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Acoustics (VTAN01) HT2 (2019/2020)
01log110
)log()log(
logloglog
loglog)log(
0
=
=
⋅=
−=⎟⎟⎠
⎞⎜⎜⎝
⎛
+=⋅
xnx
yxyx
yxyx
n
Formulae – Acoustics VTAN01
TABLE OF CONTENTS
I) Some logarithmic rules: 1
II) Fundamental acoustic definitions 1 II.1) Frequency bandwidths, weighted sound pressure level 3 II.2) One dimensional wave propagation 4
III) Room acoustics 5 III.1) Inside a room : reflection and transmission 5 III.2) Between two rooms: sound isolation and absorption 7
I) Some logarithmic rules:
yxy
x
yxyx
x
x
y
xx
xxy
−
+
=
⋅=
=
=
=⇔=
101010
10101010
)10log(10log
log
II) Fundamental acoustic definitions Sound pressure - One-dimensional harmonic plane sound field:
- Effective value (RMS, Root Mean Square) for sound pressure in a point: NOTE: For a harmonic wave,
Sound pressure level SPL - Sound pressure level: , where pref = 2·10-5 Pa (pref : approximately the quietest sound a young undamaged human hearing can detect at 1000 Hz)
- Equivalent sound level:
⎟⎠
⎞⎜⎝
⎛ +−= ϕω
ω xc
tptxp cosˆ),(
∫Δ+
Δ=
tt
t
dttxpt
p0
0
),(1~ 2
⎟⎟⎠
⎞⎜⎜⎝
⎛=⎟
⎟⎠
⎞⎜⎜⎝
⎛= ∫∫
TtL
T
refTeq dt
Tdt
ptp
TL p
0
10/)(
02
2
, 101log10)(1log10
⎟⎟⎠
⎞⎜⎜⎝
⎛= 2
2~log10
refp p
pL
2/ˆ~ pp =
;2 fπω =λπω /)2(/ == ck;/ fc=λ
;/1 Tf =
Acoustics (VTAN01) HT2 (2019/2020)
- Summing of two sound sources (if uncorrelated the last term vanishes):
SPL difference (dB) between 2 sources 0 1 2 3 4 5 6 7 8 9 10 Added dB to the highest SPL 3 2,54 2,12 1,76 1,46 1,19 0,97 0,79 0,64 0,51 0,41 - Summing of N uncorrelated sources:
- Phon curves:
Figure 1 – Phon curves
Sound intensity
- The sound energy Π and sound intensity I is )()()()()(
)()()(tvtptI
SttI
tvtFt⋅=⇒
⎪⎭
⎪⎬
⎫
Π=
⋅=Π
- The sound power level and sound intensity level are calculated (in decibels) according to
⎟⎟⎠
⎞⎜⎜⎝
⎛
Π
Π=Π
ref
L log10 and ⎟⎟⎠
⎞⎜⎜⎝
⎛=
refI I
IL log10 , where Π ref = 10-12 W and Iref = 10-12 W/m2.
Relation (function of the directivity factor Q) between Lp and L∏ : .4,3,2,1;4
log10 2 =⎟⎠
⎞⎜⎝
⎛+=Π Q
rQLL p π
∫Δ+
Δ++=
tt
ttot dttptp
tppp
0
0
)()(2~~~21
22
21
2
⎟⎠
⎞⎜⎝
⎛= ∑
=
N
n
Ltotp
npL1
10/,
,10log10
Acoustics (VTAN01) HT2 (2019/2020)
The time mean values are: ∫ ⋅=ΠT
dttvtpTS
0
)()( and ∫ ⋅=T
dttvtpT
I0
)()(1
- For a wave propagating in the positive x-direction, the previous integral yields: cpI ρ2~= ,
with c being the speed of sound in m/s and cZ ρ= the specific acoustic impedance.
cair =γP0
ρair (T = 0!)1+ Tair[
!C]2 ⋅273
"
#$
%
&'= 331.4 ⋅ 1+
Tair[!C]
2 ⋅273"
#$
%
&'
II.1) Frequency bandwidths, weighted sound pressure level II.1.a) Octave bands and third octave bands:
II.1.b) Weighed sound level:
Figure 2 - A-, B-, C- and D-weightings (10 Hz – 20 kHz).
( )∑ += 10/)(10log10 weighingLweighed
nL
Acoustics (VTAN01) HT2 (2019/2020)
II.2) One dimensional wave propagation
The general form of the equation of motion in fluids and solid media (applying Newton’s 2nd law) is
tv
xp
∂
∂−=
∂
∂ρ ; p: pressure, ρ: specific mass, ν: fluid particle velocity
For fluids, the relation between pressure and particle velocity is
xvP
tp
∂∂
−=∂∂
0γ ; γ = adiabatic index (γ air =1.4)
For solid media we have the corresponding relation between force and displacement
xuESF∂
∂−= ; E: modulus of elasticity, S: surface
II.2.a) Waves in fluid media
- For a longitudinal wave propagating in air (one dimensional propagation in positive x-direction) expressed with sound pressure and particle velocity, respectively, as the field variables are:
012
2
22
2
=∂
∂⋅−
∂
∂
tp
cxp
2
22
2
2
xvc
tv
∂
∂⋅=
∂
∂
where ργ 0Pc = is the propagation speed for the pressure wave in the air, with P0 being the atmospheric pressure. The general solution to the wave equation (with p being the field variable) is
)/()/(),( cxtpcxtptxp ++−= −+
The harmonic solution to the wave equation in complex form is
)()( ˆˆ),( kxtikxti epeptxp +−
−+ += ωω
For physical interpretation, take the real part of the result, where
+p̂ and −p̂ are the pressure amplitudes for
the waves propagating in positive and in negative direction, respectively. ω is the angular frequency and ck ωλπ == 2 is the wave number. This yields the equality λfc =
- Specific acoustic impedance is defined as vpZ ≡
- For a wave propagating in air (1-D propagation in positive x-direction) the acoustic impedance is
cvpZ ρ==+
+
Acoustics (VTAN01) HT2 (2019/2020)
II.2.b) Waves in solid media
-For longitudinal and waves (infinite medium) and quasi-longitudinal waves (finite medium), their wave equations read, respectively:
02
2
2
2
=∂
∂⋅−
∂
∂
tv
xv
E xx ρ
0' 2
2
2
2
=∂
∂⋅−
∂
∂
tv
xvE xx ρ
The propagation speed for longitudinal waves is ρEcL = , whereas for quasi-longitudinal waves it is
)1(' 2υρρ −== EEcqL , υ being the Poisson’s ratio of the material where the wave is propagating through. Particle displacement, particle velocity, strain or force can be used instead of pressure as a field variable in the wave equation.
- For shear waves the wave equation can be expressed using the transversal displacement w as:
02
2
2
2
=∂
∂⋅−
∂
∂
tw
Gxw ρ where
ρGcsh = , G being the shear modulus of the material.
)1(2 υ+=
EG
- For bending waves in beams and plates the wave equation in one dimension is
02
2
4
4
=∂
∂+
∂
∂
twS
xwB ρ
where
12
3bhEB = for a rectangular cross section.
The propagation speed depends on the frequency (dispersive waves), i.e.
4)(SB
kc f ρ
ωω
ω ⋅==
III) Room acoustics
III.1) Inside a room: reflection and transmission
III.1.a) Standing waves, eigenfrequencies
At normal incidence on a hard surface the pressure function is
tiekxptxp ω⋅= + )cos(ˆ2),(
and the particle velocity function
( ) )2/(sinˆ2),( πω −+ ⋅= tiekxvtxv
The Helmholtz equation: 0)()( 22
2
=+∂
∂ xpkxxp has, in the one dimensional case with two hard boundary
surfaces at x = 0 and x = L the solution
tfi nexLnBtxp ππ 2cos),( ⋅⎟
⎠
⎞⎜⎝
⎛=
Acoustics (VTAN01) HT2 (2019/2020)
where fn are the resonance frequencies Lnccf
nn 2
==λ
For the three dimensional case with six hard boundary surfaces the eigenfrequencies are
222
,, 2⎟⎠
⎞⎜⎝
⎛+⎟⎟
⎠
⎞⎜⎜⎝
⎛+⎟
⎠
⎞⎜⎝
⎛=
Hn
Bn
Lncf zyx
nnn zyx
nx, ny and nz being indexes indicating the order mode in each direction of the room (L, B and H).
In transmission from one medium with wave impedance Z1 = ρ1c1 to another medium with wave impedance Z2 = ρ 2c2 the transmission factor t and reflection factor r are given, respectively, as:
12
2
1122
22 22ˆˆ
ZZZ
ccc
pp
ti
t
+=
+==
ρρρ
12
12
1122
1122
ˆˆ
ZZZZ
cccc
ppri
r
+
−=
+
−==
ρρρρ
while the transmission coefficient τ and reflection coefficient ρ is
( ) ( )212
122
1122
1122 44ZZZZ
cccc
II
i
t
+=
+
⋅==
ρρ
ρρτ
( ) ( )212
212
21122
21122
ZZZZ
cccc
II
i
r
+
−=
+
−==
ρρ
ρρρ
III.1.b) Eigenfrequencies types:
Axial modes 1D Tangential modes 2D Oblique modes 3D Figure 3 – Related geometry of eigenfrequencies
Source: Sengpielaudio
III.1.c) Reverberation time
Reverberation time can be estimated by using Sabine’s formula. Sabine based his empirical formula on the sound decay of 60 dB (1/1000 SPL) after the abruptly end of a test tone (shot, shooting, etc.).
𝑇"#(𝑓) = 0,16 𝑉
𝐴(𝑓)
with: V: volume of the room in cubic meters A: effective absorption area of the room in square meter: 𝐴(𝑓) = ∝0(1). 𝑆04
056 with Si : surface of every absorption element; αi(f): absorption coefficient of each element
Acoustics (VTAN01) HT2 (2019/2020)
III.2) Between two rooms: sound isolation and absorption
III.2.a) Airborne sound insulation
- Sound reduction index R:
- Measurement of sound reduction index R of a wall of surface S:
- Spectrum adaptation term: Li given in Fig.6
-Traffic spectrum adaptation term: Li given in Fig.6
- Combined R of a wall of surface S made by different elements (Si):
- Slot leakage:
- The mass law for a single leaf wall:
- The mass law for a double leaf wall:
- Coincidence frequency (critical frequency):
III.2.b) Impact sound insulation
- Measurement of step sound level L:
- Spectrum adaptation term:
NOTE: A prime (´) in the parameters R/L and its related ones means measurements performed in situ, whereas the same letter without the prime refers to measurements performed in the laboratory.
⎟⎟⎠
⎞⎜⎜⎝
⎛+−=
)(log10)()()(
fASfLfLfR recsend
⎟⎠
⎞⎜⎝
⎛+=10)(log10)()( fAfLfL recn
⎟⎠
⎞⎜⎝
⎛=⎟⎟⎠
⎞⎜⎜⎝
⎛
Π
Π=
τ1log10log10
t
iR
⎟⎟⎠
⎞⎜⎜⎝
⎛⎟⎠
⎞⎜⎝
⎛−= ∑ −
i
fRi
iSS
fR 10/)(1101log10)(
⎟⎠
⎞⎜⎝
⎛+⋅−= −
SSfR sfR 10/)(10log10)(
hKBmcfc /
2
20 =
ʹ′ʹ′=
π
002log40)(
cmffRρπ ʹ′ʹ′
≈
002log20)(
cmffRρπ ʹ′ʹ′
≈
wnfiLn
l LC ,
2500
50
10/)(,250050, 1510log10 −−⎟
⎠
⎞⎜⎝
⎛= ∑−
wi
RiLi RC −⎟⎠
⎞⎜⎝
⎛−= ∑
=
−−
19
1
10/)(315050 10log10
wi
RiLitr RC −⎟⎟
⎠
⎞⎜⎜⎝
⎛−= ∑ − 10/)(10log10
hm ρ=''
)1(121 2
3
2 υυ −=
−=
EhIEB
Acoustics (VTAN01) HT2 (2019/2020)
III.2.c) ISO-REFERENCE CURVES Airborne sound isolation
Measurement of sound reduction index:
Figure 4 – Reference curve for air borne sound insulation (ISO 717-1)
Impact sound isolation
Measurement of step sound level Ln:
Figure 5 – Reference curve for step sound insulation (ISO 717-2)
⎟⎠
⎞⎜⎝
⎛+=10)(log10)()( fAfLfL recn
⎟⎟⎠
⎞⎜⎜⎝
⎛+−=
)(log10)()()(
fASfLfLfR recsend
Acoustics (VTAN01) HT2 (2019/2020)
Figure 6 – Spectra for calculating the spectrum adaptation terms for different frequency spectra (ISO 717-1)
Acoustics (VTAN01) HT2 (2019/2020)