Patent Application
20230054431
The invention relates to a sound detection device.
It is known to an array of sound detectors to increase the directivity of sound detection (as used herein “sound” includes ultrasound). In a phased array the signals from an array of sound detectors with relative time or phase delays that make the signals at the sound detectors coherent for sound from a selected direction. In a phased array the relative time or phase delays are selected according to the angle between the plane of the surface in which the sound detectors are located and the plane of a free space wave front of the sound from the selected direction, that is, of a wave that is not bound to the surface. The possibility of such a wave direction dependent selection of relative time or phase delays increases the sensitivity to sound from the selected direction relative to the sensitivity to sound from the other directions. The use of a plurality of sound detectors also improves the signal to noise ratio. The size of this improvement depends on the number of array elements. For sound from the selected direction, the signal to noise ratio of the sum will be higher than that of the signal from individual detectors.
However, phased arrays are neither intended nor suitable for increasing the signal to noise ratio of omnidirectional sound reception. Although a phased array obtain improved signal to noise ratios for reception signals in specific directions, the signal to noise ratio of an omnidirectional sum of such reception signals over all directions is not necessarily increased.
An ultrasonic flow meter is disclosed in an article by Kunath et al, titled “Ultrasonic flow meter with piezoelectric transducer arrays integrated in the walls of a fiber-reinforced composite duct”, published in 2013 IEEE sensors pages 1-4, EPO ref XP032308628. Kunath et al. make use of the difference between the propagation speeds of acoustic plane waves that travel with a component of their propagation direction along and opposite to the fluid flow respectively. Plane waves are used that travel between opposite walls of the duct at an oblique angle to the walls. Kunath et al. note that reproducible excitation of plate waves in the sound receiving duct wall is only possible if the sound waves are plane waves and the oblique angle between the duct wall does not change over the length of the excitation zone (i.e. when curved wave fronts are avoided).
In order to ensure plane waves, Kunath et al. uses arrays of transducers on the opposite walls of the duct each as a phased array to excite and receive selected plane waves through the duct at the oblique an angle to the walls. The phase delays used in the phased arrays compensate for delays according to the angle between the walls of the duct and the plane wave propagation direction in the duct. The fluid flow velocity can be determined from the difference between upstream and downstream propagation delay of the plane waves between the arrays.
US2005074317 discloses a linear microphone array that provides frequency independent directivity. Microphones for the highest frequencies at one end of the array and microphones for the lowest frequencies at the other end.
EP2988527 discloses use of three orthogonal linear microphone arrays to detect the location of sound sources.
WO2016073936 discloses an array of ultrasonic transducers for use as a phased array. A chip package with ultrasound waveguides between the transducers and acoustic ports.
JPH1048039 discloses an ultrasonic wave receiver with a plurality of sensors on an optical waveguiding channel. Light is transmitted along the channel. The sensors create variation of the refractive index of the channel when they receive an ultrasonic wave. Light received from the channel is used to detect the effect of ultrasound
Among others, it is an object to provide for a sound detection device wherein an array of sound detectors is used to improve the signal to noise ratio without creating a strongly direction dependent sensitivity.
A sound detection device is provided, the sound detection device comprising
a substrate;
an array of sound detectors in or on a surface of the substrate;
a processing circuit coupled to the sound detectors, the processing circuit being configured to sum signals from the sound detectors with relative time delays or phase shifts that compensate for propagation delay of sound along the array in a sound propagation mode that is bound to said surface. Thus, the size of the delays or phase shifts are defined according to the propagation speed of the sound propagation mode that arises in the detection device. Herein the detection device is configured to detect sound in a sound propagation mode that is bound to the surface of the substrate on or in which the sound detectors are located. A sum of the signals from the sound detectors is formed with relative delays or phase shifts selected to compensate for the delay due propagation of the bound mode along the array, rather than according to a direction of incoming sound in free space.
A sound propagation mode that is bound to said surface can be a propagation mode of an acoustic waveguide, wherein the surface forms one of the walls of the waveguide, or a wave propagation mode of an acoustic boundary wave. The waveguide may be a waveguide a waveguide that contains a space for fluid outside the substrate or a waveguide that contains the substrate (herein referred to as bulk propagation mode of the substrate). A boundary wave (also referred to as surface wave) is a wave that depends on the surface of the substrate in order to propagate, substantially without being affected by the thickness of the substrate or space for fluid in the direction perpendicular to that surface.
Preferably, the device contains one or more structures that define an acoustic waveguide that contains a space for fluid outside the substrate for the bound sound propagation mode. This improves the signal to noise ratio by concentrating the sound and reducing sound leakage.
In an embodiment the waveguide comprises a wall that faces the surface of the substrate, with a space in between for sound propagation. An opening at the start of the acoustic waveguide between the substrate and the wall is used to enable excitation of sound in the acoustic waveguide by incoming external sound. Such a wall also prevents external sound from reaching the sound detectors in the acoustic waveguide directly.
A plurality of arrays may be provided along the acoustic waveguide, on different sides of the space between the wall and the substrate, and a sum of signals from all these detectors may be formed, with relative delays or phase shifts to compensate for the delay due propagation through the acoustic waveguide. This increases the signal to noise ratio.
In an embodiment wherein the propagation mode that is bound to said surface is a bulk propagation mode of the substrate or a surface propagation mode of the substrate, the sound detection device comprises an acoustic impedance matching layer on a part of substrate, ahead of array of sound detectors as seen along the direction of propagation of the sound propagation mode, configured to increase sound energy transfer into the sound propagation mode or surface propagation mode of the substrate from sound in a surrounding of the substrate. Thus more sound energy will be transferred than in the absence of the acoustic impedance matching layer on the part of substrate ahead of array of sound detectors. This improves the signal to noise ratio obtained when delays or phase shifts that compensate for propagation delay of sound along the array in the bulk propagation mode or surface propagation mode of the substrate are used.
These and other objects and advantageous aspects will become apparent from a description of exemplary embodiments with reference to the following figures.
Substrate 10 and wall 14 form walls of an acoustic waveguide which provides for propagation of such an excited wave that enters the waveguide from outside the waveguide. A propagation mode of such an acoustic waveguide, wherein the surface of substrate 10 forms a wall of the waveguide, forms sound propagation mode that is bound to the surface of the substrate by the waveguide. In an embodiment, this acoustic waveguide may have further walls (not shown) extending between substrate 10 and wall 14, perpendicularly to substrate 10 and wall 14, at different positions along the direction perpendicular to the x and z direction (which will be referred to as the y-direction. But on or both of such further walls may be left out.
As shown, sound detectors 12 are located at successively increasing distances from opening 16. Sound detectors 12 may be located at successive positions along a straight line along the direction of the z-axis. But other arrangements with increasing distance to opening 16 may be used. A single one dimensional array may suffice. In an embodiment, a plurality of linear arrays may be present in parallel on or in substrate 10 at different positions along the y-direction. Preferably, sound detectors 12 are equidistantly spaced in the array, but this is not necessary. Although substrate 10 and wall 14 are show to have right angles at opening 16, it should be realized that other configurations may be used, such as an opening that flares out obliquely from the part of substrate 10 and/or wall 14 at the distances at which sound detectors 12 are located. This may be used to increase the captured sound energy.
In operation the sound detection device is embedded in a medium, such as water or another liquid, or a solid and exposed to incoming sound from outside sound detection device with a propagation direction that at least has a component in the z-direction. An incoming sound signal at opening 16 will excite a propagating signal that propagates as a guided by the acoustic waveguide formed by the surface of substrate 10 and wall 14.
Sound detectors 12 sense an effect of pressure variations due to the propagating signal as it travels through the acoustic waveguide formed between the surfaces of substrate 10 and wall 14. For example, if the incoming signal is a pulse signal, the propagating signal is a pulse signal that travels through the waveguide. Different sound detectors 12 sense the pressure variations with different propagation delay (or phase) corresponding to the different positions of sound detectors 12 along the direction of propagation and the velocity of the excited signal in the acoustic waveguide.
In its simplest form, when a single frequency or narrow frequency band signal is used, or the velocity is independent of frequency and the noise spectrum is frequency independent, processing circuit 20 may be configured to form a sum s(t−dt(i), i) of signals s(t,i) where “i” indexes the different sound detectors and t represents time, from sound detectors 12 with different relative delays dt(i) or phase shifts selected to compensate for the differences between the propagation delays to sound detectors 12. The forming may be implemented by first applying selected delays to the signals from the individual sound detectors and then summing the delayed signals. Alternatively the forming may be done in the Fourier transform domain, by applying phase factors followed by summing. In other embodiments forming the sum may comprise after applying some delays and partial summing followed by applying delays to sums of groups of signals.
The delays or phase shifts may be determined based on a known propagation speed “c” of the excited wave in the waveguide and the distances z(i) of the different sound detectors 12 from opening 16, for example by using time delays dt(i) relative to the last sound detector in the array (i=n) according to dt(i)=(z(i)−z(n))/c. In an embodiment, the delay may be determined by means of calibration for example by measuring delays with which a reference pulse is received at different sound detectors, or by determining dt(i) values that result in the highest correlation between signals from the different sound detectors 12. This can improve the signal to nose ratio when the propagation speed varies with distance, e.g. due to the presence of the detectors.
The illustrated embodiment differs from a phased array by the presence of a wall 14 broadside from substrate 10 that blocks sound arriving in a straight line from a target. But it may be noted that even apart from this, the use of relative delays or phase shifts differs from the use of relative delays or phase shifts as used in a phased array. In a phased array, relative delays or phase shifts are used to compensate for direct different travel times from a target to the different array elements, whereas in the present device relative delays or phase shifts are used to compensate for different travel times along the surface of substrate 10, from one sound detector 12 to another, no matter where the target is located.
Due to waveguide effects of the waveguide formed between substrate 10 and wall 14, the relevant signal velocity may be different for different frequency components of the signal. When the velocity is frequency dependent and the signal contains frequency components at more than a single frequency, compensations may be applied using frequency dependent phase factors or delays for the different frequency components. If the incoming signal is a pulse that contains a range of frequency components, using frequency dependent phase factors or delays reduces the effect of dispersion on the pulses detected by the different sound detectors.
The sum may be a weighted sum wherein different frequency components are weighted differently. For example, if the noise is frequency dependent, the different frequency components of the signal may be given different weight in the sum, to increase the signal to noise ratio (as is known per se for a commonly used noise model a weight factor (S(f)/(S(f)+N(f)) can be used to optimize the signal to noise ratio, where S(f) is the spectral density of the signal at frequency f and N(f) is the spectral density of the noise).
The distance between substrate 10 and wall 14 and hence the size of opening 16 is preferably less than a wavelength of the incoming sound, e.g. less than half that wavelength or between a quarter and three quarters of the shortest acoustic wavelength in the range of acoustic wavelengths for which the measurements are performed. Because the distance at opening 16 is so small the sensitivity of excitation of the wave between substrate 10 and wall 14 to the propagation direction of the incoming wave is small.
When a larger distance is used between substrate 10 and wall 14, i.e. a larger opening 16, this causes the direction sensitivity to increase with increasing distance between substrate 10 and wall 14. But the direction sensitivity is not or hardly dependent on the size of the detector array, in contrast with phased arrays, where the direction sensitivity would increase with increasing array size. The direction sensitivity due to use of distance larger than a wavelength or half a wavelength between substrate 10 and wall 14, may or may not be acceptable, dependent on the type and location of a target that must be detected.
Processing circuit 20 may be configured to sample the signals from sound detectors 12 at a predetermined sample rate, e.g. 1 MHz. Processing circuit 20 may be configured to apply frequency passband filtering to the sum and/or the signals from individual sound detectors. The band filtering may be used to select a range of acoustic wavelengths for which the measurements are performed.
The use of the sum has the effect that the signal to noise ratio due to noise from sound detectors 12 is increased compared to the signal to noise ratio of the signal from an individual sound detector 12. The signals add up coherently, but the noise only adds up incoherently. The use of sound detectors 12 that are exposed to the excited wave in the acoustic waveguide, rather than directly to the incoming sound from outside the device, ensures that any number of sound detector 12 can be used to increase the signal to noise ratio without increasing the direction sensitivity of the sound detection.
In the sum equal weight may be given to the signals from all sound detectors 12. Alternatively, the signals from different sound detectors 12 may be given different weight. For example, if the signal strength of the excited wave decreases with distance from opening 16, signals from different sound detectors 12 may be given less weight with increasing distance from opening 16. This can be used to improve the signal to noise ratio. When the noise at all sound detectors is equal and the relative signal amplitudes at different sound detectors 12 labeled “i” are A(i), an optimal estimate of the incoming signal may be obtained when the weights w(i) given to the signals from different sound detectors 12 “i” differ in proportional to the A(i) of these sound detectors 12.
In terms of narrow frequency band signals, or individual frequency components, the reflection cause a standing wave pattern. To optimize the impact of standing wave effects on the resulting signal due to the reflection in the case where a narrow frequency band signal of predetermined frequency is used, sound detectors 12 may be located at positions where the detected amplitudes are maximally increased by the standing wave effect, or at least not diminished.
In other embodiments only struts are used to keep substrate 10 and wall 14 spaced, where the struts do not close off the acoustic waveguide along the full length of the array. This reduces the decrease in acoustic signal strength along the array, and hence improves the signal to noise ratio. In another embodiment the space between the surface of substrate 10 and wall 14 is divided into a plurality of separate partitions, with at least one array of sound detectors 12 in each partition. Processing circuit 20 may be configured to form a sum of signals from sound detectors 12 in the arrays of all partitions.
In another example the solid material of substrate 10 has an outer shape that defines a waveguide for acoustic waves in the solid material, wherein the surface of substrate 10 forms a wall of the waveguide. A propagation mode of such an acoustic waveguide wherein sound propagates in parallel with the surface of substrate 10 may be used as the sound propagation mode that is bound to the surface of the substrate by the waveguide.
The acoustic impedance matching layer has the effect that direction sensitivity due to distributed direct reception of the external sound (as in a phased array), is reduced. Optimally, the acoustic impedance of acoustic impedance matching layer 80 is the geometric average of the acoustic impedances of substrate 10 and its surrounding (i.e. the square root of their product). A similar layer ahead of sound detectors 12 may be used in the embodiment of
Any type of sound detector 12 may be used. In a preferred embodiment detectors are used that use the sound to modulate properties of light, by means of a membrane on which a waveguide for the light is present.
When such a detector is used, the embedding medium is preferably a fluid such as water or air, to allow for movement of the membrane.
The intensity of light transmitted from second optical waveguides 96 to third optical waveguides via the ring resonators as a function of the wavelength of the transmitted light shows a peak at a resonance wavelength of the ring resonator to which the second and third optical waveguide 96, 97 are coupled. The processing circuit (not shown) may be configured to supply light to second optical waveguides 96 at an optical wavelength or wavelengths on the flanks of such peaks and to detect the intensities of the light transmitted from second optical waveguides 96 to third optical waveguides 97 via the ring resonators. Alternatively, other techniques for measuring resonance peak shifts may be used.
In operation, sound propagating in the negative z-direction causes membranes 92 in the column of membranes 92 to vibrate. In turn, the vibrations cause a vibrating shift of the resonance dips of the ring resonators. The shift results in variation of the intensity that is detected by the processing circuit.
As shown, a plurality of second and third optical waveguides 96, 97 may be provided, each coupled through a ring resonator of a respective one of membranes 92. Alternatively, an ongoing second optical waveguide may be used coupled to the same ring resonator on a membrane. In this case, transmission dips occur at the output of the ongoing second optical waveguide as a function of optical wavelength, and shifts of these dips caused by the sound can be measured in a similar way as with peaks. In an embodiment the ring resonators may be resonant at different wavelengths and the processing circuit may use optical wavelength multiplexing to measure vibration of different membranes simultaneously using the same ongoing second optical fiber optical fibers coupled through the ring resonators.
Instead of ring resonators, interferometers may be used to detect vibrations of membranes 92. A first optical waveguide that runs over a membrane may be used as a first arm of such an interferometer and a second optical waveguide that does not run over a membrane may be used as a second arm. In this embodiment the processing circuit may be configured to measure the sound from changes in the interference intensity of as sum of light from both arms. Instead of a second optical waveguide that does not run over the membrane a second optical waveguide may be used that runs over a part of a membrane that is known to vibrate in counter phase with the part of the membrane on which the first arm is located.
The advantage of using such optical detection techniques compared to use of piezo-electric detectors is that more optical detectors can be realized on the same area, which provides for a larger signal to noise ratio improvement.
| Number | Date | Country | Kind |
|---|---|---|---|
| 20152261.2 | Jan 2020 | EP | regional |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/NL2021/050026 | 1/18/2021 | WO |
