GB2201858A - Active noise control - Google Patents

Active noise control Download PDF

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Publication number
GB2201858A
GB2201858A GB08630422A GB8630422A GB2201858A GB 2201858 A GB2201858 A GB 2201858A GB 08630422 A GB08630422 A GB 08630422A GB 8630422 A GB8630422 A GB 8630422A GB 2201858 A GB2201858 A GB 2201858A
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Prior art keywords
reference signal
sound
frequency
engine
filter
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GB08630422A
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GB8630422D0 (en
Inventor
Stephen John Elliott
Philip Arthur Nelson
Ian Mcgregor Stothers
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Adaptive Control Ltd
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Adaptive Control Ltd
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Application filed by Adaptive Control Ltd filed Critical Adaptive Control Ltd
Publication of GB8630422D0 publication Critical patent/GB8630422D0/en
Priority to PCT/GB1987/000706 priority Critical patent/WO1988002912A1/en
Priority to EP87906587A priority patent/EP0285632B1/en
Priority to JP62505958A priority patent/JP2890196B2/en
Priority to KR1019880700638A priority patent/KR960011152B1/en
Priority to DE87906587T priority patent/DE3786165T2/en
Publication of GB2201858A publication Critical patent/GB2201858A/en
Priority to US07/448,517 priority patent/US5170433A/en
Withdrawn legal-status Critical Current

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    • 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
    • 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
    • G10K11/17821Methods 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 input signals only
    • G10K11/17823Reference signals, e.g. ambient acoustic environment
    • 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
    • G10K11/17883General 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
    • G10K2210/1282Automobiles
    • 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
    • G10K2210/3023Estimation of noise, e.g. on error signals
    • G10K2210/30232Transfer functions, e.g. impulse response
    • 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
    • G10K2210/3032Harmonics or sub-harmonics
    • 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
    • G10K2210/3046Multiple acoustic inputs, multiple acoustic outputs
    • 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
    • G10K2210/3048Pretraining, e.g. to identify transfer functions
    • 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
    • G10K2210/3049Random noise used, e.g. in model identification
    • 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
    • G10K2210/321Physical
    • G10K2210/3212Actuator details, e.g. composition or microstructure

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Acoustics & Sound (AREA)
  • Multimedia (AREA)
  • Soundproofing, Sound Blocking, And Sound Damping (AREA)
  • Vibration Prevention Devices (AREA)
  • Fittings On The Vehicle Exterior For Carrying Loads, And Devices For Holding Or Mounting Articles (AREA)

Abstract

To reduce noise inside a motor car passenger compartment, two loudspeakers 371, 372 are driven by signals derived from a reference signal x(n) by adaptive filtering carried out by a programmed microprocessor and memory unit 36 which adapts the filtering in dependence on error signals el(n) from four microphones 421, 422, 423 and 424 distributed in the passenger compartment. Reference filtering coefficients are initially determined by analysis of finite impulse responses when white noise is acoustically coupled from the loudspeakers 37 to the microphones 42, a white noise generator 48 being coupled to the unit 36. The reference signal x(n) is restricted to one or more selected harmonics or subharmonics of the fundamental noise frequency by a filter 34 which tracks the selected frequency. The selected frequency may be obtained from a coil 31 in the ignition circuit. <IMAGE>

Description

ACTIVE NOISE CONTROL The invention relates to active noise control.
In passenger compartments of cars, where a significant noise component is harmonically related to the rotation frequency of a reciprocating engine. The sound levels at low frequencies in such enclosures are difficult to attenuate using conventional passive methods and can give rise to subjectively annoying "boom". A method of actively attenuating a simple sound filed by introducing a single.
secondary sound source driven so that its output is in antiphase with the original ambient noise is described in general terms by B.
Chaplin in "The Chartered Mechanical Engineer" of January 1983, at pages 41 to 47. Other discussions are to be found in an article entitled "Active Attenuation of Noise-The State of the Art" by Glenn E. Warnaka at pages 100 to 110 in Noise Control Engineering, May June 1982 and in Internoise 83 Proceedings, sages 457 to 458 and 461 to 464, and Internoise 84 Proceedings, pages 483 to 488. Particular methods and apparatus are also described in British specifications nos. 1 577 322 and 2 149 614.
According to the present invention there is provided an active noise control system for reducing sound or vibration generated by a primary source, in which at least one reference signal containing selected harmonics or subharmonics of the said sound or vibration is supplied to means driving a plurality of secondary sources, such that the sound or vibration energy detected by sensor means arranged to sense the sound or vibration field established by the primary and secondary sources is reduced.
Preferably the system is adapted to operate in accordance with an algorithm which adjusts the outputs from the secondary sources so as to minimise a cost function on a time scale comparable with the delays associated with the propagation of the sound or vibration from the secondary sources to the sensor means.
The present invention is concerned particularly with an active noise reduction system which can control the sound throughout an enclosure, or at one or a number of 'quiet zones' within it, and which can quickly adapt to changes in the excitation of the sound field due to changes in for example, engine load or speed. In order to ensure that the sound produced by the secondary sources is of the same frequency as that produced by the engine, a signal related to the rotation rate, for example that used in the ignitions system, is used to generate a reference signal containing a number of sinusoids at harmonics or subharmonics of the basic engine rotation frequency.
These are known as engine order frequencies. These sinusoids may be obtained using a variety of methods outlined below. Rather than attempt to control all harmonics, only a selected set of engine order frequencies may, in accordance with the invention, be generated as the reference signal. For example, only the firing frequency (second engine order in a four cylinder car) and its second harmonic (fourth engine order) are used if the spectrum of the sound in the car is dominated by these components.
Alternatively, a signal containing all the engine order frequencies may be fed to a band pass filter which isolates only the particular frequency or frequencies exciting a particular resonance in the interior which could cause a "boom" to be excited. The advantage of reducing the number of frequencies fed to the controller is that an adaptive filter having fewer coefficients than would otherwise be the case can be used. This makes implementation more efficient and allows faster adaption time. The faster adaption time is particularly important in automotive applications, for example, in which the active control system has to adapt sufficiently quickly to track changes in engine speed which may occur on a very short timescale.
Other reference signals may be obtained from transducers on a wheel hub or the suspension of a vehicle to which the invention is applied. Such reference signals would contain the harmonics of wheel rotation or road noise. Transducers placed outside a vehicle may provide reference signals rep-resentative of wind noise.
Reference signals from such source may be broad band (random), in which case these reference signals may be fed directly to adaptive fitters as described hereinafter. Alternatively, if the reference signals are periodic (deterministic), control at individual harmonics can be exercised as described hereinafter.
When the enclosed space is a motor vehicle interior, the secondary sources may be loudspeakers used as the low frequency drives of a car audio system.
Examples of methods in accordance with the invention for generating the reference signals from a signal from an internal combustion engine are now discussed.
1. Selection of harmonics by filtering.
A signal is obtained from the primary source which contains components at all harmonics and subharmonics which are prevalent in the sound in a vehicle powered by the engine. This is filtered so as only to leave the most important or dominant harmonics or subharmonics. This filtering is carried out with a filter whose centre frequency can be controlled by an external signal in such a manner that the critical filter frequencies have a constant ratio compared with the engine rotation rate. This can be achieved by using, for example, charge coupled devices whose switching frequency is locked to the rotation frequency, but can also be implemented as a program running on a microprocessor, as described hereinafter.
2. Selection of harmonics or subharmonics within a band by fixed fltering.
A signal rich in harmonics and subharmonics is filtered by a band pass filter, having a centre frequency fixed at that of a pronounced "boom" in the car enclosure and a characteristic such that the reference signal only contains the harmonic(s) or subharmonic(s) which are particularly exciting the boom. This may be extended such that the filter contains a number of resonances at a number of boom frequencies of the car, or even such that the filter has a frequency response which models the acoustic response of the car interior to the primary excitation. The input signal to the filter may be a signal from the engine containing all important harmonics and subharmonics and may be in the form of a pulse train.
3. Generation of specific harmonics or subharmonics locked to the engine rotation frequency.
This method may be accomplished by using phase lock loops to generate sinusoidal signals, with frequencies bearing an integer relationship to a square wave signal from the engine, which are then added together to form the reference signal. Alternatively the signal from the engine can be used to control a number of tunable oscillators, each producing a sinusoid at a selected harmonic or subharmonic frequency.In one arrangement for such a bank of tunable oscillators, the period of the square wave signal at the engine rotation rate is measured with a counter passed to a microprocessor which implements a number of digital oscillators using difference equations of the form x1(n) = 6(n) + 2 cos(IwO)xI(n - 1) - xI(n - 2) where #o= 2gfC/Nfs, I is the order of the harmonic or subharmonic to be generated, fc fc is the frequency of the counter, which counts N pulses during a period, and fs is the sample rate used for the difference equation. # (n) is a unit sample sequence to initiate the oscillators formed by the difference equations above. The second and fourth harmonic may be generated for example.
It is advantageous if the sample frequency (fs) is derived from the counter frequency (fc) by a frequency division circuit for example, so that the ratio fs/fc is exactly an integer number.
An alternative difference equation which may be used to implement the digital oscillator has the form of a series approximation to a trigonometric function, for example: y2 y4 y6 y8 xI(n) = 1 - -- + -- - -- + -- #cos(y) 2! 4! 6! 8! The variable y is the accumulated phase of the oscillator, given by n y(n) = # #i(n) i=O #i(n) = I#o where wo is calculated from the measured period of the reference signal, as above, for every new sample (n). The series approximation above can be used for y(n) in the range -E/2 ( y(n) < For For values of y(n) outside this range the symmetry properties of the cosine waveform are utilised, until y(n) ? Tr. When y(n) > the natural overflow properties of the two's complement number representation is used to allow y(n) to 'wrap-around' to y(n) # and the series expansions and symmetry properties discussed above are again used. In this way the digital representation of y(n) is kept within the range - Tr < y(n) < #, and xI(n) is within the range + 1.
The calculations of the coefficients used in the difference equations forming the digital oscillators, together with the difference equations themselves may be implemented on a dedicated processor, or may form part of the program which also implements a controller that generates the outputs used to drive the secondary sources from the reference signals described above.
The controller is designed to be adaptive so as to quickly track changes in engine speed and load. The outputs of the secondary sources are adaptively controlled so that some measurable cost function in minimised. This cost function would typically be the sum of the mean square outputs from a number of microphones in the enclosed space. The controller can be implemented as a digital adaptive FIR filter, using the basic update algorithm described by S. Elliott and P. Nelson in "Electronics Letters", at pp. 979-981, 1985. A number of additions must be made to this basic algorithm, however, to enable it to work quickly and efficiently in this particular example. The basic algorithm, refered to hereinafter as the stochastic gradient algorithm, is presented below, in order to highlight the necessary alterations.If the i'th coefficient of the adaptive filter driving the m'th secondary source at sample number n is wmi(n), then each of these coefficients should be adjusted at every sample according to the equation
where ais a convergence coefficient, eg(n) is the sampled output from the Q'th sensor and rum(") is a sequence formed by filtering the reference signal discussed above (x(n), say) with a digital filter which models the response of the Q'th sensor to excitation of the m'th secondary source. These digital filters, generating each rQm(n), have only two coefficients in the implementation described in the 'Electronic Letters' article, since control at only a single, fixed, frequency was being attempted.In the present example, however, these filters must model the relevant response over a range of frequencies, governed by the frequency range which the active system is attempting to control. It has been found that under certain circumstances this filter need only model the overall delay in the response to ensure the stability of the adaptive filter. It is more common, however, to have these filters incorporating a delay and then some reverberant response. This may be implemented using either digital FIR or IIR filters whose coefficients are adjusted adaptively during an initialisation phase, so as to accurately match the desired responses.It is also possible.to continue this initial adaption process during the operation of the active control system by feeding training signals to each secondary source which are suitably uncorrelated with each other and with the primary excitation. This may be necessary to track changes in the acoustic response of the enclosure. Alternatively if the change is due to some well-defined cause, such as a passenger sitting down or a window being opened, this change may be detected with mechanical transducers and the information used to switch between a variety of filters modelling the response of the enclosure under a variety of conditions.
Another important consideration concerning the use of adaptive algorithm in this example concerns the effect of unwanted, low level, harmonic or subharmonic components in the reference signal.
Suppose that the method used to generate the reference signal, as described above, is designed to produce only I frequencies. Even though there may only be I desired harmonics in such a system, there will in practice also be a number of other harmonics or subharmonic frequencies at low level, because of the finite cut-off rate of the filters, for example. These components may also be being generated by the primary source and therefore present in the enclosure and hence at the outputs of sensors such as microphones and thus the adaptive algorithm will attempt to cancel them by enormously amplifying the low level, spurious harmonic reference signals. This can cause numerical overflow problems in the adaptive filter coefficients. This may be prevented in a number of ways: (1) The use of only 2.I coefficients in the adaptive filter.
(2) The deliberate injection of random noise into the reference signal.
(3) The insertion of a 'leak' into the algorithm so that, in the equation above, the past coefficient value, wmi (n), is multiplied by a factor close to but not equal to unity before being updated.
(4) The addition of an extra term in the update equation which minimises a cost function involving 'effort' as well as 'error', as described in ISVR Technical Report No. 136, 1985, published by the Institute of Sound and Vibration Research at the University of Southampton.
A number of other adaptive algorithms may also be implemented to.
adjust the coefficients of the digital filters in the controller driving the secondary sources. These alternative algorithms are best described in matrix form.
Assuming the availability of a sampled reference signal, x(n), which is correlated with the output of the primary source, but is unaffected by the action of the secondary sources. The output to the m'th secondary sources, ym(n), may be obtained by passing this reference signal through a digital filter whose i'th coefficient is Yni(n) at the n'th sample, so that
The sampled output from the P'th error sensor, ef(n), is equal to the sum of the contributions from the primary source, dl(n), and each of the secondary sources. The response of the path between the m'th secondary source and P'th error sensor is modelled as a Jth order FIR filter with coefficients cemj so that
Therefore
In order to obtain a matrix expression for the error surface we must now make the assumption that the filter coefficients in the controller are time invariant, i.e., the controller only adapts very slowly compared to the time scale of the response of the system to be controlled.Then wmi(n - j) = wmi and
If we let
where the sequences r@m(n) for each 1 and m are called the filtered reference signals1 then
or e#(n) = d#(n) + r#T(n)w 'where r#T(n) = [r#1(n) r#1(n-1) ... r#@(n-I+1) r#2(n) ...I#2(n-I+1) r#3(n) ... r#M(n) ... r#M(n-I+1) wT = [w10 w11 w1I-1 w20 w2I-1 w30 ... wMo wMI-1] So if eT(n) = [e@(n) e2(n) ... eL(n)] dT(n) = [d@(n) d2(n) ... dL(n)] then e(n) = d(n) + R(n)w where RT(n) = [r@ (n) r2 (n) ... rL (n)] If the cost function is written as
Where E is the expectation operator, then J = E(dT(n)d(n)) + 2wTE(RT(n)d(n)) + wTE(RT(n)R(n)w Using the standard theory of matrix quadratic forms, the minimum of J, Jmin, is obtained with wopt = -A-1b = -E(RT(n)R(n))-1E(RT(n)d(n)) giving Jmin = c - bTA-1b = E(dT(n)d(n)) - E(dT(n)R(n))E(RT(n)R(n))-1E(RT(n)d(n)) The true gradient may be written #J = 2E(RT(n) d(n) + RT(n) R(n) w(n)} #w #J #w= 2E(RT(n) e(n)} The time domain steepest descent algorithm may thus be written as wk+1 = wk - 2 E(RT(n) e(n)) In a practical implementation the true expectation could be approximated by an MA or AR averaging process.Alternatively the instantaneous gradient could be used to update each filter coefficient every sample, as in the time domain "stochastic gradient" algorithm w(n + 1) = w(n) - 2 RT(n) e(n), which is the matrix representation of the algorithm described above.
It is clear from this formulation that the stability and convergence properties of this algorithm, in the limit of slow adaption, are governed by the eigenvalue spread of the matrix E(RT(n) R(n)). This matrix depends only on the response of the system to be controlled, the positioning of the sources and sensors within that system and the spectral properties of the reference signal, x(n). It is possible that an unfortunate placing of these sources and sensors could cause this matrix to become ill conditioned, so that it has a large eigenvalue spread. This would create very slow "modes" in the convergence properties of such an algorithm.
This problem could be removed by using a Newton's method algorithm, the exact form of which may be written as wk+1 = wk - 2 E((RT(n) R(n))-1E(RT(n) e(n)) Again, various types of averaging could be used to give a practical approximation to the expectation operator. It should be noted however that the time-independent matrix E(RT(n) R(n)) depends only on the response of the system to be controlled and on the reference signal, and these are assumed to be known and stationary. This suggests a variety of stochastic Newton's method ("SNM") algorithms. The most obvious of these uses a modified or "normalised" set of reference signals Q(n), such that E([RT(n) R(n)])-1 RT(n) = OT(n).
The computation of each of these reference signals will take somewhat longer than for R(n) alone since none of the elements of Q(n) are necessarily time delayed versions of any other elements. The complete S & algorithm, again using instantaneous versions of E(RT(n) e(n)), becomes wn+1 = wn - 2 OT(n) e(n).
The invention will now be described by way of example with reference to the accompanying drawings, in which: Fig. 1 is a block schematic diagram of an active sound control apparatus for an enclosed space, Fig. 2(a), (b) and (c) are graphical representations of the behaviour of an element of an apparatus embodying the invention, Fig. 3 is a block diagram of a reference signal generator for an apparatus embodying the invention, Fig. 4 is a block diagram of another reference signal generator for an apparatus embodying the invention, and Fig. 5 is a block diagram of a microprocessor-based apparatus embodying the invention, Fig. 6 is a block diagram of part of an embodiment in which two reference signals are combined, Fig. 7 is a flow chart illustrating processing in a further embodiment of the invention, and Fig. 8 is a schematic diagram of a heterodyne and averaging method of obtaining inphase and quadrature components of an error sequence in another embodiment of the invention.
In Fig. 1 an enclosure 10, which may be the interior of the passenger or driver compartment of an internal combustion engine driven vehicle, for example a motor car, is represented schematically together with an active sound control apparatus embodying the invention and having in this example two secondary sound sources 11, which may be two low frequency loudspeakers of a car stereo audio system, and three microphones 12. The secondary sources 11 are driven by a controller circuit3 which comprises a plurality of adaptive filters 14. Each adaptive filter 14 drives a respective one of the secondary sources 11 with an output signal which the filter 14 produces as a result of its action on a reference signal supplied thereto by a reference signal generator 15.The reference signal is generated by the generator 15 from an input signal 16 which is periodic at the rotation rate or the firing rate of the internal combustion engine (not shown).
The purpose of the output from the secondary sources 11 driven by the controller 13 is to reduce the sound level, due to the internal combustion engine, within the enclosure 10. Since the primary source of the sound to be reduced is periodic, the reference signal generated by the generator 15 is, in accordance with the invention, arranged to contain one or more sinusoidal components at harmonics or subharmonics of the rotation or firing rate of the engine, and the adaptive filters are adjusted automatically by signals from the microphones 12, the adjustment being such as to minimise a cost function such as the sum of the mean square outputs of the microphones 12.
The secondary sources 11 may in another embodiment be shakers, and the microphones 12 replaced by accelerometers.
It will be noted that the secondary sources 11 and the microphones 12 or other sensors are distributed in the enclosed space 10.
Since the reference signal contains harmonics or subharmonics of the input signal 16, which is periodic at the engine rotation or firing rate, the reference signal contains engine order frequencies.
The generator 15 is arranged to select engine order frequencies that ensure that the sound produced by the loudspeakers 11 is of the same frequency or frequencies as the sound produced in the enclosure 10 by the engine, even during changes in engine conditions such as load or speed. The number of engine order frequencies in the reference signals is restricted so that the adaptive filters have a relatively small number of coefficients and can therefore adapt quickly.
The input signal 16 can be obtained from a moving part of the engine or part of the ignition circuitry; for example.
Fig. 2(a) illustrates graphically the response of the reference signal generator 15 when implemented in the form of a tracking filter, i.e., a filter having a centre frequency so controlled that the output frequencies have a constant ratio to the dominant input frequencies, so that in Fig. 2(a), the frequency f0 is N x (engine rotation rate), and the reference signal contains only the first N harmonics of the engine rotation rate, where N is an integer. If the input signal is a voltage pulse train as represented by Fig. 2(b), where 8T is the periodic time of the engine rotation rate, the first eight harmonics of the engine rotation rate are present in the reference signal. The spectrum, by Fourier analysis, of the reference signal is then illustrated by Fig. 2(c), i which A is amplitude.With the response of Fig. 2(a), only the first six harmonics would be usable.
The tracking filter can be in the form of charge coupled devices having a switching frequency locked to the engine rotation rate.
An alternative reference signal generator using a plurality of tracking band pass filters is illustrated by Fig. 3 in which the input signal 16, a square wave at, for example, 128 times the engine rotation rate, is divided by 32 and then by 2. Division by 32 produces a square wave at four times the engine rotation rate which is supplied to a first bandpass filters 17 having a centre frequency f4 which is arranged to track four times the fundamental frequency of the square wave supplied thereto. The further division by 2 produces a square wave at twice the engine rotation rate, which is supplied to a second bandpass filter 18 having a centre frequency f2 which is arranged to track twice the fundamental frequency of the square wave supplied thereto.The bandpass filters 17 and 18 produce respectively sinusoidal output signals at f2 and f4 which are linearly summed at an adder 19 to produce the reference signal.
Further dividers and tracking bandpass filters can of course be added to or inserted in the circuit of Fig. 3 so that the reference signal contains the desired set of engine order frequencies.
Another reference signal generator may consist of a fixed frequency filtering circuit which selects harmonics and/or subharmonics from an input signal rich in the harmonics of the engine rotation rate or firing rate. The circuit may be a bandpass filter having a centre frequency fixed at the frequency of a pronounced resonance excited in the enclosure by the engine or other primary source of sound or vibration. For example, a bandpass filter may be arranged to have a response that models the acoustic reponse of a motor car passenger compartment to the engine.
A further implementation of the reference signal generator may comprise a plurality of phase lock loops used to generate sinusoidal signals having respective frequencies with integer relationships to a square wave input signal from the engine or other primary source, the sinusoidal signals being added together to form the reference signal. Thus a reference signal consisting of specific harmonics and/or harmonics locked to the primary source fundamental, such as engine rotation rate, is generated. An alternative generator for such a reference signal is illustrated in Fig. 4 in which a square wave 20 at the primary source fundamental is used to control a plurality of tunable oscillators 25,26 each producing a sinusoidal signal at a chosen harmonic or subharmonic frequency to be added at the adder 19 which produce the reference signal by simple addition of the sinusoidal signals.
In the generator of Fig. 4, a square wave 20 at an engine rotation rate is supplied to a bistable circuit 21 to divide the rate by two and thereby produce a pulse train in which the duration of each pulse is equal to the prevailing periodic time of the square wave 20. This periodic time is then measured by a counter 22 which is enabled throughout the duration of each positive pulse from the bistable circuit 21 and counts clock pulses supplied by a clock pulse generator 23 which generates the clock pulses at a fixed, suitably high rate fc.
The contents of the counter 22 are read at the end of each positive pulse from the bistable circuit 21 by a trigonometric function generator 24 which is triggered by the trailing pulse of each positive pulse from the circuit 21 and generates two digital outputs representing respectively cos(2w0) and cos(4UJ where W0 is given by to = 2Ef 2Trf c/Nfs in which N is the number of clock pulses counted by the counter 22 in the duration of one positive pulse from the circuit 21, and fs is a sample rate used in two digital oscillators 25 and 26 which receive respectively the digital outputs cos(2X0) and cos(4X0) from the function generator 24.The digital sinusoidal outputs from the two oscillators 25 and 26 are superposed by a digital adder 19' which supplies the reference signal as a digital signal. The trigonometric function generator 24, oscillators 25 and 26 and adder 19' can be implemented by a microprocessor with a suitable program.
The microprocessor can be used to produce the reference signal in the form.
xI(n) = #(n) + 2 cos(I#o)xI(n - 1) - x1(n - 2) where I is the order of the harmonic or subhnrmonic being generated, 6(n) is a unit sample sequence which initiates the simulation of the oscillator, and n is the sample number.
Fig. 5 represents in block form an active sound control apparatus embodying the invention for reducing the level of engine generated sound in the passenger compartment of a motor car having an ignition circuit including a low tension coil 31 from which a voltage signal 32 at the firing rate of the engine is taken and supplied to a waveform shaper 33 which in response thereto produces a pulse train at the engine firing rate. It is assumed in the present example that the engine firing rate is twice the engine rotation rate fO. Thus the shaper 33 provides a signal having a fundamental frequency which is a single harmonic, (2fro) of the engine rotation rate.A reference signal generator is provided in the form of a proprietory tracking filter 34, manufactured by Bruel and Kjaer under type number 1623, which receives the output of the shaper 33 as an input signal and as a trigger signal and produces a sinusoidal output signal at the selected harmonic 2fo. This sinusoidal signal is sampled with an analog to digital converter 35 to produce a reference sequence x(n) of digitised samples which are supplied as data to a processor and memory unit 36.
Mounted within the motor car passenger compartment are two loudspeakers 371 and 372' which are in positions normally used for car stereo reproduction. The loudspeakers are driven by a multiplexer 38 through respective low pass filters 39 and output amplifiers 40. The filters 39 have a cut off frequency of 460 Hz and are provided to prevent aliasing. The multiplexer 38 is controlled by the processor and memory unit 36, through control lines which are not shown, and receives a single input signal from a digital to analog converter 41. The purpose of the loudspeakers 371 and 372 is to generate in the passenger compartment audio waves that will cancel those set up directly by mechanical transmission from the engine to the compartment. The digital to analog converter 41 is supplied by the processor and memory unit 36 with output data which consists of two interleaved sequences of digitised samples y1(n) and y2(n) which are converted by the converter 41 into interleaved sequences of analog samples and separated into respective sequences by the multiplexer 38 for application to the low pass filters 39 so that in effect the loudspeaker 371 is driven by the sequence y1(n) and the loudspeaker 372 is driven by the sequence y2(n).In Fig. 5 each sequence is represented by the expression ym(n), so that in this example m may be 1 or 2, In order to ensure that the acoustic outputs from the loudspeakers 371 and 372 have the correct phase and amplitude to effect cancellation of the engine noise, error signals are picked up from the compartment and utilised by the processor and memory unit 36. The acoustic error signals, if present, are sensed by four microphones 421, 422, 423 and 424, which are placed respectively either side of a driver headrest and a passenger headrest, there being only two seats in the compartment in the present example.The electrical outputs from the microphones are respectively amplified by amplifiers 43 and passed through low pass filters 44 to a fourinput multiplexer 45 which supplies a single analog output to an analog to digital converter 46. The filters 44 are provided to prevent aliasing and have a cut-off frequency of 460 Hz.
The multiplexer 45 and the converter 46 convert the four filtered microphone outputs into data stream consisting of four interleaved sequences of digitised samples el(n), e2(n), e3(n) and e4(n), which correspond respectively to the filtered outputs of the microphones 421, 422, 423 and 424. In Fig. 5, each sequence is represented hy eg(n) so that in this example g may be 1, 2, 3 or 4.
The processor and memory suit 36 receves a square wave at 1.2 kilohertz from a sample rate oscillator 47 which determines the rate at which the converters 35, 41 and 46 convert samples and the frame duration of processing carried out by the unit 36. Thus in the present example, the unit 36 completes its processing frame within 833 milliseconds. A crystal clock oscillator (not shown) with a frequency of 10 Megahertz is included in the unit 36.
The unit 36 simulates two adaptive filters, each having two coefficients, so that: y (n) = wm0x(n) + w,lx(n - 1) describes the relation between the output sequence ym(n) to a loudspeaker and the reference signal x(n), where the coefficients are wmn and wml. Hence with the two lc > udspeakers 371 and 372: y1(n) = wlox(n) + w11x(n - 1) and y2(n) 2 W20X(ll) + w21x(n - 1).
The values of the coefficients wmO and wml are calculated by the unit 36 from the relationship:
in which a is a fixed convergence coefficient, r@m(n - i) is a value of a filtered reference signal rQm, and i = O or 1.
The filtered reference signal rQm is a sequence formed by filtering the reference signal x(n) with a filter that models the effect of the acoustic coupling between the mth loudspeaker and the microphone. The unit 36 simulates this filtering as digital FIR (Finite Impulse Response) filtering. Coefficients for the digital FIR filtering are adjusted adaptively during an initialisation program in which a white noise generator 48 is energised.
In the initialisation program, a white noise signal is generated by the generator 40, filtered by a low pass filter 49 to prevent aliasing, the filter having a cut off frequency of 460 Hz, and subsequently sampled and converted by an analog to digital converter 50. The digital output of the converter 50 is used to drive the loudspeakers 371 and 372' and the resulting digital input to the unit 36 from the microphones 421, 422, 423 and 424 is used to determine the values of reference filter coefficients cQmj where j = 0, ,34. The unit 36 performs a 35 coefficient FIR modelling of the impulse response between the mth loudspeaker and the @th microphone at the @th sample. Such modelling is described in "Adaptive Signal Processing" by B. Widrow and S.D.Stearns, published in 1985 by Prentice Hall.
The filtered reference sequence is then given by
The operation of the unit 36 is such that, having obtained the error samples eQ(n) and the filtered reference signal rQm(n), each adaptive filter coefficient wmi for each output ym(n) is updated by a quantity proportional to the sum of the computed products of e@(n) and r@m(n - i) in accordance with the equation
The new set of adaptive coefficients wmi is then stored and used to filter the next sample of the reference signal, x(n + 1).
The unit 36 includes RAM for temporary storage and computation, and EPROM for program storage. Calculated coefficients wmi and and and reference sequences rum(") are held in RAM. The convergence coefficient is entered at a set of manually operable switches.
In a preferred embodiment constructed in accordance with Fig.
5, the unit 36 includes a Texas Instruments TMS 32010 microprocessor. The input signal rate from ignition circuit in the constructed embodiment is 100 Hz to 200 Hz, and the waveform shaper 33 is a monostable circuit triggered by the leading edge of the input signal to produce pulses of a constant width which is small relative to the sample period set by the sample rate of 1.2 kilohertz. The low pass filters 39, 44 and 49 are active filter modules supplied by Remo Limited under no. 1431/L.
Only a small amount of separate additional RAM is required with the TMS 32010 which has considerable internal RAM and operates as described in the TMS 32010 Users' Guide published in 1983 by Texas Instruments, Inc. Data buses between the unit 36 and the converters 35, 41, 46 and 50 are 12 bit buses. Other buses and lines required for synchronisation and control are omitted for clarity.. It will be noted that the values of the coefficients wmi and cR,j can be initially set to zero.
A family of algorithms which are alternatives to the SNM algorithm uses a bank of adaptive digital filters working in parallel for each secondary source. Each individual filter is fed by a reference signal containing a subset of the harmonics or subharmonics to be controlled. For example, Figure 6 of the accompanying drawings shows two parallel FIR filters each fed by pure tone reference signals, at the second and fourth engine order frequencies in this case. The outputs of these filters are added together to form the output to the secondary source. Each of these parallel filters may be updated by any of the algorithms discussed above. For example, the said stochastic gradient algorithm may be modified so that
where blini is the i'th coefficient of the FIR filter fed from the I'th harmonic of the engine, driving the m'th secondary source.The advantage of such an algorithm is that each harmonic frequency is controlled independently and the convergence of an harmonic does not couple with the convergence of any other harmonic, as is the case when a 21 coefficient filter is used to filter I harmonics simultaneously. In this case I filters each with 2 coefficients could be used to filter I harmonics individually, and their response combined afterwards. The disadvantage of this algorithm is that a filtered reference signal needs to be generated for each source (m), sensor (R) and harmonic (I), to give each rQmI(n).
Another approach to controlling a number of harmonics is to take the Fourier transform of each of the error signals and to update a set of coefficients controlling each harmonic of each secondary output independently. The outputs of each of these filters are combined together, for each secondary source, via an inverse Fourier transform, to generate the output waveform for this source as indicated in Figure 7 of the accompanying drawings.For a single harmonic in the frequency domain, the complex value of the R'th error signal will be given by
where A R is the value of Ewith no active control, wm is the complex amplitude of the voltage to the m'th secondary source and is the complex transfer function between the @'th sensor and m'th source at the frequency of the harmonic of interest.
This may be expressed in matrix form as E=A+CW Where ET = tEX Ez ... EL] AT = [A1 Az ... AL] WT = [W@ W2 ... WM]
C = C11 C12 .... C1M #C21 C22 .... .. # CL1 ..... CLM The cost function in this case may be written as J = ERE where the superscript H denotes the complex conjugate of the transposed vector or matrix. Therefore J = AHA + WHCHA + ARC W + Note that aJ # = 2CHA + 2CHC W = 2CHE aW so that the steepest descent algorithm may be written Wk+1 = Wk where Mk and Ek are the complex values of the filter response and error output respectively at the k'th iteration.
This algorithm does not seem to appear in the active control literature. This is probably because the Newtons method algorithm, below is no more difficult to implement after initialisation to form the matrix needed to premultiply Ek. However, in some cases it may be that the matrix C changes with time and a separate 'identification' algorithm is used in parallel with the adaptive control algorithm to track these changes. In such cases the steepest descent algorithm may be considerably more computationally efficient to implement than that below.
The frequency domain version of the Newton's method algorithm may be written Wk+1 = Wk - 2 [CHC]-1CHEk A special case of this algorithm does appear in the literature, in which the number of error sensors is equal to the number of secondary sources (L = M), so that C is a square matrix, and the algorithm reduces to Wk+1 = Wk - 2 C-1Ek This algorithm has been presented by Pierce (1985, David W.
Taylor Naval Ship Research and Development Center Report no. 85/047.
An algorithm for active adaptive control of periodic interface).
If the convergence coefficient, , is set equal to one half, the algorithm also reduces to the iterative matrix algorithm described in White and Cooper (1984, Applied Acoustics 17, 99-109. An adaptive controller for multivariable active control).
In practice the most advantageous algorithm will probably be derived from a judicious mixture of time and frequency domain concepts. For example, one implementation of a Fourier transformer operating on each error sequence e g(n) to produce the inphase and quadrature frequency components of eR(n) at 1W0 is illustrated in Figure 8 of the accompanying drawings. The slowly varying outputs from such a circuit represent the real and imaginary parts of the frequency domain signal ER defined above, so these signals can be used with any of the frequency domain algorithms discussed above to update a bank of adaptive filters driven by this frequency component driving each secondary source, as in Figure 6.

Claims (8)

1. An active noise control system for reducing sound or vibration generated by a primary source, in which at least one reference signal containing at least one selected harmonic or subharmonic of the said sound or vibration is supplied to means driving a plurality of secondary sources, such that the sound or vibration energy detected by sensor means arranged to sense the sound or vibration field established by the primary and secondary sources is reduced.
2. A system according to claim 1, wherein the said one reference signal is generated by filtering a periodic input signal having its fundamental frequency locked to a predominant frequency of the exterior source.
3. A system according to claim 2, wherein the filtering is effected by a tracking filter.
4. A system according to claim 3, wherein the periodic input signal is a harmonic of the said predominant frequency.
5. A system according to any preceding claim, wherein the means for driving the secondary sources include a digital processor with data and program memory.
6. A system according to any preceding claim, wherein the system is adapted to operate in accordance with an algorithm which adjusts the outputs from the secondary sources so as to minimise a cost function on a time scale comparable with the delays associated with the propagation of the sound or vibration from the secondary sources to the sensor means.
7. A system according to claim 1, wherein the reference signal is generated by apparatus as described hereinbefore with reference to Fig. 3 or Fig. 4 of the accompanying drawings.
8. An active nose control system substantially as described hereinbefore with reference to Fig. 5 or 6 or 7 or 8 of the accompanying drawings.
GB08630422A 1986-10-07 1986-12-19 Active noise control Withdrawn GB2201858A (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
PCT/GB1987/000706 WO1988002912A1 (en) 1986-10-07 1987-10-06 Active vibration control
EP87906587A EP0285632B1 (en) 1986-10-07 1987-10-06 Active vibration control
JP62505958A JP2890196B2 (en) 1986-10-07 1987-10-06 Active vibration control device or related improvements
KR1019880700638A KR960011152B1 (en) 1986-10-07 1987-10-06 Active vibration control system
DE87906587T DE3786165T2 (en) 1986-10-07 1987-10-06 ACTIVE VIBRATION CONTROL.
US07/448,517 US5170433A (en) 1986-10-07 1989-12-11 Active vibration control

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GB08624053A GB2203016A (en) 1986-10-07 1986-10-07 Active sound control apparatus

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Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2228648A (en) * 1989-02-27 1990-08-29 Toshiba Kk Active noise silencer
GB2228647A (en) * 1989-02-28 1990-08-29 Toshiba Kk Active silencer for refrigerators
GB2236640A (en) * 1989-08-22 1991-04-10 Volkswagen Ag A device for the active reduction in noise level of a periodically operating noise source
US5010576A (en) * 1990-01-22 1991-04-23 Westinghouse Electric Corp. Active acoustic attenuation system for reducing tonal noise in rotating equipment
US5222148A (en) * 1992-04-29 1993-06-22 General Motors Corporation Active noise control system for attenuating engine generated noise
US5321759A (en) * 1992-04-29 1994-06-14 General Motors Corporation Active noise control system for attenuating engine generated noise
US5332061A (en) * 1993-03-12 1994-07-26 General Motors Corporation Active vibration control system for attenuating engine generated vibrations in a vehicle
US5359662A (en) * 1992-04-29 1994-10-25 General Motors Corporation Active noise control system
US5617315A (en) * 1992-08-31 1997-04-01 Mazda Motor Corporation Active vibration damping system for a vehicle
US5651072A (en) * 1992-07-06 1997-07-22 Mazda Motor Corporation Vibration damping system for vehicle
US5690321A (en) * 1992-09-29 1997-11-25 Mazda Motor Corporation Vibration damping system for vehicle

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2254979B (en) * 1991-04-20 1994-08-31 Rover Group Active enhancement of recurring sounds
JP2530779B2 (en) * 1991-09-05 1996-09-04 株式会社日立製作所 Noise reduction device
US5485523A (en) * 1992-03-17 1996-01-16 Fuji Jukogyo Kabushiki Kaisha Active noise reduction system for automobile compartment
GB2360900B (en) * 2000-03-30 2004-01-28 Roke Manor Research Apparatus and method for reducing noise
US7450725B2 (en) 2001-12-17 2008-11-11 Mahle International Gmbh Digital filter modeling for active noise cancellation

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2110504A (en) * 1981-11-26 1983-06-15 George Brian Barrie Chaplin Improved method of and apparatus for cancelling vibrations from a source of repetitive vibrations
GB2122052A (en) * 1982-06-09 1984-01-04 Plessey Co Plc Reducing noise or vibration
EP0098594A2 (en) * 1982-07-07 1984-01-18 Nissan Motor Co., Ltd. A method and apparatus for controlling the sound field in a vehicle cabin or the like
GB2126837A (en) * 1982-08-19 1984-03-28 British Aerospace Noise suppression
GB2132053A (en) * 1982-12-15 1984-06-27 Lord Corp Active attenuation of noise in a closed structure
GB2149614A (en) * 1983-10-31 1985-06-12 Secr Defence Active noise reduction apparatus

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1577322A (en) * 1976-05-13 1980-10-22 Bearcroft R Active attenuation of recurring vibrations

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2110504A (en) * 1981-11-26 1983-06-15 George Brian Barrie Chaplin Improved method of and apparatus for cancelling vibrations from a source of repetitive vibrations
GB2122052A (en) * 1982-06-09 1984-01-04 Plessey Co Plc Reducing noise or vibration
EP0098594A2 (en) * 1982-07-07 1984-01-18 Nissan Motor Co., Ltd. A method and apparatus for controlling the sound field in a vehicle cabin or the like
GB2126837A (en) * 1982-08-19 1984-03-28 British Aerospace Noise suppression
GB2132053A (en) * 1982-12-15 1984-06-27 Lord Corp Active attenuation of noise in a closed structure
GB2149614A (en) * 1983-10-31 1985-06-12 Secr Defence Active noise reduction apparatus

Cited By (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2228648A (en) * 1989-02-27 1990-08-29 Toshiba Kk Active noise silencer
US5052041A (en) * 1989-02-27 1991-09-24 Kabushiki Kaisha Toshiba Silencer
GB2228648B (en) * 1989-02-27 1993-06-09 Toshiba Kk Silencer
GB2228647A (en) * 1989-02-28 1990-08-29 Toshiba Kk Active silencer for refrigerators
GB2228647B (en) * 1989-02-28 1993-06-02 Toshiba Kk Active silencer for refrigerators
GB2236640B (en) * 1989-08-22 1994-04-06 Volkswagen Ag A device for the active reduction in noise level of a periodically operating noise source
GB2236640A (en) * 1989-08-22 1991-04-10 Volkswagen Ag A device for the active reduction in noise level of a periodically operating noise source
US5010576A (en) * 1990-01-22 1991-04-23 Westinghouse Electric Corp. Active acoustic attenuation system for reducing tonal noise in rotating equipment
US5222148A (en) * 1992-04-29 1993-06-22 General Motors Corporation Active noise control system for attenuating engine generated noise
US5321759A (en) * 1992-04-29 1994-06-14 General Motors Corporation Active noise control system for attenuating engine generated noise
US5359662A (en) * 1992-04-29 1994-10-25 General Motors Corporation Active noise control system
US5651072A (en) * 1992-07-06 1997-07-22 Mazda Motor Corporation Vibration damping system for vehicle
US5617315A (en) * 1992-08-31 1997-04-01 Mazda Motor Corporation Active vibration damping system for a vehicle
US5690321A (en) * 1992-09-29 1997-11-25 Mazda Motor Corporation Vibration damping system for vehicle
US5332061A (en) * 1993-03-12 1994-07-26 General Motors Corporation Active vibration control system for attenuating engine generated vibrations in a vehicle

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KR880701936A (en) 1988-11-07
GB8624053D0 (en) 1986-11-12

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