characterized by flux density into energy of mechanical vibration, and a small number of separate narrow radial protuberances detachably fastened to said ring.
2. The vibrator defined in claim 1 in which -said material is piezoelectric material.
3. The vibrator defined in claim 1 in which said material is electrostrictive material.
4. The vibrator defined in claim 1 in which said material is rnagnetostrictive material.
5. The vibrator defined in claim 1 in which said protuberances are'insidc said ring.
6. The vibrator defined in claim 1 in which said protuberances are outside said ring.
7. The vibrator defined in claim 1 in which said protuberances are made of metal.
8. The vibrator defined in claim 1 in combination with 25 additional weights fastened radially onto said protuberances.
9. A mass-loaded ring vibrator, said vibrator comprising a ring, said ring being made of piezoelectric mate rial, and a pair of electrodes formed' one on the inside and one on the outside of said ring, and a small number of separate narrow radial protuberances fastened to said ring.
10. The vibrator defined in claim 9 in which said electrodes are made ofsilver.
11. A mass-loaded ring vibrator, said vibrator comprising a ring, said ring being made of electrostrictive material, a pair of electrodes formed one on the inside and one on the outside of said ring, and a small number of Separate narrow radial protuberances fastened to said ring.
12. The vibrator definedin. claim 11 in which said electrodes are made of silver.
13. A mass-loaded ring vibrator, said vibrator comprising a ring, said ring being made of magnetostrictive material, a toroidal winding on said ring, and a small num- Pierce Oct. 11, 1932 Thuras Sept. 5, 1950
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Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2926622A (en) * 1955-08-23 1960-03-01 Gulton Ind Inc Ultrasonic soldering pot
US3111595A (en) * 1959-09-25 1963-11-19 Acoustica Associates Inc Low frequency resonant transducers
US3139603A (en) * 1960-12-29 1964-06-30 Acoustica Associates Inc Mass-loaded electromechanical transducer
FR2123048A1 (en) * 1970-08-07 1972-09-08 Electronique Appliquee
US3731267A (en) * 1971-01-04 1973-05-01 O Brandt Electro-acoustic transducer
EP0169727A2 (en) * 1984-07-25 1986-01-29 Westinghouse Electric Corporation Broadband radial vibrator transducer
US4642802A (en) * 1984-12-14 1987-02-10 Raytheon Company Elimination of magnetic biasing using magnetostrictive materials of opposite strain
US5229980A (en) * 1992-05-27 1993-07-20 Sparton Corporation Broadband electroacoustic transducer

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1882398A (en) * 1928-08-17 1932-10-11 Pierce George Washington Magnetostrictive vibrator
US2521136A (en) * 1949-04-28 1950-09-05 Commerce National Bank Of Hydrophone

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1882398A (en) * 1928-08-17 1932-10-11 Pierce George Washington Magnetostrictive vibrator
US2521136A (en) * 1949-04-28 1950-09-05 Commerce National Bank Of Hydrophone

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2926622A (en) * 1955-08-23 1960-03-01 Gulton Ind Inc Ultrasonic soldering pot
US3111595A (en) * 1959-09-25 1963-11-19 Acoustica Associates Inc Low frequency resonant transducers
US3139603A (en) * 1960-12-29 1964-06-30 Acoustica Associates Inc Mass-loaded electromechanical transducer
FR2123048A1 (en) * 1970-08-07 1972-09-08 Electronique Appliquee
US3731267A (en) * 1971-01-04 1973-05-01 O Brandt Electro-acoustic transducer
EP0169727A2 (en) * 1984-07-25 1986-01-29 Westinghouse Electric Corporation Broadband radial vibrator transducer
EP0169727A3 (en) * 1984-07-25 1987-05-27 Gould Inc. Broadband radial vibrator transducer
US4642802A (en) * 1984-12-14 1987-02-10 Raytheon Company Elimination of magnetic biasing using magnetostrictive materials of opposite strain
US5229980A (en) * 1992-05-27 1993-07-20 Sparton Corporation Broadband electroacoustic transducer

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