while this invention is susceptible of embodiments in may different forms , there is shown in the drawings and will herein be described in detail preferred embodiments of the invention . the present disclosure is to be considered as an exemplification of the principles of the invention and is not intended to limit the broad aspect of the invention to the embodiments illustrated . referring now to the drawings , and particularly to fig1 - 3 , an acoustic transducer in accordance with the present invention is disclosed . the acoustic transducer 10 includes a conductive diaphragm 12 and a perforated member 40 supported by a substrate 30 and separated by an air gap 20 . a very narrow air gap or width 22 exists between the diaphragm 12 and substrate 30 allowing the diaphragm to move freely in its plane , thereby relieving any intrinsic stress in the diaphragm material and decoupling the diaphragm from the substrate . a number of small indentations 13 are made in the diaphragm to prevent stiction in the narrow gap between the diaphragm and substrate . the lateral motion of the diaphragm 12 is restricted by a support structure 41 in the perforated member 40 , which also serves to maintain the proper initial spacing between diaphragm and perforated member . the support structure 41 may either be a continuous ring or a plurality of bumps . if the support structure 41 is a continuous ring , then diaphragm 12 resting on the support structure 41 forms tight acoustical seal , leading to a well controlled low frequency roll - off of the transducer . if the support structure 41 is a plurality of bumps , then the acoustical seal can be formed either by limiting the spacing between the bumps , by the narrow air gap 22 , or a combination thereof . the conducting diaphragm 12 is electrically insulated from the substrate 30 by a dielectric layer 31 . a conducting electrode 42 is attached to the non - conductive perforated member 40 . the perforated member contains a number of openings 21 through which a sacrificial layer ( not shown ) between the diaphragm and perforated member is etched during fabrication to form the air gap 20 and which later serve to reduce the acoustic damping of the air in the air gap to provide sufficient bandwidth of the transducer . a number of openings are also made in the diaphragm 12 and the perforated member 40 to form a leakage path 14 which together with the compliance of the back chamber ( not shown ), on which the transducer will be mounted , forms a high - pass filter resulting in a roll - off frequency low enough not to impede the acoustic function of the transducer and high enough to remove the influence of barometric pressure variations . the openings 14 are defined by photo lithographic methods and can therefore be tightly controlled , leading to a well defined low frequency behavior of the transducer . the attachment of the perforated member 40 along the perimeter 43 can be varied to reduce the curvature of the perforated member due to intrinsic internal bending moments . the perimeter can be a continuous curved surface ( fig1 - 3 ) or discontinuous , such as corrugated ( fig4 ). a discontinuous perimeter 43 provides additional rigidity of the perforated member 40 thereby reducing the curvature due to intrinsic bending moments in the perforated member 40 . turning to fig5 - 7 , an alternative embodiment of an acoustic transducer in accordance with the present invention is depicted . the transducer 50 includes a conductive diaphragm 12 and a perforated member 40 supported by a substrate 30 and separated by an air gap 20 . the diaphragm 12 is attached to the substrate through a number of springs 11 , which serve to mechanically decouple the diaphragm from the substrate , thereby relieving any intrinsic stress in the diaphragm . moreover , the diaphragm is released for stress in the substrate and device package . the lateral motion of the diaphragm 12 is restricted by a support structure 41 in the perforated member 40 , which also serves to maintain the proper initial spacing between diaphragm and perforated member 40 . the support structure 41 may either be a continuous ring or a plurality of bumps . if the support structure 41 is a continuous ring , then diaphragm 12 resting on the support structure 41 forms tight acoustical seal , leading to a well controlled low frequency roll - off of the transducer . if the support structure 41 is a plurality of bumps , then the acoustical seal can be formed by limiting the spacing between the bumps , or by providing a sufficiently long path around the diaphragm and through the perforations 21 . the conducting diaphragm 12 is electrically insulated from the substrate 30 by a dielectric layer 31 . a conducting electrode 42 is attached to the non - conductive perforated member 40 . the perforated member contains a number of openings 21 through which a sacrificial layer ( not shown ) between the diaphragm 12 and the perforated member is etched during fabrication to form the air gap 20 and which later serves to reduce the acoustic damping of the air in the air gap to provide sufficient bandwidth of the transducer . a number of openings are made in the support structure 41 to form a leakage path 14 ( fig6 ) which together with the compliance of the back chamber ( not shown ) on which the transducer can be mounted forms a high - pass filter resulting in a roll - off frequency low enough not to impede the acoustic function of the transducer and high enough to remove the influence of barometric pressure variations . the openings 14 are preferably defined by photo lithographic methods and can therefore be tightly controlled , leading to a well defined low frequency behavior of the transducer . the attachment of the perforated member along the perimeter 43 can be varied to reduce the curvature of the perforated member due to intrinsic internal bending moments . the perimeter 43 can be smooth ( fig5 - 7 ) or corrugated ( fig8 and 11 ). a corrugated perimeter provides additional rigidity of the perforated member thereby reducing the curvature due to intrinsic bending moments in the perforated member . in operation , an electrical potential is applied between the conductive diaphragm 12 and the electrode 42 on the perforated member . the electrical potential and associated charging of the conductors produces an electrostatic attraction force between the diaphragm and the perforated member . as a result , the free diaphragm 12 moves toward the perforated member 40 until it rests upon the support structure 41 , which sets the initial operating point of the transducer with a well defined air gap 20 and acoustic leakage through path 14 . when subjected to acoustical energy , a pressure difference appears across the diaphragm 12 causing it to deflect towards or away from the perforated member 40 . the deflection of the diaphragm 12 causes a change of the electrical field , and consequently capacitance , between the diaphragm 12 and the perforated member 40 . as a result the electrical capacitance of the transducer is modulated by the acoustical energy . a method to detect the modulation of capacitance is shown in fig9 . in the detection circuit 100 , the transducer 102 is connected to a dc voltage source 101 and a unity - gain amplifier 104 with very high input impedance . a bias resistor 103 ties the dc potential of the amplifier input to ground whereby the dc potential “ vbias ” is applied across the transducer . assuming in this circuit a constant electrical charge on the transducer , a change of transducer capacitance results in a change of electrical potential across the transducer , which is measured by the unity - gain amplifier . another method to detect the modulation of capacitance is shown in fig1 . in the detection circuit 200 , the transducer 202 is connected to a dc voltage source 201 and a charge amplifier configuration 205 with a feedback resistor 203 and capacitor 204 . the feedback resistor ensures dc stability of the circuit and maintains the dc level of the input of the amplifier , whereby the dc potential “ vbias - vb ” is applied across the transducer . assuming in this circuit a constant potential across the transducer , due to the virtual ground principle of the amplifier , a change of capacitance causes a change of charge on the transducer and consequently on the input side of the feedback capacitor leading to an offset between the negative and positive input on the amplifier . the amplifier supplies a mirror charge on output side of the feedback capacitor to remove the offset , resulting in a change of output voltage “ vout .” the charge gain in this circuit is set by the ratio between the initial transducer capacitance and the capacitance of the feedback capacitor . an advantage of this detection circuit is that the virtual ground principle of the amplifier eliminates any parasitic capacitance to electrical ground in the transducer , which otherwise attenuate the effect of the dynamic change of the microphone capacitance . however , care should be taken to reduce parasitic capacitances to minimize the of gain of any noise on the signal “ vb ” and the inherent amplifier noise . while the specific embodiment has been illustrated and described , numerous modifications come to mind without significantly departing from the spirit of the invention , and the scope of protection is only limited by the scope of the accompanying claims .