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Brüel & Kjær 2003, 1 Simulation of Couplers by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas Schuhmacher Brüel & Kjær AES, Workshop 7, 2003 March 23rd

by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

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Page 1: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 1

Simulation of Couplers

bySøren Jønsson, Bin Liu, Lars B. Nielsen,

Andreas SchuhmacherBrüel & Kjær

AES, Workshop 7, 2003 March 23rd

Page 2: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 2

AgendaIntroduction to CouplersTraditional Simulation using LPMFEM/BEM SimulationComparison of ResultsConclusion

Page 3: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 3

Introduction to Couplers

Critical properties of Acoustic Couplers

Must allow for REPEATABLE measurementsMust be possible to CALIBRATEMust be ACCURATE and STABLEShould be STANDARDIZED

Design to improve voice quality & intelligibilityDesign to meet telecom & audio standardsComparison of transducers, headsets, handsets, earphones etc.

Page 4: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 4

Introduction to Couplers

Acoustic Couplers overview

IEC 318 (ITU-T P.57 Type 1) Ear Simulator

IEC 711 (ITU-T P.57 Type 2) Ear Simulator

ITU-T P.57 Type 3.1 Concha bottom Simulator

ITU-T P.57 Type 3.2 Simplified Pinna Simulator

ITU-T P.57 Type 3.3 Pinna Simulator

Increasing realism

&complexity

Page 5: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 5

Ear Simulators and Standards

Ear Anatomy and Definitions

97010 0 200 500 2k 5k1k-20

-10

0

10

20

30

dB

F requency Sensitivi ty Respon se for Ty pe 4185 , re 1 kHz Open Ear Frequen cy Sensitivity Respon se Closed E ar Freque ncy Sensitivity Respon se

(Hz)

VolumesConcha 4.3 cm3

Ear canal 1.0 cm3

Behind drum 0.65 cm3

Total ear 6.0 cm3

Page 6: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 6

Ear Simulators and StandardsITU-T Type 2 - IEC 711 occluded ear simulator- Standardized - accepted as a reference worldwide- Bruel & Kjær Type 4157 (and used in 4158/59/95)- Intented for calibration of insert earphones, sealed and unsealed (hearing aids)in the frequency range from 100-7.000Hz

- Simulates the ear canal from app. 10mm behind EEP and in

97010 0 200 500 2k 5k1k-20

-10

0

10

20

30

dB

F requency Sensitivi ty Respon se for Ty pe 4185 , re 1 kHz Open Ear Frequen cy Sensitivity Respon se Closed E ar Freque ncy Sensitivity Respon se

(Hz)

Page 7: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 7

Ear Simulators and Standards

97010 0 200 500 2k 5k1k-20

-10

0

10

20

30

dB

F requency Sensitivi ty Respon se for Ty pe 4185 , re 1 kHz Open Ear Frequen cy Sensitivity Respon se Closed E ar Freque ncy Sensitivity Respon se

(Hz)

~170u

~69u

IEC 711 coupler:Requirements in according to standard:

Acoustical transfer impedance specified

Equivalent volume at 500Hz equal to 1.26cm3

With of principal volume 7.5mm

Length of principal volume must produce ½-wavelength resonance at 14kHz, i.e. ~12.4mm

Page 8: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 8

Ear Simulators and Standards

IEC711 couplerSetup for measuring transfer impedance

Page 9: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 9

Ear Simulators and StandardsIEC-711 coupler typical measured data with tolerance curves from IEC60711

-5

0

5

10

15

20

25

30

35

40

100 1000 10000 100000

Frequency (Hz)

dB

TypicalLower Tolerance Upper Tolerance

Page 10: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 10

Traditional Simulation Using LPM

2,

8,6,4,2

cnaa

c

aaaat

at

ZCMAcZ

CCCc

VC

=

=

++==

ρρ

Ear-canal impedance:Tube w. ridgid walls analogto an LC transmissionline, i.e:

Page 11: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 11

Traditional Simulation Using LPM

ablj

banlZa

ρω5612

3 +=

Narrow slitsEar drum impedance:Two slits terminated by volumes,i.e. RLC-helmholtz resonatorstuned to match drum-impedance

Page 12: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 12

Traditional Simulation Using LPM

Fr e q u e n c y

1 0 0 Hz 2 0 0 Hz 3 0 0 Hz 4 0 0 Hz 6 0 0 Hz 8 0 0 Hz 2 . 0 KHz 3 . 0 KHz 5 . 0 KHz 7 . 0 KHz 1 0 KHz 2 0 KHzDB( I r ( Ra 5 ) / ( I ( Ra 5 ) * I ( Ra 5 ) ) ) DB( - I i ( Ra 5 ) / ( I ( Ra 5 ) * I ( Ra 5 ) ) )

1 0 0

1 5 0

2 0 0

SEL>>

i ma g

r e a l

Ac o u s t i c i mp e d a n c e o f s l i t 1

DB( I r ( Ra 7 ) / ( I ( Ra 7 ) * I ( Ra 7 ) ) ) DB( - I i ( Ra 7 ) / ( I ( Ra 7 ) * I ( Ra 7 ) ) )

1 5 0

2 0 0

1 0 1

I ma g

r e a l

Ac o u s t i c i mp e d a n c e o f s l i t 2

Page 13: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 13

Traditional Simulation Using LPM

IEC-711 couplerLPM simulationUndamped resp.

Fr e q u e n c y

1 0 0 Hz 1 . 0 KHz 1 0 KHz 2 0 KHzd b ( V( o u t * f ) )

- 4 0

- 2 0

0

2 0

4 0

5 0

Page 14: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 14

Traditional Simulation Using LPM

Page 15: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 15

Traditional Simulation Using LPM

IEC-711 couplerLPM simulationDamped response

Fr e q u e n c y

1 0 0 Hz 1 . 0 KHz 1 0 KHz 2 0 KHzDB( V( o u t * f ) )

- 1 0

0

1 0

2 0

3 0

4 0

5 0

Tr a n s f e r i mp e d a n c e o f I EC7 1 1 c o u p l e r

Page 16: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 16

Transfer impedance simulation (LPM)IEC-711 coupler: Measured data and simulated data using LPM

-10

0

10

20

30

40

50

100 1000 10000 100000

Frequency (Hz)

dB

Measured dataLPM-simulation

Page 17: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 17

Standard FEM Simulation

Numerical model solving the Helmholtz equation inside the couplerModels the air inside without visco-thermal effects (loss-free)Allows for computation of acoustic modes (frequency and mode shape)

Page 18: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 18

Transfer impedance simulation (FEM)

Frequency response ([email protected]) of full model

-30-20-10

01020304050

100 1000 10000 100000

Frequency (Hz)

Pre

ssu

re (

dB

) re

f. @

500H

z 1373 Hz

5052 Hz12800 Hz

Page 19: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 19

Visco-Thermal fluid

Thermal conductivity and viscosity play a role near the boundariesThe thermal & viscous mode only exist within a small boundary layerIn large spaces, the acoustic mode dominates

Acoustic mode

Boundary layerThermal + Viscous + Acoustic mode

Boundary

Page 20: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 20

Visco-Thermal FEM

Finite Element model based on the narrow gap equation- const. pressure/zero particle velocity in thickness direction- small gap width compared with acoustic wavelengthNo need to mesh in the thickness direction Includes visco-thermal effects

Thin Slit 2D FE Model

Page 21: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 21

Visco-Thermal FEM – Test Case

2.57 mm

1.11 mm

Thickness: 0.17 mm

Page 22: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 22

2D FE model of Slit

hard wall

hard wall

open endnormal velocityexcitation

hard wall

Page 23: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 23

Simulation on SlitAcoustic input impedance – FE simulations vs. lumped-parameter model

Page 24: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 24

Coupler ModelMixed FEM/BEM model (4818 elements & 2337 nodes)

Page 25: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 25

Model Setup

Vibrating piston

Response point (for transfer impedance simulation)

Page 26: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 26

Coupler Response @ 1000 HzSound pressure map

Page 27: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 27

Frequency Response

Page 28: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 28

Conclusion

A complete BEM/FEM model of the IEC 711 coupler (B&K Type 4157) taking visco-thermal effects into account was presented.

Comparison between a measurement and simulation of the transfer impedance show excellent agreement.

A more correct and detailed 3D simulation of the coupler can be done using BEM/FEM compared to traditional LPM.

The performance of virtual couplers can be evaluated at the veryearly design stage using the proposed BEM/FEM technique.

Page 29: by Søren Jønsson, Bin Liu, Lars B. Nielsen, Andreas

Brüel & Kjær 2003, 29

Any Questions ?