CA2154027A1 - Apparatus for cancelling vibration - Google Patents

Apparatus for cancelling vibration

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Publication number
CA2154027A1
CA2154027A1 CA002154027A CA2154027A CA2154027A1 CA 2154027 A1 CA2154027 A1 CA 2154027A1 CA 002154027 A CA002154027 A CA 002154027A CA 2154027 A CA2154027 A CA 2154027A CA 2154027 A1 CA2154027 A1 CA 2154027A1
Authority
CA
Canada
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.)
Abandoned
Application number
CA002154027A
Other languages
French (fr)
Inventor
Malcolm 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
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 filed Critical GEC Marconi Ltd
Publication of CA2154027A1 publication Critical patent/CA2154027A1/en
Abandoned legal-status Critical Current

Links

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

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

21~027 P/60236/FAF ~ A

An apparatus for cancelling vibrations 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, ~ fiately 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, EP43565-A1, and GB-2107960-A disclose examples of apl,ara.us 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 lltili~ing 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 l<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 Ihe 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 be had to observing the correlation between the weights, independent adjustment no longer being possible.
An al,p~us 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 (~ l ) circuit 13, a processor 15, and an inverse ~ l circuit 17. Controller 9 comprises an FFT circuit 19 and a processor 21. Updates modifying circuitry 10 comprises an inverse ~ l circuit 23, an arithmetic circuit 25, and an FFr 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.
~ `~ l 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,(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 ~l circuit 17. Circuit 17 inverse Fourier transforms the y,(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 21~4027 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 rem~inin~ 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 ~ l` circuit 19 of controller 9 where it is Fourier transformed from the time domain to the frequency domain. ~ l` circuit 19 provides to processor 21 a plurality of frequency components et(f) of e(t).
Retllrning to the frequency components x,(f) provided by ~ l` 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 Plimin~te this residual noise. Thus, any aKempt to elimin~tP 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 rnicrophone 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 FFI circuit 19. The resulting frequency components or provisional filter updates x,(f).C(f).e,(f) are supplied by processor 21 to updates modifying circuitry 10. After further 21~2~

processing by circuitry 10 (further details of which will be given later), the actual filter updates (x,(f). C(f). et(f))' are supplied to ~ "~k~ic circuit 12. Circuit 12 calculates the new weights for adaptive control filter 5 according to the e~uation:
wt+l(f) = w,(f) - a.(Xt(f).c(f).et(f))~ (1), where wt+,(f) is the new weight, wt(f) is the previous weight and a 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 elimin~te cletect~d 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-l 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-l)+n<N, i.e. m<N-n+l. Thus, the constraint m<N-n+l 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 S, with regard to the previous values for N and n, let the size of the 2 1 5 ~ 7 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 x,(f) of x(t) are presented to processor 15 where each is multiplied by its respective weight w,(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 l~ l circuit 13 is updated between the performance of successive ~-l`s 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 mcN-n+1. Since N = 128 and n = 321 m< 97. The constrained weights applied by filter S are obtained as follows.
The aforementioned provisional updates x,(f). C(f). et(f) are passed by processor 21 to inverse ~-l circuit 23 of updates modifying ciL~ ilry 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. ~rithm~tic 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) (taking the limit where the least updates are set to zero giving the greatest flexibility for filter S) or n- 1 updates are set to zero.
The resulting updates are passed to ~ l 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,(f). C(f). e,(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 - ~ 1 S 4 0 2 ~

regard must be had to other weights.
There are three conditions which relate to the aforementioned m<N-n+1 constraint which require special consideration. The three conditions will be considered respectively in the following three paragraphs.
Consider the m<N-n+l 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 ~ l process performed by ~ l` circuit 13 of the apparatus, the ~1 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+l 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+l 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.

' 2l~n27 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 l<n<N remains.
The choice of the precise update to use in the range l<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 ch~n~;ing 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 quickiy, 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 constraint is still observed), the advantage would be that the corresponding convolution window is symmetric, and a simple S-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 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 l<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.
2. An apparatus according to claim 1 wherein: said means for resolving comprises first Fourier transform means; and said means for combining comprises first inverse Fourier transform means.
3. An apparatus according to claim 2 further comprising: means for deriving provisional updates to said weights applied by said means for applying; means for modifying said provisional updates to provide actual updates; and means for utilising the actual updates to calculate the weights applied by said means for applying, said correlation between the weights applied by said means for applying being introduced by the modification carried out by said means for modifying
4 An apparatus according to claim 3 wherein said means for modifying comprises: second inverse Fourier transform means for transforming said provisional updates from the frequency domain to the time domain to provide the equivalent time domain updates; means for setting to zero substantially the last n-1 updates of said time domain updates; and second Fourier transform means 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 for modifying comprises a convolution operation in the frequency domain.
6. An apparatus according to claim 3 wherein: said means for deriving provisional updates comprises detector means for detecting any residual vibrations remaining after said destructive interference and providing an output signal representative thereof, further Fourier transform means for transforming the output signal of said detector means from the time domain to the frequency domain thereby to resolve the signal into its frequency components, model filter means for multiplying the frequency components of said reference signal by a frequency dependent function which is a transfer function from said actuator means to said detector means thereby to provide modelled frequency components, and means for multiplying said modelled frequency components by the frequency components of the output signal of said detector means to provide said provisional updates;
and said means for utilising the actual updates calculates said weights applied using the equation:
wt+1(f) = wt(f) - .alpha..(xt(f) C(f).et(f))' , where wt+1(f) are the calculated weights, wt(f) are the previous weights, .alpha. 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.
CA002154027A 1994-07-18 1995-07-17 Apparatus for cancelling vibration Abandoned CA2154027A1 (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
GB9414484.7 1994-07-18
GB9415763.3 1994-08-04
GB9415763A GB2291559B (en) 1994-07-18 1994-08-04 An apparatus for cancelling vibrations

Publications (1)

Publication Number Publication Date
CA2154027A1 true CA2154027A1 (en) 1996-01-19

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CA002154027A Abandoned CA2154027A1 (en) 1994-07-18 1995-07-17 Apparatus for cancelling vibration

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

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