Ljud i byggnad och samhälle (VTAF01)
– Building Acoustics (Part 1 – Sound Insulation)
Juan Negreira
Concept Developer – Ecophon (Spain)
Visiting Lecturer – Lund University (Sweden)
… recap from past lectures
• Time & frequency domains
• Narrow band & Octaves & 1/3-octave
• Sound pressure level (SPL / L
p)
– Hand held (measurements)
• Sound intensity level (SIL / L
I)
– Plane/cylindrical/spherical prop.
• SWL / SPL / SIL
• Diffuse field
L" = 10 log )p+
p,-.+ = 20 log )p p,-.
L
0= 10 log I
I
2Outline
Introduction
Airborne Sound Insulation
Impact Sound Insulation
Conclusions
Introduction (I)
• Sound transmission
– Airborne
– Structure-borne
• Transmission paths
– Direct transmission (D)
– Flanking paths (F
i)
P
iIncident wave power P
rReflected wave power P
tTransmitted wave power
P
aPower reduction due to absorption
Introduction (II)
Introduction (III)
Transmission coefficient:
Absorption coefficient:
Reflection coefficient:
[-]
i
a
P
P a =
i
t
P
P t =
[-]
[-]
i
r
P
P r =
= 1 +
+ r a
t
Introduction (IV)
i
t
P
P t =
Reduction index:
Outline
Introduction
Airborne Sound Insulation
Impact Sound Insulation
Conclusions
DEF: Reverberation time
• Reverberation time
– Time for sound to decrease 60 dB from initial level
» “Clarity vs. Intensity” compromise
– Not necessarily coincident with listener feeling – Why 60 dB?
– Values dependent on ussage
» Ex: general auditorium: 1.5 - 2.5 sec.
– Calculation (Sabine’s law)
= å
=
=
i
i i
eff
f S
V f
A f V
T f
RT 0 . 16 ( )
) 16 (
. 0 ) ( )
(
60a
V: room volume / Aeff: effective absorption area / : individual absorption coefficients / Si: surface of each element with
ai
ai T20 / T30 ?
DEF: Reverberation time
• Reverberation time
= å
=
=
i
i i
eff
f S
V f
A f V
T f
RT 0 . 16 ( )
) 16 (
. 0 ) ( )
(
60a
V: room volume / Aeff: effective absorption area / : individual absorption coefficients / Si: surface of each element with
ai
ai
Nomenclature
• R(f): sound reduction index (laboratory)
• R
w: weighted sound reduction index (laboratory)
• R’(f) : apparent sound reduction index (in-situ)
• R’
w: weighted apparent sound reduction index (in-situ)
• D
nT(f): standardised level difference (in-situ)
• D
nT,w: weighted standardised level difference (in-situ)
• C
50-3150: spectrum adaptation term
• C
tr: spectrum adaptation term due to traffic noise
Statement of results: R’
w(C
50-3150; C
tr) / R
w(C
50-3150; C
tr) / D
nT,w(C
50-3150; C
tr)
”Rule of thumb”: Difference between lab and in-situ ~4 dB!
NOTE: There are more single-number indicators, but they are not included here to not make it even more complicated (see ISO 717-1:2013) NOTE2: ”to normalise” means ”to scale” with a reference area of 10 m2, whereas when ”standardising” a reference T60of 0.5 s is used
NOTE3: In the course, for the sake of simplicity, DnTwill not be used, we will stick to R and R’.
NOTE4: a prime (’) next to R/Rwis used to distinguish between in-situ and lab measurements respectively.
Measurement sound reduction index (I)
L
S(f) : SPL in the sending room [dB]
L
R(f) : SPL in the receiving room [dB]
S : wall area [m
2]
A(f) : Absorption area in receiving room [m
2]
Wall’s reduction index [dB]
(= transmission loss):
÷÷ø çç ö
è + æ
-
= ( ) ( ) 10log ( )
)
( A f
f S L f
L f
R S R
NOTE: Loudspeaker and microphone positions are defined in the corresponding ISO standard.
In practice, A(f) is calculated by measuring T60(f)
Measurement sound reduction index (II)
• Example of (lab) measured curve:
‒ High values Þ Better insulation Þ ”Quieter”
÷÷ø çç ö
è + æ
-
= ( ) ( ) 10log ( ) )
( A f
f S L f
L f
R S R
÷ø ç ö
è + æ
-
= 0.5
) log (
10 ) ( )
( )
( T60 f
f L f
L f
DnT S R
Dn(f): level difference
NOTE: For in-situ measurements, the curve would be R’(f) instead, since it would account for flanking tranmission. In Sweden nowadays DnT(f)
and DnT,ware used instead of R’(f) for in-situ measurements, to correlate better with human perception. In this course, however, we will stick
to R(f) and R’(f) and thus Rwand R’w.
63 125 250 500 1000 2000 4000 15
20 25 30 35 40 45 50 55 60
Frequency [Hz]
R [dB]
ISO Evaluation of sound reduction index (I)
• Reference curve (ISO 717-1)
ISO Evaluation of sound reduction index (II)
*for measurements in 16 one-third-octave band. If measurements are performed in 5 octave bands, the sum should not exceed 10 dB.
“[…] the reference curve is shifted in steps of 1dB towards the measured one, until the sum of the unfavourable deviations is as large as possible, but not more than 32dB*”
“[…] an unfavourable deviation at a
particular frequency occurs when the result of measurements is less than the reference value”
“[…] the value, in dB, of the reference curve
has at 500 Hz, after shifting in accordance
with this procedure, is R
w”
Spectrum adaptation terms
• Defined in ISO 717-1: take into account different source spectra
− C
tr: A-weighted urban traffic noise spectrum
− C
50-3150: frequency adaptation term
w i
Ri
Li R
C ÷-
ø ç ö
è - æ
=
å
=
- -
19 1
10 / ) ( 3150
50 10log 10
w i
Ri Li
tr R
C ÷÷ø-
çç ö è - æ
= 10log
å
10( - )/10Statement of results:
• R’
w(C
50-3150; C
tr)
• R
w(C
50-3150; C
tr)
NOTE: large negative values indicate poor airborne insulation at
low frequencies
Remember…
… Laboratory vs. Field situation (flanking transmission comes into play)
[REF] Vigran(2008)
ISO 717-1:2013 ISO 10140-2:2010
R
wISO 717-1:2013 ISO 16283-1:2014
R’
wSS-EN12354-1:2000
Prediction of R’wfrom the individual acoustic performances (Rw) of the elements involved in the junction, as sum of individual contributions
Airborne sound insulation – example
DEF: Combined reduction index
÷ ø ç ö
è
æ + +
-
= 1 ( 10
-10
-...)
log
10 S
1 R1/10S
2 R2/10R S
R
1, R
2… individual reduction indeces S: total area, i.e. S = S
1+S
2+…
Combined reduction index:
Leakages
• Power of the opening (leakage)
• The reduction index of the wall then becomes
S S
li
l
= P ×
P
÷ ø ç ö
è
æ +
× -
=
÷÷ Þ ø çç ö
è
æ +
P
× P -
÷÷ = ø çç ö
è æ
P P +
× P -
=
-
S R S
S R S
R l e
withLeakag
l i
t i
t l
10
10
/log 10
log 10 log
10
Example: influence of leakages
Sealing of windows is of crucial importance
NOTE: Example ofleakage detection
3 mm
1 2 30m
m
3 mm
0 5 10 15 20 25 30 35 40 45
100 160 250 400 630 1000 1600 2500
R (dB)
Frequency (Hz)
Unsealed window Sealed in 2 Sealed in 1 and 2
Exercises
2.- What is the influence of a crack in a wall whose dimensions are 1 mm in width and 1 m in length in a wall of 2.40 m height and 4 m length? The sound reduction index of the wall without leakage is 50 dB.
How much the combined sound reduction index would be if the sound reduction index of the wall would increase up to 60 dB?
1.- A 9 m
2facade has a sound reduction index of 60 dB and has installed a 1 m
2double window whose reduction index is 30 dB.
a) What does it mean that the material of the wall has a reduction index of 60dB? How much energy does the material let through?
b) Calculate the combined sound reduction index of the facade
Outline
Introduction
Airborne Sound Insulation
Impact Sound Insulation
Conclusions
Nomenclature
• L
n(f): normalised impact sound level (laboratory)
• L
n,w: weighted normalised impact sound level (laboratory)
• L’
n(f): apparent normalised impact sound level (in-situ)
• L’
n,w: weighted normalised impact sound level (in-situ)
• L’
nT(f): apparent standardised impact sound level (in-situ)
• L’
nT,w: weighted normalised impact sound level (in-situ)
• C
l,50-2500: spectrum adaptation term
Statement of results: L’
nT,w(C
l,50-2500) / L’
n,w(C
l,50-2500) / L
n,w(C
l,50-2500)
”Rule of thumb”: Difference between lab and in-situ ~4 dB!
NOTE: There are more single-number indicators, but they are not included here to not make it even more complicated (see ISO 717-2:2013) NOTE2: ”to normalise” means ”to scale” with a reference area of 10 m2, whereas when ”standardising” a reference T60of 0.5 s is used
NOTE3: LnTprovides a straightforward link to the subjective impression of impact sound insulation and is used as indicator in Sweden for field measurements. In the course, however, and to facilitate comparisons, we will stick to Lnand L’n
NOTE4: a prime (’) next to an L indicator is used to distinguish between in-situ and lab measurements respectively
Measurement impact sound insulation (I)
L
n(f): normalised impact sound level [dB]
L
R(f): SPL in the receiving room [dB]
A(f): absorption area in the receiving room
÷ ø ç ö
è + æ
= 10
) log (
10 )
( )
( A f
f L f
L
n RImpact sound level:
• ISO Tapping Machine
‒ Standardised: 1 hit per 0.1 s
‒ 5 steel cylinders which alternatively hit the floor
NOTE: Tapping machine and microphone positions are defined in the pertinent ISO standard.
Measurement impact sound insulation (II)
• Example of measured curve:
‒ High values Þ Higher sound transmission Þ ” Noisier”
0 10 20 30 40 50 60 70
100 160 250 400 630 1000 1600 2500
Ln[dB]
Frequency [Hz]
ISO Evaluation of impact sound insulation (I)
• Reference curve (ISO 717-2)
ISO Evaluation of impact sound insulation (II)
*for measurements in 16 one-third-octave band. If measurements are performed in 5 octave bands, the sum should not exceed 10 dB.
“[…] the reference curve is shifted in steps of 1dB towards the measured one, until the sum of the unfavourable deviations is as large as possible, but not more than 32dB*”
“[…] an unfavourable deviation at a
particular frequency occurs when the result of measurements exceed the reference value”
“[…] the value, in dB, of the reference curve
has at 500 Hz, after shifting in accordance
with this procedure, is L
n,w”
Spectrum adaptation term
• Defined in ISO 717-2
− C
I,50-2500: improves correlation with subjective response at low frequencies
Statement of results:
• L’
nT,w(C
l,50-2500)
• L’
n,w(C
l,50-2500)
• L
n,w(C
l,50-2500)
NOTE: large positive values indicate poor impact insulation at low frequencies
w n f
i Ln
l L
C 2500 ,
50
10 / ) ( , 2500
50
, 10log 10 ÷-15-
ø ç ö
è
= æ
å
-
Remember…
… Laboratory vs. Field situation (flanking transmission comes into play)
[REF] Vigran(2008)
ISO 717-2:2013 ISO 10140-3:2010
L
n,wISO 717-2:2013 ISO 16283-2:2014
L’
n,wSS-EN12354-2:2000
Prediction of L’n,wfrom individual acoustic performances (Ln,w)
Sound classes (Sweden)
• Ljudklass A: the soundclass corresponds to very good acoustic conditions
• Ljudklass B: it comprises slightly better acoustic conditions than
soundclass BBR. Certain individuals can still, in some cases, be disturbed.
This sound class is the minimum if good living environment is requested
• Ljudklass BBR: this is the minimum requirements in Swedish buildings
• Ljudklass D: corresponds to noise conditions that are intended to be
applied when sound class C cannot be achieved, e.g. in connection with
some refurbishment works
BBR and SS 25267:2004
Ljudkrav för bostäder A [dB]
B [dB]
BBR [dB]
(D) [dB]
Luftljudsisolering 61 57 53 49
Stegljudsnivå 48 52 56 60
Installationsbuller 22/27 26/31 30/35 30/35
Trafikbuller 22/37 26/41 30/45 34/49
*Installation and traffic noise have not been addressed in this lecture. For more information about how to measure and evaluate, see the correspondent ISO standards
Example from SS 25267:2004 – Sound class A
NOTE: Nowadays, there is a newer version of the standard, i.e. SS 25267:2015, which uses DnT,wand L’nT,was single number indicators for field measurements. However and as previously stated, in the course we will stick to R’wand Ln,wto be able to compare
in-situ and laboratory measurements in a more straightforward way.
The problem: lack of harmonisation (I)
[REF] Rasmussen(2010)
The problem: lack of harmonisation (II)
[REF] Rasmussen(2010)
Outline
Introduction
Airborne Sound Insulation
Impact Sound Insulation
Conclusions
Conclusions
• ISO procedures (sound insulation)
– Airborne sound insulation – Impact sound insulation
NOTE: Check out theacoustic glossary
References (I)
ISO 10140 series:
• ISO (2010), ISO 10140-1: Acoustics – Laboratory measurement of sound insulation of
building elements – Part 1: Application rules for specific products, International Organization for Standardization, Geneva, Switzerland.
• ISO (2010), ISO 10140-2: Acoustics – Laboratory measurement of sound insulation of building elements – Part 2: Measurement of airborne sound insulation, International Organization for Standardization, Geneva, Switzerland.
• ISO (2010), ISO 10140-3: Acoustics – Laboratory measurement of sound insulation of building elements – Part 3: Measurement of impact sound insulation, International Organization for Standardization, Geneva, Switzerland.
• ISO (2010), ISO 10140-4: Acoustics – Laboratory measurement of sound insulation of building elements – Part 4: Measurement procedures and requirements, International Organization for Standardization, Geneva, Switzerland.
• ISO (2010), ISO 10140-5: Acoustics – Laboratory measurement of sound insulation of building elements – Part 5: Requirements for test facilities and equipment, International Organization for Standardization, Geneva, Switzerland.
References (II)
ISO 717 series:
• ISO (2013), ISO 717-1: Acoustics – Rating of sound insulation in buildings and of building elements – Part 1: Airborne sound insulation, International Organization for Standardization, Geneva, Switzerland.
• ISO (2013), ISO 717-2: Acoustics – Rating of sound insulation in buildings and of building elements – Part 1: Impact sound insulation, International Organization for Standardization, Geneva, Switzerland.
ISO 16283 series:
• ISO (2014), ISO 16283-1: Acoustics – Field measurement of sound insulation in buildings and of building elements – Part 1: Airborne sound insulation, International Organization for
Standardization, Geneva, Switzerland.
• ISO (2014), ISO 16283-2: Acoustics – Field measurement of sound insulation in buildings and of building elements – Part 2: Impact sound insulation, International Organization for
Standardization, Geneva, Switzerland.
• ISO (2014), ISO 16283-3: Acoustics – Field measurement of sound insulation in buildings and of building elements – Part 3: Façade sound insulation, International Organization for
Standardization, Geneva, Switzerland.