The present invention generally relates to a capacitive microphone having a capability of acceleration noise cancelation. The microphone of the invention may find applications in smart phones, telephones, hearing aids, public address systems for concert halls and public events, motion picture production, live and recorded audio engineering, two-way radios, megaphones, radio and television broadcasting, and in computers for recording voice, speech recognition, VoIP, and for non-acoustic purposes such as ultrasonic sensors or knock sensors, among others.
A capacitance microphone converts acoustic signal to its mechanical vibration, and further converts to a capacitance signal.
“Squeeze film” and “squeezed film” refer to a type of hydraulic or pneumatic damper for damping vibratory motion of a moving component with respect to a fixed component. Squeezed film damping occurs when the moving component is moving perpendicular and in close proximity to the surface of the fixed component (e.g., between approximately 2 and 50 micrometers). The squeezed film effect results from compressing and expanding the fluid (e.g., a gas or liquid) trapped in the space between the moving plate and the solid surface. The fluid has a high resistance, and damps the motion of the moving component as the fluid flows through the space between the moving plate and the solid surface.
In capacitive microphones as shown in
Co-pending U.S. application Ser. No. 15/393,831 to the same assignee, which is incorporated herein by reference, teaches a so-called lateral mode microphone in which the movable membrane/diaphragm does not move into the fixed backplate, and the squeeze film damping is substantially avoided. An embodiment of the lateral mode microphone is shown in
However, such a lateral mode capacitive microphone suffers a problem. An acceleration of the microphone may affect the accuracy of sound detection. An acceleration of 1G on the direction that is normal to the flat area of conductor 202 (or membrane 202) causes a signal to be detected, whose value may be 13% of 1 Pa sound pressure. Signal to Acceleration Ratio (SAR) may be used to define this effect. For example, the SAR for a single slot design structure disclosed in the co-pending U.S. application Ser. No. 15/393,831 can be around 7.6, which is much smaller than the typical SAR 70-100 for a conventional MEMS microphone. A microphone with low SAR will suffer from inaccurate signal detection when the microphone vibrates at low frequency. For example, if the microphone, or a device using such a microphone (e.g. a cellphone), is being used in a running automobile, the shake or vibration of the device along the automobile is actually an acceleration applied on membrane 202 and may be “misread” as a sound signal.
Co-pending U.S. application Ser. No. 15/623,339 to the same assignee, which is incorporated herein by reference, provides an improved lateral mode capacitive microphone, in which the low SAR effect is compensated. Co-pending U.S. application Ser. No. 15/623,339 teaches a motional sensor is used in the microphone to estimate the noise introduced from acceleration or vibration of the microphone for the purpose of compensating the microphone output through a signal subtraction operation. In an embodiment, the motional sensor is identical to the lateral microphone, except that the movable membrane in the motional sensor has air ventilation holes for lowering the movable membrane's air resistance, and making the movable membrane responsive only to acceleration or vibration of the microphone.
However, random air ventilation holes will not have the most desired SAR compensation. Advantageously, the present invention provides a solution to such a problem.
The present invention provides a capacitive microphone having a capability of acceleration noise cancelation. The microphone includes (1) a moveable functional membrane comprising a basic functional membrane with an area Ao; and (2) a moveable reference membrane comprising a basic reference membrane. The basic reference membrane has one or more holes through the membrane's thickness, and the moveable reference membrane would be identical to the moveable functional membrane if the basic reference membrane does not have said one or more holes.
In various embodiments, the present invention utilizes a reference moving membrane that can detect the acceleration signal. The measured acceleration signal can then be used to cancel out the component of actual acceleration signal in the total (“gross”) signal as measured by the lateral microphone in real-time, through a signal subtraction operation.
The above features and advantages and other features and advantages of the present invention are readily apparent from the following detailed description of the best modes for carrying out the invention when taken in connection with the accompanying drawings.
The present invention is illustrated by way of example, and not by way of limitation, in the figures of the accompanying drawings and in which like reference numerals refer to similar elements. All the figures are schematic and generally only show parts which are necessary in order to elucidate the invention. For simplicity and clarity of illustration, elements shown in the figures and discussed below have not necessarily been drawn to scale. Well-known structures and devices are shown in simplified form in order to avoid unnecessarily obscuring the present invention. Other parts may be omitted or merely suggested.
In the following description, for the purposes of explanation, numerous specific details are set forth in order to provide a thorough understanding of the present invention. It is apparent, however, to one skilled in the art that the present invention may be practiced without these specific details or with an equivalent arrangement.
Where a numerical range is disclosed herein, unless otherwise specified, such range is continuous, inclusive of both the minimum and maximum values of the range as well as every value between such minimum and maximum values. Still further, where a range refers to integers, only the integers from the minimum value to and including the maximum value of such range are included. In addition, where multiple ranges are provided to describe a feature or characteristic, such ranges can be combined.
Without being bound by any particular theory or model, the present invention provides a mechanism of acceleration noise cancelation in MEMS capacitance microphone. A concept SAR (signal acceleration ratio) is used to measure how the effect of acceleration noise cancellation is. Then an Electro-Acoustic model is built to find the optimized hole density of cancelation structure, which indicates a few important factors that are related to the optimized hole density. Eventually, a conclusion of optimized hole density is addressed through linear approach. It has been discovered that, when HD is in a range of e.g. from 0.012% to 2.647% or a subrange thereof, the corresponding SAR values are at least 10%, 20%, 30%, 50%, 100%, 200%, or 300% higher than those SAR values when HD exceeds the range. For example, SAR values of the microphones according to the present invention may be at least 500, 1000, 2000, 3000, 6000, 9000, 12000, 15000, 24000 or even higher.
In order to minimize the effect of acceleration noise, a cancellation approach including two (or more) structures can be used at same time. One structure is a functional microphone (e.g. that including a moveable functional membrane 22 as shown in
As shown in
In typical embodiments of the invention, a reference membrane does not give exactly the same acceleration noise signal as a functional membrane because of the mass loss due to those opening holes. The more holes that are opened on the membrane, the less mass the membrane has. Less mass typically results in less deflection under acceleration. If there is too much mass loss, the acceleration noise cannot be compensating effectively. On the other hand, if there is only a few holes or the size of opening holes are too small, sound wave will still partially hit on the reference membrane and then cause a mechanical vibration, which weakens the desired sound signal after the minus operation. Therefore, it is a tradeoff between mass loss and weakened sound signal. There must be an optimized point where the noise compensation works most effectively.
Without being bound by any particular theory or model, a concept SAR (signal acceleration ratio) is defined as the ratio of the sound signal under 1 Pa sound pressure to the acceleration signal from 1 gravity (1 g) acceleration. For a capacitance microphone, signal comes from the capacitance change, which further comes from the change of membrane deflection. Thus SAR can also be expressed by SAR=Da/Dg, wherein Da is the amplitude of membrane vibration caused by 1 Pa pressure acoustic wave, and Dg is the membrane deflection caused by 1 g acceleration. For the membrane with opening holes, different hole density defines different SAR after compensation, which represents the effectiveness of acceleration noise cancelation.
Without being bound by any particular theory or model, an electro-acoustic model is used to study SAR performance of this acceleration noise compensation approach under different conditions. With this electro-acoustic model, a plot demonstrating the relationship between SAR and Hole Density (HD) on a reference membrane is shown in
In an embodiment of the invention as shown in
X=(−4.95×10−5)+(2.57×10−6)(Ao)−1/3+(−9.44×10−5)(Ma/Mo)2/3; and
Y=(−5.93×10−3)+(1.62×10−4)(Ao)−1/3+(−4.71×10−3)(Ma/Mo)2/3.
The following table lists some exemplary values of Ao (m2), Ma/Mo, and the Full Width at 10% Maximum:
In an embodiment of the invention as shown in
X=(−6.47×10−5)+(3.30×10−6)(Ao)−1/3+(−1.21×10−4)(Ma/Mo)2/3; and
Y=(−2.91×10−3)+(8.08×10−5)(Ao)−1/3+(−2.35×10−3)(Ma/Mo)2/3.
The following table lists some exemplary values of Ao (m2), Ma/Mo, and the Full Width at 20% Maximum:
In an embodiment of the invention as shown in
X=(−7.64×10−5)+(3.86×10−6)(Ao)−1/3+(−1.41×10−4)(Ma/Mo)2/3; and
Y=(−1.98×10−3)+(5.40×10−5)(Ao)−1/3+(−1.57×10−3)(Ma/Mo)2/3.
The following table lists some exemplary values of Ao (m2), Ma/Mo, and the Full Width at 30% Maximum:
In an embodiment of the invention as shown in
X=(−8.65×10−−5)+(4.35×10−6)(Ao)−1/3+(−1.59×10−4)(Ma/Mo)2/3; and
Y=(−1.37×10−3)+(3.96×10−5)(Ao)−1/3+(−1.18×10−3)(Ma/Mo)2/3.
The following table lists some exemplary values of Ao (m2), Ma/Mo, and the Full Width at 40% Maximum:
In an embodiment of the invention as shown in
X=(−9.53×10−5)+(4.81×10−6)(Ao)−1/3+(−1.76×10−4)(Ma/Mo)2/3; and
Y=(−1.09×10−3)+(3.15×10−5)(Ao)−1/3+(−9.47×10−4)(Ma/Mo)2/3.
The following table lists some exemplary values of Ao (m2), Ma/Mo, and the Full Width at 50% Maximum:
In an embodiment of the invention as shown in
X=(−1.11×10−4)+(6.23×10−6)(Ao)−1/3+(−2.27×10−4)(Ma/Mo)2/3; and
Y=(−4.44×10−4)+(1.70×10−5)(Ao)−1/3+(−5.74×10−4)(Ma/Mo)2/3.
The following table lists some exemplary values of Ao (m2), Ma/Mo, and the Full Width at 80% Maximum:
In the following, various embodiments of a lateral mode microphone as shown in
As shown in
Given the same strength/intensity of acoustic pressure, the mutual capacitance can be varied the most (or maximally varied) by an acoustic pressure impacting upon conductor 201 and/or conductor 202 along a certain direction among the above range of impacting directions as shown in
Referring back to
An acoustic pressure can impact, but impact much less than that against functional device 290 as shown in
In exemplary embodiments of the invention, the lateral microphone 200 may be a MEMS (Microelectromechanical System) microphone, AKA chip/silicon microphone. Typically, a pressure-sensitive diaphragm is etched directly into a silicon wafer by MEMS processing techniques, and is usually accompanied with integrated preamplifier. For a digital MEMS microphone, it may include built in analog-to-digital converter (ADC) circuits on the same CMOS chip making the chip a digital microphone and so more readily integrated with digital products.
In an embodiment as shown in
In functional device 290 as shown in
As shown in
Referring to
As described in U.S. application Ser. No. 15/393,831, the movable working membrane 202 may have a shape of square. As shown in
In some embodiments as shown in
Air flow working restrictors can help solve the leakage problem associated with microphone design. In conventional parallel plate design as shown in
In order to prevent this large leakage, a structure is designed and shown in
In the following, a preferred embodiment of the invention will be analyzed using some theories and modeling. However, it should be understood that the present invention is not limited or bound by any particular theory and modeling.
On reference membrane 202r as shown in
In the embodiment such as that shown in
In the foregoing specification, embodiments of the present invention have been described with reference to numerous specific details that may vary from implementation to implementation. The specification and drawings are, accordingly, to be regarded in an illustrative rather than a restrictive sense. The sole and exclusive indicator of the scope of the invention, and what is intended by the applicant to be the scope of the invention, is the literal and equivalent scope of the set of claims that issue from this application, in the specific form in which such claims issue, including any subsequent correction.
This application is a Continuation-in-Part of U.S. non-provisional application Ser. No. 15/623,339 filed on Jun. 14, 2017, which is a Continuation-in-Part of U.S. non-provisional application Ser. No. 15/393,831 filed on Dec. 29, 2016 and patented as U.S. Pat. No. 10,171,917 on Jan. 1, 2019, the contents of which two prior applications are incorporated herein by reference in its entirety.
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Entry |
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Ganji et al., “Design and fabrication of a new MEMS capacitive microphone using a perforated aluminum diaphragm”, Jan. 15, 2009, Sensors and Actuators A: Physical, vol. 149, Issue 1, pp. 29-37. |
Ganji et al., “Design and fabrication of a new MEMS capacitive microphone using a perforated aluminum diaphragm”, Jan. 15, 2009, Sensors and Actuators A: Physical, vol. 149, Issue 1, pp. 29-37 (Year: 2009). |
Number | Date | Country | |
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20190174234 A1 | Jun 2019 | US |
Number | Date | Country | |
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Parent | 15623339 | Jun 2017 | US |
Child | 16270574 | US | |
Parent | 15393831 | Dec 2016 | US |
Child | 15623339 | US |