Explanation of Acoustical Principles¶
Introduction¶
Model¶
Model description¶
Name |
Pos X |
Pos Y |
Pos Z |
Units |
---|---|---|---|---|
Source |
-50 |
0 |
2 |
m |
Receiver |
50 |
0 |
2 |
m |
Symbol |
Value |
Units |
Comment |
---|---|---|---|
Distance S/R |
100 |
m |
|
Distance ref |
1 |
m |
|
Source height |
2 |
m |
|
Receiver height |
2 |
m |
|
dp |
100 |
m |
distance S->R Projected on the ground |
Calculation parameters for 3 reference modelizations¶
All acoustic calculations were carried out under homogeneous conditions.
Ground reflection case without screen
Model 1 : acoustic propagation with ground reflection and without screen
Symbol |
Value |
Units |
Comment |
---|---|---|---|
Gs |
0 |
ground factor 9613-2 source region |
|
Gr |
0 |
ground factor 9613-2 receiver region |
|
Gm |
0 |
ground factor 9613-2 intermediate region |
|
σe |
20000 |
kRayls, flow resistivity |
|
e |
1 |
m |
ground thickness |
dp1 |
50 |
m |
ground distance source -> reflection point; Descartes’ law: tan β = hs/dp1 = hr/(dp-dp1) |
cos β |
0.999200959 |
cosine of the ground reflection angle |
|
sin β |
0.03996803 |
||
length |
100.079968 |
m |
reflected path length |
Screen case
Model 2 : acoustic propagation with ground reflection and thin screen between the source and the receiver
Name |
Value |
Units |
Comment |
---|---|---|---|
Single thin screen |
|||
Position |
(-25, 10) à (-25,-10) |
||
Screen/source distance |
25 |
m |
|
Screen height |
8 |
m |
|
e |
0.3 |
m |
screen thickness |
9613-2 calculation parameters
Symbol |
Value |
Units |
Comment |
---|---|---|---|
a* |
0 |
m |
component of the distance parallel to the edge of the screen between the source and the receiver (9613-2) |
ll |
10 |
m |
perpendicular horizontal dimension SR left |
lr |
10 |
m |
horizontal dimension perpendicular SR right |
dSS,top |
25.71 |
m |
distance between the source and the first diffraction edge for the vertical path |
dSR,top |
75.24 |
m |
distance between the second diffraction edge and the receiver for the vertical path |
dSS,lat |
26.93 |
m |
distance between source and first diffraction edge for side paths |
dSR,lat |
75.66 |
m |
distance between second diffraction ridge and receiver for side paths |
Note
The component a corresponds to the component of the distance along the y axis. In our example, it is zero, but in general it is not.
Reflection case
Name |
Value |
Units |
Comment |
---|---|---|---|
Position |
(-52,10) à (-52,-10) |
||
β_reflex |
0.0 |
rad |
angle of incidence |
ρ_reflex |
1.0 |
acoustic reflection coefficient |
|
l_min |
8.0 |
m |
minimum reflective length dimension |
dS,O |
1.85 |
m |
source distance to reflection point |
dO,R |
101.85 |
m |
distance from reflection point to receiver |
DIr |
0 |
source directivity index -> receiver image |
Acoustic¶
Source spectrum |
Source directivity |
|||
---|---|---|---|---|
Frequency |
Lw(fc) dB re 1 pW |
W(fc) W |
Module |
Phase |
16 Hz |
0 |
1E-12 |
1 |
0 |
20 Hz |
0 |
1E-12 |
1 |
0 |
25 Hz |
0 |
1E-12 |
1 |
0 |
31.5 Hz |
0 |
1E-12 |
1 |
0 |
40 Hz |
0 |
1E-12 |
1 |
0 |
50 Hz |
80 |
0.0001 |
1 |
0 |
63 Hz |
80 |
0.0001 |
1 |
0 |
80 Hz |
80 |
0.0001 |
1 |
0 |
100 Hz |
80 |
0.0001 |
1 |
0 |
125 Hz |
80 |
0.0001 |
1 |
0 |
160 Hz |
80 |
0.0001 |
1 |
0 |
200 Hz |
80 |
0.0001 |
1 |
0 |
250 Hz |
80 |
0.0001 |
1 |
0 |
315 Hz |
80 |
0.0001 |
1 |
0 |
400 Hz |
80 |
0.0001 |
1 |
0 |
500 Hz |
80 |
0.0001 |
1 |
0 |
630 Hz |
80 |
0.0001 |
1 |
0 |
800 Hz |
80 |
0.0001 |
1 |
0 |
1 kHz |
80 |
0.0001 |
1 |
0 |
1.25 kHz |
80 |
0.0001 |
1 |
0 |
1.6 kHz |
80 |
0.0001 |
1 |
0 |
2 kHz |
80 |
0.0001 |
1 |
0 |
2.5 kHz |
80 |
0.0001 |
1 |
0 |
3.15 kHz |
80 |
0.0001 |
1 |
0 |
4 kHz |
80 |
0.0001 |
1 |
0 |
5 kHz |
80 |
0.0001 |
1 |
0 |
6.3 kHz |
80 |
0.0001 |
1 |
0 |
8 kHz |
80 |
0.0001 |
1 |
0 |
10 kHz |
80 |
0.0001 |
1 |
0 |
12.5 kHz |
0 |
1E-12 |
1 |
0 |
16 kHz |
0 |
1E-12 |
Lw |
93.80 |
dB |
Atmospheric absorption¶
This part details the global and model-specific parameters for the calculation of atmospheric absorption
Weather parameters¶
Symbol |
Value |
Physical values |
---|---|---|
R |
8.31441 |
Ideal gas constant |
Absolute_zero |
273.15 |
Temperature 0°C in K |
M |
0.029 |
Molar mass of air |
y |
1.41 |
Ratio of the specific heats respectively at constant pressure and volume |
Reference atmospheric pressure |
101325 |
Pa |
Reference sound pressure |
293.15 |
K |
Reference sound pressure |
0.00002 |
Pa |
Reference sound power |
1E-12 |
W |
Specific model
Symbol |
Value |
Units |
---|---|---|
Temperature |
20 |
°C |
Pressure |
101325 |
Pa |
Hygrometry |
70 |
% humidity in the air |
Atmospheric attenuation calculation¶
Atmospheric attenuation in Iso 9613-1 Standard¶
Atmospheric attenuation in default Solver¶
Atmospheric attenuation in Code_TYMPAN¶
The calculations are identical to the note of the default solver. Note that in the Code_Code_TYMPAN implementation: * Modulus and phase calculation for each Aatmi third octav band. * The calculation being made in spectrum of p²(fc), the attenuation is squared.
Implementation¶
void AtmosphericConditions::compute_absorption_spectrum(): Calculates the atmospheric absorption spectrum α for the weather conditions of the model.
AtmosphericConditions::compute_length_absorption(double length) const: Returns the atmospheric attenuation spectrum in explicit state (physical quantity), corresponds to the Aatmi(f) of the DefaultSolver.
void TYChemin::calcAttenuation(const TYTabEtape& tabEtapes, const AtmosphericConditions& atmos): Calculates the atmospheric attenuation from the power spectrum of the source taking into account the directivity and as a function of the path length.
OSpectre TYTrajet::getPEnergetique(const AtmosphericConditions& atmos): Calculates the squared sound pressure spectrum, p²(fc). In energy, p²(fc) = W(fc)*divGeom*Aatmi(fc)²
Atmospheric calculation¶
Sound celerity calculation, c¶
Symbol |
Value |
Units |
Comment |
---|---|---|---|
tk |
293.15 |
K |
Temperature in Kelvin |
c |
344.25 |
m/s |
Sound speed |
Impedance calculation¶
Symbol |
Value |
Units |
Comment |
---|---|---|---|
ρ |
1.21 |
kg.m-3 |
Air density |
z |
415.02 |
kg.m-2s-1 |
acoustic specific characteristic impedance. Usually denoted z0 = ρ*c |
Note
In Code_TYMPAN ρ, the density of air, is calculated from the molar mass of air M and the weather conditions according to the following ideal gas formula: ρ = PM / RT
Atmospheric absorption¶
Mole fraction of water vapor
Symbol |
Value |
Units |
Comment |
---|---|---|---|
T01 |
273.16 |
K |
Isothermal temperature at the triple point |
Relative pressure |
1 |
Pa/Pa |
Relative pressure |
C |
-1.63712658 |
Exponent C, see Appendix B2 ISO 9613-1, dimensionless quantity |
|
Psat |
2336.630453 |
Pa |
Saturating vapor pressure |
h molar |
1.614252472 |
% |
Mole fraction of water vapor |
Atmospheric absorption spectrum
Symbol |
Value |
Units |
Comment |
---|---|---|---|
frO |
53173.95674 |
Hz |
Oxygen relaxation frequency |
frn |
460.9906921 |
Hz |
Nitrogen relaxation frequency |
Frequency |
Order |
Exact frequency |
f² |
α (dB.m-1) atmospheric absorption coefficient |
k (m-1) acoustic wave number |
---|---|---|---|---|---|
16 Hz |
0 |
15.8 |
251.2 |
5.75329E-06 |
0.289273495 |
20 Hz |
1 |
20.0 |
398.1 |
9.11237E-06 |
0.364173754 |
25 Hz |
2 |
25.1 |
631.0 |
1.44272E-05 |
0.458467594 |
31.5 Hz |
3 |
31.6 |
1000.0 |
2.2828E-05 |
0.577176504 |
40 Hz |
4 |
39.8 |
1584.9 |
3.60861E-05 |
0.726622168 |
50 Hz |
5 |
50.1 |
2511.9 |
5.69587E-05 |
0.914763112 |
63 Hz |
6 |
63.1 |
3981.1 |
8.96923E-05 |
1.151618528 |
80 Hz |
7 |
79.4 |
6309.6 |
0.000140718 |
1.449801829 |
100 Hz |
8 |
100.0 |
10000.0 |
0.000219517 |
1.825192365 |
125 Hz |
9 |
125.9 |
15848.9 |
0.000339472 |
2.29778105 |
160 Hz |
10 |
158.5 |
25118.9 |
0.000518179 |
2.892734954 |
200 Hz |
11 |
199.5 |
39810.7 |
0.000776135 |
3.641737544 |
250 Hz |
12 |
251.1 |
63095.7 |
0.001132366 |
4.584675937 |
315 Hz |
13 |
316.2 |
100000.0 |
0.001596482 |
5.771765042 |
400 Hz |
14 |
398.1 |
158489.3 |
0.002160413 |
7.266221682 |
500 Hz |
15 |
501.2 |
251188.6 |
0.002797920 |
9.147631123 |
630 Hz |
16 |
631.0 |
398107.2 |
0.003478850 |
11.51618528 |
800 Hz |
17 |
794.3 |
630957.3 |
0.004194039 |
14.49801829 |
1 kHz |
18 |
1000.0 |
1000000.0 |
0.004977810 |
18.25192365 |
1.25 kHz |
19 |
1258.9 |
1584893.2 |
0.005921435 |
22.9778105 |
1.6 kHz |
20 |
1584.9 |
2511886.4 |
0.007184447 |
28.92734954 |
2 kHz |
21 |
1995.3 |
3981071.7 |
0.009016418 |
36.41737544 |
2.5 kHz |
22 |
2511.9 |
6309573.4 |
0.011800116 |
45.84675937 |
3.15 kHz |
23 |
3162.3 |
10000000.0 |
0.016125980 |
57.71765042 |
4 kHz |
24 |
3981.1 |
15848931.9 |
0.022911167 |
72.66221682 |
5 kHz |
25 |
5011.9 |
25118864.3 |
0.033582957 |
91.47631123 |
6.3 kHz |
26 |
6309.6 |
39810717.1 |
0.050353926 |
115.1618528 |
8 kHz |
27 |
7943.3 |
63095734.4 |
0.076620551 |
144.9801829 |
10 kHz |
28 |
10000.0 |
100000000.0 |
0.117507392 |
182.5192365 |
12.5 kHz |
29 |
12589.3 |
158489319.2 |
0.180531919 |
229.778105 |
16 kHz |
30 |
15848.9 |
251188643.2 |
0.276238144 |
289.2734954 |
Atmospheric attenuation
Aatmos |
||
---|---|---|
Frequency |
||
16 Hz |
0.999934 |
28.927350 |
20 Hz |
0.999895 |
36.417375 |
25 Hz |
0.999834 |
45.846759 |
31.5 Hz |
0.999737 |
57.717650 |
40 Hz |
0.999585 |
72.662217 |
50 Hz |
0.999344 |
91.476311 |
63 Hz |
0.998968 |
115.161853 |
80 Hz |
0.998381 |
144.980183 |
100 Hz |
0.997476 |
182.519237 |
125 Hz |
0.996099 |
229.778105 |
160 Hz |
0.994052 |
289.273495 |
200 Hz |
0.991104 |
364.173754 |
250 Hz |
0.987048 |
458.467594 |
315 Hz |
0.981788 |
577.176504 |
400 Hz |
0.975434 |
726.622168 |
500 Hz |
0.968301 |
914.763112 |
630 Hz |
0.960740 |
1151.618528 |
800 Hz |
0.952862 |
1449.801829 |
1 kHz |
0.944302 |
1825.192365 |
1.25 kHz |
0.934099 |
2297.781050 |
1.6 kHz |
0.920614 |
2892.734954 |
2 kHz |
0.901401 |
3641.737544 |
2.5 kHz |
0.872970 |
4584.675937 |
3.15 kHz |
0.830558 |
5771.765042 |
4 kHz |
0.768147 |
7266.221682 |
5 kHz |
0.679337 |
9147.631123 |
6.3 kHz |
0.560055 |
11516.185278 |
8 kHz |
0.413902 |
14498.018294 |
10 kHz |
0.258501 |
18251.923651 |
12.5 kHz |
0.125124 |
22977.810498 |
16 kHz |
0.041573 |
28927.349543 |