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Active acoustic absorption General presentation - applications

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Title: Active acoustic absorption General presentation - applications


1
Active acoustic absorption General presentation
- applications
  • Dr. Hervé Lissek
  • Laboratoire dElectromagnétisme et dAcoustique
  • EPFL
  • herve.lissek_at_epfl.ch

2
Introduction ANC
  • Usual active noise control (ANC)
  • aims at interfering a primary sound field (the
    unwanted noise) with a synthesized secondary
    sound field
  • Efficient for harmonic sound in 1-D propagation,
    even more if stationary

3
Introduction 3D ANC
  • Contra-productive for complex 3D non-stationary
    noises

4
Introduction Active absorber
  • Aim of this research
  • design a broadband acoustic absorber
  • Principle
  • active impedance control of a resonator

surface active Za1
contrôle1
absorption active
5
Introduction Active absorber
  • Aim of this research
  • design a broadband acoustic absorber
  • Principle
  • active impedance control of a resonator
  • Assessed applications
  • room acoustics
  • active noise attenuation (harmonic noise
    sources)
  • low frequency control, modal control

6
Building acoustics room acoustics
  • Reflection coeffiction r function of Zms
  • Reflection factor R function of Zms
  • Absorption factor a function of r (R), then of Zms

WrRWi
F
v
q
Wi
7
Building acoustics sound insulation
  • Mechanical impedance of the material
  • Sound insulation depends on Zms

8
Principle of passive damping
Acoustic field
param of absorption S (absorbing area) Mms
(material mass) Cms (material suspension) Rms
(losses)
S
  • Acoustic impedance _at_ interface
  • Za(w) (Rms jwMms (jwCms)-1)/S (R,M,C system,
    w pulsation)
  • _at_ resonance ( )
  • Za(wr) Rms /S proportional to Zc r.c
    (characteristic impedance)

9
Principle of passive absorption
Acoustic field
factors of absorption S (absorbing area) Mms
(material mass) Cms (material suspension) Rms
(losses)
S
  • _at_ resonance ( )
  • Za(wr) Rms /S proportional to Zc r.c
    (characteristic impedance)
  • Note when ZaZc (impedance matching)
  • ? transparency the material is totally absorbent

10
Specifications of active acoustic absorbers
  • Acoustic resonator
  • ? resonance frequency fr , quality factor Q
  • The aim of active absorption
  • allow the modification of fr and Q, by way of
    simple (electric) control
  • ? modification of the properties of the absorber
  • make it more absorbent at resonance (acoustic
    impedance Za to match characteristic impedance Zc
    of the medium)
  • make it absorbent over a wider frequency range
  • possibility to shift the resonance frequency

11
behaviour of passive absorption
Za(wwr) ½ Zc
factors of absorption S (absorbing area) Mms
(material mass) Cms (material suspension) Rms
(losses)
aim enhance losses
fr30 Hz
12
Ideal behaviour of active absorption
factors of absorption S (absorbing area) Mms
(material mass) Cms (material suspension) variabl
e Rms
Za(wwr) Zc ? TOTAL ABSORPTION
Df
aim enhance bandwidth
13
Principle of active absorption
  • GOAL
  • Active control modification of Rms
  • Za(w) (Rms (controlled) jwMms
    (jwCms)-1)/S2Zc

14
Principle of active resonance shift
  • GOAL
  • Active control modification of fr
  • Za(w) (Rms jwMms(controlled)
    (jwCms(controlled))-1)/S2

15
Application  active materials 
Resonator electrodynamic loudspeaker
q
Gq
GP
16
Calculationsnormalized acoustic admittance
(Zc/Za)
as feedback gains increase
17
Calculationsabsorption coefficient (a f(Za))
as feedback gains increase
18
Experimental results
19
Experimental resultsmeasured normalized
admittance
20
Experimental resultsmeasured absorption
coefficients
21
Conclusion
  • Validation of the concept of active materials
  • calculations promise good performances, even
    without specific transducer (usual loudspeaker)
  • experimental results show good tendency
  • not much expensive in regards with the acoustic
    gains
  • cheap actuators (usual loudspeakers)
  • cheap sensors (back-electret microphones)
  • simple electric control (discrete components)

22
Perspectives
  • Optimization in progress
  • dedicated transducers
  • enhanced control
  • assess energy transfer
  • Potential transfer of technology industries
    concerned with non-stationary broadband or narrow
    band noises
  • ?optimize the concept within applied frameworks
  • aircraft engines (SNECMA)
  • electric industry
  • railway industry
  • buildings
  • etc...

23
THANK YOU FOR YOUR ATTENTION
  • herve.lissek_at_epfl.ch
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