• Aucun résultat trouvé

A. Debray Contribution to the study of dissipative silencers : effect of structural vibrations, effect of flow 2000

N/A
N/A
Protected

Academic year: 2022

Partager "A. Debray Contribution to the study of dissipative silencers : effect of structural vibrations, effect of flow 2000"

Copied!
137
0
0

Texte intégral

(1)
(2)
(3)
(4)
(5)

x hard wall

d y

(6)

frequency (Hz) frequency (Hz)

0 2000 4000 6000 8000 10000

ï150 ï100 ï50 0

0 2000 4000 6000 8000 10000

0 50 100 150 200

(7)

R z

r

hard wall

(8)

frequency (Hz) frequency (Hz)

0 2000 4000 6000 8000 10000

ï200 ï150 ï100 ï50 0

0 2000 4000 6000 8000 10000

0 50 100 150 200

(9)
(10)
(11)
(12)
(13)
(14)
(15)
(16)
(17)
(18)
(19)
(20)
(21)
(22)
(23)
(24)

porous material

L

0 z

perforated

screen

(25)
(26)
(27)

0 0.2 0.4 0.6 0.8 1 0

0.2 0.4 0.6 0.8 1

a Rh(a)

(28)

frequency (Hz) frequency (Hz)

0 500 1000 1500

ï25 ï20 ï15 ï10 ï5 0

0 500 1000 1500

0 10 20 30 40 50

frequency (Hz) frequency (Hz)

0 500 1000 1500

ï75 ï70 ï65 ï60 ï55 ï50 ï45 ï40 ï35

0 500 1000 1500

0 10 20 30 40 50

radial position (m) radial position (m)

0 0.01 0.02 0.03 0.04 0.05

ï0.5 ï0.4 ï0.3 ï0.2 ï0.1 0 0.1 0.2

0 0.01 0.02 0.03 0.04 0.05

0.9 0.92 0.94 0.96 0.98 1

(29)

radial position (m) radial position (m)

0 0.01 0.02 0.03 0.04 0.05

ï0.5 0 0.5 1 1.5 2

0 0.01 0.02 0.03 0.04 0.05

0 2 4 6 8 10 12 14 16 18

(30)
(31)

z

0

(32)
(33)

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

(34)
(35)
(36)
(37)
(38)

wall rigid impervious porous material

Front view Side view

(39)
(40)
(41)
(42)
(43)

.

.

.

.

.

.

(44)
(45)
(46)
(47)
(48)
(49)
(50)
(51)

hard wall

(52)
(53)
(54)
(55)

. . .

.

.

.

(56)
(57)
(58)
(59)
(60)

frequency (Hz) frequency (Hz)

0 200 400 600 800 1000

ï10 ï8 ï6 ï4 ï2 0

0 200 400 600 800 1000

0 20 40 60 80 100 120 140

(61)

5 10 15 20 25 30 35 40 45 ï16

ï14 ï12 ï10 ï8 ï6 ï4 ï2 0

0 20 40 60 80

ï9 ï8 ï7 ï6 ï5 ï4 ï3 ï2 ï1 0

(62)

frequency (Hz) frequency (Hz)

0 200 400 600 800 1000

ï10 ï8 ï6 ï4 ï2 0

0 200 400 600 800 1000

0 20 40 60 80 100 120 140

(63)

5 10 15 20 25 30 35 40 ï25

ï20 ï15 ï10 ï5 0

0 10 20 30 40 50 60

ï10 ï8 ï6 ï4 ï2 0

(64)

0 0.5 1 1.5 2 2.5 3 ï200

ï150 ï100 ï50 0 50 100 150 200

mode 1 mode 2

mode 3

(65)

ï20 ï1.5 ï1 ï0.5 0 0.5 1 1.5 2 0.5

1 1.5 2 2.5 3

x=1

x=0

30.4 30.6 30.8 31 31.2 31.4 31.6 31.8 32

ï1.2 ï1 ï0.8 ï0.6 ï0.4 ï0.2 0 0.2 0.4

x=1

x=0

(66)

51.6 51.8 52 52.2 52.4 52.6 52.8 53 53.2 53.4 ï0.4

ï0.2 0 0.2 0.4 0.6 0.8 1 1.2

1.4

x=0

x=1

x x

0 0.2 0.4 0.6 0.8 1

0 0.2 0.4 0.6 0.8 1 1.2 1.4

0 0.2 0.4 0.6 0.8 1

0 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08

(67)

x x

0 0.2 0.4 0.6 0.8 1

ï0.5 ï0.4 ï0.3 ï0.2 ï0.1 0

0 0.2 0.4 0.6 0.8 1

31.25 31.3 31.35 31.4 31.45

x x

0 0.2 0.4 0.6 0.8 1

ï0.8 ï0.7 ï0.6 ï0.5 ï0.4 ï0.3 ï0.2 ï0.1 0

0 0.2 0.4 0.6 0.8 1

52.35 52.36 52.37 52.38 52.39 52.4

(68)
(69)
(70)
(71)
(72)
(73)
(74)
(75)
(76)
(77)
(78)
(79)
(80)
(81)

imaginary part of impedance

real part of impedance

frequency (Hz) frequency (Hz)

0 1000 2000 3000 4000 5000

ï30 ï25 ï20 ï15 ï10 ï5 0 5

0 1000 2000 3000 4000 5000

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2

imaginary part of impedance

real part of impedance

frequency (Hz) frequency (Hz)

0 1000 2000 3000 4000 5000

ï35 ï30 ï25 ï20 ï15 ï10 ï5 0 5

0 1000 2000 3000 4000 5000

0 0.5 1 1.5 2 2.5 3 3.5

(82)

imaginary part of impedance

real part of impedance

frequency (Hz) frequency (Hz)

0 1000 2000 3000 4000 5000

ï30 ï25 ï20 ï15 ï10 ï5 0 5

0 1000 2000 3000 4000 5000

0 0.5 1 1.5 2 2.5

(83)
(84)

termination

muffler

acoustic source

acoustic source downstream 4 microphones upstream

fan

thermometer thermometer

PC

HP 3566/67 A flowmeter

anechoic 4 microphones

lined expansion

chamber

(85)
(86)

frequency (Hz) frequency (Hz)

modulus of T

modulus of R

0 500 1000 1500

10ï5 10ï4 10ï3 10ï2 10ï1 100

0 500 1000 1500

0.4 0.45 0.5 0.55 0.6 0.65 0.7 0.75 0.8

frequency (Hz) frequency (Hz)

modulus of T

modulus of R

0 500 1000 1500

10ï3 10ï2 10ï1 100

0 500 1000 1500

0.35 0.4 0.45 0.5 0.55 0.6 0.65 0.7 0.75 0.8

frequency (Hz) frequency (Hz)

modulus of T

modulus of R

0 500 1000 1500

10ï4 10ï3 10ï2 10ï1 100

0 500 1000 1500

0.35 0.4 0.45 0.5 0.55 0.6 0.65 0.7 0.75 0.8

(87)

frequency (Hz) frequency (Hz)

modulus of T

modulus of R

0 500 1000 1500

0.3 0.4 0.5 0.6 0.7 0.8 0.9

0 500 1000 1500

10ï8 10ï6 10ï4 10ï2 100

modulus of R modulus of T

frequency (Hz) frequency (Hz)

0 500 1000 1500

10ï3 10ï2 10ï1 100

0 500 1000 1500

0.65 0.7 0.75 0.8 0.85 0.9

(88)

modulus of R modulus of T

frequency (Hz) frequency (Hz)

0 500 1000 1500

10ï3 10ï2 10ï1 100

0 500 1000 1500

0.65 0.7 0.75 0.8 0.85 0.9

modulus of R modulus of T

frequency (Hz) frequency (Hz)

0 500 1000 1500

10ï4 10ï3 10ï2 10ï1 100

0 500 1000 1500

0.65 0.7 0.75 0.8 0.85 0.9

modulus of R modulus of T

frequency (Hz) frequency (Hz)

0 500 1000 1500

10ï4 10ï3 10ï2 10ï1 100

0 500 1000 1500

0.65 0.7 0.75 0.8 0.85 0.9

(89)

D C B

A

(90)
(91)

frequency (Hz) frequency (Hz)

0 500 1000 1500

ï60 ï50 ï40 ï30 ï20 ï10 0

0 500 1000 1500

0 50 100 150 200

frequency (Hz) frequency (Hz)

0 500 1000 1500

ï12 ï10 ï8 ï6 ï4 ï2 0

0 500 1000 1500

0 5 10 15 20 25 30 35 40 45

(92)

frequency (Hz) frequency (Hz)

0 500 1000 1500

ï12 ï10 ï8 ï6 ï4 ï2 0

0 500 1000 1500

0 5 10 15 20 25 30 35 40

frequency (Hz) frequency (Hz)

0 500 1000 1500

ï50 0 50 100 150 200

0 500 1000 1500

ï60 ï50 ï40 ï30 ï20 ï10 0

(93)
(94)
(95)
(96)

Multi-layered or porous material

Impervious rigid wall

Plane wave

(97)

10 cm 3 cm material 1 3 cm

material 1

(98)

0 200 400 600 800 1000 0

0.1 0.2 0.3 0.4 0.5 0.6 0.7

m=100000

frequency (Hz)

Absorption

m=300000

m=10000

m=1000

1002 103 104

10 20 30 40 50 60

frequency (Hz)

Attenuation (dB/m)

(99)

lining

102 103 104

0 10 20 30 40 50 60

frequency (Hz)

Attenuation (dB/m)

(100)

1002 103 104 10

20 30 40 50 60

frequency (Hz)

Attenuation (dB/m)

1002 103 104

0.2 0.4 0.6 0.8 1

frequency (Hz)

Absorption

(101)

3 cm

3 cm 20 cm

material 1

material 1

(102)

1002 103 104 10

20 30 40 50 60 70

frequency (Hz)

Attenuation (dB/m)

0 500 1000 1500 2000 2500 3000

0 0.2 0.4 0.6 0.8 1

frequency (Hz)

Absorption

(103)

0 200 400 600 800 1000 10

20 30 40 50 60 70 80

frequency (Hz)

Attenuation (dB/m)

2000 400 600 800 1000

20 40 60 80 100 120

frequency (Hz)

Attenuation (dB/m)

(104)

0 200 400 600 800 0

0.1 0.2 0.3 0.4 0.5 0.6 0.7

frequency (Hz)

Absorption

0 200 400 600 800

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8

frequency (Hz)

Absorption

(105)

2 cm 20 cm 2.81 cm

2.81 cm material 1

plate material 3

2 cm

0 200 400 600 800

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

frequency (Hz)

Absorption

(106)

0 200 400 600 800 0

1 2 3 4 5 6 7 8 9

frequency (Hz)

Attenuation (dB/m)

(107)
(108)
(109)
(110)
(111)
(112)
(113)

II I

L

III porous material

z=L z=0

a b

z

(114)
(115)
(116)
(117)

ï4000 ï2000 0 2000 4000 ï1500

ï1000 ï500 0 500 1000 1500

ï30 ï20 ï10 0 10 20 30

ï100 ï50 0 50 100

(b) (a)

ï600 ï400 ï200 0 200 400 600 ï800

ï600 ï400 ï200 0 200 400 600 800

ï5 0 5

ï60 ï40 ï20 0 20 40 60 80

(b)

(a)

(118)
(119)
(120)
(121)
(122)
(123)
(124)

0 500 1000 1500 0.3

0.4 0.5 0.6 0.7 0.8 0.9 1

0 500 1000 1500

10

ï3

10

ï2

10

ï1

10

0

(125)

0 500 1000 1500 0.2

0.3 0.4 0.5 0.6 0.7 0.8 0.9

0 500 1000 1500

10

ï4

10

ï3

10

ï2

10

ï1

10

0

(126)
(127)

0 500 1000 1500 0.3

0.4 0.5 0.6 0.7 0.8 0.9 1

0 500 1000 1500

10

ï3

10

ï2

10

ï1

10

0

(128)

0 500 1000 1500 0.2

0.3 0.4 0.5 0.6 0.7 0.8 0.9

0 500 1000 1500

10

ï4

10

ï3

10

ï2

10

ï1

10

0

(129)
(130)
(131)
(132)
(133)
(134)
(135)
(136)
(137)

Références

Documents relatifs

Effects caused by the necessarily finite grain size used in simulations of flew m porous media are systematically Studied in Dvo dimensional hydrodynamic cellular automata vnth

It is difficult in general to calculate the prop- erties of phonons in disordered systems, but it is possible to do so in the long wavelength limit using a Debye approximation

(GODELIER, 2004 : 194-195). Au cœur de la dynamique locale, on s'interroge sur la reproduction sociale et matérielle, sur les stratégies de reproduction dans des contextes

In addition to the increase in particle delivery to the diseased lobe, a greater number of particles deposited in the 3D domain in the localized diseased cases compared to the

A convenient extension of the Wessely–Moser rearrangement for the synthesis of substituted alkylaminoflavones as neuroprotective agents in vitro.. Ronan Larget, Brian Lockhart,

Elle permet en particulier de minorer le nombre de certains points spéciaux ou de certaines droites concourantes, comme le nombre de sommets ou de droites nor- males concourantes,

Le tableau ci-dessous, extrait de [1], donne pour chaque système de racines irréductible réduit les multiplicités des racines simples dans la plus haute racine positive, et les

Thus the experiment leads to the measurement of the variation of the Stokes force Fx exerted on a sphere of radius a moving, at a constant velocity Ux, at a