approach to sound system design sound: a little bit of physics spl and sound propagation in free...
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Approach to Sound System Design
• Sound: a little bit of Physics
• SPL and sound propagation in free field
• Room Acoustic: some useful definitions
• Intelligibility
• Sound System Design: some suggestions
• Q & A
What we call sound is simply the What we call sound is simply the sensation produced by the ear when sensation produced by the ear when
stimulated by these vibrations.stimulated by these vibrations.
SOUND is produced by vibrating objects. These move air, “pushing” and “pulling” from its resting state
These small fluctuations in air pressure travel away from the source at relatively high speed, gradually dying off as their energy is absorbed by the medium.
PROPERTIES OF SOUND
A sound wave is a series of pressure changes moving through the air. Amplitude
(dB) is the difference between maximum and minimum pressure: defines the loudness
Wavelength(m) is the physical distance between two maxima( or minima): depends on the speed of sound in the medium and on the frequency:
V = * f
[Velocity = Wavelength * Frequency]
Frequency(Hz) is the rate at which the pressure changes occur: defines the pitch and timbre of the sound
In other materials, the speed of sound can vary quite substantially.
Sound Speed(m/s) Refers to the speed of travel of the sound wave. This varies between mediums and is also dependant on temperature.
AUDIBLE RANGE
The ear can hear sounds ranging from 20Hz to 20kHz.
It is most sensitive to frequencies between 500Hz and 4000Hz, which corresponds almost exactly to the speech band.
MEASURABLE CHARACTERISTICS
Just how can we measure a sound? Acoustic Power (Watts)Measures energy output by a source, that sound's ability to do work
Pressure (Pa)Measures fluctuations about the local atmospheric pressure. Use of root-mean-square (rms) rather that peak-to-peak measures.
Intensity (W/m²) The amount of sound energy within a specific area normal to the direction of propagation
irms
rms
rms
rms
P
P
P
PSPL
0
12
0
21 log20log10
Sound pressure level (SPL) or sound level Lp is a logarithmic
measure of the rms pressure (force/area) of a particular sound relative to a reference sound source.
It is usually measured in decibel (dB(SPL), dBSPL, or dBSPL).
It can be useful to express sound pressure in this way when dealing with hearing, as the perceived loudness of a sound correlates roughly logarithmically to its sound pressure
Sound Power refers to the absolute power of a sound source (in Watts) whereas Sound Power Level refers to the magnitude of that power relative to a reference power (in dB).
0
1
log10a
aW W
WL
The sound pressure ( dB) of a given speaker can be easily calculated knowing the sensivity and the driving power (W)
SPL= Sensivity + LSPL= Sensivity + LWW
Sound propagation in free field
0
1log20)(r
rrSPL
2
0
12
0
2101 log10
4/
4/log10
r
r
rW
rWL rr
i
Sound propagation in free field
Walking away from a sound source, the perceived level of the sound decrease
This is known as the standard inverse square law for point sources.
Practically results in 6 dB reduction in relative intensity per doubling of distance.
NOTE:
1 dB increase is barely audible
3 dB is a generally noticeable change
10 dB is considered as twice as loud
Mathematically looks like
New level= Old level + 20xlog(old distance)- 20xlog(new distance)
0
5
10
15
20
25
30
35
40
45
50
55
60
65
1 10 100 1000
r : distance from the source (m)
Att
en
ua
tio
n o
f A
co
us
tic
Pre
ssu
re d
BL*=L+20logD - 20logD*
Sound:Sound:
Wind & Wind & Temperature Temperature
GradientsGradients
Sound and Barriers: a matter of wavelengthSound and Barriers: a matter of wavelength
Sound waves will propagate away from the source until they encounter one of the room's boundaries where, in general, some of the energy will be absorbed, some transmitted and the rest reflected
back into the room.
Room Acoustic
Striking Sound
Reflected Sound
Absorbed Sound
Transmitted Sound
Part of the sound emitted from the source will go directly to the listener, part will be absorbed, and reflected by walls.
S L
Direct Sound
Early Reflections
Reverberant Field
In the created field the sound does not have directivity and the inverse square low doesn’t hold anymore.
.
The indirect sound after several reflections from different surfaces becomes “ diffuse” creating a steady state field
This is called reverberation
dB
Time
Background Noise
Reverberant Field LR Early
Reflections LER
Direct Sound LD
T0 T1 TN
When the sound source is turned off, direct sound will stop and only the reverberant field will remain
After some seconds even the reverberant field decays.
The length of time taken for a sound to decay 60 dB after the source has ceased transmitting is defined as Reverberation time
Volume: defines if a sound reinforcement system is needed or not. Defines directly the reverberation timeShape: flat, parallel walls, domes, defines echoes and reflectionsThese are fixed and can be hardly changed
Primary: volume, shape, linear dimensions
Room Acoustic depends on:
Secondary: Walls, Ceiling, Materials, Furniture
Treatment can be suggested to improve the room Treatment can be suggested to improve the room acousticacoustic
T
A
I
Ia
Different materials reflect sound in different way:
Carpet with foam base
Marble
The reverberation time affects most of the acoustic features of the room.
Reverberation time, RT60, depends on room dimensions and absorption of the walls
aS
VRT
161.060
whereRT is the reverberation time in seconds,V is the volume of the room in cubic meters, is the average absorption coefficient of the room, andS is the total surface area of the room in square meters
a
ini
iininn
s
as
S
asasasa
1
1221 ..
In acoustic, rooms with smaller reverberation times are appropriate for speech, whereas spaces designed for music require longer reverberation times.
More complex equations was developed to take care of different environment
)1ln(
161.060 aS
VRT
zyx a
Z
a
Y
a
X
S
VRT
222161.0260
In every room coexist a Direct Sound and a Reverberant Field
There is a point in which the Direct SPL and Reverberant SPL are equal. This point is at a distance , from the source, called CRITICAL DISTANCE
60
057.0RT
QVDC Where Q is the directivity of the
source
Every point farther than the Dc from the source will hear just the Reverberant field. The inverse square law is no more valid
Room Acoustic is as important as the sound system itself.
What is a “good sound?
Fidelity. Is given by the frequency response. It depends on each item of the audio chain
Loudness: must be sufficient to achieve the required effect. Is determined by the dynamic range of the sound system
Intelligibility: is linked by the signal/noise ratio and the direct-to-reverberant sound ratio at listener’s ear.It depends directly on room acoustic
ability to hear a sound
ability to detect the structure of a sound
This distinction is more important in speech than in music
Audibility Clarity
Speech• Is made of consonant and vowels• Vowels range from 250-500hz, carry power• Consonants range from 1-4kHz, carry information
Lose consonants = Lose intelligibility
Intelligibility
Measure of the degree of understanding spoken language
Is not a physical quantity as Ampere, Volt, Watt
There are many index to express this degree, many way to measure, and predict it
Factors Affecting IntelligibilityIn on-to-one conversation there aren’t any problems of intelligibility
Sound System Bandwidth and Frequency Response
Signal-to-Noise Ratio
Room Reverberation
Geometric Factors
Distortions
Non Linear Factors
Bandwidth and Frequency Response
Sound system have to guarantee a response from 100 to 10000 Hz.
Limits are fixed by worse performance
Frequency contribution to Intelligibility
0
5
10
15
20
25
30
35
125 250 500 1 2 4 8
Fequecy (Hz)
Inte
lligi
bilit
y (%
)
Signal to Noise Ratio
SPL must be adequate and heard comfortably (normal conversation 70-90 dB)
Noise masks direct sound and lowers intelligibility
Increasing S/N ratio increases intelligibility
Intelligibility becomes independent from S/N for S/N>25 dB
SPL vs Intelligibility
0
20
40
60
80
100
10 35 60 85 110
SPL (dB)
Inte
lleg
ibilit
y (
%)
S/N vs Intelligibility
0
20
40
60
80
100
120
-10 -5 0 5 10 15 20
Ratio S/N (dB)
Inte
llig
ibili
ty (
%)
Reverberation and Reflections
Long RT60’s decrease intelligibility
Late reflections (> 50 ms) smear and blur direct speech
Early reflections ( < 35-50 ms) are perceived as reinforce
Distortion
Clipping
Intermodulation
Acoustic distortion
Are form of NOISE
Specification of various items that compose the sound system have to be carefully studied
Measure and Predicting Intelligibility
Design for speech intelligibility is as important as design for gain, SPL and coverage
While it is quite easy to calculate SPL and RT60 there aren’t models to calculate Intelligibility degree taking care of all parameters
There are more way and several index to express Intelligibility Degree
Subject Based ( AI, %ALCONS) Quantitative ( STI, RaSTI)
Predicting %ALCONS
ALCONS is an index expressing Intelligibility degree, in terms of lost consonants in the talker-listener path
The simplest Peutz formula take care of Directivity, RT60, Room Volume, Number of Speakers, Distance Loudspeaker-Listener
The modified Peutz formula includes also Direct SPL, Reverberant SPL, and Noise SPL
%ALCONS INDEX
High Q’s and Large V’s improve %ALCONS
Long D’s, long RT60’s lowers %ALCONS
This formula fails when strong non-linear effect are present
Excellent
Good Fair
Bad Unacceptable
%ALCONS 0 5 10 15 20 30
VQ
NRTDALCONS
)(200%
6022
2
STI and RaSTIThese methods are fully independent of human being and are fully quantitative
Take care of all factors affecting the intelligibility because measures the corruption of a speech based signal during the talker-to-listener path
Varies from 0 = no intelligibility
to 1= perfect intelligibility
STI and RaSTI main features:
Replace speech with a high frequency noise (consonants-vowels) modulated in amplitude by a low frequency signal (phonems)
Knowing the m(f) means predict intelligibility
Alcons and RaSTI are linkedSTI (RASTI) 0 – 0.3 0.3 - 0.45 0.45 – 0.60 0.60 – 0.75 0.75 - 1
Unacceptable Bad Fair Good Excellent
% AL cons 100 – 33% 33-15% 15-7% 7-3% 3-0%
Common Intelligibility Scale (CIS)There is a common scale to simplify to define the limits There is a common scale to simplify to define the limits
of acceptable intelligibilityof acceptable intelligibility
CIS
0
10
20
30
40
50
60
70
80
90
100
0 0.2 0.4 0.6 0.8 1
Common Intellegibility Scale
Exi
stin
g In
telli
gib
ility
Sca
le
STI*100
100-%Alcons
Standard CEI Standard CEI EN60849 EN60849 states that states that CIS> 0.7CIS> 0.7
CIS=0.7CIS=0.7
%AL%ALconscons=12=12
STI=0.5STI=0.5
Speech Intelligibility Optimisation: Practical Criteria
Sound quality and intelligibility are not the same thing Aim the loudspeaker to the listener: keep as much sound as possible off the walls and the ceiling
Provide a direct line between loudspeaker and listener
Ensure adequate bandwidth
Avoid frequency response anomalies (corner bass increment)
Minimize D where possible
Ensure S/N ratio>10dB
Avoid delays> 50ms ( inter speaker spacing< 15m)
Use high Q in reverberant environment
Minimize SPL variations
Improve RT and acoustic environment
A sound system is basically composed of
1) Electro-Acoustic components ( speakers, microphones detectors)
2) Electronic items (mixer, amplifier, digital processors, music/message sources)
3) Environment ( Room Acoustic, RT60)
Any result is a mesh of these components, and the lower quality component will lower the performance of all the others together
A Sound Reinforcement system is a system for accurately amplifying, reproducing, and sometimes recording audio, so that persons not near the original source may experience the sound as if they were.
PA system, controls to mix the signals coming from the various microphones or other input sources (such as Tuner, CD, MP3 and so on).
How to approach a study of a sound system
1) Establish the required system functions on the basis of the user’s needs.
2) Analyse the characteristics of the environment
3) Choose the loudspeakers on the basis of the nature and dimensions of the space, the type of message to be transmitted (speech/music), and the noise level of the
environment.
4) Choose amplifiers that are suitable for driving the speakers selected and with a sufficient number of inputs for all the sounds sources.
5) Define the sound sources (microphones, tuners, cassette, players, etc.).
6) Evaluate the connection system for the speakers and establish cable sections.
It is advisable to begin your study of a sound system with the loudspeakers, after which the amplifier power and model can be defined, and finally the sound sources and appropriate connection system can be selected.Specifically, you
need to
The The Sound Sound System System Design Design
flow chartflow chart
Speaker Placement
There are essentially two types of speaker system;
A centrally located system
A distributed system/multi point diffusion
Centrally Located Centrally Located SystemSystemMinimize the Minimize the
Reverberant field but Reverberant field but can result in long can result in long speaker/listener speaker/listener
distancesdistances
Need for Loudness Need for Loudness CalculationCalculation
Need for Coverage Need for Coverage CalculationCalculation
9 x H1315 9 x H1315 Central Central Cluster Cluster
Distributed Distributed systemsystem Increase the Reverberant Increase the Reverberant
field, lower the field, lower the speaker/listener distancespeaker/listener distance
Small-medium size Small-medium size spacesspaces
MQ60H: 180MQ60H: 18000 coverage, 97dB coverage, 97dB
3m away3m away
DM61: 120DM61: 12000 coverage, 96dB coverage, 96dB 3m away IP553m away IP55
Medium-Large size Medium-Large size spacesspaces
Speaker positioning in corridorsSpeaker positioning in corridors
MQ30P: 92dB after MQ30P: 92dB after 10 m10 m
h
l r
Square compact
S
Hexagonal compact
S
Square Edge-to-Edge
S
Hexagonal Edge-to-Edge
S
2rS
3rS
rS 2
rS 2
2tan)(
lhr
Several RAIN DIFFUSION Several RAIN DIFFUSION coveragecoverage
• A rule of thumb for distributed system is calculate the ratio
CoverageSpea
TotalAreaN
ker
1m 2m 4m 8m 16m1m 2m 4m 8m 16m
90dB90dB 66dB66dB78dB78dB84dB84dB 72dB72dB
1m 2m 4m 8m 16m1m 2m 4m 8m 16m
996dB6dB 772dB2dB884dB4dB990dB0dB 778dB8dB
1m 2m 4m 8m 16m1m 2m 4m 8m 16m
93dB93dB 69dB69dB81dB81dB87dB87dB 75dB75dB
1W1W
44WW
2W2W
SPL 1W/1mSPL 1W/1mrPSensrSPL log20log10)(
Line Loss and Wire Section
The load is considered to be concentrated at the end ofthe line. If the speakers are distributed alongthe line, the section can be almost halved.
Thank you for your kind attention!
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