EP0693747A2 - An apparatus for cancelling vibrations - Google Patents

An apparatus for cancelling vibrations Download PDF

Info

Publication number
EP0693747A2
EP0693747A2 EP95304332A EP95304332A EP0693747A2 EP 0693747 A2 EP0693747 A2 EP 0693747A2 EP 95304332 A EP95304332 A EP 95304332A EP 95304332 A EP95304332 A EP 95304332A EP 0693747 A2 EP0693747 A2 EP 0693747A2
Authority
EP
European Patent Office
Prior art keywords
updates
frequency components
vibrations
filter
reference signal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
EP95304332A
Other languages
German (de)
French (fr)
Other versions
EP0693747A3 (en
Inventor
Malcolm Alexander Swinbanks
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
BAE Systems Electronics Ltd
Original Assignee
GEC Marconi Ltd
Marconi Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority claimed from GB9414484A external-priority patent/GB9414484D0/en
Application filed by GEC Marconi Ltd, Marconi Co Ltd filed Critical GEC Marconi Ltd
Publication of EP0693747A2 publication Critical patent/EP0693747A2/en
Publication of EP0693747A3 publication Critical patent/EP0693747A3/en
Ceased legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K11/00Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/16Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/175Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound
    • G10K11/178Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound by electro-acoustically regenerating the original acoustic waves in anti-phase
    • G10K11/1781Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound by electro-acoustically regenerating the original acoustic waves in anti-phase characterised by the analysis of input or output signals, e.g. frequency range, modes, transfer functions
    • G10K11/17813Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound by electro-acoustically regenerating the original acoustic waves in anti-phase characterised by the analysis of input or output signals, e.g. frequency range, modes, transfer functions characterised by the analysis of the acoustic paths, e.g. estimating, calibrating or testing of transfer functions or cross-terms
    • G10K11/17817Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound by electro-acoustically regenerating the original acoustic waves in anti-phase characterised by the analysis of input or output signals, e.g. frequency range, modes, transfer functions characterised by the analysis of the acoustic paths, e.g. estimating, calibrating or testing of transfer functions or cross-terms between the output signals and the error signals, i.e. secondary path
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K11/00Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/16Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/175Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound
    • G10K11/178Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound by electro-acoustically regenerating the original acoustic waves in anti-phase
    • G10K11/1785Methods, e.g. algorithms; Devices
    • G10K11/17853Methods, e.g. algorithms; Devices of the filter
    • G10K11/17854Methods, e.g. algorithms; Devices of the filter the filter being an adaptive filter
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K11/00Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/16Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/175Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound
    • G10K11/178Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound by electro-acoustically regenerating the original acoustic waves in anti-phase
    • G10K11/1785Methods, e.g. algorithms; Devices
    • G10K11/17857Geometric disposition, e.g. placement of microphones
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K11/00Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/16Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/175Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound
    • G10K11/178Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound by electro-acoustically regenerating the original acoustic waves in anti-phase
    • G10K11/1787General system configurations
    • G10K11/17879General system configurations using both a reference signal and an error signal
    • G10K11/17881General system configurations using both a reference signal and an error signal the reference signal being an acoustic signal, e.g. recorded with a microphone
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K11/00Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/16Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/175Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound
    • G10K11/178Methods or devices for protecting against, or for damping, noise or other acoustic waves in general using interference effects; Masking sound by electro-acoustically regenerating the original acoustic waves in anti-phase
    • G10K11/1787General system configurations
    • G10K11/17879General system configurations using both a reference signal and an error signal
    • G10K11/17883General system configurations using both a reference signal and an error signal the reference signal being derived from a machine operating condition, e.g. engine RPM or vehicle speed
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K2210/00Details of active noise control [ANC] covered by G10K11/178 but not provided for in any of its subgroups
    • G10K2210/10Applications
    • G10K2210/128Vehicles
    • G10K2210/1281Aircraft, e.g. spacecraft, airplane or helicopter
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K2210/00Details of active noise control [ANC] covered by G10K11/178 but not provided for in any of its subgroups
    • G10K2210/30Means
    • G10K2210/301Computational
    • G10K2210/3018Correlators, e.g. convolvers or coherence calculators
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K2210/00Details of active noise control [ANC] covered by G10K11/178 but not provided for in any of its subgroups
    • G10K2210/30Means
    • G10K2210/301Computational
    • G10K2210/3025Determination of spectrum characteristics, e.g. FFT
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K2210/00Details of active noise control [ANC] covered by G10K11/178 but not provided for in any of its subgroups
    • G10K2210/30Means
    • G10K2210/301Computational
    • G10K2210/3042Parallel processing
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K2210/00Details of active noise control [ANC] covered by G10K11/178 but not provided for in any of its subgroups
    • G10K2210/30Means
    • G10K2210/301Computational
    • G10K2210/3045Multiple acoustic inputs, single acoustic output
    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K2210/00Details of active noise control [ANC] covered by G10K11/178 but not provided for in any of its subgroups
    • G10K2210/30Means
    • G10K2210/301Computational
    • G10K2210/3051Sampling, e.g. variable rate, synchronous, decimated or interpolated

Definitions

  • This invention relates to an apparatus for cancelling vibrations, be they vibrations in a gas, liquid or solid.
  • GB-2054999-A, EP-43565-A1, and GB-2107960-A disclose examples of apparatus for cancelling vibrations which employ frequency domain filtering.
  • the vibrations to be cancelled must be periodic and the resolving into the frequency components synchronised to this periodicity, or, in the case where the vibrations are random (aperiodic), the resolving into the frequency components must be a continuously updated process.
  • an apparatus for cancelling vibrations comprising: means for providing a reference signal representative of the vibrations to be cancelled; filter means comprising means for resolving the reference signal into its frequency components, means for applying weights to these frequency components, and means for combining the weighted frequency components to provide an output signal of said filter means; and actuator means responsive to said output signal to produce vibrations which destructively interfere with the vibrations to be cancelled, said means for resolving utilising N updates of said reference signal to resolve it into its frequency components, said means for resolving being updated by n times between successive resolutions of the reference signal into its frequency components where 1 ⁇ n ⁇ N, there being a correlation between the weights applied by said means for applying so as to reduce discontinuity in the operation of said filter means.
  • the invention arose in the making of an apparatus for cancelling vibrations employing frequency domain filtering. It was decided that block processing be used by the frequency domain filter to improve the processing efficiency of the apparatus, i.e. the filter would take a block of data, rather than just one sample, and process it all in one go to provide a number of sequential outputs. First trials of the apparatus were not successful, since it was found that in two cases the filter outputs were discontinuous, the first case being where the vibrations to be cancelled are periodic and the resolving into the frequency components not synchronised to this periodicity, the second case being where the vibrations are random. Even when attempting to cancel a pure tone not synchronised, in addition to the production of the cancelling tone, unwanted side bands were produced.
  • the apparatus is for cancelling engine noise in an aircraft cabin.
  • the apparatus includes a loudspeaker 1 located in the region of the aircraft cabin where it is desired that the noise produced by an engine 3 be cancelled.
  • the loudspeaker 1 produces the aforementioned interfering anti-phase vibrations.
  • the apparatus further includes an adaptive control filter 5, a model filter 7, a controller 9, updates modifying circuitry 10, an arithmetic circuit 12, and an error microphone 11, which microphone 11 is located in the aforementioned region of the aircraft cabin.
  • Control filter 5 comprises a fast Fourier transform (FFT) circuit 13, a processor 15, and an inverse FFT circuit 17.
  • Controller 9 comprises an FFT circuit 19 and a processor 21.
  • Updates modifying circuitry 10 comprises an inverse FFT circuit 23, an arithmetic circuit 25, and an FFT circuit 27.
  • a reference signal x(t) representative of the noise to be cancelled at time t is supplied to control filter 5.
  • This signal may be obtained from a microphone located in the aforementioned region of the aircraft cabin, or by means of a tachometer from the aircraft engine 3 itself.
  • FFT circuit 13 Fourier transforms x(t) from the time domain to the frequency domain and provides to processor 15 a plurality of frequency components x t (f) of x(t). Processor 15 multiplies each x t (f) by an appropriate weight (see below). Let the resulting frequency components be y t (f). Processor 15 provides the y t (f) to inverse FFT circuit 17. Circuit 17 inverse Fourier transforms the y t (f) from the frequency domain to the time domain to provide to loudspeaker 1 an appropriate driving signal y(t) to cancel the noise.
  • the weights utilised by processor 15 perform amongst other things, a phase inversion of x(t) to provide the interfering anti-phase signal.
  • An explanation of the derivation of the weights utilised by processor 15 will now be given.
  • Error microphone 11 detects any residual noise remaining after interference between the primary noise produced by noise source 3 and the interfering sound produced by loudspeaker 1.
  • a signal e(t) representative of this residual noise passes from microphone 11 to FFT circuit 19 of controller 9 where it is Fourier transformed from the time domain to the frequency domain.
  • FFT circuit 19 provides to processor 21 a plurality of frequency components e t (f) of e(t).
  • each of these components also passes to model filter 7, where it is multiplied by a frequency dependent function C(f).
  • C(f) is the transfer function from loudspeaker 1 to microphone 11, and it is necessary that this function be involved in the derivation of the weights utilised by processor 15 to take account of the physical path from loudspeaker 1 to microphone 11 within the aircraft cabin.
  • microphone 11 is detecting the residual noise at a different physical location within the aforementioned cabin region to the physical location where loudspeaker 1 is attempting to eliminate this residual noise.
  • any attempt to eliminate the residual noise at one location by the generation of interfering sound at another different location must take into account the physical path travelled by the sound between the locations.
  • C(f) is a previously determined transfer function which describes the change which the physical path within the cabin from loudspeaker 1 to microphone 11 will have on the passage of sound therealong.
  • the frequency components x t (f).C(f) resulting after multiplication by C(f) pass to processor 21 of controller 9, where each is multiplied by a respective frequency component e t (f) from FFT circuit 19.
  • the resulting frequency components or provisional filter updates x t (f).C(f).e t (f) are supplied by processor 21 to updates modifying circuitry 10.
  • the actual filter updates (x t (f). C(f). e t (f))' are supplied to arithmetic circuit 12.
  • the weights utilised by filter 5 phase invert the reference representative of the noise, attempt to eliminate detected residual noise, and take into account the physical path from the actuator which produces the cancelling sound to the detector which detects residual noise.
  • filter 5 For correct operation of the apparatus, the operation of filter 5 must take account of filter settling time, otherwise discontinuous filter outputs result.
  • each FFT performed by circuit 13 of filter 5 is performed on 128 samples of reference signal x(t).
  • 64 complex frequency components x t (f) of x(t) are presented to processor 15 where each is multiplied by its respective weight w t (f).
  • the resulting 64 complex frequency components y t (f) are passed to inverse FFT circuit 17 where they are inverse transformed to 128 'samples' of y(t).
  • the number of samples of x(t) by which FFT circuit 13 is updated between the performance of successive FFTs be 32.
  • samples of x(t) are taken by filter 5 and 32 samples of y(t) are provided by filter 5.
  • the aforementioned provisional updates x t (f). C(f). e t (f) are passed by processor 21 to inverse FFT circuit 23 of updates modifying circuitry 10, where they are inverse Fourier transformed from the frequency domain to the time domain to provide to arithmetic circuit 25 the equivalent 128 time domain updates.
  • Arithmetic circuit 25 sets to zero the last 31 (128 - 97) of these 128 updates so as to effectively leave 97 updates for a 97 weight filter. Note, it is the last 31 updates that are set to zero since it is the 97th (mth) data output that is the first accurate data output, see above.
  • N-m or N-(N-n+1) (taking the limit where the least updates are set to zero giving the greatest flexibility for filter 5) or n-1 updates are set to zero.
  • the resulting updates are passed to FFT circuit 27 where they are Fourier transformed from the time domain to the frequency domain to provide to arithmetic circuit 12 the actual constrained frequency domain updates (x t (f). C(f). e t (f))'.
  • Circuit 12 calculates the new constrained weights according to equation (1).
  • the FFT process effectively assumes periodic behaviour, i.e. it fits a set of periodic functions to the data samples on the assumption that the data is periodic outside the N sample block.
  • the FFT process will always be accurate without the need to observe the m ⁇ N-n+1 constraint. Therefore, when the vibrations to be cancelled are periodic, and the resolving of the reference signal representative of these vibrations into its frequency components is synchronised to this periodicity, then constraint for successful operation is not required. In all other circumstances, i.e.
  • n is greater than 1 and constraint for correct operation is required (unless the data is periodic and synchronised).
  • n may be chosen from the upper end of the range, i.e. the end approaching N, with a consequent benefit in processing efficiency.
  • the disadvantage is that the corresponding convolution window involves complex, asymmetric coefficients.
  • the advantage would be that the corresponding convolution window is symmetric, and a simple 5-point convolution would suffice.
  • the resolving of the reference signal into its frequency components need not be by means of Fourier transformation, for example frequency sampling filtering could be used.

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Acoustics & Sound (AREA)
  • Multimedia (AREA)
  • Soundproofing, Sound Blocking, And Sound Damping (AREA)
  • Vibration Prevention Devices (AREA)

Abstract

An apparatus for cancelling vibrations comprising: means for providing a reference signal representative of the vibrations to be cancelled; filter means (5) comprising means (13) for resolving the reference signal into its frequency components, means (15) for applying weights to these frequency components, and means (17) for combining the weighted frequency components to provide an output signal of said filter means (5); and actuator means (1) responsive to said output signal to produce vibrations which destructively interfere with the vibrations to be cancelled, said means (13) for resolving utilising N updates of said reference signal to resolve it into its frequency components, said means (13) for resolving being updated by n times between successive resolutions of the reference signal into its frequency components where 1<n<N, there being a correlation between the weights applied by said means (15) for applying so as to reduce discontinuity in the operation of said filter means (5).

Description

  • This invention relates to an apparatus for cancelling vibrations, be they vibrations in a gas, liquid or solid.
  • It is known to cancel vibrations by obtaining a reference signal representative of the vibrations to be cancelled, inverting this signal, and using the inverted signal to cause vibrations in anti-phase with the vibrations to be cancelled, which interfere therewith, thereby to effect the cancellation.
  • It is further known to resolve the reference signal into its frequency components, appropriately filter these components, and combine the filtered components to provide the signal which causes the anti-phase vibrations. The filtering in the frequency domain effects the required phase inversion, and may also be used to further refine the interfering vibrations so that complete cancellation is achieved. By choosing frequency domain rather than time domain control, the control is effectively diagonalised, thereby making for much faster adjustment - the controls can be adjusted in pairs (in-phase and quadrature) for each centre frequency, without interaction with neighbouring controls as in time domain control.
  • GB-2054999-A, EP-43565-A1, and GB-2107960-A disclose examples of apparatus for cancelling vibrations which employ frequency domain filtering. However, in each, for successful operation, either the vibrations to be cancelled must be periodic and the resolving into the frequency components synchronised to this periodicity, or, in the case where the vibrations are random (aperiodic), the resolving into the frequency components must be a continuously updated process.
  • According to the present invention there is provided an apparatus for cancelling vibrations comprising: means for providing a reference signal representative of the vibrations to be cancelled; filter means comprising means for resolving the reference signal into its frequency components, means for applying weights to these frequency components, and means for combining the weighted frequency components to provide an output signal of said filter means; and actuator means responsive to said output signal to produce vibrations which destructively interfere with the vibrations to be cancelled, said means for resolving utilising N updates of said reference signal to resolve it into its frequency components, said means for resolving being updated by n times between successive resolutions of the reference signal into its frequency components where 1<n<N, there being a correlation between the weights applied by said means for applying so as to reduce discontinuity in the operation of said filter means.
  • The invention arose in the making of an apparatus for cancelling vibrations employing frequency domain filtering. It was decided that block processing be used by the frequency domain filter to improve the processing efficiency of the apparatus, i.e. the filter would take a block of data, rather than just one sample, and process it all in one go to provide a number of sequential outputs. First trials of the apparatus were not successful, since it was found that in two cases the filter outputs were discontinuous, the first case being where the vibrations to be cancelled are periodic and the resolving into the frequency components not synchronised to this periodicity, the second case being where the vibrations are random. Even when attempting to cancel a pure tone not synchronised, in addition to the production of the cancelling tone, unwanted side bands were produced.
  • It was realised that a correlation could be introduced between the frequency domain filter weights that would greatly reduce the discontinuity of the filter outputs in the aforementioned two cases. Thus, contrary to that situation apparently the most desirable that there be complete freedom to adjust the weights independently to achieve the best cancellation of vibrations, regard must he had to observing the correlation between the weights, independent adjustment no longer being possible.
  • An apparatus for cancelling vibrations in accordance with the present invention will now be described, by way of example, with reference to the accompanying drawing which is a block schematic diagram of the apparatus.
  • The apparatus is for cancelling engine noise in an aircraft cabin.
  • Referring to the drawing, the apparatus includes a loudspeaker 1 located in the region of the aircraft cabin where it is desired that the noise produced by an engine 3 be cancelled. The loudspeaker 1 produces the aforementioned interfering anti-phase vibrations. The apparatus further includes an adaptive control filter 5, a model filter 7, a controller 9, updates modifying circuitry 10, an arithmetic circuit 12, and an error microphone 11, which microphone 11 is located in the aforementioned region of the aircraft cabin. Control filter 5 comprises a fast Fourier transform (FFT) circuit 13, a processor 15, and an inverse FFT circuit 17. Controller 9 comprises an FFT circuit 19 and a processor 21. Updates modifying circuitry 10 comprises an inverse FFT circuit 23, an arithmetic circuit 25, and an FFT circuit 27.
  • A reference signal x(t) representative of the noise to be cancelled at time t is supplied to control filter 5. This signal may be obtained from a microphone located in the aforementioned region of the aircraft cabin, or by means of a tachometer from the aircraft engine 3 itself.
  • FFT circuit 13 Fourier transforms x(t) from the time domain to the frequency domain and provides to processor 15 a plurality of frequency components xt(f) of x(t). Processor 15 multiplies each xt(f) by an appropriate weight (see below). Let the resulting frequency components be yt(f). Processor 15 provides the yt(f) to inverse FFT circuit 17. Circuit 17 inverse Fourier transforms the yt(f) from the frequency domain to the time domain to provide to loudspeaker 1 an appropriate driving signal y(t) to cancel the noise.
  • The weights utilised by processor 15 perform amongst other things, a phase inversion of x(t) to provide the interfering anti-phase signal. An explanation of the derivation of the weights utilised by processor 15 will now be given.
  • Error microphone 11 detects any residual noise remaining after interference between the primary noise produced by noise source 3 and the interfering sound produced by loudspeaker 1. A signal e(t) representative of this residual noise passes from microphone 11 to FFT circuit 19 of controller 9 where it is Fourier transformed from the time domain to the frequency domain. FFT circuit 19 provides to processor 21 a plurality of frequency components et(f) of e(t).
  • Returning to the frequency components xt(f) provided by FFT circuit 13, each of these components also passes to model filter 7, where it is multiplied by a frequency dependent function C(f). C(f) is the transfer function from loudspeaker 1 to microphone 11, and it is necessary that this function be involved in the derivation of the weights utilised by processor 15 to take account of the physical path from loudspeaker 1 to microphone 11 within the aircraft cabin. To explain, microphone 11 is detecting the residual noise at a different physical location within the aforementioned cabin region to the physical location where loudspeaker 1 is attempting to eliminate this residual noise. Thus, any attempt to eliminate the residual noise at one location by the generation of interfering sound at another different location must take into account the physical path travelled by the sound between the locations. C(f) is a previously determined transfer function which describes the change which the physical path within the cabin from loudspeaker 1 to microphone 11 will have on the passage of sound therealong.
  • The frequency components xt(f).C(f) resulting after multiplication by C(f) pass to processor 21 of controller 9, where each is multiplied by a respective frequency component et(f) from FFT circuit 19. The resulting frequency components or provisional filter updates xt(f).C(f).et(f) are supplied by processor 21 to updates modifying circuitry 10. After further processing by circuitry 10 (further details of which will be given later), the actual filter updates (xt(f). C(f). et(f))' are supplied to arithmetic circuit 12. Circuit 12 calculates the new weights for adaptive control filter 5 according to the equation: w t+1 (f) = w t (f) - α.(x t (f).C(f).e t (f))'
    Figure imgb0001
    where wt+1(f) is the new weight, wt(f) is the previous weight and α is a convergence coefficient. Circuit 12 passes the new weights to processor 15 of filter 5.
  • Thus, the weights utilised by filter 5 phase invert the reference representative of the noise, attempt to eliminate detected residual noise, and take into account the physical path from the actuator which produces the cancelling sound to the detector which detects residual noise.
  • For correct operation of the apparatus, the operation of filter 5 must take account of filter settling time, otherwise discontinuous filter outputs result.
  • Consider a conventional filter operating on running data, i.e. as each new data sample is taken in a new filtered output is calculated, the processing efficiency of such filters can be improved by the use of block processing, i.e. a block of data is taken and processed all in one go to provide a number of sequential outputs. A delay (the block update refresh time) is necessarily involved, but, if it can be tolerated, the advantage is greater processing efficiency.
  • To take a block of N data samples, if it is desired to obtain n<N accurate output data, account must be taken that any filtering operation requires the filter output to settle. If the filter is an m point or weight filter, then the first m-1 data outputs are inaccurate, and only once m data samples have been filtered does the output become accurate. Thus, to provide n valid data output after the filter has settled, it is required that (m-1)+n≦N
    Figure imgb0002
    , i.e. m≦N-n+1
    Figure imgb0003
    . Thus, the constraint m≦N-n+1
    Figure imgb0004
    must be observed by the filter to provide n valid data ouput. Let N=128 and n=32, then m≦97, i.e. the filter must have 97 or fewer weights.
  • Returning to filter 5, with regard to the previous values for N and n, let the size of the FFT performed by circuit 13 of filter 5 be 128 samples, i.e. each FFT performed by circuit 13 is performed on 128 samples of reference signal x(t). Thus, 64 complex frequency components xt(f) of x(t) are presented to processor 15 where each is multiplied by its respective weight wt(f). The resulting 64 complex frequency components yt(f) are passed to inverse FFT circuit 17 where they are inverse transformed to 128 'samples' of y(t). Let the number of samples of x(t) by which FFT circuit 13 is updated between the performance of successive FFTs be 32. Thus, at each update 32 samples of x(t) are taken by filter 5 and 32 samples of y(t) are provided by filter 5.
  • For filter 5 to provide n valid data output, it must observe the constraint m≦N-n+1
    Figure imgb0005
    . Since N = 128 and n = 32, m≦ 97. The constrained weights applied by filter 5 are obtained as follows.
  • The aforementioned provisional updates xt(f). C(f). et(f) are passed by processor 21 to inverse FFT circuit 23 of updates modifying circuitry 10, where they are inverse Fourier transformed from the frequency domain to the time domain to provide to arithmetic circuit 25 the equivalent 128 time domain updates. Arithmetic circuit 25 sets to zero the last 31 (128 - 97) of these 128 updates so as to effectively leave 97 updates for a 97 weight filter. Note, it is the last 31 updates that are set to zero since it is the 97th (mth) data output that is the first accurate data output, see above. Note also, that N-m or N-(N-n+1)
    Figure imgb0006
    (taking the limit where the least updates are set to zero giving the greatest flexibility for filter 5) or n-1 updates are set to zero. The resulting updates are passed to FFT circuit 27 where they are Fourier transformed from the time domain to the frequency domain to provide to arithmetic circuit 12 the actual constrained frequency domain updates (xt(f). C(f). et(f))'. Circuit 12 calculates the new constrained weights according to equation (1). Thus, it will be seen that a correlation has been introduced between the weights of filter 5, i.e. it is now a necessary requirement that the weights of filter 5 are not adjusted independently to achieve the best cancellation of noise - when adjusting one weight regard must be had to other weights.
  • There are three conditions which relate to the aforementioned m≦N-n+1
    Figure imgb0007
    constraint which require special consideration. The three conditions will be considered respectively in the following three paragraphs.
  • Consider the m≦N-n+1
    Figure imgb0008
    constraint when n = 1, i.e. a running, continuously updated filter, then m≦N, i.e. m is permitted to equal N, therefore there is no constraint - no updates need be set to zero for successful operation.
  • Consider the FFT process performed by FFT circuit 13 of the apparatus, the FFT process effectively assumes periodic behaviour, i.e. it fits a set of periodic functions to the data samples on the assumption that the data is periodic outside the N sample block. Thus, if the data is indeed truly periodic on the block length, the FFT process will always be accurate without the need to observe the m≦N-n+1
    Figure imgb0009
    constraint. Therefore, when the vibrations to be cancelled are periodic, and the resolving of the reference signal representative of these vibrations into its frequency components is synchronised to this periodicity, then constraint for successful operation is not required. In all other circumstances, i.e. when the data is periodic and there is no synchronisation, or when the data is random, constraint for successful operation is required -unless, of course, as explained above (see previous paragraph), the resolving into the frequency components is a continuously updated process, when no constraint is required.
  • Consider the m≦N-n+1
    Figure imgb0010
    constraint when n = N, i.e. the number of samples by which FFT circuit 13 is updated between successive Fourier transformations equals the size of the FFT performed by circuit 13, then m = 1, i.e. all the updates apart from the first must be set to zero. Such a severe constraint results in a filter which is of very little use at all, and the consequent requirement is that the data must be constrained instead to be periodic on the length scale N of the FFT.
  • Thus, for block processing (and its associated advantages), n is greater than 1 and constraint for correct operation is required (unless the data is periodic and synchronised). However, when n = N the constraint is so severe that for useful operation the data must be periodic and synchronised, i.e. useful operation is not possible when the data is random and n = N. Therefore, in the limit, the range 1<n<N remains.
  • The choice of the precise update to use in the range 1<n<N depends on the nature of the vibrations to be cancelled. If the vibrations are in the main random, then it is best to choose n from the lower end of the range, i.e. the end approaching 1, since the updating is then sufficiently fast to manage the rapidly changing random vibrations. There is, of course, a consequent penalty in processing efficiency. If the vibrations are in the main narrow band or tonal, i.e. comprise a series of reasonably discrete frequencies which, if they change, change only slowly, then n may be chosen from the upper end of the range, i.e. the end approaching N, with a consequent benefit in processing efficiency. Of course, if the change in discrete frequencies occurs more quickly, then, in effect, random noise is approached, and a lower value of n must be chosen. A further factor affecting the choice of n is, of course, the flexibility required in the choice of weights for the filter - as explained above, the larger n the greater the constraint on the filter weights.
  • It is to be appreciated that the process of inverse Fourier transformation, truncation, and Fourier transformation performed by updates modifying circuitry 10 could be approximated by a simpler convolution operation performed entirely in the frequency domain. Arithmetic circuit 25 of circuitry 10 uses a 97 point truncation step-function, i.e. points 1 to 97 = 1 and points 98 to 128 = 0. However the disadvantage is that the corresponding convolution window involves complex, asymmetric coefficients. Yet, if there were to be used a reduced 64 point truncation step-function, i.e. points 1 to 64 = 1 and points 65 to 128 = 0 (note, the m≦N-n+1
    Figure imgb0011
    constraint is still observed), the advantage would be that the corresponding convolution window is symmetric, and a simple 5-point convolution would suffice.
  • It is also to be appreciated that the resolving of the reference signal into its frequency components need not be by means of Fourier transformation, for example frequency sampling filtering could be used.

Claims (6)

  1. An apparatus for cancelling vibrations comprising: means for providing a reference signal representative of the vibrations to be cancelled; filter means (5) comprising means (13) for resolving the reference signal into its frequency components, means (15) for applying weights to these frequency components, and means (17) for combining the weighted frequency components to provide an output signal of said filter means (5); and actuator means (1) responsive to said output signal to produce vibrations which destructively interfere with the vibrations to be cancelled, said means (13) for resolving utilising N updates of said reference signal to resolve it into its frequency components, said means (13) for resolving being updated by n times between successive resolutions of the reference signal into its frequency components where 1<n<N, there being a correlation between the weights applied by said means (15) for applying so as to reduce discontinuity in the operation of said filter means (5).
  2. An apparatus according to claim 1 wherein: said means (13) for resolving comprises first Fourier transform means (13); and said means (17) for combining comprises first inverse Fourier transform means (17).
  3. An apparatus according to claim 2 further comprising: means (11, 9, 7) for deriving provisional updates to said weights applied by said means (15) for applying; means (10) for modifying said provisional updates to provide actual updates; and means (12) for utilising the actual updates to calculate the weights applied by said means (15) for applying, said correlation between the weights applied by said means (15) for applying being introduced by the modification carried out by said means (10) for modifying.
  4. An apparatus according to claim 3 wherein said means (10) for modifying comprises: second inverse Fourier transform means (23) for transforming said provisional updates from the frequency domain to the time domain to provide the equivalent time domain updates; means (25) for setting to zero substantially the last n-1 updates of said time domain updates; and second Fourier transform means (27) for transforming the resultant updates from the time domain to the frequency domain to provide said actual updates.
  5. An apparatus according to claim 3 wherein the modification carried out by said means (10) for modifying comprises a convolution operation in the frequency domain.
  6. An apparatus according to claim 3 or claim 4 or claim 5 wherein: said means (11, 9, 7) for deriving provisional updates comprises detector means (11) for detecting any residual vibrations remaining after said destructive interference and providing an output signal representative thereof, further Fourier transform means (19) for transforming the output signal of said detector means (11) from the time domain to the frequency domain thereby to resolve the signal into its frequency components, model filter means (7) for multiplying the frequency components of said reference signal by a frequency dependent function which is a transfer function from said actuator means (1) to said detector means (11) thereby to provide modelled frequency components, and means (21) for multiplying said modelled frequency components by the frequency components of the output signal of said detector means (11) to provide said provisional updates; and said means (12) for utilising the actual updates calculates said weights applied using the equation: w t+1 (f) = w t (f) - α.(x t (f).C(f).e t (f))'
    Figure imgb0012
    , where wt+1(f) are the calculated weights, wt(f) are the previous weights, α is a convergence coefficient, and (xt(f). C(f). et(f))' are said actual updates where xt(f) are the frequency components of the reference signal, C(f) is said transfer function; and et(f) are the frequency components of the output signal of the detector means (11).
EP95304332A 1994-07-18 1995-06-21 An apparatus for cancelling vibrations Ceased EP0693747A3 (en)

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
GB9414484A GB9414484D0 (en) 1994-07-18 1994-07-18 An apparatus for cancelling vibrations
GB9414484 1994-07-18
GB9415763A GB2291559B (en) 1994-07-18 1994-08-04 An apparatus for cancelling vibrations
GB9415763 1994-08-04

Publications (2)

Publication Number Publication Date
EP0693747A2 true EP0693747A2 (en) 1996-01-24
EP0693747A3 EP0693747A3 (en) 1997-12-29

Family

ID=26305292

Family Applications (1)

Application Number Title Priority Date Filing Date
EP95304332A Ceased EP0693747A3 (en) 1994-07-18 1995-06-21 An apparatus for cancelling vibrations

Country Status (3)

Country Link
EP (1) EP0693747A3 (en)
JP (1) JPH0883086A (en)
CA (1) CA2154027A1 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112066909A (en) * 2020-08-24 2020-12-11 南京理工大学 Anti-vibration interference measurement method based on inclined plane high-precision extraction

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2054999A (en) 1979-06-28 1981-02-18 Nat Res Dev Signal Processing Systems
EP0043565A1 (en) 1980-07-03 1982-01-13 Hitachi, Ltd. Vibration/noise reduction device for electrical apparatus
GB2107960A (en) 1981-10-21 1983-05-05 George Brian Barrie Chaplin Method and apparatus for cancelling vibrations

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0288577B1 (en) * 1986-10-30 1992-06-03 Fujitsu Limited Echo canceller with short processing delay and decreased multiplication number and method for controlling an echo signal
GB8801014D0 (en) * 1988-01-18 1988-02-17 British Telecomm Noise reduction
US5233540A (en) * 1990-08-30 1993-08-03 The Boeing Company Method and apparatus for actively reducing repetitive vibrations
US5309378A (en) * 1991-11-18 1994-05-03 Hughes Aircraft Company Multi-channel adaptive canceler
GB9222103D0 (en) * 1992-10-21 1992-12-02 Lotus Car Adaptive control system

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2054999A (en) 1979-06-28 1981-02-18 Nat Res Dev Signal Processing Systems
EP0043565A1 (en) 1980-07-03 1982-01-13 Hitachi, Ltd. Vibration/noise reduction device for electrical apparatus
GB2107960A (en) 1981-10-21 1983-05-05 George Brian Barrie Chaplin Method and apparatus for cancelling vibrations

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112066909A (en) * 2020-08-24 2020-12-11 南京理工大学 Anti-vibration interference measurement method based on inclined plane high-precision extraction

Also Published As

Publication number Publication date
EP0693747A3 (en) 1997-12-29
JPH0883086A (en) 1996-03-26
CA2154027A1 (en) 1996-01-19

Similar Documents

Publication Publication Date Title
US5838802A (en) Apparatus for cancelling vibrations
JP2889114B2 (en) Active noise canceller
KR950005181B1 (en) Adaptive active noise cancellation apparatus
US4490841A (en) Method and apparatus for cancelling vibrations
US5365594A (en) Active sound and/or vibration control
Kuo et al. Frequency-domain delayless active sound quality control algorithm
KR0164236B1 (en) Non-integer sample delay active noise canceller
EP0724415A1 (en) Single and multiple channel block adaptive methods and apparatus for active sound and vibration control
CN105679304B (en) Variable bandwidth non-delay sub-band algorithm for broadband active noise control system
GB2149614A (en) Active noise reduction apparatus
CN110718205B (en) Active noise control system without secondary path and implementation method
Kuo et al. Frequency-domain periodic active noise control and equalization
JPH05501488A (en) In-wire selection erasure system
DE69513849T2 (en) REDUCTION OF THE CALCULATION LOAD IN THE ADAPTIVE UPDATE OF CONTROL FILTERS IN ACTIVE SYSTEMS
Pauline et al. Variable-stage cascaded adaptive filter technique for signal de-noising application
EP0693747A2 (en) An apparatus for cancelling vibrations
JP3646809B2 (en) Time domain adaptive control system
EP0805432A2 (en) Feedback method of noise control having multiple inputs and ouputs
JPH0651787A (en) Active silencer
EP0694234B1 (en) Control system for periodic disturbances
JPH05313672A (en) Noise controller
JPH0973295A (en) Active control device
DE69231855T2 (en) CHEAP REGULATOR
Karna et al. Delayless Identification in ANC Systems Using Subbband Adaptive Techniques
JP3273051B2 (en) Active noise control device and adaptive noise control method

Legal Events

Date Code Title Description
PUAI Public reference made under article 153(3) epc to a published international application that has entered the european phase

Free format text: ORIGINAL CODE: 0009012

AK Designated contracting states

Kind code of ref document: A2

Designated state(s): DE ES FR GB IT NL SE

PUAL Search report despatched

Free format text: ORIGINAL CODE: 0009013

AK Designated contracting states

Kind code of ref document: A3

Designated state(s): DE ES FR GB IT NL SE

17P Request for examination filed

Effective date: 19980625

RAP1 Party data changed (applicant data changed or rights of an application transferred)

Owner name: BAE SYSTEMS ELECTRONICS LTD.

GRAG Despatch of communication of intention to grant

Free format text: ORIGINAL CODE: EPIDOS AGRA

17Q First examination report despatched

Effective date: 20020128

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: THE APPLICATION HAS BEEN REFUSED

18R Application refused

Effective date: 20020725