JP6274497B2 - Parametric speaker - Google Patents

Description

  The present invention relates to a parametric speaker, and more particularly to a parametric speaker that can reduce distortion components and obtain high-quality reproduced sound.

A parametric speaker is known as a speaker that can generate a sound field with a much narrower directivity than a normal speaker. In recent years, this parametric speaker has been researched and developed so that it can be applied to individual guidance for each booth of exhibits, traffic alert-free alerting and guidance, etc.
The feature of the parametric speaker is that directivity is very sharp and only a person in a specific space can hear the sound limitedly. Because of this feature, it is possible to achieve individual guidance and quieter surroundings. Therefore, guidance in public facilities such as stadiums, theaters, schools, and amusement facilities, and introduction to railways and transportation facilities are expected. For example, it is actually introduced at tourist attractions, etc., and announcements can be given only to people at specific platforms in the station, or escalators can be alerted only to those who get on and off. It is also expected to be used for evacuation guidance at the time of disaster in tunnels where sound reverberation and reverberation are intense. Furthermore, applied research on noise reduction of high-volume game consoles at amusement facilities, and installed in acoustic traffic lights for visually impaired people at pedestrian crossings, to make announcements to visually impaired people, and at the same time realize quietness of the surrounding environment Applied research is also being conducted.
As described above, the parametric loudspeaker that has very directivity and can realize the quietness of surroundings is a technology that is expected to be applied in various fields in a modern society where noise is a social problem.

Here, the reproduction principle of the parametric speaker is that a strong ultrasonic wave is emitted and an audible sound is obtained by utilizing the nonlinearity of air in the propagation process. As shown in FIG. 1, the basic configuration of this parametric speaker includes an external sound source 5, a carrier signal source 6, a modulation means 2, an amplification means 3, and an ultrasonic radiation means 4, and such a basic configuration. , The input audible signal is subjected to transmission processing and radiated from the ultrasonic radiation means 4 to obtain a reproduced sound of the sound source.
The modulation unit 2 is a unit that performs modulation processing of an ultrasonic band carrier signal using an audible signal, and is realized by, for example, a modulator. The amplifying unit 3 is a unit that amplifies the obtained modulation signal and supplies it to the ultrasonic radiation unit 4 and is realized by, for example, an amplifier. The ultrasonic radiation means 4 is generally composed of one or a plurality of ultrasonic emitters. The demodulation process for obtaining an audible signal from the modulated ultrasonic wave radiated from the ultrasonic radiation means 4 utilizes the self-demodulation phenomenon of the ultrasonic wave propagating in the air.

ここで、ω_cはキャリア信号の角周波数、e (t )は包絡線関数を示す。
例えば、振幅変調（ＡＭ）の場合には、mを変調度として、

と表される。また、位相変調（Phase Modulation, PM）であれば、mを変調指数として、

で表される。
また、増幅手段で増幅された信号v (t )は、時間領域では変調信号f(t )をK' 倍したものとして、v (t ) = K' f (t )と表され、周波数領域ではV(ω) = K' F (ω)と表される。
さらに、超音波放射手段から放射される音源音圧をp(t )と表わし、パラメトリック差音の音圧をp_S(t )と表わす。 Note that an example of the flow of modulating the audible signal and radiating the reproduced sound will be described based on the schematic configuration (FIG. 2) of the parametric speaker described above.
When an audible signal from an external sound source is expressed by s (t) and the signal is handled in the time domain (t) and the angular frequency domain (ω), the modulation signal f (t) generated by the modulation means is expressed by the following equation: It is represented by (1).

Here, ω _c represents the angular frequency of the carrier signal, and e (t) represents the envelope function.
For example, in the case of amplitude modulation (AM), m is a modulation degree,

It is expressed. For phase modulation (PM), m is the modulation index,

It is represented by
The signal v (t) amplified by the amplifying means is expressed as v (t) = K ′ f (t) in the time domain, with the modulated signal f (t) multiplied by K ′, and in the frequency domain V (ω) = K ′ F (ω).
Further, the sound source sound pressure radiated from the ultrasonic radiation means is represented as p (t), and the sound pressure of the parametric difference sound is represented as p _S (t).

ここで、K＝K’K”と置き、また、LCR直列回路のアドミッタンスに相当する次のH（ω）を導入する。

これらから、初期音圧P（ω）は、次の式で表わされる。

これから、超音波放射手段の出力P(ω)は、変調手段の出力信号F(ω)に超音波放射手段の伝送特性（伝達関数）H(ω)が掛けられて決定されることが分かる。 The ultrasonic radiation means 4 often uses an ultrasonic element such as a piezoelectric ceramic using a mechanical resonance phenomenon as a drive source in order to generate high sound pressure ultrasonic waves. An equivalent circuit (LCR circuit) near the mechanical resonance of the ultrasonic emitter in that case can be shown in FIG. In addition, the electroacoustic characteristic reflects a resonance phenomenon and exhibits a peak-like single peak characteristic as shown in FIG. Here, C _d is the capacitance of the piezoelectric ceramic, and L, C, and R are an equivalent inductance (coil), an equivalent capacitance (capacitor), and an equivalent resistance that determine the resonance of the piezoelectric mechanical vibration, respectively. In FIG. 2, when it is assumed that the frequency characteristic and phase characteristic of the sound source sound pressure P (ω) radiated from the ultrasonic radiation means are proportional to the current I (ω) flowing through the equivalent resistance of the ultrasonic radiation means, the proportionality is obtained. When the constant is K ″, the current I (ω) is determined by the ratio of the applied voltage V (= K′F) of the ultrasonic radiation means and the impedance of the LCR series circuit from FIG. It is represented by

Here, K = K′K ″ is set, and the next H (ω) corresponding to the admittance of the LCR series circuit is introduced.

From these, the initial sound pressure P (ω) is expressed by the following equation.

From this, it can be seen that the output P (ω) of the ultrasonic radiation means is determined by multiplying the output signal F (ω) of the modulation means by the transmission characteristic (transfer function) H (ω) of the ultrasonic radiation means.

  Although it is a parametric speaker as mentioned above, in order to expand an application range in the future, the further performance improvement of a parametric speaker is desired. In particular, it is important to further reduce the distortion component in the reproduced sound wave of the parametric speaker in order to obtain a voice / musical sound with high intelligibility and a high-quality reproduced sound that is easy to hear and has no sense of incongruity. The distortion component is caused by a nonlinear demodulation process such as a nonlinear characteristic of the ultrasonic transducer constituting the ultrasonic wave radiating means 4 or a non-linear demodulation process in which a sound wave waveform is distorted due to air nonlinearity and a harmonic component is generated. These are components of various distortions that occur. Since the sound propagation process shown in FIG. 2 is a nonlinear propagation process, it is considered that the reproduced sound of the parametric speaker includes various distortion components. On the other hand, it can be said that the conventional electrodynamic speaker has a low sound signal level of the sound source and the sound propagation process is linear propagation.

Therefore, various techniques have been developed for the purpose of reducing distortion components in parametric speaker signal transmission or sound reproduction.
For example, in Patent Document 1, an audio signal that is an audible sound and a carrier signal that is a carrier wave in an ultrasonic band generated by a carrier wave generation unit are input, the carrier signal is amplitude-modulated with the audio signal, and ultrasonic radiation is performed. In a modulator that generates a signal indicating an ultrasonic wave that self-demodulates to an audible sound in the air when radiated from the means 4, a gain adjusting means for adjusting the level of the audio signal, and an amplitude of an output from the gain adjusting means are compression adjusted. Amplitude compression means, envelope information generation means for generating envelope information output from the amplitude compression means, a carrier signal that becomes a carrier wave in the ultrasonic band, and an operation using envelope information from the envelope generation means And an envelope carrier wave signal generating means for generating an envelope carrier wave signal that becomes a carrier wave including envelope information, and an audio signal A modulator, characterized in that it comprises, a SSB modulation means for SSB modulation is disclosed.
According to this modulator, an audible sound with suppressed distortion can be obtained by a parametric speaker. When the audio signal is equal to silence, generation of a carrier wave can be suppressed to save power.

Further, Patent Document 2 outputs a speaker unit that generates a secondary sound wave that is an audible sound by a non-linear parametric action of a primary sound wave output by an ultrasonic vibrator, and a drive signal that drives the ultrasonic vibrator. A drive signal generation unit, and the drive signal generation unit outputs a modulated signal having a frequency half that of the secondary sound wave generated by the speaker unit and a carrier wave oscillation circuit that outputs a carrier wave signal having an ultrasonic frequency. An electroacoustic conversion comprising: a modulated signal generating circuit; and a modulation circuit that receives a carrier wave and the modulated signal and outputs a drive signal modulated by a carrier-suppressed double-band modulated method to a speaker unit An apparatus is disclosed.
According to this technique, the directivity is sharp while being relatively small, and the amount of accumulated primary sound waves can be reduced, and the generated secondary sound is less distorted and can be formed at a relatively low cost. An acoustic conversion device can be realized.

Japanese Patent No. 4799303 JP-A-4-123699

  However, neither of the techniques disclosed in Patent Documents 1 and 2 is sufficient to suppress the above-described distortion component, and in order to realize a high-intelligibility parametric speaker, technical development for further distortion suppression is desired. It was.

  For example, the technique of Patent Document 1 employs SSB modulation for a carrier signal and a sideband signal, thereby reducing the generation of second-order harmonics due to nonlinear interaction between sidebands, compared to DSB modulation. Although the generation of distortion can be suppressed, the generation of distortion due to nonlinear interaction still remains in the frequency component in the sideband, and it has been desired to reduce the distortion component in the demodulation process of sound propagation in the air. Here, the distortion component in the demodulation process of sound propagation in the air is mainly a distortion component generated when the sound wave waveform is distorted and many harmonic components are generated in the propagation process of the sound wave radiated from the parametric speaker. It is.

  In addition, the technique of Patent Document 2 employs modulation using a carrier-suppressed double-sideband modulated system, so that a filter for removing one sideband is not required and the cost is low, but compared to SSB modulation. Since there is no carrier wave, the reduction of the second harmonic becomes insufficient, and the generation of distortion cannot be controlled sufficiently. Further, since distortion in the demodulation process of sound propagation in the air cannot be reduced, there is a problem that it is difficult to obtain high-quality reproduced sound that is easy to hear and has no sense of incongruity.

  In view of the above problems, an object of the present invention is to provide a parametric speaker that can further reduce distortion components in the demodulation process of sound propagation in the air and can obtain a high-quality reproduced sound.

  The present inventors have repeatedly studied to solve the above problems. As a result, the sound wave reproduced by the parametric loudspeaker is caused by the finite amplitude sound wave phenomenon that the medium air has non-linearity and high sound pressure ultrasonic waves propagate due to the distortion component included in the sound wave reproduced from the parametric speaker. In the propagation process, many distortions and high-frequency components occur, and due to the principle of demodulating the parametric speaker, in addition to the reproduced sound components, from the mutual interference propagation state of two or more sound waves, harmonic components and difference / chords We focused on the fact that many coupled sounds that generate other intermodulation distortion are generated, and further, distortion components are generated from the ultrasonic emitter or ultrasonic element that is the sound generator.

  As a result of further earnest research, the inventors have developed a means for correcting the audible signal in consideration of the influence of the nonlinear propagation process of the ultrasonic wave in the speaker driving means, which is generated by the nonlinear demodulation process. It has been found that various distortion components can be reduced by feedback processing or feedforward processing, and that high-quality reproduced sound can be realized, and the present invention has been completed.

The present invention is based on such knowledge, and the gist thereof is as follows.
(1) Modulation means for modulating a carrier signal in an ultrasonic band with an audible signal from an external sound source to generate a modulation signal, amplification means for amplifying the generated modulation signal, and the amplified modulation signal An ultrasonic radiation means for radiating an ultrasonic wave based on the parametric speaker, wherein the parametric speaker detects a sound pressure of the ultrasonic wave output from the ultrasonic radiation means, and a signal of the detected output sound pressure Based on the above, the waveform of the demodulated audible signal when affected by the nonlinear propagation process is predicted and generated by a nonlinear propagation model, and the generated waveform is compared with the waveform of the input audible signal, corrects the audio signal, an audible signal correction means for sending and the corrected audio signal to the modulating means, a parametric loudspeaker, characterized in that it further comprises.

ここで、ｔは時間（秒）、e(t)は包絡線関数を示す。 ( 2 ) The parametric speaker according to ( 1 ) above, wherein a waveform model when the audible signal is affected by a nonlinear propagation process is derived by the following equation.

Here, t represents time (seconds), and e (t) represents an envelope function.

( 3 ) The parametric speaker according to (1) or (2) , wherein the modulation signal includes the carrier signal and a sideband signal obtained by modulating the carrier signal.

(4) the ultrasound emitting means comprises a ultrasonic wave based on the carrier signal, and an ultrasonic based on the sideband signal, in the above (3), characterized in that the radiation by a separate ultrasonic emitter Parametric speaker described.

( 5 ) In the ultrasonic emitter, the ultrasonic wave based on the emitted carrier signal and the ultrasonic wave based on the emitted sideband signal are arranged so as to intersect at an angle of 10 ° or less. The parametric speaker according to ( 4 ) above, characterized in that.

( 6 ) The ultrasonic emitter is configured by a plurality of blocks including a plurality of ultrasonic elements, and radiates an ultrasonic wave based on the carrier signal and an ultrasonic wave based on the sideband signal by separate blocks. The parametric speaker according to (4) above, characterized in that:

( 7 ) The parametric speaker according to ( 6 ), wherein the block including the ultrasonic element has a rectangular shape, a checkered pattern, a concentric circle, or a radiation shape.

( 8 ) The attenuation band of the frequency characteristic in the ultrasonic radiation means is a characteristic that is proportional to the square of the frequency as the frequency increases in the lower band and inversely proportional to the square of the frequency in the upper band. The parametric speaker according to any one of (1) to ( 7 ), wherein the parametric speaker is controlled and a carrier signal and a sideband signal exist in the lower band or the upper band.

( 9 ) The frequency characteristics of the ultrasonic waves reproduced by the ultrasonic radiation means are the attenuation frequency band of the ultrasonic radiation means, and if the lower frequency band of the ultrasonic radiation means, the frequency characteristics are increased. Frequency characteristic correction means for controlling the frequency band to be proportional to the square of the frequency and inversely proportional to the square of the frequency in the upper band, and carrier and sideband components in the lower band or the upper band. The parametric speaker according to any one of (1) to ( 7 ) above, wherein

( 10 ) The parametric speaker software according to any one of (1) to (9 ) above , wherein the ultrasonic wave output from the ultrasonic radiation means in the parametric speaker is incorporated into the parametric speaker. And a waveform of a demodulated audible signal at the time of being influenced by the nonlinear propagation process based on the detected output sound pressure signal is predicted by a nonlinear propagation model, and the generated waveform and Software for functioning to correct the audible signal by comparing the waveform of the input audible signal.

  ADVANTAGE OF THE INVENTION According to this invention, it becomes possible to provide the parametric speaker which can obtain the reproduction sound of high sound quality by reducing the distortion in the process of modulation and demodulation of sound propagation in the air.

It is the figure typically shown about one Embodiment of the conventional parametric speaker. It is the figure which showed schematic structure of the conventional parametric speaker. The sound pressure frequency characteristic of the ultrasonic emitter is shown, (a) is an equivalent circuit near the resonance of the ultrasonic element, and (b) is a diagram showing the current frequency characteristic of the LCR series circuit. It is the figure typically shown about one Embodiment of the parametric speaker according to this invention. It is the figure which showed an example of the frequency characteristic of the input audio signal and the output sound pressure from the external sound source of the conventional parametric speaker. In the parametric speaker according to the present invention, (a) shows an example of the frequency characteristic of the audible signal and the audible signal corrected by the audible signal correcting means, and (b) shows an example of the frequency characteristic of the output sound pressure of the parametric speaker. FIG. It is the flowchart which showed an example of the flow of correction | amendment by the audible signal correction | amendment means according to this invention. It is the figure which showed one Embodiment of the parametric according to this invention using the audible signal correction | amendment means. It is the figure which showed one Embodiment of the nonlinear propagation model production | generation means according to this invention. It is the figure typically shown about other embodiment of the parametric speaker according to this invention. It is the figure typically shown about other embodiment of the parametric speaker according to this invention. It is the figure typically shown about one Embodiment of the ultrasonic radiation means according to this invention. It is the figure typically shown about other embodiment of the ultrasonic radiation means according to this invention. It is the figure typically shown about other embodiment of the ultrasonic radiation means according to this invention. It is the figure typically shown about other embodiment of the ultrasonic radiation means according to this invention. It is a figure for demonstrating the crossing angle of the ultrasonic wave based on a carrier signal, and the ultrasonic wave based on a sideband signal about an ultrasonic emitter. It is a figure showing the sound pressure frequency characteristic of an ultrasonic emitter, and shows the case where a sideband signal exists in the zone | band above a resonance peak. It is the figure which showed the frequency characteristic based on the demodulation conversion principle of a parametric speaker. FIG. 6 is a diagram showing demodulation difference sound characteristics and ultrasonic frequency characteristics of a USB-type SSB-modulated ultrasonic emitter. It is the figure which showed schematic structure of the parametric speaker according to this invention.

<Parametric speaker>
A parametric speaker according to the present invention will be described with reference to the drawings as necessary.
As shown in FIG. 4, a parametric speaker 100 according to the present invention includes a modulation unit 20 that modulates an ultrasonic band carrier signal with an audible signal from an external sound source 50 to generate a modulation signal, and the generated modulation signal. And an ultrasonic radiation means 40 for radiating an ultrasonic wave based on the amplified modulation signal.
The parametric speaker 100 according to the present invention further includes an audible signal correction unit 10 that corrects the audible signal in consideration of the influence of the nonlinear propagation process of the ultrasonic wave, and sends the corrected audible signal to the modulation unit. It is characterized by providing.

  Here, the ultrasonic wave refers to a sound wave exceeding the audible range that cannot be heard by the human ear, for example, a sound wave having a frequency of 16 kilohertz or more. An audible signal from an external sound source is a signal that is a sound source of a parametric speaker, and is a signal in a frequency band that a person can feel as vibration of the eardrum. For example, it refers to signals such as human voices and music, but is not particularly limited. Furthermore, a carrier signal is a signal that is generally a signal having a frequency sufficiently higher than that of an audible signal and that carries information such as an audible signal and is subjected to the modulation.

(Audible signal correction means)
The parametric speaker 100 of the present invention includes an audible signal correcting means 10 as shown in FIG. The audible signal correcting means 10 corrects the audible signal from the external sound source 50 in consideration of the influence of the nonlinear propagation process of the ultrasonic wave, and reduces various distortion components generated by the nonlinear demodulation process and the like. The corrected audible signal is sent to the modulation means 20 described later.
Here, “correction taking into account the effect of the nonlinear propagation process of ultrasound” means that the waveform of the ultrasound is distorted in the nonlinear propagation process of air, a lot of high-frequency components are generated, and the mutual interference propagation state of the sound wave From this, it is a correction that eliminates the influence in consideration of the influence of the generation of a large number of combined sounds that cause intermodulation distortion in addition to the harmonic component and difference / chord.
By providing the audible signal correcting means 10, feedback processing (processing for removing adverse effects due to the actually detected nonlinear propagation process) or feedforward processing for reducing various distortion components generated by the nonlinear propagation process of the parametric speaker 100. (A process for removing the adverse effects caused by the non-linear propagation process predicted in advance) is possible, and it is possible to realize a high-quality reproduced sound that is easy to hear and has no sense of incongruity.

When correction by the audible signal correcting means 10 is not performed, for example, as shown in FIG. 5, the input audible signal s (t) (FIG. 5 (a)) is input, and the fundamental wave component of s (t) is The frequency characteristic is changed, and a sound pressure signal p _s (t) (solid line in FIG. 5B) after a nonlinear propagation process by air is obtained. Here, the broken line in FIG. 5 (b) indicates the distortion of the harmonics and hybrid harmonic waves generated in the process of the transmission system of the parametric speaker. From this, p _s (t) (solid line in FIG. 5 (b)) becomes the input audible signal s (t) (FIG. 5 (a)) due to distortion caused by the nonlinear propagation process (broken line in FIG. 5 (b)). It turns out that it becomes a frequency characteristic different from.
On the other hand, when the correction by the audible signal correcting means 10 is performed, for example, as shown in FIG. 6 (a), the input audible signal s (t) (FIG. 5 (a) solid line) is corrected and corrected audible. The signal s ′ (t) (solid line in FIG. 6 (a)) is sent to the modulation means, and the sound is reproduced by the sound propagation process by air through the amplification means and the ultrasonic radiation means. As a result, the frequency characteristic of the sound pressure p _s ′ (t) obtained is equal to or equal to the input audible signal s (t) (FIG. 5 (a) solid line), as shown by the solid line in FIG. 6 (b). It will be similar. Here, the broken line in FIG. 6B is the frequency characteristic of the distortion, and a marked level reduction can be realized compared with the distortion characteristic of the broken line in FIG. 5B when the correction by the audible signal correcting means 10 is not performed. .

  A modulation means for modulating a carrier signal in the ultrasonic band with an audible signal from an external sound source to generate a modulation signal, an amplification means for amplifying the generated modulation signal, and the amplified modulation signal A circuit composed of ultrasonic radiation means for emitting ultrasonic waves may be referred to as a main circuit below. Also, based on the detection means for detecting the output sound pressure of the ultrasonic radiation means and the detected output sound pressure signal, a prediction signal is generated based on the nonlinear propagation model when affected by the nonlinear propagation process. The circuit having the processed signal and the comparing means for comparing the inputted audible signal may be called a sub-circuit.

Further, as described above, the audible signal correcting means 10 is not particularly limited as long as it takes into account the influence of the non-linear propagation process of ultrasonic waves. For example, as shown in FIG. A waveform model (FIG. 7B) when the audible signal input from the external sound source is affected by the nonlinear propagation process is generated, and the waveform model of the audible signal considering the influence of the nonlinear propagation process (FIG. 7). 7 (b)) and the level-adjusted waveform of the input audible signal (FIG. 7 (c)) to extract a difference, and the extracted difference is used as the input audible signal. By applying, it is possible to correct the audible signal (to obtain a corrected waveform (FIG. 7A)).
In that case, feedback processing of distortion reduction processing such as distortion prediction is performed based on a model simulating the generation of distortion reflecting the characteristics of the nonlinear propagation process, and the audible signal can be corrected, so that nonlinear demodulation in a parametric speaker is possible. It is preferable because various distortion components generated by the process can be more effectively and easily reduced, and high-quality reproduced sound that is easy to hear and has no sense of incongruity can be obtained.

  Further, as shown in FIG. 8, the audible signal correcting unit 10 detects the sound pressure of the ultrasonic wave output from the ultrasonic wave radiating unit 40 by the detecting unit 13, and converts the detected sound pressure signal into a detected output sound pressure signal. Based on this, the waveform of the demodulated audible signal when affected by the nonlinear propagation process is predicted and generated by the nonlinear propagation model means 11, and the generated waveform and the waveform of the inputted audible signal are compared by the comparing means 12. By comparing, the audible signal can be corrected. With such an easy configuration, feedback processing for reducing various distortion components generated by the non-linear propagation process of the parametric speaker 100 (predicted in advance based on the sound pressure of the ultrasonic wave detected by the detecting means 13). To remove the adverse effects caused by the nonlinear propagation process), and it is possible to realize a high-quality reproduced sound that is easy to hear and has no sense of incongruity.

Here, the non-linear propagation model generation means 11 is, for example, a model equation of the non-linear propagation process is simulated by a circuit or the like from the signal of the output signal detected by the detection means 13, and the audible signal is affected by the non-linear propagation process. A waveform model of the desired demodulated audible signal (FIG. 7B) is generated. As a result, the generation of the parametric reproduction sound is simulated, and for example, as shown in FIG. 9, it is constituted by a square means, a detection means, and a differentiation means based on the equation (1). Alternatively, it may be a means of incorporating an input / output relationship obtained from the KZK equation (see Kamakura, “Basics of Nonlinear Acoustics”, Aichi Publishing, 1996).
The squaring means is realized by, for example, a squaring circuit and squares the envelope function, and the detecting means is realized by, for example, a detecting circuit and extracts a low-frequency component from the squared signal. The differentiating means is a circuit that is realized by, for example, a differentiating circuit and differentiates with respect to time.
The detection means 13 is a means for detecting the electroacoustic operation of the ultrasonic radiation means 40. For example, there are a microphone for detecting emitted ultrasonic waves and / or a sensor for detecting vibrations of the ultrasonic emitter element and / or a sensor for detecting current flowing in the ultrasonic emitter element, but there is no particular limitation.
Further, the comparison means 12 is a means for comparing the audible signal taking into account the influence of the nonlinear propagation process and the inputted audible signal and sending the corrected audible signal s ′ (t) to the modulation means 20. . For example, it is performed by an operational amplifier, but is not particularly limited. The audible signal s (t) input from the external sound source is compared with the signal of the nonlinear propagation model generation unit 11 to output an audible signal s ′ (t) and sent to the modulation unit 20. Thus, the comparison means 12 generates a comparison signal between the audible signal s (t) from the external sound source and the signal generated by the non-linear propagation model generation means 11, and as the audible signal s ′ (t), the comparison signal is generated. It is sent to the modulation means 20. Thus, when the corrected audible signal s' (t) is subjected to sound reproduction processing by the nonlinear sound propagation process of the modulating means, the amplifying means, the ultrasonic radiating means and the air, the characteristics equivalent to the audible signal s (t) In addition, an audible sound with reduced distortion can be obtained.

これより、前記可聴信号が非線形伝搬過程の影響を受けた際の波形モデルについては、例えば、前記（５）式によって導出することができる。
前記（１）式を用いて、音源音圧が大きくない条件のもと、非線形音場を数式で扱うことにより歪を予想することができるからである。 The model equation of the nonlinear propagation process is, for example, Berktay's model equation (5) shown below (HOBerktay, Possible exploitation of nonlinear acoustics in underwater transmitting applications, Sound & Vib., 2, pp. 435-461 (1965)) Or, Merklinger's formula (HMMerklinger, Improved efficiency in the parametric transmitting array, J. Acoust. Soc. Am., 58, pp. 784-787 (1975)) or KZK's formula.
Here, t represents time (seconds), and e (t) represents an envelope function.

From this, the waveform model when the audible signal is affected by the nonlinear propagation process can be derived, for example, by the equation (5).
This is because distortion can be predicted by treating the nonlinear sound field with a mathematical expression under the condition that the sound source sound pressure is not large by using the expression (1).

Here, when the sound pressure of the ultrasonic wave is large and has a large amplitude, it is called a finite amplitude ultrasonic wave. A distortion component or the like depending on a finite amplitude sound wave can be formulated by a nonlinear sound field equation originating from a wave equation such as the KZK equation. On the other hand, when the sound source sound pressure is not so high, the parametric difference sound p _s (t) is given by the second-order derivative with respect to the square time of the envelope of the modulated primary wave. From this, the secondary difference sound when the primary initial wave is p (t) = P ₀ e (t) sin [ω _c t + φ (t)] can be given by the above equation (5). Are known. (HOBerktay, Possible exploitation of nonlinear acoustics in underwater transmitting applications, Sound & Vib., 2, pp. 435-461 (1965))

(Modulation means)
The parametric speaker 100 of the present invention includes a modulation means 20 as shown in FIG. The modulation means 20 means means for modulating the carrier signal with an audible signal from the external sound source 50 to generate a modulated signal. Here, for example, the modulation signal modulates an ultrasonic carrier signal (frequency f _C ) with an audible sound signal from the external sound source 50, and a carrier signal and a sideband signal (frequency f _C + fs and / or f _C −). fs) is a signal having two types of signal components. As a modulation method for obtaining a modulation signal composed of the carrier signal and the sideband signal, a double side-band (DSB) amplitude having two sideband components in the upper and lower frequency bands of the carrier component after the modulation processing. Modulation method (AM modulation method) and single sideband (Single Side-Band, SSB) amplitude modulation method with one sideband component in the upper or lower frequency band of the carrier component, etc. A single sideband modulation method is more preferable because harmonics are reduced and distortion can be further suppressed. For example, if the upper sideband signal is removed and only the lower sideband sideband signal is used, the sideband signals do not interact with each other, so the distortion component is smaller than the double sideband amplitude modulation method. A reproduced sound close to an audible signal from the external sound source 50 can be obtained.

(Amplification means)
The amplifying means 30 is means for amplifying the modulation signal generated by the modulating means 20. The amplifying means 30 is not particularly limited as long as it can amplify the modulated signal to an output signal with a large energy.

(Ultrasonic radiation means)
The parametric speaker 100 of the present invention includes the ultrasonic radiation means 40 as shown in FIG. The ultrasonic radiation means 40 is a means for emitting an ultrasonic wave based on the modulation signal amplified by the amplification means 30, and is generally composed of one or a plurality of ultrasonic emitters.
The ultrasonic emitter refers to a device that is configured by an ultrasonic element such as an aerial ultrasonic sensor using a piezoelectric ceramic as a vibrator and can generate ultrasonic waves. “Radiation” means that a parametric speaker emits energy in the form of ultrasonic waves.

Here, when the modulation signal includes the carrier signal and a sideband signal obtained by modulating the carrier signal, the ultrasonic wave radiating means, as shown in FIG. And ultrasonic waves based on the sideband signals are preferably emitted by separate ultrasonic emitters 41a and 41b (separated drive system).
By radiating with the separate emitters 41a and 41b, the carrier signal and the sideband signal are not mixed, and the ultrasonic elements constituting each ultrasonic emitter receive only one signal out of the carrier signal and the sideband signal. Therefore, it is possible to suppress the occurrence of intermodulation distortion between the carrier signal and the sideband signal, which occurs when a common ultrasonic emitter is used for the processing of the carrier signal and the sideband signal. In addition, each emitter only needs to handle either the carrier signal or the sideband signal, so that the burden on each ultrasonic emitter (element constituting the ultrasonic emitter) is reduced, and the input resistance of the ultrasonic element is reduced. In addition, there is an effect that the durability can be improved and an effect that the power consumption can be reduced because the ultrasonic element that handles the carrier signal may have a narrow band.

  Here, as for the ultrasonic emitter in the separated drive system, any ultrasonic emitter based on the carrier signal and ultrasonic wave based on the sideband signal may be emitted by separate ultrasonic emitters 41. There is no particular limitation. For example, as shown in FIG. 10, the carrier signal and the sideband signal are driven by one ultrasonic emitter 41a, 41b. At this time, the waveform of the sideband signal is, for example, an upper sideband (USB) that is obtained by modulating a sine wave sound source signal and exists above the frequency of the carrier signal. In addition, the shape of the ultrasonic emitter 41 may be a circle, an ellipse, a rectangle, a ring, or the like. Furthermore, one signal may be driven by a plurality of ultrasonic emitters.

  Each of the ultrasonic emitters includes a plurality of blocks each including a plurality of ultrasonic elements. The ultrasonic wave based on the carrier signal and the ultrasonic wave based on the sideband signal are separated by separate blocks. Radiation is preferred. This is because it is easy to make the ultrasonic emitter into a desired shape, and a higher-quality reproduced sound can be obtained. When the ultrasonic emitter is constituted by a block composed of a plurality of ultrasonic elements, for example, as shown in FIG. 11, the carrier signal and the sideband signal are individually divided into two ultrasonic emitters 43 and 44 divided into two blocks. It is preferable that the blocks 43a to e and 44a to d of the elements constituting the ultrasonic emitters are configured to correspond to one amplification means 42. Here, one block can be configured to include a block or a plurality of blocks. By making the block with the elements arranged close to each other, the degree of synthesis of the sound waves emitted from each block is improved and the demodulation conversion efficiency is reduced less than when separated and driven by individual emitters. This is because the sound pressure level of the sound can be maintained.

  In addition, as shown in FIGS. 12-15, the block which consists of the said ultrasonic element has a rectangle (FIG. 12, FIG. 13), a checkered pattern (FIG. 14 (a)), a concentric circle (FIG. 14 (b), FIG. It is preferable to have a shape of a)) or radiation (FIG. 15B). This is because a good sound radiation field with little direction dependency can be obtained, and the restrictions during installation can be reduced.

Here, as shown in FIG. 12, the said rectangular block means the shape comprised from a single or several rectangle, for example. The rectangular blocks can be further classified into “single row block division”, “multiple block division” and the like. As shown in FIG. 12 (a), the one-row block division is composed of blocks in which an ultrasonic emitter is alternately input with a small-diameter ultrasonic element one by one and a carrier signal A and a sideband signal B are input. It has been done. Further, as shown in FIG. 12B, the plural block division is constituted by the blocks alternately arranged, for example, three by three.
In the “single row block division” and “multiple block division”, since the ultrasonic elements are arranged in one row direction, the acoustic characteristics of the ultrasonic emitter as a whole are the sound emission characteristics in the vertical and horizontal directions. Different. For this reason, there arises a restriction that it is necessary to install the parametric speaker in consideration of the listening position when the parametric speaker is used. In order to improve this, there is a method in which the arrangement of the ultrasonic elements is arranged with less directivity. As an arrangement with less directivity, as shown in FIG. 13 (a), ultrasonic elements are alternately arranged in a zigzag pattern, or as shown in FIG. 13 (b), ultrasonic elements are arranged obliquely. There is a method of arranging with an angle from the vertical or horizontal direction.
Here, “directionality” refers to the state of the sound radiation pattern, and the radiated sound field of the ultrasonic emitter, which is the synthesis of the sound radiated from the individual ultrasonic elements, is separated from the direction of the sound axis (0 °). The sound level varies depending on the direction. For example, in FIG. 12, the ultrasonic elements for reproducing either the signal A or B are arranged in a vertical row and arranged at intervals from the other, so that the ultrasonic emitter in FIG. 12 is viewed from the front. The sound pressure level changes differently in the horizontal direction moving left and right and the vertical direction moving up and down. In terms of acoustic engineering, such a state is said to have different sound radiation patterns in the horizontal and vertical directions (other arbitrary directions) and have directivity (difference in directivity). On the other hand, in FIG. 13, the “directionality” is an arrangement that is completely eliminated but is eliminated. “Directionality” or “directivity” depends on the arrangement state of the ultrasonic elements or blocks and the outer shape of the ultrasonic emitter (circular, polygonal, etc.). For example, in FIGS. 12 to 15, the concentric ultrasonic emitter shown in FIG. There is a considerable directionality in the element arrangement and shape of the ultrasonic emitters other than those in FIG.

Further, as an array in which directionality is further reduced, there is a checkered pattern, a concentric circle, or a radiation shape. As for the shape of the block made of ultrasonic elements, the checkered pattern shape is a pattern shape in which ultrasonic elements are alternately arranged in a rectangular shape as shown in FIG. And sideband signals are input alternately.
Further, regarding the shape of the block made of ultrasonic elements, the shape of the concentric circle is to divide the block so that the centers are the same as shown in FIGS. 14 (b) and 15 (a). In addition, regarding the shape of the block made of the ultrasonic element, the shape of the radiation is to divide the block radially as shown in FIG.
By making the block division into an array with less directivity, a good sound radiation sound field with less direction dependency can be obtained, and restrictions during installation can be reduced.

Further, as shown in FIG. 16, the ultrasonic emitter generates an ultrasonic wave based on the carrier signal A radiated along the sound axis a and an ultrasonic wave based on the radiated sideband signal B. It is preferable that the sound axes intersect at an angle of 10 ° or less. This is because the reproduction sound pressure can be increased and the sound field intersection area becomes larger. The two ultrasonic emitters can generate a concentrated (focus) sound field by mutually controlling the interval between the two ultrasonic emitters and the inclination angle of the sound axis a as shown in FIG.
Note that “the angle of the ultrasonic wave based on the radiated carrier signal and the ultrasonic wave based on the radiated sideband signal” is radiated from separate ultrasonic emitters as shown in FIG. This is the angle α at which the traveling direction (sound axis) of the ultrasonic waves intersects.

  Further, the attenuation band of the frequency characteristic in the ultrasonic radiation means is controlled to a characteristic that is proportional to the square of the frequency as the frequency increases in the lower band and inversely proportional to the square of the frequency in the upper band. However, it is preferable that a carrier signal and a sideband signal exist in the lower band or the upper band. Thereby, the mid-high frequency characteristics of the demodulated difference sound can be flattened as indicated by a flat line beside the solid line on the left in FIG. As a result, in the flattened band, high-fidelity playback that can achieve the same sound quality as the sound source signal can be performed, and further, the band can be expanded to the low-frequency side, improving the sound quality of the demodulated playback sound. Because it does.

Here, a typical sound pressure frequency characteristic of the ultrasonic emitter is shown in FIG. When the amplified modulation signal is converted into sound by the ultrasonic emitter, as shown in FIG. 17, the frequency fc of the carrier signal is adjusted to the frequency at which the resonance peak is maximum, and the sideband signal has the resonance peak. It is set to exist in the upper or lower level attenuation band. FIG. 17 represents the sound pressure frequency characteristics of the ultrasonic emitter, and illustrates the case where the sideband signal is present in the band above the resonance peak.
The “frequency characteristic attenuation band” is, for example, a band in which the left and right I (ω) are attenuated when viewed from the peak of the peak of the frequency characteristic as shown in FIG. The “lower band” is a band in which the left I (ω) is attenuated, and the “upper band” is a band in which the right I (ω) is attenuated.
FIG. 18 shows the frequency characteristics based on the demodulating conversion principle of the parametric speaker. In the demodulating conversion of the parametric speaker, assuming that the carrier signal fc and the sideband signal fc + fs existing in the ultrasonic parametric speaker band are output at the same level and reproduced by an emitter having a flat frequency characteristic (flat broken line), The frequency characteristic of the difference sound fs (sound source audible signal) obtained by demodulation is proportional to the square of the frequency.
On the other hand, when the ultrasonic emitter having the characteristics shown in FIG. 17 is used, the frequency characteristic of the difference sound fs (sound source audible signal) obtained by demodulation is “increases with approximately the square of the frequency” in the low frequency range. In the middle and high range, the level tends to drop from the square line. In other words, when the frequency of the sound source is low, the carrier signal and the sideband signal are present in close frequency bands, so that both are reproduced at almost the same level, and the characteristic is “rising at approximately the square of the frequency”. It tends to be close. However, as the sound source frequency increases, the sideband signal is demodulated and reproduced in a low-level band away from the carrier signal, and therefore, as shown by the one-dot chain line in FIG. The level falls off the line toward the high region and becomes a flattening tendency. Although the direction of flattening is in this way, the demodulation characteristic is determined depending on the fluctuation of the frequency characteristic of the ultrasonic emitter attenuation band and / or the slope of the level reduction, and therefore the characteristic is not completely flat. .
For this reason, the slope of the attenuation band of the ultrasonic emitter is “decreased by approximately one-quarter of the frequency (1 / f ² )” in the case of the upper band of resonance (USB), and the lower band (LSB). In this case, control is performed so that the frequency rises to approximately the square of the frequency (∝f ² ), so that the frequency fc of the carrier signal and the frequency fc + fs of the sideband signal are present in the band on the slope characteristics. It is preferable to set to.

  Furthermore, the frequency characteristics of the ultrasonic waves reproduced by the ultrasonic radiation means can be expressed as the attenuation frequency band of the ultrasonic radiation means, and the lower frequency band of the ultrasonic radiation means as the frequency increases. Frequency characteristic correction means for controlling the frequency band to be proportional to the square of the frequency and inversely proportional to the square of the frequency in the upper band, and carrier and sideband components in the lower band or the upper band. Is preferably present. As a result, high-fidelity playback that can achieve the same sound quality as that of the sound source signal can be achieved in the flattened band, and further, the frequency band can be expanded to the low frequency side. It is because it improves.

The sound pressure frequency characteristic of the ultrasonic emitter rarely has a gentle single resonance peak as shown in FIG. For example, the sound pressure frequency characteristic of the ultrasonic emitter is shown by a broken line on the right side of FIG. 19 due to the influence of the sound emission state and reflection depending on the resonance and shape of various members constituting the ultrasonic emitter element. Thus, the upper and lower characteristics of resonance tend to attenuate with undulating fluctuations. Here, FIG. 19 shows USB type SSB modulation ultrasonic emitter frequency characteristic control and driving method.
In connection with countermeasures against this, in the case of USB-type SSB modulation, as shown in the right graph of FIG. 19, the reproduction frequency characteristic of the ultrasonic wave reproduced from the ultrasonic emitter is 1 / f ² attenuation band. It is necessary to have. As a result, as shown in FIG. 18, this is a measure to compensate by applying the inverse characteristic of 2f ² which is a demodulation characteristic, and the main middle and high frequencies can be made flat frequency characteristics.

In order to realize this, the first policy is that the resonance frequency of the ultrasonic emitter itself is controlled, and / or the second policy is that the attenuation band of the operating band is It is necessary that the characteristics are electrically corrected by a filter or the like.
As shown in FIG. 20, “electrically correcting the attenuation band” means that the audible signal corrected by the audible signal correcting unit 10 is SSB modulated by the SSB modulating unit 27 and then the frequency characteristic correcting unit 53. It is feasible. Preferably, further, as shown in FIG. This is because the main mid-high range can be made to have a flatter frequency characteristic.
Here, the frequency characteristic correction means 53 is a characteristic correction filtering means for sideband signals, and is made so as to realize the above-described reproduction sound characteristics. The carrier signal side level adjusting means 52 adjusts the carrier signal level so that the carrier signal level exists on the slope of the reproduced sound characteristics of the sideband signal.
The two measures may be performed simultaneously, but the second measure is not necessary if the measure on the ultrasonic emitter side is realized.

In a state where the reproduction frequency characteristic of the ultrasonic wave reproduced from the ultrasonic emitter is realized to have an attenuation band of 1 / f ² , the frequency of the sideband signal is further 1 / f ² (on the horizontal axis) If the frequency is a logarithmic scale, it is set to be a linear slope. As a result, the characteristics of the mid-high frequency band after demodulation are flattened. Furthermore, if the frequency of the carrier signal is also shifted from the maximum value of the single peak so as to be present in the 1 / f ² slope portion (logarithmic scale linear portion), as shown by the solid line in the left-hand side characteristic of FIG. The flat part is enlarged on the low frequency side.
Thereby, in the flattened band, high-fidelity reproduction that can obtain a sound equivalent to the external sound source signal can be performed, the band can be expanded to the low band side, and the sound quality of the demodulated reproduced sound is improved.

  In the first and second measures, DSB modulation or SSB modulation may be used, and composite drive or separation drive may be used. Further, the ultrasonic emitter for reproducing the carrier signal and the sideband signal may have the same performance, but may be a dedicated element. For example, for carrier signals, since the frequency of the carrier signal is almost fixed, it is considered to use an ultrasonic element capable of reproducing a high sound pressure in a narrow band, such as a bolted Langevin vibrator or a composite piezoelectric vibrator. It is done. For the sideband signal, an ultrasonic emitter with controlled band characteristics is used.

<Software>
Next, “software for functioning to correct the audible signal” according to the present invention will be described.
The software for functioning to correct an audible signal according to the present invention is incorporated in a parametric speaker to detect the sound pressure of the ultrasonic wave output from the ultrasonic radiation means, and the detected output sound pressure A waveform of a demodulated audible signal when it is affected by a nonlinear propagation process based on the signal of the signal is generated using a nonlinear propagation model, and the generated waveform is compared with the waveform of the input audible signal. The audible signal is corrected so as to function.

By incorporating the software having the above configuration into the parametric speaker, it is possible to obtain the effect of correcting the audible signal according to the present invention described above.
In addition, as a specific method of installing the software, a method of recording in a parametric speaker circuit or the like in the manufacture of a parametric speaker, a method of installing the software using a medium, or a download by the Internet or the like There are installation methods. Here, examples of the medium include, but are not limited to, a DVD, a CD, a USB memory, a hard disk, and the like.

  According to the present invention, it is possible to reduce distortion or the like in the process of modulation and demodulation of sound propagation in the air. As a result, it is possible to realize a high-quality reproduced sound that is easy to hear and has no sense of incongruity, which is not possible in the past.

2, 20 Modulating means 3, 30, 31 Amplifying means 4, 40, 41, 42 Supersonic radiation means 5, 50 External sound source 6 Carrier signal source 7, 70, 71 Ultrasonic wave 10 Audible signal correcting means 11 Non-linear propagation model generating means 12 Comparison means 13 Detection means 27 SSB modulation means 31a, 41a Carrier signals 31b, 41b Sideband signals 43a-e Blocks (carrier signals) composed of ultrasonic elements
44a-d Blocks composed of ultrasonic elements (sideband signals)
52 Level adjustment means 53 Frequency characteristic correction means 100, 101 Parametric speaker

Claims (10)

A modulation means for modulating a carrier signal in an ultrasonic band with an audible signal from an external sound source to generate a modulation signal, an amplification means for amplifying the generated modulation signal, and an ultrasonic signal based on the amplified modulation signal. In a parametric speaker comprising an ultrasonic radiation means for radiating sound waves,
The parametric speaker detects the sound pressure of the ultrasonic wave output from the ultrasonic radiation means, and based on the detected output sound pressure signal, the waveform of the demodulated audible signal when affected by a non-linear propagation process Is predicted by a non-linear propagation model, and the generated waveform is compared with the waveform of the input audible signal to correct the audible signal and send the corrected audible signal to the modulation means. A parametric speaker, further comprising signal correction means. The parametric speaker according to claim 1 , wherein a waveform model when the audible signal is affected by a nonlinear propagation process is derived by the following equation.

Here, t represents time (seconds), and e (t) represents an envelope function. The parametric speaker according to claim 1 or 2 , wherein the modulation signal includes the carrier signal and a sideband signal obtained by modulating the carrier signal. The parametric speaker according to claim 3 , wherein the ultrasonic radiation means radiates ultrasonic waves based on the carrier signal and ultrasonic waves based on the sideband signal by separate ultrasonic emitters. . In the ultrasonic emitter, the ultrasonic wave based on the emitted carrier signal and the ultrasonic wave based on the emitted sideband signal are arranged so as to intersect at an angle of 10 ° or less. The parametric speaker according to claim 4 . The ultrasonic emitter is constituted by a plurality of blocks consisting of a plurality of ultrasonic elements, the ultrasonic wave based on the carrier signal, and an ultrasonic based on the sideband signal, that emitted by separate blocks The parametric speaker according to claim 4 , wherein the speaker is a parametric speaker. The parametric speaker according to claim 6 , wherein the block made of the ultrasonic element has a rectangular shape, a checkered pattern, a concentric circle, or a radiation shape. The attenuation band of the frequency characteristic in the ultrasonic radiation means is controlled to a characteristic that is proportional to the square of the frequency as the frequency increases if the lower band, and inversely proportional to the square of the frequency if the upper band, The parametric speaker according to any one of claims 1 to 7 , wherein a carrier signal and a sideband signal exist in the lower band or the upper band. The frequency characteristics of the ultrasonic waves reproduced by the ultrasonic radiation means are the attenuation frequency band of the ultrasonic radiation means, and the lower band of the frequency characteristics of the ultrasonic radiation means, the frequency Frequency characteristic correction means is further provided for controlling the frequency to be proportional to the square and inversely proportional to the square of the frequency in the upper band, and carrier and side band components exist in the lower band or the upper band. The parametric speaker according to any one of claims 1 to 7 , wherein Software for a parametric speaker according to any one of claims 1 to 9,
By incorporating it in a parametric speaker, the sound pressure of the ultrasonic wave output from the ultrasonic radiation means in the parametric speaker is detected, and when it is affected by the nonlinear propagation process based on the detected output sound pressure signal Software for predicting and generating a waveform of a demodulated audible signal using a non-linear propagation model, and comparing the generated waveform with the waveform of the input audible signal to function to correct the audible signal .

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