Title: When Sound Waves meet Solid Surfaces
1When Sound WavesmeetSolid Surfaces
- Applications of wave phenomena in room acoustics
- By Yum Ji CHAN
- MSc (COME) candidate
- TU Munich
20 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
31.0 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
4Ranges of frequency under interest
Piano
51.1 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)
61.2 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
71.3 Diffraction Interference
- Edge interference due to finite plates
- Reflection on flat surface Deviation from
ray-like behaviour
81.4 Fresnel zone
- Imagine each beam shown below have pathlengths
differered by ?/2 - What happens if
- Black Green?
- Black Green Red?
91.5 Conclusion drawn from experiment
- Theory for reflectors in sound is more
complicated than those for light - Sizing is important for reflectors
102.0 Elements controlling sound in a room
- Reflectors
- Diffusers
- Absorbers
112.1 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
122.2 Size of Reflectors
- Never too small
- Diffraction
- Absorption
- No need to be too big
- Imagine a mirror for light!
- Example worksheet
132.3 Diffusers
- Scattering waves
- With varied geometries
Type 1
142.4 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
152.5 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)
162.6 Absorption at other frequency ranges (B)
- Low frequency absorbers
- Plate absorbers, make use of bending waves
- Composite board resonators (VPR in German)
172.7 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)
182.7 Asymmetric FE matrices
- FE matrices are usually symmetric
- Maxwell-Betti theorem
- Coupling conditions make matrices asymmetric
192.7 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)
202.8 Why is it like that?
- Consider Rayleigh coefficient
- Compare increase of PE to increase of KE
Compression
Vibration
213 Parameters in room acoustics
- Reverberation time
- Clarity / ITDG (Initial time delay gap)
- Binaural parameter
223.1 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)
233.2 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)
243.3 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
253.4 Binaural parameter
- Feel of spaciousness
- The difference of sound heard by left and right
ears
263.5 Applications Reverberant room
- Finding the optimum positions of resonators in
the test room
(Source My Masters thesis)
273.5.1 Application Reverberant room
- Mesh size 0.2 m
- 30000 degrees of freedom
- Largest error of eigenvalue 2
283.5.2 Impulse response function
- Reverberation time
- The effect of amount of resonators
- The effect of internal damping inside resonators
(Source My Masters thesis)
293.5.3 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
303.5.3 Getting impulse response functions
- Frequency domain
- Time domain
313.6 Are these all?
- Amount of parameters are increasing
- Models are still necessary to be built for
acoustic delicate rooms - Concert halls
323.7 A failed example
- New York Philharmonic hall
- Models were not built
- Size of reflectors
(Source Spektrum der Wissenschaft)
334.1 Acoustic problems with the finite element
(FE) method
- Wave equation
- Discretization using linear shape functions
- Variable describing acoustic strength
- Corresponding force variables
344.2 1D Example
- 100 m long tube, unity cross section
- Mesh size 1 m, 2 m and 4 m
354.2 1D Example
- Discretization error in diagram
364.3 Numerical error
- Possible, but not significant if precision of
storage type is enough
375 Conclusion
- Is acoustics a science or an art?
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