The present invention relates to a method for acquiring audio signals and an audio acquisition system capable of implementing said method.
In the television and movie fields and the like, there is an increasing need to record sounds accurately in the three-dimensional environment in which shooting is taking place, so that they can be reproduced faithfully at the user's premises.
Recording sounds in a three-dimensional environment involves the necessity of knowing the pressure and speed of the air particles in a certain spatial point.
To this end, it is currently known to use microphone probes which comprise multiple microphone capsules arranged on a surface, e.g. a spherical surface.
One example of such probes is the microphone probe available on the market under the name “EigenMike32” and manufactured by the American company “mhAcoustics”.
Each of the capsules B detects one audio signal coming from a different spatial direction.
By appropriately combining these signals it is possible to obtain a signal corresponding to the signal that would be measured by a microphone having certain desired characteristics.
Thanks to these probes, the user can use “virtual” microphones having the desired characteristics of directivity (cardioid, supercardioid or the like) and position (azimuth, elevation, etc.).
Probes of this type are generally used in combination with graphic systems in order to display for the user any noise sources and identify any mechanical defects in a machine (e.g. a broken tooth of a toothed wheel) or any sources of noise pollution.
For this purpose, much importance is attributed in the known probes to the microphone directivity, and much effort is being made to define optimal filters which can ensure the best possible directionality.
Once the optimal theoretical filters have been identified, the audio signal of the virtual microphone required by the user is generated by appropriately weighing the filter outputs and by applying thereto delays and gains which are suitably calculated and then combined together in order to obtain certain forms of microphone directivity.
A first limit of these probes is related to the fact that the use of predetermined theoretical filters, although it provides good directivity, often does not ensure a good audio signal quality.
Moreover, another limit of these known probes is the fact that they can only provide good directivity up to certain frequencies, typically around 4 kHz, whereas beyond which the directivity tends to deteriorate.
These probes are therefore not suitable for use in the television or cinematographic environment, wherein, in addition to the microphone directionality, it is also very important to be able to acquire high-quality audio signals.
It is the object of the present invention to provide a method for acquiring audio signals and a related audio acquisition system which can overcome the drawbacks of the prior art.
This object is achieved through a method and a system incorporating the features set out in the appended claims, which are intended as an integral part of the present description.
The present invention is based on the idea of processing the signals acquired by the capsules of the probe by starting from actual probe data measured empirically during a probe characterization step.
In particular, filters are used which, instead of being calculated theoretically, are determined empirically during a probe characterization step in which the impulse responses of the capsules to one or more predetermined test signals are detected.
Thus, when in operation, the system allows to detect high-quality audio signals because any differences in the performance of the capsules from the nominal specifications will not affect the quality of the detected signal.
Also, it is thus possible to take into account the effect of the probe support, which de facto interrupts the perfect symmetry of the probe.
Furthermore, the probe can maintain good directivity of the virtual microphone even at high frequencies over 4 kHz, in that the signal of the virtual microphone is not based on a theoretical filtering process, but on a filtering process which depends on the actual characteristics of the probe, and in particular on the impulse responses of the capsules, calculated by starting from test signals determined beforehand during a probe characterization step.
Further objects and advantages of the present invention will become apparent from the following description of an embodiment thereof as shown in the annexed drawings, which are supplied by way of non-limiting example, wherein:
Referring now to
In the first step 200 of the method, the microphone probe 11 is placed into an anechoic chamber (or a similar environment) in which one or more test signals are generated, preferably at least one sinusoidal signal whose frequency is changed over substantially the whole audible frequency spectrum, i.e. a so-called “logarithmic sine sweep”, from whose convolution with an inverse signal (i.e. “reversed” on the time axis) the probe response to the impulse is obtained: this technique is per se known and therefore it will not be described any further; it must however be pointed out that it can also be found in the main standards defining impulse response measurements (e.g. the ISO 3382 standard).
For each test signal, the impulse responses of each capsule B are recorded by varying in regular steps (action schematized in block 201) azimuth and elevation of the direction from which the test signal is coming; in
This provides a set of transfer functions between every single capsule and loudspeaker (which generates the signal) for each direction around the probe centre.
The probe is thus characterized along the three spatial dimensions by a number of transfer functions equal to Y×M×K, where:
Y is the number of microphone capsules of the microphone probe 11,
M is the azimuth of the test signal relative to a spherical coordinate centre originating from the centre of the probe A,
K is the elevation of the test signal relative to that coordinate system.
These transfer functions are expressed in matrix form by means of the matrix of the IRs impulse responses, which is stored in a memory area of the audio acquisition system associated with the probe.
A size of the IRs matrix (the number of rows for example) is equal to Y, whereas the other size of the IRs matrix (the number of columns for example) is equal to M×K.
The IRs matrix contains data that characterizes the probe's capsules; since it has been measured empirically, this data is not the nominal data.
The actual characteristics of the probe 11 are thus advantageously detected and it is possible, in operation, to acquire a signal of better quality because it is taken into consideration the fact that each of the Y microphone capsules B may behave differently from the other ones, as well as the fact that the probe is not perfectly spherical, at least due to the presence of a support.
Once this first step of PROBE CHARACTERIZATION has been carried out, and after having consequently defined the IRs matrix, it is possible to use the microphone probe 11 in order to acquire sound, or audio signals, in an environment.
In a three-dimensional environment, the signals received by the Y capsules may come from multiple spatially distributed sources.
In order to choose which source must be listened to and recorded by the probe, it is necessary to synthesize a virtual microphone by starting from the signals detected by the Y microphone capsules.
In other words, the audio signals picked up by the real capsules B of the microphone probe 11 are processed in a manner such as to obtain a signal which ideally corresponds to the one that would be acquired by a microphone whose parameters could be chosen at will by an operator, more specifically pointing direction and directivity.
By “microphone directivity” it is meant the way in which the sensitivity of the microphone varies as the sound incidence angle changes: it may be, for example, cardioid, supercardioid, cardioid of the 3rd order or the like.
The other parameters of a microphone are, more in general, sensitivity, response curve, noise, distortion, dynamic range, impedance, and transient response; in the present text, however, only pointing direction and directivity will be taken into account as parameters of the virtual microphone, leaving out the remaining parameters listed above.
The operator thus chooses the parameters of one or more virtual microphones to be used in the environment where the sound field is to be picked up, e.g. to concentrate on certain areas of the environment to be detected with (virtual) microphones having a certain directivity.
The definition of the parameters of the virtual microphones is schematized in
In accordance with the teachings of the present invention, the virtual microphones are generated in the method step designated in
As will be better explained below, the operator interacting with the audio acquisition system defines the parameters of the virtual microphone(s) by giving inputs to the system, e.g. by moving a joystick and selecting in real time an area of the environment to be listened to.
Based on the operator inputs, the system generates (step 204 in
The matrix A is thus that matrix which represents the directivity model of the virtual microphone, i.e. that spatial figure which the virtual microphone must tend to.
The elements ai,j generally have a value, preferably between 0 and 1, which depends on the spatial coordinates (azimuth and elevation) and directivity of the desired virtual microphone.
The mathematical expression of directivity (e.g. cardioid, supercardioid, cardioid of the 3rd order, etc.) is per se known and is described by functions known in the literature; therefore, the man skilled in the art can create the matrix A corresponding to the desired microphone(s).
The matrix H of FIRs filters is then generated (step 203 in
that is (in standard notation):
H=A·[IRs(ω)]*T*([IRs(ω)]*T·IRs(ω)+ε(ω))−1 (2)
where:
IRs(ω) is the impulse response matrix generated in the previously described characterization step,
A is the “target function” generated on the basis of the virtual microphone parameters chosen by the operator,
ε(ω) is a “regularization” parameter to prevent that the filtering process may produce undesired low-frequency and high-frequency artifacts, ε(ω) is a matrix of size N×N with the diagonal elements equal to a same value
Conj[IRs(ω)] is an operation that outputs the conjugate transpose matrix of the matrix IRs(ω),
H is a matrix of size Y×N.
The choice of the value of the regularization parameter ε in the Kirkeby algorithm is preferably made empirically during the probe characterization step, when, while measuring the impulse responses of the capsules, the signals detected by the probe are recorded.
In this step, ε is changed until a high-quality recorded signal is obtained.
The effect of the filtering is in fact to modify, frequency per frequency, the amplitudes of the signals received by the capsules, so that the sum thereof gives at the output the signal of the desired virtual microphone.
In this step, some frequencies of the signals coming from the capsules must be amplified, e.g. in order to fill spectral holes, while other frequencies must be lowered because they would be emphasized too much in the signal of the virtual microphone.
Depending on the chosen ε, the filter matrix calculated by means of the Kirkeby algorithm will compensate differently for the frequencies of the signals coming from the capsules Y and, as a result, the quality of the signal of the virtual microphone will change. In particular, at the low or high frequencies it is necessary to use a different regularization parameter from the one used in the central band, so as to limit the inversion produced by Kirkeby's formula and to prevent the calculated filter from becoming unstable and annoying artifacts from being produced during the listening phase.
In particular, in order to obtain a good quality virtual signal, the regularization parameter ε must in substance be chosen in a manner such that it is sufficiently high at high frequencies (in particular over 14 kHz) and at low frequencies (in particular under 100 Hz) while being sufficiently low within a central frequency band, so that the frequency amplification or damping obtained by means of the filtering obtained with the Kirkeby algorithm will be lower at the high and low frequencies and greater in the central frequency range.
The preferred values of
0.09≦
0.001≦
Referring back to the matrix equation (1), it can be observed that the generated filter matrix H is affected both by the operator's choices (which have an impact on the determination of the target function A) and by the actual probe characterization (which influences the determination of the IRs matrix, block 206 in
This advantageously leads to obtain from the process of filtering the signals received by the real capsules B an extremely natural result of the acoustic field of the environment, which will be faithful to the characteristics of the environment while providing flexibility based on the parameters set by the operator.
Once the matrix H has been thus determined, the virtual microphones are synthesized by filtering the signals picked up by the capsules through the filters determined in accordance with the above-described method.
The signal coming from each capsule is combined (step 207), by means of a convolution operation, with a suitable filter and is then added to the other signals in order to obtain the signal of the desired virtual microphone:
where:
Virtual_Mic—1 . . . N indicates the audio signal detected by each virtual microphone,
FIR—i,1 . . . N indicates the element i,1 . . . N of the matrix H, Chi indicates the signal picked up by the i-th microphone capsule of the probe.
A graphic diagram of said convolution is also shown in
The above-described method advantageously allows the virtual microphone parameters to be changed in real time.
The operator can change the parameters of the virtual microphone in use (e.g. in order to follow an actor in a cinematographic scene or the action taking place in a certain point of the environment) by acting upon a dedicated control console.
Upon receiving an input corresponding to a change in the parameters of one of the virtual microphones or a request to add or eliminate a virtual microphone, the system will recalculate the filter matrix H.
The flow chart of this operation is shown in
After turning on a virtual microphone (step 500), it is checked whether an input has arrived which requires a change to the azimuth (step 501); if not, it is checked whether an input has arrived which requires a change in elevation (step 502) and, if also this check gives a negative result, it is checked whether an input has arrived which requires a change in directivity (step 503).
If this last check is also negative, the method goes back to step 501.
Otherwise, if any one of the checks made in the steps 501 to 503 gives a positive result, then the coefficients of the target functions A are recalculated based on the new input (step 504).
After the coefficients have been changed, they can be used by the processor to generate the filter matrix H.
The algorithm schematized in
In short, therefore, when the operator varies the azimuth and/or elevation and/or directivity of the virtual microphone (and thus the parameters thereof), the coefficients of the target function matrix A are changed accordingly and the matrix H is re-calculated.
According to a further improvement, it is also possible to change a virtual microphone without generating a sensation of “jerky” motion affected by disturbances or ground noise: this can be done by executing a dynamic “crossfade” between the audio coming from the virtual microphone in use and that coming from the virtual microphone to which the operator wants to move.
In substance, when the operator changes the virtual microphone in use and chooses a second one, the switch between a first matrix H corresponding to a first microphone (the microphone in use) and a second matrix H corresponding to a second microphone (the microphone to which the operator wants to move) is carried out gradually by means of an ordered set of transaction matrices (i.e. transaction filters). The sound picked up by the capsules B is filtered with the transaction matrices according to their order. More in detail, the ordered set of transaction matrices T1, T2, T3 . . . Tn allows to switch between the first matrix and the second matrix as follows: at the beginning the sound is filtered by the first matrix, then it is filtered by transaction matrix T1, then by transaction matrix T2, then by transaction matrix T3 and so on till to arrive at the second matrix.
Each of the transaction matrices T1, T2, T3 . . . Tn comprises submatrices corresponding to submatrices belonging to either the first matrix or the second matrix. In particular, transaction matrix Tk (corresponding the k-th matrix of the ordered set of transaction matrices, with k=2 . . . n) comprises a number of submatrices corresponding to submatrices of the second matrix greater than a previous transaction matrix Tk-1 comprises. Moreover, transaction matrix Tk comprises a number of submatrices corresponding to submatrices of the first matrix lower than the previous transaction matrix Tk-1 comprises.
Then, using a mathematical syntax, the transaction matrices comprise submatrices so that:
#S2k>#S2k-1 and #S1k<#S1k-1, k=2 . . . n
where:
#S2k indicates the number of submatrices of the transaction matrix Tk that correspond to submatrices of the second matrix,
#S2k-1 indicates the number of submatrices of the transaction matrix Tk-1 that correspond to submatrices of the second matrix,
#S1k indicates the number of submatrices of the transaction matrix Tk that correspond to submatrices of the first matrix,
#S1k-1 indicates the number of submatrices of the transaction matrix Tk-1 that correspond to submatrices of the first matrix,
index k is any integer value between 2 and n, where n is the number of the transaction matrices.
As a result, the transaction matrix T1 is the most similar to the first matrix, whereas the transaction matrix Tn is the most similar to the second matrix.
In a preferred embodiment, all submatrices have the same sizes and in particular a size (row or column) is equal to N.
The switch between different filters (i.e the different matrices) can be done by a standard “crossfade” (i.e. a decrease in the level of an audio signal corresponding to a filter while the audio signal corresponding to another filter increases) between the audio coming from a filter in use and that coming from a following filter: the signal of the filter in use and the one of the following filter are then mixed so as to progressively fade the volume of the former to zero and progressively increase the volume of the latter to the maximum value, thus giving the user a sensation of great smoothness.
Referring now to
The system 1 allows to pick up audio signals coming from an environment.
The system 1 comprises a microphone probe 11 comprising a plurality of capsules (e.g. a 32-channel microphone probe called “em32 Eigenmike”, sold by company mhAcoustics), whose signals are pre-amplified and converted into digital form.
The probe 11 is connected to an electronic computer 3 equipped with an audio interface 2 (e.g. an EMIB firewire audio interface), which receives the signals from the probe and transmits them, after having possibly processed them, to a processor 300, e.g. a DSP (Digital Signal Processor), programmed for executing the above-described audio acquisition method.
The system 1 further comprises a data or command input unit 4, also connected to the computer 3, e.g. through a USB (Universal Serial Bus) port, by means of which an operator can supply information about the area where sound must be acquired or directly enter the parameters of one or more virtual microphones (e.g. by selecting predefined forms of directivity by means of buttons).
The data or command input unit 4 may be, for example, a control console equipped with a joystick for controlling the pointing of the virtual microphones.
The system 1 further comprises a recorder 5 and/or an analog output 6 and/or a digital output 7 through which it can record or transmit the signal picked up by the virtual microphone(s).
In the example of
In addition to the parts designated by the same reference numerals in
The video camera 8 frames the environment where the scene whose audio is to be acquired is taking place; for this purpose, the video camera 8 is a wide angle video camera, e.g. of the “dome” type typically used for surveillance purposes or the like.
The video camera 8 transmits the acquired video signal to the graphic interface means 9, which comprise a monitor for displaying the images taken by the video camera 8.
The same graphic interface means 9 are operationally connected to the data or command input unit 4, and therefore receive information about the virtual microphone(s) selected by the operator.
The graphic interface means 9 process this information and translate it graphically; in particular, they display, superimposed on the images taken by the video camera 8, a mobile pointer which indicates the area being listened to by the virtual microphone chosen by the operator.
Preferably, the shape and size of the pointer are related to the microphone's directivity and orientation, so as to reflect the parameters of the microphone in use and allow it to be controlled more intuitively by the operator.
The data or command input unit 4 may advantageously be fitted with a control lever or a slider or the like to allow an operator to zoom in or out the sound field of the virtual microphone in a quick and intuitive manner.
Through the data or command input unit 4, the operator thus moves the microphone within the filmed scene and can listen separately to different sound sources included in the taken image.
By moving the joystick, the operator moves the virtual microphone and can follow the movement thereof thanks to the images displayed by the graphic interface means 9. By acting upon the slider the operator can control directivity, and the pointer's size changes accordingly.
In a further alternative embodiment, the pointer may be replaced with coloured areas corresponding to the regions being listened to by the microphone; for example, the best received area may be displayed in red, the other areas being displayed with colder colours according to their reception quality. When the virtual microphone is moved or its directivity is changed, the colour of the images will change as well.
In this example, the operator has the possibility of setting the parameters of the virtual microphone through the data or command input unit 4 or the graphic interface 90, thereby pointing the virtual microphone (in terms of azimuth and elevation) and selecting its directivity (cardioid, supercardioid, cardioid of the 3rd order, etc.).
The graphic interface means 90 of
By interacting with the touch screen, the operator can move the microphone or change the extent of the space to be listened to, i.e. change the microphone's orientation and directivity.
The virtual microphone data thus set by the user is sent to the processor 300, where the execution of some code portions allows for the generation of the above-mentioned target function A and the calculation of the Kirkeby algorithm, which is made by using the IRs matrix of impulse responses (measured in the aforementioned PROBE CHARACTERIZATION step) pre-loaded into the memory and relating to the microphone probe 11.
The filter matrix H is then generated as previously described.
The file containing the FIRs filter coefficients is then used in order to carry out the filtering process with the audio data coming from the microphone probe 11.
The virtual microphone signal synthesized by said filtering process is returned to a Jack interface 15, which may then deliver it to digital outputs (ADAT) provided on the EMIB card or divert it towards a memory card.
Every time the virtual microphone's parameters are changed (e.g. when directivity is changed), the Kirkeby algorithm is executed again and a new matrix H is calculated, so that a change is made in real time.
In this respect, the processor 3 or the processor 300 preferably comprises a memory area (e.g. a flash memory) which stores the matrix
calculated during the probe characterization step and therefore dependent on the capsules' impulse responses calculated by using the predetermined and known test signals.
This solution allows to reduce the computational cost required by the above-described audio acquisition method; when the matrix H is to be re-calculated, it is not necessary to re-calculate Γ, but only the product of the matrices A and Γ.
Although the present invention has been described herein with reference to some preferred embodiments, it is apparent that those skilled in the art may make several changes to the above-described audio acquisition system and audio acquisition method.
In particular, the various elements and logic blocks of the audio acquisition system may be composed and distributed in many different ways while still carrying out, as a whole, the same functions or functions being equivalent to those described herein.
Number | Date | Country | Kind |
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TO2009A000713 | Sep 2009 | IT | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IB2010/054210 | 9/17/2010 | WO | 00 | 4/6/2012 |