US3814864A - Condenser microphone having a plurality of discrete vibratory surfaces - Google Patents

Condenser microphone having a plurality of discrete vibratory surfaces Download PDF

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US3814864A
US3814864A US00272070A US27207072A US3814864A US 3814864 A US3814864 A US 3814864A US 00272070 A US00272070 A US 00272070A US 27207072 A US27207072 A US 27207072A US 3814864 A US3814864 A US 3814864A
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electrode
grooves
base
vibratile
diaphragm
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    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R19/00Electrostatic transducers
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R7/00Diaphragms for electromechanical transducers; Cones
    • H04R7/16Mounting or tensioning of diaphragms or cones
    • H04R7/24Tensioning by means acting directly on free portions of diaphragm or cone

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  • ABSTRACT The diaphragm of a condenser microphone is broken 52 us. c1 179/11111 up into many small Pieeee so that eeeh attains a 1511 1111.01 1.
  • the front plate or diaphragm must be under tension, when in final position, to bring its natural resonant frequency out of the range (higher) than the sounds to be picked up. It is highly desirable to keep the spacing between the plates as close as possible to keep the incremental dynamic capacitance change as high as possible to provide maximum output. There are limitations on the closeness of the two plates due to the applied polarizing voltage which tends to pull the plates together, and there must be space for the amplitude swings of the diaphragm due to impingement of sound thereon so that the diaphragm will not touch the back plate during these swings. Both or either one of the above could cause the one to touch the other which would interfere with the operation. The present construction and the simplicity of the currently existing consenser microphones would make it appear that improvements thereon would consist largly of refinements in design.
  • My design makes it possible to manufacture parts for the microphone in such a way that dependence on critical manufacturing tolerances is eliminated and these parts may be made by production methods which greatly decrease the overall expense by as much as a factor of 10.
  • my invention contemplates making the diaphragm effectively into a series of effective areas by using a series of concentric ring contacts which provide a series of concentric ring areas capable of independent vibration, each ring area being so narrow that the dia- 2 phragrn tension does not have to be great to raise the natural period above the resonance point in the desired range.
  • One way to do this is to provide a generally convex surface or crown having annular grooves concentric with the axis leaving a series of concentric raised portions. A flexible'diaphragm is stretched over that surface in contact with the high points on the convex surface to thus break the diaphragm up into annular sections.
  • the high points could be continuous annular rings they could be in a series of annularly arranged high points providing different shaped apices.
  • the spacing of the rings could also be changed so that each annular ring would be of a different width thus causing the natural resonance points for each ring to be at a different frequency.
  • the arrangement of the points could also be arranged to have different spacing to further break the resonance.
  • FIG. 1 is a highly enlarged sectional view of a microphone
  • FIG. 2 is a top plan view of the conductive back plate on a reduced scale to that of FIG. 1.
  • FIG. 3 is view similar to FIG. 2 of a modification thereof
  • FIG. 4 is a view similar to FIG. I of a modification thereof.
  • a casing ltl of generally cylindrical form having an inwardly extending flange 10a at one end and the other end interiorly threaded at 10b. interiorly a ring i2 is threaded in the end 10b.
  • a body of stiff insulating material comprising a circular base 14 having a circular flange 14a extending upwardly from the base, has secured thereto the conductive back plate, or disc 16, which constitutes one electrode of the condenser.
  • the back plate is of generally circular disc form having a stem 16a which may bear against the base and serves as a spacer and forms a back space between the back plate and the base.
  • the stem 16a has an axially threaded opening 16b whereby the electrode may be secured to the base k4 by a threaded fastener 18, the head of which engages the bottom of the base.
  • a threaded fastener 18 the head of which engages the bottom of the base.
  • a series of concentric grooves 160 which may vary in number but are shown as three in the drawing, are cut into surface to such a depth that they almost touch at their edges leaving a plurality of circular concentric ridges l6e the highest portions of which are disposed along and follow the contour of the original surface and are sharp or of minimum area.
  • a depression 16d of the same contour as the grooves is provided at the center.
  • the grooves preferably vary in depth from the ridges l6e to their centers by approximately 0.001 inch or less.
  • Air holes or ducts 16f extend from the bottom of the grooves preferably to the bottom of the back plate 16 opening into the space between the disc 16 and the support 14.
  • grooves that have a parti-circular cross section.
  • the objective of the groove shape is to provide, together with the other electrode, maximum incremental capacitance change with impinging sound pressure while providing sufficient space for motional amplitude to occure and at the same time providing a damping means for prevention of the generation of resonance effects. It will -be apparent that zones of decreasing cross section of the grooves are provided, adjacent the ridges or points of contact of the diaphragm, which provide increased damping toward the points of contact with the diaphragm. The entraped air in these zones serves to increase the diaphragm stiffness and therefor the natural resonant frequency.
  • FIGS. 3 and 4 show an electrode I6, where the walls 16d of the grooves are normal to the surface, as can best be seen from FIG. 4.
  • the grooves, as best seen from FIG. 3 are eccentric to each other, thus providing ridges of varying width. It is apparent that the shape of the grooves as shown in FIG. 4, could be used in the electrode of FIG. I, where the grooves are concentric.
  • the other or vibrating electrode, or membrane 24 is comprised of a thin non-conducting flexible base material on the side toward the disc 16, having a flexible conducting surface on the outer side thereof.
  • a thin non-conducting flexible base material on the side toward the disc 16, having a flexible conducting surface on the outer side thereof.
  • One such material can be one of the fluorocarbon, polyester or polycarbonate foils such as Teflon with aluminum placed thereon by evaporation although the conducting material could be placed thereon by other means.
  • the flexible material 24 is secured in a zone at its periphery to a ring 26.
  • the ring and the material or membrane are ordinarily formed separately with the membrane stretched and secured to the ring in a stretched condition.
  • the assembly is then placed over the electrode 16 and then the base and electrode as an assembly 14 inserted into the housing or shell 10.
  • the adjustment ring 12 msy be of such a size that it easily threaded into the shell to directly engage the base 14 and hold the base toward the flanged end of the shell to thus clamp the ring 26 between the flange 10a of the shell and the ring 14a on the base 14. Under these conditions, the tension on the diaphragm 24 may be determined by the relative position of the electrode 16 and the base 14.
  • the relative position of the electrode 16 and the base 14 can be fixed by the screws 18 and 20 this allows a fixed but resilent tension to be placed on the membrane 24.
  • the arrangement shown also permits of further tightning the membrane by moving the base electrode 16 upward relative to the base I4.
  • thediaphragm tension may be fairly fixed when a ring such as 12 is used with a spring and the base and disc are secured together in the position shown.
  • the structure shown enables the tension on the diaphragm to be obtained by screwing in the ring 12 in sofar that the spring 28 is fully com pressed to cause the ring 14a to clamp the diaphragm ring 26 to the flange 100.
  • This pressure may be further varied by adjusting the plate 16 relative to the base 14 by means of the screws 18 20.
  • the spring could be eliminated and the ring 12 have direct contact with the base 14.
  • Constant tension of the diaphragm may be obtained by positioning the parts as shown in the drawing where the ring 14a on the base is out of contact with the ring 26 and the pressure is through the spring 28 and this tension may be varied by changing the position of the ring 12 and base 14 to the diaphragm by the back plate 16 or the relative position of the back plate and base by means of the screws 18 20.
  • the plastic and aluminum diaphragm are not suitable because of ambient conditions, of which temperature may be an example.
  • ambient conditions of which temperature may be an example.
  • the ridges at their peaks could be of insulating material provided by anodizing or otherwise coating of the back electrode in its convex form and then forming the grooves after anodization to leave anodized ridges.
  • the adjustments shown for tension would be useful.
  • the diaphragm may be permanently polarized to provide a self contained electric field by heating and cooling the dielectric material comprising the active microphone surface in the presence of a suitable electric fieldas is well known in the art or electrons may be directly implanted therein.
  • An electro-acoustic transducer having a vibratile conducting electrode and a fixed conducting electrode, the improvement in which comprises a surface on the fixed electrode having a plurality of projections which decrease in height from the midpoint outwardly toward the edge with the vibratile electrode stretched over the fixed electrode with said projections having ridges which are on a line having a convex curvature and whereby each point of contact provides substantially the same amount of tension on the diaphragm as the other points and wherein said points are provided by annular grooves in a convex surface.
  • said adjustment means includes a spring means between the fixed electrode and a support having a base is adjustably mounted in the housing.

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Signal Processing (AREA)
  • Multimedia (AREA)
  • Electrostatic, Electromagnetic, Magneto- Strictive, And Variable-Resistance Transducers (AREA)

Abstract

The diaphragm of a condenser microphone is broken up into many small pieces so that each attains a natural high frequency resonance above the range of sounds to be picked up with the sum total of the pieces providing an output as great as a single diaphragm with a lower impedance by providing a series of concentric ring contacts wih a diaphragm stretched over the rings, the highest points or ridges of which lie on a convex surface, to break up the diaphragm into annular sections.

Description

United States Patent 1191 Victoreen 1 June 4, 1974 CONDENSER MICROPHONE HAVING A 2,787,671 4/1957 Grosskopfet al 179/11 1 R 3 AT 2.910539 10/1959 Hartsfield 179/111 R ggggig OF mSCRETE w R ORY 3,041,418 6/1962 Luzzery 179/111 R 3,372.245 3/1968 Yoshida a 111. 179/111 R [76] inventor: John A. Victoreen, 350 N. Maitland Ave., Maitland, Fla. 32751 Primary ExaminerThomas W. Brown [22] Filed, Juiy 14 1972 Attorney, Agent, or Firm-J. Darrell Douglass [21] Appl. No.: 272,070 [57] ABSTRACT The diaphragm of a condenser microphone is broken 52 us. c1 179/11111 up into many small Pieeee so that eeeh attains a 1511 1111.01 1. 111m 19/00 tel high ftequehey teeehehee above the range of [58] Field of Search 179/181 R, 111 R Sounds to he Pieked up with the sum total of the pieces providing an output as great as a single dia- 56] References Cited phragm with a lower impedance by providing a series UNITED, STATESPATENTS v of Concentric ring contacts wih a diaphragm stretched 1 over the rings, the highest points or ridges of which lie 1 x2 a on a convexsurface, to break up the diaphragm into GISZ 1 v l,975,8()l 10/1934 Rieber 1 1 179/11 1- R e t 2,500.043 3 1950 Munson et al. 179/111' R v 12 Claims, 4 Drawing Figures I6!) I61: 16c loo I60 16 I40 Q b 7: 14
g. a 8 g a: 2'0 l8 PAJTENTEDJM 4m 3.814.864
SHEU 1 (If 2 l CONDENSER MICROPHONE HAVING A PLURALITY OF DISCRETE VIBRATORY SURFACES BACKGROUND OF THE INVENTION 1. Field of the Invention The construction of prior microphones consist essentially of a back plate, which is one plate of a condenser and a diaphragm which is spaced closely to the back plate that is the other plate of the condenser. A polarizing voltage is applied between the two plates, and the capacitance change provides the output from the device.
2. Description of the Prior Art In the prior art, the front plate or diaphragm must be under tension, when in final position, to bring its natural resonant frequency out of the range (higher) than the sounds to be picked up. It is highly desirable to keep the spacing between the plates as close as possible to keep the incremental dynamic capacitance change as high as possible to provide maximum output. There are limitations on the closeness of the two plates due to the applied polarizing voltage which tends to pull the plates together, and there must be space for the amplitude swings of the diaphragm due to impingement of sound thereon so that the diaphragm will not touch the back plate during these swings. Both or either one of the above could cause the one to touch the other which would interfere with the operation. The present construction and the simplicity of the currently existing consenser microphones would make it appear that improvements thereon would consist largly of refinements in design.
SUMMARY OF THE INVENTION 'of the diaphragm and tension thereof, which determines the upper level of natural resonant frequency, may be largely eliminated. One may reduce the natural period by reducing the operational size of the unit which ordinarily results in bad signal to noise ratio. By using a design where the diaphragm is broken up into many small pieces, each one attains such a natural high frequency that the tension of the diaphragm becomes relatively unimportant and the size of the pieces becomes insignificant, with a sum total output which is as great as a single diaphragm and a signal to noise ratio which may be as good or better than a diaphragm of the same size.
My design makes it possible to manufacture parts for the microphone in such a way that dependence on critical manufacturing tolerances is eliminated and these parts may be made by production methods which greatly decrease the overall expense by as much as a factor of 10.
Basically my invention contemplates making the diaphragm effectively into a series of effective areas by using a series of concentric ring contacts which provide a series of concentric ring areas capable of independent vibration, each ring area being so narrow that the dia- 2 phragrn tension does not have to be great to raise the natural period above the resonance point in the desired range. One way to do this is to provide a generally convex surface or crown having annular grooves concentric with the axis leaving a series of concentric raised portions. A flexible'diaphragm is stretched over that surface in contact with the high points on the convex surface to thus break the diaphragm up into annular sections. Instead of the high points being continuous annular rings they could be in a series of annularly arranged high points providing different shaped apices. The spacing of the rings could also be changed so that each annular ring would be of a different width thus causing the natural resonance points for each ring to be at a different frequency. The arrangement of the points could also be arranged to have different spacing to further break the resonance.
BRIEF DESCRIPTION OF THE DRAWING FIG. 1 is a highly enlarged sectional view of a microphone;
FIG. 2 is a top plan view of the conductive back plate on a reduced scale to that of FIG. 1.
FIG. 3 is view similar to FIG. 2 of a modification thereof;
FIG. 4 is a view similar to FIG. I of a modification thereof.
DESCRIPTION OF THE PREFERRED EMBODIMENT In the drawing, which is greatly enlarged, there is shown a casing ltl of generally cylindrical form having an inwardly extending flange 10a at one end and the other end interiorly threaded at 10b. interiorly a ring i2 is threaded in the end 10b. A body of stiff insulating material comprising a circular base 14 having a circular flange 14a extending upwardly from the base, has secured thereto the conductive back plate, or disc 16, which constitutes one electrode of the condenser. The back plate is of generally circular disc form having a stem 16a which may bear against the base and serves as a spacer and forms a back space between the back plate and the base. The stem 16a has an axially threaded opening 16b whereby the electrode may be secured to the base k4 by a threaded fastener 18, the head of which engages the bottom of the base. It is pointed out that the structure illustrated is for the purpose of explanation and a better understanding of the invention; certain of the dimensions as well as the forms are exaggerated for that purpose. A single screw 18 could be used to secure the electrode or back plate 16 and the base 14, together, but it is desirable to be able to adjust the relative positions of the parts 14 l6 and therefor screws 20 are threaded through the base 14 to engage with the bottom of rear of the disc 16 which together with the screw 18 enable the position of the disc 16 relative to the base 14 to be accuratly adjusted. As will later appear this also enables an adjustment of the diaphragm tension. Although it is contemplated that the positional relationship between the back plate or electrode disc l6 and the base 14 may be fixed as stated, it could be and is shown in this drawing as being adjustable to enable a degree of adjustment of The shape of the outer face of the electrode 16 can best be understood by an explanation of the manner in which it is made. The outer face of the back plate 16 is convex. It may be of parti-spherical form. For instance for a disc of A inch dia., the face would be formed on such a radius that a crown or center 0.005 inch higher than the edge is provided. Then a series of concentric grooves 160, which may vary in number but are shown as three in the drawing, are cut into surface to such a depth that they almost touch at their edges leaving a plurality of circular concentric ridges l6e the highest portions of which are disposed along and follow the contour of the original surface and are sharp or of minimum area. At the center a depression 16d of the same contour as the grooves is provided. The grooves preferably vary in depth from the ridges l6e to their centers by approximately 0.001 inch or less. Air holes or ducts 16f extend from the bottom of the grooves preferably to the bottom of the back plate 16 opening into the space between the disc 16 and the support 14.
It has been found that superior results are obtained by providing grooves that have a parti-circular cross section. The objective of the groove shape is to provide, together with the other electrode, maximum incremental capacitance change with impinging sound pressure while providing sufficient space for motional amplitude to occure and at the same time providing a damping means for prevention of the generation of resonance effects. It will -be apparent that zones of decreasing cross section of the grooves are provided, adjacent the ridges or points of contact of the diaphragm, which provide increased damping toward the points of contact with the diaphragm. The entraped air in these zones serves to increase the diaphragm stiffness and therefor the natural resonant frequency. This points up the fact that the cross section contour of the grooves 160, as well as the size of the ducts 16f, may be varied from that shown and described to vary the damping, the main criterion apparently being that the grooves preferably do not provide ridges with side walls normal to the surface, although such may also be useful. The grooves are preferebly concentric to each other, but there could be some eccentricity of the grooves to each other to provide ridges of varying width. FIGS. 3 and 4 show an electrode I6, where the walls 16d of the grooves are normal to the surface, as can best be seen from FIG. 4. In addition, the grooves, as best seen from FIG. 3 are eccentric to each other, thus providing ridges of varying width. It is apparent that the shape of the grooves as shown in FIG. 4, could be used in the electrode of FIG. I, where the grooves are concentric.
It is pointed out that ideally the high portions of the ridges 16c are disposed on such a line that the pressure of the diaphragm against the points is the same but that there could be some variation, due to manufacturing tolerances, where this condition might not be exactly obtained. This would still have no material effect on its operation due to the small vibrational areas.
The other or vibrating electrode, or membrane 24, is comprised of a thin non-conducting flexible base material on the side toward the disc 16, having a flexible conducting surface on the outer side thereof. One such material can be one of the fluorocarbon, polyester or polycarbonate foils such as Teflon with aluminum placed thereon by evaporation although the conducting material could be placed thereon by other means. The flexible material 24 is secured in a zone at its periphery to a ring 26. The ring and the material or membrane are ordinarily formed separately with the membrane stretched and secured to the ring in a stretched condition. The assembly is then placed over the electrode 16 and then the base and electrode as an assembly 14 inserted into the housing or shell 10. It is contemplated that the adjustment ring 12 msy be of such a size that it easily threaded into the shell to directly engage the base 14 and hold the base toward the flanged end of the shell to thus clamp the ring 26 between the flange 10a of the shell and the ring 14a on the base 14. Under these conditions, the tension on the diaphragm 24 may be determined by the relative position of the electrode 16 and the base 14.
As shown in the drawing, a spring 28 is disposed between the ring 12 and the base 14 which urges the base 14 and electrode 16 with the diaphragm 24 toward the flange 10a. The ring 26 eventually engages the flange 100. Under this condition shown, a constant tension is exerted on the diaphragm by virtue of the spring 28. In the drawing the ring 12 engages the spring 28 or other compressible material which in turn engages the base 14 and as the ring 12 is threaded inward the base 14, the ring 26, with its membrane, moved into contact with the flange at which time the membrane has been stretched into the multiple point engagement with the base electrode. Since the relative position of the electrode 16 and the base 14 can be fixed by the screws 18 and 20 this allows a fixed but resilent tension to be placed on the membrane 24. The arrangement shown also permits of further tightning the membrane by moving the base electrode 16 upward relative to the base I4. Thus thediaphragm tension may be fairly fixed when a ring such as 12 is used with a spring and the base and disc are secured together in the position shown.
Thus, to summarize, the structure shown enables the tension on the diaphragm to be obtained by screwing in the ring 12 in sofar that the spring 28 is fully com pressed to cause the ring 14a to clamp the diaphragm ring 26 to the flange 100. This pressure may be further varied by adjusting the plate 16 relative to the base 14 by means of the screws 18 20. Obviously in this case the spring could be eliminated and the ring 12 have direct contact with the base 14. Constant tension of the diaphragm may be obtained by positioning the parts as shown in the drawing where the ring 14a on the base is out of contact with the ring 26 and the pressure is through the spring 28 and this tension may be varied by changing the position of the ring 12 and base 14 to the diaphragm by the back plate 16 or the relative position of the back plate and base by means of the screws 18 20.
It is pointed out that the adjustment discussed such as the ability to use a spring to keep constant tension on the diaphragm, the screws connecting the back electrode to the base for relative positional variations are all in the nature of refinements and do not detract from the base electrode and the diaphragm stretched across it are such that a simplified structure may be realized and none of the adjustments needed.
It is contemplated that there may be occasions where the plastic and aluminum diaphragm are not suitable because of ambient conditions, of which temperature may be an example. In this instance and possibly for other reasons it may be desirable to use a simple metallic diaphragm which would not be inherently insulated from the base electrode. In this instance the ridges at their peaks could be of insulating material provided by anodizing or otherwise coating of the back electrode in its convex form and then forming the grooves after anodization to leave anodized ridges. With the use of a plain metallic diaphragm the adjustments shown for tension would be useful.
Although it has been stated that the device is to be used in the conventional way of condenser microphones by the application of a polarization voltage it is contemplated that the diaphragm may be permanently polarized to provide a self contained electric field by heating and cooling the dielectric material comprising the active microphone surface in the presence of a suitable electric fieldas is well known in the art or electrons may be directly implanted therein.
I claim:
I. An electro-acoustic transducer having a vibratile conducting electrode and a fixed conducting electrode, the improvement in which comprises a surface on the fixed electrode having a plurality of projections which decrease in height from the midpoint outwardly toward the edge with the vibratile electrode stretched over the fixed electrode with said projections having ridges which are on a line having a convex curvature and whereby each point of contact provides substantially the same amount of tension on the diaphragm as the other points and wherein said points are provided by annular grooves in a convex surface.
2. An apparatus as described in claim 1 wherein said grooves are concentric to each other.
3. An apparatus as described in claim 1 where said grooves are eccentric to each other.
4. An apparatus as described in claim 1 wherein said grooves are concave in cross section.
5. An apparatus as described in claim 1 wherein said grooves are square in cross section.
6. An apparatus as described in claim 4 wherein said concave grooves decrease in depth crosswise to their edges to the point of contact with the vibratile electrode to provide a decreasing acoustical friction from the edges towardthe center and to provide mechanical damping and wherein the vibratile electrode is stretched over the fixed electrode.
7. An apparatus as described in claim 4 wherein a space is provided back of the fixed electrode and ducts communicate with the grooves and said space.
8. An apparatus as described in claim 1 wherein means is provided to adjust the position of the fixed electrode relative to the periphery of the vibratile electrode and wherein the vibratile electrode has a holding means at its periphery and wherein a housing is provided and the holding means of the vibratile electrode is engaged with the housing.
9. An apparatus as described in claim 8 wherein said housing has a cylindrical inner wall with an inwardly extending flange at one end and a ring is in threaded engagement with the other end.
10. An apparatus as described in claim 8 wherein said adjustment means includes a spring means between the fixed electrode and a support having a base is adjustably mounted in the housing.
11. An apparatus as descriped in claim 10 wherein said adjustment means is arranged to adjust the position of the fixed electrode relative to the base.
12. An apparatus as described in claim 9 wherein said holding means for the vibratile electrode is engaged with said flange and a base is provided for the fixed electrode and the fixed electrode is axially adjustable relative to the base and means is provided to hold said base in clamping engagement with the said holding means and said flange.

Claims (12)

1. An electro-acoustic transducer having a vibratile conducting electrode and a fixed conducting electrode, the improvement in which comprises a surface on the fixed electrode having a plurality of projections which decrease in height from the midpoint outwardly toward the edge with the vibratile electrode stretched over the fixed electrode with said projections having ridges which are on a line having a convex curvature and whereby each point of contact provides substantially the same Amount of tension on the diaphragm as the other points and wherein said points are provided by annular grooves in a convex surface.
2. An apparatus as described in claim 1 wherein said grooves are concentric to each other.
3. An apparatus as described in claim 1 where said grooves are eccentric to each other.
4. An apparatus as described in claim 1 wherein said grooves are concave in cross section.
5. An apparatus as described in claim 1 wherein said grooves are square in cross section.
6. An apparatus as described in claim 4 wherein said concave grooves decrease in depth crosswise to their edges to the point of contact with the vibratile electrode to provide a decreasing acoustical friction from the edges toward the center and to provide mechanical damping and wherein the vibratile electrode is stretched over the fixed electrode.
7. An apparatus as described in claim 4 wherein a space is provided back of the fixed electrode and ducts communicate with the grooves and said space.
8. An apparatus as described in claim 1 wherein means is provided to adjust the position of the fixed electrode relative to the periphery of the vibratile electrode and wherein the vibratile electrode has a holding means at its periphery and wherein a housing is provided and the holding means of the vibratile electrode is engaged with the housing.
9. An apparatus as described in claim 8 wherein said housing has a cylindrical inner wall with an inwardly extending flange at one end and a ring is in threaded engagement with the other end.
10. An apparatus as described in claim 8 wherein said adjustment means includes a spring means between the fixed electrode and a support having a base is adjustably mounted in the housing.
11. An apparatus as descriped in claim 10 wherein said adjustment means is arranged to adjust the position of the fixed electrode relative to the base.
12. An apparatus as described in claim 9 wherein said holding means for the vibratile electrode is engaged with said flange and a base is provided for the fixed electrode and the fixed electrode is axially adjustable relative to the base and means is provided to hold said base in clamping engagement with the said holding means and said flange.
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Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3958662A (en) * 1975-02-18 1976-05-25 Bell Telephone Laboratories, Incorporated Tensioned diaphragm mounting for an electroacoustic transducer
US4081626A (en) * 1976-11-12 1978-03-28 Polaroid Corporation Electrostatic transducer having narrowed directional characteristic
DE2825756A1 (en) * 1977-06-13 1978-12-14 Polaroid Corp ELECTROACOUSTIC CONVERTER
US4409441A (en) * 1981-07-02 1983-10-11 Polaroid Corporation Ultrasonic transducer for use in a vibratory environment
WO2000035246A1 (en) * 1998-12-07 2000-06-15 American Technology Corporation Electrostatic transducer with nonplanar configured diaphragm
WO2011059384A1 (en) * 2009-11-10 2011-05-19 Ehrlund Goeran Electro acoustic transducer
US8155354B2 (en) 2005-07-01 2012-04-10 Ehrlund Goeran Electro acoustic transducer
US9685730B2 (en) 2014-09-12 2017-06-20 Steelcase Inc. Floor power distribution system
US9998820B2 (en) * 2016-01-19 2018-06-12 Donald Pierce Bearden Acoustic resonator for audio headphones
US20230097631A1 (en) * 2021-09-29 2023-03-30 Aac Acoustic Technologies (Shenzhen) Co., Ltd. Diaphragm, MEMS Microphone Using Same, and Manufacturing Method for Same

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US3958662A (en) * 1975-02-18 1976-05-25 Bell Telephone Laboratories, Incorporated Tensioned diaphragm mounting for an electroacoustic transducer
US4081626A (en) * 1976-11-12 1978-03-28 Polaroid Corporation Electrostatic transducer having narrowed directional characteristic
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US4409441A (en) * 1981-07-02 1983-10-11 Polaroid Corporation Ultrasonic transducer for use in a vibratory environment
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US8155354B2 (en) 2005-07-01 2012-04-10 Ehrlund Goeran Electro acoustic transducer
WO2011059384A1 (en) * 2009-11-10 2011-05-19 Ehrlund Goeran Electro acoustic transducer
US9685730B2 (en) 2014-09-12 2017-06-20 Steelcase Inc. Floor power distribution system
US10050424B2 (en) 2014-09-12 2018-08-14 Steelcase Inc. Floor power distribution system
US11063411B2 (en) 2014-09-12 2021-07-13 Steelcase Inc. Floor power distribution system
US11594865B2 (en) 2014-09-12 2023-02-28 Steelcase Inc. Floor power distribution system
US9998820B2 (en) * 2016-01-19 2018-06-12 Donald Pierce Bearden Acoustic resonator for audio headphones
US20230097631A1 (en) * 2021-09-29 2023-03-30 Aac Acoustic Technologies (Shenzhen) Co., Ltd. Diaphragm, MEMS Microphone Using Same, and Manufacturing Method for Same

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