Flow and Flow Noise Analysis of HSM by Using CAA++

Transactions of the Korean Society for Noise and Vibration Engineering.
2014.
Mar,
24(3):
205-212

- Received : November 22, 2013
- Accepted : January 22, 2014
- Published : March 20, 2014

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In this paper, sunroof buffeting analysis for Hyundai simple model(HSM) is studied computationally. For validation, the velocity profile of boundary layer around the opening of HSM was obtained and compared with experimental results. The analysis of sunroof buffeting is done in two parts. First a steady state solution is obtained using the Reynolds Averaged Navier Stokes (RANS) solver, and then the computed flow field information is used as input for CAA++. Second transient simulation by CAA++ is performed for the peak sound pressure levels and peak frequencies of buffeting noise over the ranges of flow velocities. The benchmark results of frequency and sound pressure levels showed the general phenomena and matched well with the experimental data obtained by Hyundai Motor Car.
Geometries of HSM
Dimension of HSM opening
The experimental tests were performed for following results.
• The boundary velocity profiles at hot-wire positions denoted with A, B and C as illustrated in
Fig. 3
, when the cavity opening is closed. In this case, experiment is performed when flow velocity is 60 km/h.
• Frequency Response Test for estimating the acoustic resonance frequency and Q-factor of HSM cavity, when the cavity opening is opened and free stream velocity is 0 km/h.
• Sunroof buffeting SPL and frequencies over a range of flow velocities. In this case, frees stream flow velocities are 20, 30, 40, 50, 60, 70, 80, 90, and 100 km/h. The 1st peak SPL and frequencies are tested at the positions of microphone in
Fig. 3
.
Positions of hot-wire for boundary layer profile and microphone for sunroof buffeting
The resonance frequency of 27.6 Hz and Q-factor of 10.52 are obtained by Frequency Response Test.
Figure 4
shows the comparison with two Q-factors of 10.52 and 105.2, when cavity is analogized with a simple spring-mass system with the resonant frequency of 27.6 Hz. As shown in
Fig. 4
, HSM can be assumed as a high acoustic absorbing and dissipating system. In numerical analysis, failure to consider acoustic energy loss in the interior of HSM can be anticipated to result in many differences with experimental results from
Fig. 4
.
Damped acoustic pressure in the cases of Q factor of 10.52 and 105.2
A simple cavity as illustrated in
Fig. 5
is the practical example to estimate discrete tones related to fluid dynamic oscillation and flow modes generated around HSM opening. The frequencies of fluid dynamic oscillations are approximated by Rossister, 1964 in reference
^{(3)}
, as follows,
where
U_{∞}
is the free stream velocity and
L
is cavity opening length. The parameter
k
is empirically approximated to 0.56, which is the ratio of convective velocity to free stream velocity. Equation (1) calculates frequency of
n^{th}
mode based on the parameter
n
which can be approximated as the number of vortex near opening area.
M_{∞}
is free stream Mach number and can be neglected because of
M_{∞}
≪1.
Two dimensional simple cavity
Acoustic modes and acoustic resonant frequencies can be easily obtained from Helmholtz equations by numerical analysis with considering real geometries of HSM, in the form.
Here Φ
_{m}
is
m^{th}
acoustic mode,
f_{m}
is
m^{th}
acoustic resonant frequency and
c
is the speed of sound. Acoustics modes of a cavity are a special case in which a standing wave is established near the mouth opening area and the interior of the cavity. Each acoustic frequency and acoustic mode is
m^{th}
eigenvalue and eigenvector of Helmholtz equation with homogeneous boundary conditions. The numerical method is explained in reference
^{(2)}
in detail. In this study, the inverse power method was applied for this eigenvalue problem.
The 1st acoustic mode and acoustic velocities around HSM opening are shown in (a) and (b) of
Fig. 6
and the second acoustic mode is illustrated in
Fig. 7
. The 1st acoustic resonance frequency was calculated as 28.3 Hz and the 2nd frequency as 104.1 Hz. As shown in (b) of
Fig. 6
, the flow of the 1st acoustic mode near the HSM opening flows up and down according to acoustic pressure of the cavity interior.
Acoustic 1st mode
Acoustic pressure of acoustic 2nd mode
At certain flow speeds, the vortex shedding frequency coincides with the acoustic resonance frequency of cavity. In this case, large pressure fluctuation is generated and the flow around opening area is strongly influenced by acoustic field. This state is known as acoustic locked flow. The typical phenomena of acoustics locked flow are large magnitude of unsteady pressure fluctuations above the dynamic pressure and periodic vortex formations as acoustic resonance frequency.
Figure 8
shows three possible resonance regions obtained from Eq. (1) and acoustic resonant frequencies as marked red circle. Possibilities to be several regions of acoustic locked flows in the cavity flows can be found in reference
^{(1)}
. As shown
Fig. 8
, vortex shedding frequency increases according to the free stream velocity but acoustic resonant frequency is independent of flow velocities.
Possible resonance regions
^{(4)}
.
Pressure data at the location of microphone is recorded at every time step and then the 1st peak SPL and frequency are obtained from the acoustic pressure data. Fast Fourier transform(FFT) tool is used to get frequency spectrum from the simulated data.
SPL is defined as following relation. Here
p
is the perturbation amplitude and
p_{ref}
= 2×10
^{−6}
Pa.
The time step for NLAS computation is set to be 3×10
^{−4}
, which provides sufficient stability on existing mesh and resolve all possible 1st and 2nd acoustic resonant frequencies.
The domain is decomposed into 4 parts to do parallel computations on 4 processors. This case was run on 4 processors by using about the number of 400,000 meshes. The approximate turnaround time for this unsteady simulation was around 48 hours.
Boundary layer velocity profile when flow velocity 60 km/h
Steady state flow results when flow velocity 60 km/h
The 1st peak frequencies and SPL according to free stream velocities are compared with the experimental results supplied by HMC in
Figure 11
.
1st peak SPL and resonance frequencies
As the flow velocity is increased from zero, the peak SPL increase approximately linearly with flow velocity in all of the numerical and experimental results. The 1st peak SLP reach to the maximum value at the free stream velocity of 50 km/h in experimental results. And the SPL decreases as the flow velocity increases. But in the case of numerical results, the maximum 1st SPL was calculated at the free stream velocity of 60 km/h. The maximum SPL of numerical analysis was over estimated as the value of 135 dB which is 6 dB greater than the experimental results.
In current state, the main cause of this difference is attributed to simulation under the assumption which HSM is an un-damped system. The experimental results include the effects of the small Q-factor caused by large acoustic energy dissipation generated in the interior of HSM.
The acoustic locked flows are generated in wider range of velocities than the experimental results because of no considering the effects of small Q-factor. These phenomena are found in the undamped system as reference
^{(2)}
. (b) in
Figure 11
compares the 1st peak frequencies of the experimental and numerical results. And (c) shows the 1st and 2nd peak frequencies in the interior of cavity and near the opening of the cavity.
All results of experiment and numerical simulation show only region II in
Fig. 8
is activated as dominant acoustic locked flow over the range of flow velocities. But in flow velocity of 20 km/h or 30 km/h, a weak acoustic locked flow denoted as region I in
Fig. 8
overlapped with the dominant acoustic locked flow can be anticipated because the frequencies of these ranges are close to 1st acoustic resonant frequency. This kind of example can be found in reference
^{(1,2)}
.
In the case of experiment, the 1st peak frequency at the free stream velocity of 20 km/h can be estimated to show the characteristics of the 2nd mode of flow. But the result of frequency at 30 km/h is attributed to abrupt change of the flow state from the 2nd to the 1st flow mode. In the case of numerical analysis compared with the experiment, the frequencies at these two velocities were predicted as the frequencies of the flow 2nd mode.
The 1st peak frequencies at the position of the microphone do not clearly show the natural frequency by Strouhal number. In the cases of flow velocity of 90 and 100 km/h, it is very difficult to define the flow state is the acoustic locked flow or not by only considering the frequency of the interior of cavity. But the peak frequency of the vortex shedding near the HSM opening precisely shows the Rossiter’s relations as (c) in
Fig. 11
. In the case of numerical simulation, the flow state above the flow velocity of 90 km/h can be anticipated to escape from the influence of acoustic fields.
# A part of this paper was presented at the KSNVE 2012 Annual Autumn Conference
Young-Nam Kim received Ph.D. degree in Aerospace Engineering from Korea Advanced Institute of Science and Technology in 2012. He is the CEO of Flow＆Noise Inc. and he has been working in the field of CFD and CAA since 1995.
Jun-Hee Chae received M.A. degree in Mechanical Engineering from Korea Aerospace University in 1996. He is working as the Technical Support Manager of Flow＆Noise Inc. and he has been working in the field of CFD since 1996.

1. Introduction

Sunroof buffeting is typical example of cavity noise. The cavity noise is generated by coupling hydrodynamic self-sustained oscillation flows around the cavity opening which act as acoustic sources and acoustic modes which are generated in cavity as acoustic resonator. Hydrodynamic self-sustained oscillations of the separated shear layer near the opening of the cavity can excite the resonant acoustic modes of the cavity. Flow-acoustic resonance occurs when the frequency of the self-sustained shear layer oscillations is close to the acoustic resonant frequency of the cavity. High amplitude pressure oscillations and the formation of regular and distinct vortex structures are fundamental characteristics of the acoustic locked flows in the cavity.
In case of automobiles, it is generally known that buffeting frequency is about 25 Hz and sound pressure level(SPL) is above 100 dB.
In recent application, researchers are using computational aero acoustics(CAA) approach. But CAA simulation requires highly expensive and time-consuming computations on dense grid. CAA++ was developed to overcome these difficulties by Metacomp Technologies Inc, which is used in conjunction with computational fluid dynamics( CFD) to simulate unsteady flow and aeroacoustic noise. CAA++ can be applied to general aeroacoustic problems such as broad band noise, discrete tone noise and acoustic resonance problems. Furthermore, CAA++ can reduce computational times and enhance the accuracy by confining computational domain size near acoustic sources, using non-reflecting boundary conditions, coarse mesh and synthetic turbulence model.
The purpose of this study is to perform computational aeroacoustic simulations with HSM and compare the analysis results to the experimental results provided by HMC(Hyundai Motor Company). After validation of boundary layer velocity profile through the steady state simulation by CFD++, the present study investigates sunroof buffeting noise of HSM.
The cavity of HSM contains many acoustic absorbing materials in the interior, which Q-factor is very low compared with the cases of general cavities. But in this study, the prediction of the buffeting frequencies and the corresponding sound pressure levels(SPL) were simulated as the case of neglecting acoustic dissipation in the interior of HSM.
2. Benchmark Problem

All experiments for HSM have been performed in Hyundai Aeroacoustic Wind Tunnel. The dimensions of HSM are shown as illustrated in
Fig. 1
. Thick acoustic absorbing materials are adhered on all inner walls of HSM cavity for considering the same order of acoustic absorbing and dissipation effects as a real car interior. The details of the cavity opening are shown as
Fig. 2
.
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3. Numerical Analysis

- 3.1 Steady State

Steady compressible Reynolds averaged Navier-Stokes(RANS) equations are used to simulate the flow fields of HSM in commercially available solver CFD++(Metacomp Technologies). The two equation cubic k-turbulence model is used for the steady RANS flows. This case was run on 4 processors using about the number of 1,200,000 meshes. The approximate turnaround time for this simulation was around 4 hours. The domain is decomposed into 4 parts to do parallel computations on 4 processors.
- 3.2 Transient Analysis

CAA++ non linear acoustic solver(NLAS) is used for the HSM buffeting noise simulations. The steady state solutions obtained from the steady state RANS by CFD++ is used to provide the initial conditions for unsteady calculation, the mean flow field, acoustic boundary conditions and turbulent statistics for the small scale turbulent acoustic source for NLAS simulations. In general, NLAS uses a confined computational domain by using non-reflecting boundary conditions because acoustic sources only exist around the cavity region.
NLAS is based on viscous non-linear perturbation equations made from compressible unsteady Navier-Stokes equations. Flow with large scale is calculated directly and smaller turbulent scales than grid size are modeled by the synthetic turbulent model (4). Detailed equations and explanations referring to NLAS are described in reference
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4. Results ＆ Discussions

The steady state results were obtained when free stream velocity 60 km/h. And the boundary layer velocity profiles are compared with the experimental results at the positions denoted in
Fig. 3
.
Figure 9
shows the boundary layer mesh used for numerical analysis and the boundary layer velocity profiles compared with experimental results. All the numerical and experimental results show the boundary layer thickness increases according to distance from the beginning of HSM opening and numerical results predicts the boundary layer velocity profile with reasonable accuracy.
Figure 10
shows the surface pressure and local velocity vectors around the front of HSM. The results show the strong vortex lines are formed near the front of HSM and A-pillar.
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5. Conclusions

The acoustic resonant mode and frequencies was predicted by numerical analysis of Helmholtz equation. The acoustic resonant frequency was accurately estimated when compared to experiments. Flow natural frequency of the vortex shedding near the opening of HSM was estimated by theoretical approach considering a simple cavity model.
The map of acoustic resonant locked flow is suggested by using the numerical results of acoustic resonance mode and frequency, and Rossiter’s relation. This map shows three resonant flow states are possible as increasing free stream velocity.
Steady state flow analysis was conducted for validation at the flow velocity of 60 km/h. the boundary layer velocity profiles are exactly predicted compared with the experiments.
In the transient analysis, the 1st peak SPL and frequencies in the position of microphone were compared with the experimental results. The maximum SPL is over predicted and the acoustic locked flows are estimated in more wide range of flow velocity compared with the experiments. The 1st peak frequency at the flow velocity of 30 km/h shows lower value than the experiment.
The cause of the difference between numerical and experimental results is attributed to simulation without considering the acoustic dissipation in the interior of HSM. But in this study, numerical results suggest the reasonable explanation of the buffeting process and acoustic locked flows for an undamped system.
Acknowledgements

We are thankful to HMC for supplying the experimental results in this study.

BIO

Velikorodny A.
,
Yan T.
,
Oshkai P.
2010
Quantitative Imaging of Acoustically Coupled Flows Over Symmetrically Located Side Branches
Exp Fluids
48
245 -
264
** DOI : 10.1007/s00348-009-0731-5**

Stoneman S. A. T.
,
Hourigan K.
,
Stokes A. N.
,
Welsh M. C.
1988
Resonant Sound Caused by Flow Past Two Plates in Tandem in a Duct
J. Fluid Mech
192
455 -
484
** DOI : 10.1017/S0022112088001946**

Rossister J. E.
1964
Wind Tunnel Experiments of the Flow over Rectangular Cavities at Subsonic and Transonic Speeds, Aero. Res. Counc. R & M., 3438

Batten P.
,
Ribaldone E.
,
Casella M.
,
Chakravarthy S
2004
Towards a Generalized Non-linear Acoustics Solver, AIAA 2004-3001
10th AIAA/ CEAS Aeroacoustics Conference

2008
CFD++ User Manual, Version 10.1.2
Metacomp Technologies
USA

Ryu K. W.
,
Lee J. S.
2002
Numerical Analysis of the Unsteady Pressure fluctuation Generated from the Interaction between a Vortex Flow with a Forward Step
Transactions of the Korean Society for Noise and Vibration Engineering
12
(3)
213 -
220
** DOI : 10.5050/KSNVN.2002.12.3.213**

Citing 'Flow and Flow Noise Analysis of HSM by Using CAA++
'

@article{ SOJDCM_2014_v24n3_205}
,title={Flow and Flow Noise Analysis of HSM by Using CAA++}
,volume={3}
, url={http://dx.doi.org/10.5050/KSNVE.2014.24.3.205}, DOI={10.5050/KSNVE.2014.24.3.205}
, number= {3}
, journal={Transactions of the Korean Society for Noise and Vibration Engineering}
, publisher={The Korean Society for Noise and Vibration Engineering}
, author={김, 영 남
and
채, 준 희}
, year={2014}
, month={Mar}