US3833770A

US3833770A - Electrostatic acoustic transducer

Info

Publication number: US3833770A
Application number: US00230435A
Authority: US
Inventors: N Atoji; T Aoi
Original assignee: Matsushita Electric Industrial Co Ltd
Current assignee: Panasonic Holdings Corp
Priority date: 1971-03-11
Filing date: 1972-02-29
Publication date: 1974-09-03
Anticipated expiration: 1991-09-03
Also published as: FR2186799A1; FR2186799B1; GB1387453A; DE2211729A1; CA947856A; JPS5632839B1

Abstract

A high-fidelity electrostatic acoustic transducer comprising a pair of fixed electrodes with a multiplicity of small openings and supported opposite to each other and a vibrating film electret with a conductive layer formed on one side thereof, the vibrating film being held between the fixed electrodes as an acoustic transducer section. An electrostatic field is generated between the electret and one of the fixed electrodes by the electret and thereby the second higher harmonics generated between one of the fixed electrodes and the vibrating film electret are capable of being eliminated on the other fixed electrode.

Description

United States Patent 1 1 Atoji et a1.

ELECTROSTATIC ACOUSTIC TRANSDUCER Inventors: Nobuhisa Atoji, Shijonawato; Takahisa Aoi, Moriguchi, both of Japan Matsushita Electric Industrial Co., Ltd.,- Osaka, Japan Filed: Feb. 29, 1972 Appl. No.: 230,435

Assignee:

Foreign Application Priority Data Mar. 11, 1971 Japan 46-13828 US. Cl. ..L 179/111 E, 307/88 ET Int. Cl H04r 19/00 Field of Search 179/111 R, 111 E;

References Cited UNITED STATES PATENTS 11/1961 Williamson 179/111 R Sept. 3, 1974 3,118,022 1/1964 Sessler et al. 179/111 R 3,160,715 12/1964 Gussing 179/111 R Primary Examiner-Kathleen H. Claffy Assistant Examiner-Th0mas L. Kundert Attorney, Agent, or Firm-Stevens, Davis, Miller & Mosher [5 7 ABSTRACT 5 Claims, 5 Drawing Figures l l lq'lgl 3 Ln: 1/] 1 A 1 1 V2] VA? PAIENIEMP awn SHEEI 30F 3 W W M W NH,

FREQUENCIES (HZ) ELECTROSTATIC ACOUSTIC TRANSDUCER An object of the present invention is to provide an electrostatic acoustic transducer comprising a pair of fixed electrodes with a multiplicity of openings, said electrodes being supported opposite to each other, and

a single vibrating film electret with a conductive layer formed on one side thereof, said vibrating film electret being held between said fixed electrodes.

The acoustic transducer according to the present invention requires no DC voltage as in the conventional acoustic transducer. Simple in construction and easy to operate, the acoustic transducer according to the invention permits higher harmonic distortion to be reduced greatly. In addition, since a very thin plastic vibrating film electret is employed, the acoustic efficiency is improved, resulting in a great commercial value.

The above and other objects, features and advantage will be made apparent from the detailed description taken in conjunction with the accompanying drawings,

in which: I

FIGS. 1 and 2 are diagrams showing the operating principle of a speaker embodying the present invention;

' FIG. 3 is a diagram for explaining the operation of shown in FIGS. 1 and 2. In these figures, the referencenumeral 1 shows a vibratin gfilm electret made of a high polymersuch as plastic resin with permanent surface charges. On one side of this high polymer vibrating .film electret is coated or deposited by evaporation a very thin layer 2 of conductive paint or metal such as aluminum or silver. The numerals 4 and 4' show fixed electrodes with numerous openings necessary for acoustic radiation, and the

numerals

3 and 3 layers of air existing betweenthe vibrating film l and the fixed electrode 4 and between thevibrating film l and the ness of the vibrating film l is negligibly small compared with the distances d, and d The symbol E denotes an electrostatic field caused by the electret. When the signal v is applied, the circuit of FIG. 2 may be simplified as shown in FIG. 3 for convenience of illustration. The force dF is defined as a force acting on a minute area dS on the vibrating film 1 due to an electric field generated in an airgap between the fixed electrode 4 and the conductive layer 2, and the force dF is defined as a force acting on the minute area dS on the vibrating film 1 due to an electric field generated in an airgap between the fixed electrode 4 and the vibrating film 1. An electrostatic voltage U is generated between the fixed electrode 4 and the vibrating film l by the permanent electric charges Q, on the surface of the vibrating film electret 1. Since the conductive layer 2 on the vibrating film 1 equivalently acts as being electrostatically grounded, the electric force lines due to the charge Q charged on the vibrating film 1 exist in the airgap 3' but do not exist in the airgap 3. Accordingly, in the airgap 3, no static electricity (DC. voltage) U, due to the charge Q, is generated between the vibrating film 1 (the conductive layer 2) and the fixed electrode 4. The force dF which is generated only due to an AC signal e is expressed as F. o ei /ztd. m as Therefore, the combined force applied to the area d8 of the vibrating film 1 is dF (dF dF )dS From this equation (3 is obtained the force f applied to the unit area, which is fixed electrode 4" respectively. As shown inFIG. 1, the

AC'signal V is applied between the fixed electrodes 4 and 4' after being boosted by the transformer T included in a power circuit. Capacitors C and C are provided for balance and the resistor R for controlling the higher harmonics. FIG.. 2 shows an example in which a push-pull transfonner T is employed as a power source.

The operating principle of the above-described embodiment will be now explained in detail. Referring to FIGS. 1 and 2, it is assumed that the distancesbetween the fixed electrode 4 and the conductive layer 2 on the thin vibrating film electret 1 and between the other fixed electrode 4'- and the conductive layer 2 are set at d, and d respectively. It is also assumed that the thick The most'significant feature of the invention'is that the second higher harmonics in equation 1 are reduced from second higher harmonics in equation 2, thereby lessening the second higher harmonics greatly. This fact is apparent from

theequations

3 and 4. From the equation 4, alternating element F of the force F applied to the whole of the vibrating film is obtained when 1, 2 h

where Y If 1; d8.

In the equation 5, assuming that d, d d and e e where V is the volume velocity and equals jw Y. It-is understood from the equation 6 that the higher harmonics are capable of being sharply reduced if the relation e/U I is satisfied.

As can be seen from the above description, the acoustic transformer according to the present invention employs a sheet of plastic vibrating film electret with a conductive layer'on one side thereof, whereby an AC-derived force is generated in one of the opposite fixed electrodes by superimposing an AC signal upon the electrostatic voltage U due to the permanent surface charge Q Higher harmonics generated at this time are eliminated'by the other fixed electrode.

An electret capacitor speaker is shown in FIG. 4 as an exampleof the present invention. In this figure, the reference numerals 1 to 5 denote like components sis those shown in FIGS. 1 and 2. The numeral 6 shows fa ring of metal or plastics to which a vibrating film is a tached by fusion or supersonic wave or by the agency of a high polymer bonding agent. The numerals 7 an d 7 show fastening means of plastic for applying tensio to the vibrating film 1, the fixed electrodes 4 and being secured to the fastening means 7 and 7. The n i merals 8 and 9 show a boltand a nut respectively f r securing the whole transducer, and

numerals

10 and 10 take-out portions of lead wires made of conductive paint or printed member for the fixed electrodes 4 an 4, which are connected to the

lead wires

12 and 13. The conductive layer 2 of the vibrating film l is i contact with the lead wire 11. The resistor R as show in FIGS. 1 and 2 is very high in resistance value, an

' may be replaced by the contact resistance between th conductive layer 2 and the lead wire 11. In FIG. 5th higher harmonic distortion characteristics of the speaker constructed as above described are compare with those of the conventional speaker of the electrostatic type. It is obvious from the figure that the second higher harmonic distortion characteristic A according to the present invention is superior to the like characteristic B of the conventional speaker. The characteristic curve C shows'an output soundpressure level according to the present invention.

What we claim is:

1. An electrostatic acoustic transducer comprising a pair of fixed electrodes each with a multiplicity of openings,,said electrodes being supported opposite to each other, and a single vibrating film electret with a conductive layer formed on one outer surface thereof facing only one of said electrodes, said vibrating film connected capacitors is inserted between said output terminals of said boosting transformer, and a' junction point between the pair of capacitors is connected through a resistor to said conductive layer.

4. An electrostatic acoustic transducer according to claim 1, in which said conductive layer is connected with an intermediate terminalof the secondary winding of a push-pull transformer, and the end terminals of said secondary winding of said push-pull transformer are connected with the fixed electrodes respectively.

5. An electrostatic acoustic transducer comprising an annular frame, a single layer vibrating film electret having a conductive layer formed on one outer surface and attached to the uppersurface of said frame, a pair of fixed electrodes between which said vibrating film electret is interposed, said conductive layer being in spaced facing relation to only one of said electrodes, and a fastening means for supporting said annular frame and said fixed electrodes, said fastening means beingprovided with a conductive layer and terminals electrically connected withsaid fixed electrodes.

Claims

1. An electrostatic acoustic transducer comprising a pair of fixed electrodes each with a multiplicity of openings, said electrodes being supported opposite to each other, and a single vibrating film electret with a conductive layer formed on one outer surface thereof facing only one of said electrodes, said vibrating film electret being held between said fixed electrodes and separated therefrom by an air layer.

2. An electrostatic acoustic transducer according to claim 1, in which said pair of fixed electrodes are connected with the output terminals of the secondary winding of a boosting transformer.

3. An electrostatic acoustic transducer according to claim 1, in which said pair of fixed electrodes are connected with the output terminals of the secondary winding of a boosting transformer, a pair of series-connected capacitors is inserted between said output terminals of said boosting transformer, and a junction point between the pair of capacitors is connected through a resistor to said conductive layer.

4. An electrostatic acoustic transducer according to claim 1, in which said conductive layer is connected with an intermediate terminal of the secondary Winding of a push-pull transformer, and the end terminals of said secondary winding of said push-pull transformer are connected with the fixed electrodes respectively.

5. An electrostatic acoustic transducer comprising an annular frame, a single layer vibrating film electret having a conductive layer formed on one outer surface and attached to the upper surface of said frame, a pair of fixed electrodes between which said vibrating film electret is interposed, said conductive layer being in spaced facing relation to only one of said electrodes, and a fastening means for supporting said annular frame and said fixed electrodes, said fastening means being provided with a conductive layer and terminals electrically connected with said fixed electrodes.