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THE HARD CASE Small room acoustics Magne Skålevik Brekke & Strand, Oslo, Norway www.akutek.info

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Page 1: MS Hard Case Pres

THE HARD CASE

Small room acoustics

Magne SkålevikBrekke & Strand, Oslo, Norway

www.akutek.info

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The Hard Case

Cuboid room, dimensions given, take it or leave it

Hard walls

Hard floor

Soft material elements not wanted

Ceiling – the only possible absorbing surface

Sources with harmonic spectra

Speech, music, media playback, etc

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The Hard Case

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The Hard Case

Sound absorbing ceiling

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The Hard Case

Sound absorbing ceiling

Horizontal (tangential) modes untreated2-D reverberant field

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Disturbing speech response

ohEh?

Pitch fluctuation in various positions reveals uneven vowel response

Inherent pitch fluctuations (intonation) in speech

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Flutter-echo

He-he-he-he-

Flutter echo is a temporal feature of a complex mode, thus accompanied by tones

Lo-lo-lo-lo-

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Discriminating pitch response

Intonation can be HARD, since room-modes often are ”out-of-key”

Some notes (tones) are emphasised, others are not

Fast passages blurred out due to long tonal decays

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Hard Case fundamental modes

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Hard Case harmonic modes

f

1 2 3

ANY cuboid mode = the fundamental of a harmonic spectrum -> Pitch

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Periodic response, period T

dB dB

t(s) f(Hz)

Pulse train RT>>T Line spectrum

T 1/T

dB dB

t(s) f(Hz)

Decay 60dB per RTDf=2.2/RT

dB dB

t(s) f(Hz)

DF1/DF

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Periodic response measuredLine spectrum spacing 17Hz Reverberation phase spectrum

Pitch detection 17Hz (EAC) Flutter period T 1/17 s =59ms

Bandpass envelope 150-250Hz

200Hz

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Cuboid acoustic highlights

Any cubiod mode Fi,j,k defines a periodic response with period T=1/ Fi,j,k

Complex mode = the harmonic series of modes with fundamental frequency Fi,j,k = 1/T

Periodic room response can be perceived as Pitch response

Supported pitch (musical notes) are defined by the harmonic series 1/T, 2/T, ...

Flutter-echo of period T is the temporal percetion of a harmonic series with spectral spacing 1/T and at least two audible components

Audible effect above the Schroeder limit, too

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The Hard Case is very common

Many rooms are used for speech

Music may be less common, but more sensitive

Minimalistic interior styles

Carpets often unwanted or forbidden

Acoustic wall-treatment conflict with furniture, fixtures, aesthetics or economy

Cubiod geometry is encouraged by gravity and the tempting simplicity of right angles

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Hard Case Tonal Response Cuboids’ respond to the PITCH of vowels and musical tones

Human perception sensitive to pitch, pitch draws attention

Problem easy to perceive, but...

Hard to measure with blind methods

Hard to predict (slanted walls makes prediction harder)

Hard to avoid

Hard to accept

Hard to handle

Smallest dimension of hard treatment > l/4 It takes >50cm thickness to control response down to 170Hz (E3) Horizontal modes ignores ceiling absorbers

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Measurement case

Parallel walls 6.5m apart (26Hz)

One wall 28cm deep zig-zagshape (=l/4 at 300Hz )

Schroeder region above 125Hz

Disturbing voice response heard in the 150-300Hz range

...together with a flutter-echo

Hard to detect with blind measurement

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Measured voice response

Voice sweep

Line spectrum spacing 26Hz

Pitch detection 26Hz (EAC)

Spectrogram

300Hz

300Hz

Reverberation phase

Reverberation phase spectrum

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0,2

0,4

0,6

0,8

1

1,2

1,4

1,6

1,8

2

0 100 200 300 400 500 600

RT

(s)

frequency (Hz)

narrowband RT voice

broadband RT voice

Decays in 5.3Hz narrowband vs 1/3 oct broadband, RT(s)

Wall zig-zag depth > l/4

Narrowband decay deviates normal-distributed from broadband decay: s=26%

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Softening the Hard Case

Smallest dimension > l/4

Element density depends on wall-to-wall distance and RT requirement.

With walls distance D and scattering s=0.5, reverberation times RT> D/17 kan be acheived

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Conclusions

Hard case cuboids respond strongly and unevenly to speech and music, due to coinciding harmonic spectra

Walls should be treated with sound scattering elements

Obtainable RT’s depend on longest wall-to-wall distance D, and the scattering coefficient

RT’s down to D/17 can be obtained Treatment thickness > l/4 in problem range, e.g.

50cm at 170Hz Audibility is more than loudness; Tonal RT is

important

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Further work

Narrowband RT distribution to be investigated further

Lower limit of problem range remains to determine

Methods for predicting, measuring and assessing Tonal Response in rooms

Criteria for music and speech

More insight in horizontal 2D-acoustics

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www.akutek.info

Thank you

The www center for search, research and open sources in acoustics

More info?

[email protected]

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A semi-hard case

66m2 floor, 3.8m high, ceiling a=0.7

Schroeder region above 125Hz

3 walls with average alfa=0.25

Hard Zig-zag wall deviates from by 28cm (=l/4 at 300Hz )

wall to wall distance 6.5m (mode=26Hz)

Prolonged narrowband RT’s are heard in the 150-300Hz range

...together with a flutter-echo

Plan view

a=0.25

a=0.25

a=0.25 a=0.05