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When Sound Waves meet Solid Surfaces

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When Sound Waves meet Solid Surfaces Applications of wave phenomena in room acoustics By Yum Ji CHAN MSc (COME) candidate TU Munich 0 Introduction Phemonena of sound ... – PowerPoint PPT presentation

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Title: When Sound Waves meet Solid Surfaces


1
When Sound WavesmeetSolid Surfaces
  • Applications of wave phenomena in room acoustics
  • By Yum Ji CHAN
  • MSc (COME) candidate
  • TU Munich

2
0 Introduction
  • Phemonena of sound waves
  • Equipments on surfaces to control sound intensity
  • Applications in room acoustics
  • Numerical aspects of finite element method in
    acoustics
  • Conclusion

3
1.0 Nature of sound
  • Sounds are mechanical waves
  • Sound waves have much longer wavelength than
    light
  • Speed of sound in air c 340m/s
  • Wavelength for sound ?
  • c f ?
  • When f 500 Hz, ? 68 cm
  • Typical wavelength of visible light 4-7 10-7
    m
  • Conclusion
  • Rules for waves more important than rules for rays

4
Ranges of frequency under interest
Piano
5
1.1 Measurement of Sound intensity
  • Acoustic pressure in terms of sound pressure
    level (SPL)
  • Unit decibel (dB), pref 2 10-5 Pa
  • Acoustic power
  • More parameters are necessary in noise
    measurements (out of the scope)

6
1.2 Huygens principle
  • From wikipedia
  • It recognizes that each point of an advancing
    wave front is in fact the center of a fresh
    disturbance and the source of a new train of
    waves and that the advancing wave as a whole may
    be regarded as the sum of all the secondary waves
    arising from points in the medium already
    traversed.
  • Diffraction Interference apply

7
1.3 Diffraction Interference
  • Edge interference due to finite plates
  • Reflection on flat surface Deviation from
    ray-like behaviour

8
1.4 Fresnel zone
  • Imagine each beam shown below have pathlengths
    differered by ?/2
  • What happens if
  • Black Green?
  • Black Green Red?

9
1.5 Conclusion drawn from experiment
  • Theory for reflectors in sound is more
    complicated than those for light
  • Sizing is important for reflectors

10
2.0 Elements controlling sound in a room
  • Reflectors
  • Diffusers
  • Absorbers

11
2.1 Weight of Reflectors
  • Newtons second law of motion
  • Difference in acoustic pressure acceleration
  • Mass is the determining factor at a wide
    frequency range
  • Transmitted energy (i.e. Absorption in rooms) is
    higher
  • At low frequencies
  • When the plate is not heavy enough

12
2.2 Size of Reflectors
  • Never too small
  • Diffraction
  • Absorption
  • No need to be too big
  • Imagine a mirror for light!
  • Example worksheet

13
2.3 Diffusers
  • Scattering waves
  • With varied geometries

Type 1
14
2.4 Absorbers
  • Apparent solution Fabrics and porous materials
  • Reality it is effective only at HF range
  • Needed in rooms where sound should be damped
    heavily (e.g. lecture rooms)
  • Because clothes are present
  • Other absorbers make use of principles in
    STRUCTURAL DYNAMICS

15
2.5 Absorption at other frequency ranges (A)
  • Hemholtz resonator-based structures
  • Analogus to spring-mass system
  • Example worksheet
  • The response around resonant frequency depends on
    damping
  • Draw energy out of the room

(Source http//physics.kenyon.edu/EarlyApparatus
/index.html)
16
2.6 Absorption at other frequency ranges (B)
  • Low frequency absorbers
  • Plate absorbers, make use of bending waves
  • Composite board resonators (VPR in German)

17
2.7 Comparison between a composite board
resonator and a plate
  • VPR Resonator assembly
  • Modelled as a fluid-solid coupled assembly with
    FE
  • Asymmetric FE matrices

(Owner of the resonator Müller-BBM GmbH)
(Source My Masters thesis)
18
2.7 Asymmetric FE matrices
  • FE matrices are usually symmetric
  • Maxwell-Betti theorem
  • Coupling conditions make matrices asymmetric

19
2.7 Comparison between a composite board
resonator and a plate
  • Bending waves without air backing (Uncoupled, U)
  • Compressing air volume with air backing (Coupled,
    C)

(Source My Masters thesis)
20
2.8 Why is it like that?
  • Consider Rayleigh coefficient
  • Compare increase of PE to increase of KE

Compression
Vibration
21
3 Parameters in room acoustics
  • Reverberation time
  • Clarity / ITDG (Initial time delay gap)
  • Binaural parameter

22
3.1 Impulse response function of a room
  • The sound profile after an impulse (e.g. shooting
    a gun or electric spark in tests)

(Courtesy of Prof. G. Müller)
23
3.2 Reverberation time
  • The most important parameter in general
    applications
  • Definition SPL drop of 60 dB
  • Formula drawn by Sabine
  • Depends on volume of the room and the equivalent
    absorptive area of the room
  • Samples to listen
  • Rooms with extremely long RT Reverberant room

(Courtesy of Müller-BBM)
24
3.3 Clarity / ITDG
  • Clarity Portion of early sound (within 80 ms
    after direct sound) to reverberant sound
  • ITDG Gap between direct sound and first
    reflection, should be as small as possible

25
3.4 Binaural parameter
  • Feel of spaciousness
  • The difference of sound heard by left and right
    ears

26
3.5 Applications Reverberant room
  • Finding the optimum positions of resonators in
    the test room

(Source My Masters thesis)
27
3.5.1 Application Reverberant room
  • Mesh size 0.2 m
  • 30000 degrees of freedom
  • Largest error of eigenvalue 2

28
3.5.2 Impulse response function
  • Reverberation time
  • The effect of amount of resonators
  • The effect of internal damping inside resonators

(Source My Masters thesis)
29
3.5.3 Getting impulse response functions
  • Convolution
  • Effect comes after excitation
  • Mathematical expression
  • Expression in Fourier (frequency) domain
  • Y(f) X(f) H(f)
  • X(f) 1 for impulse
  • H(f) Impulse response functionin time domain

30
3.5.3 Getting impulse response functions
  • Frequency domain
  • Time domain

31
3.6 Are these all?
  • Amount of parameters are increasing
  • Models are still necessary to be built for
    acoustic delicate rooms
  • Concert halls

32
3.7 A failed example
  • New York Philharmonic hall
  • Models were not built
  • Size of reflectors

(Source Spektrum der Wissenschaft)
33
4.1 Acoustic problems with the finite element
(FE) method
  • Wave equation
  • Discretization using linear shape functions
  • Variable describing acoustic strength
  • Corresponding force variables

34
4.2 1D Example
  • 100 m long tube, unity cross section
  • Mesh size 1 m, 2 m and 4 m

35
4.2 1D Example
  • Discretization error in diagram

36
4.3 Numerical error
  • Possible, but not significant if precision of
    storage type is enough

37
5 Conclusion
  • Is acoustics a science or an art?

38
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