Engineering Acoustics/Flow-induced oscillations of a Helmholtz resonator and applications

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The significance of movement excited acoustic resonance lies within the massive variety of functions by which it happens. Sound manufacturing in organ pipes, compressors, transonic wind tunnels, and open sunroofs are only some examples of the numerous functions by which movement excited resonance of Helmholtz resonators might be discovered.[4] An instability of the fluid movement coupled with an acoustic resonance of the cavity produce massive strain fluctuations which are felt as elevated sound strain ranges.
Passengers of highway automobiles with open sunroofs typically expertise discomfort, fatigue, and dizziness from self-sustained oscillations contained in the automotive cabin. This phenomenon is brought on by the coupling of acoustic and hydrodynamic movement inside a cavity which creates sturdy strain oscillations within the passenger compartment within the 10 to 50 Hz frequency vary. Some results skilled by automobiles with open sunroofs when buffeting embrace: dizziness, short-term listening to discount, discomfort, driver fatigue, and in excessive instances nausea. The significance of lowering inside noise ranges contained in the automotive cabin depends primarily in lowering driver fatigue and bettering sound transmission from leisure and communication gadgets.
This Wikibook web page goals to theoretically and graphically clarify the mechanisms concerned within the flow-excited acoustic resonance of Helmholtz resonators. The interplay between fluid movement and acoustic resonance shall be defined to supply a radical clarification of the conduct of self-oscillatory Helmholtz resonator programs. As an software instance, an outline of the mechanisms concerned in sunroof buffeting phenomena shall be developed on the finish of the web page.

As talked about earlier than, the self-sustained oscillations of a Helmholtz resonator in lots of instances is a steady interplay of hydrodynamic and acoustic mechanisms. Within the frequency area, the movement excitation and the acoustic conduct might be represented as switch features. The movement might be decomposed into two quantity velocities.

qr: movement related to acoustic response of cavity

qo: movement related to excitation

Determine 1 reveals the suggestions loop of those two quantity velocities.

Determine 1

Lumped parameter mannequin[edit]

The lumped parameter mannequin of a Helmholtz resonator consists of a rigid-walled quantity open to the setting by means of a small opening at one finish. The scale of the resonator on this mannequin are a lot lower than the acoustic wavelength, on this approach permitting us to mannequin the system as a lumped system.

the place re is the equal radius of the orifice.

Determine 2 reveals a sketch of a Helmholtz resonator on the left, the mechanical analog on the center part, and the electric-circuit analog on the appropriate hand facet. As proven within the Helmholtz resonator drawing, the air mass flowing by means of an influx of quantity velocity consists of the mass contained in the neck (Mo) and an end-correction mass (Mend). Viscous losses on the edges of the neck size are included in addition to the radiation resistance of the tube. The electrical-circuit analog reveals the resonator modeled as a compelled harmonic oscillator. [1] [2][3]

Determine 2

V: cavity quantity

ρ{displaystyle rho }

: ambient density

c: pace of sound

S: cross-section space of orifice

Ok: stiffness

Ma{displaystyle M_{a}}

: acoustic mass

Ca{displaystyle C_{a}}

: acoustic compliance

The equal stiffness Ok is said to the potential power of the movement compressed contained in the cavity. For a inflexible wall cavity it’s roughly:

The equation that describes the Helmholtz resonator is the next:

P^e{displaystyle {hat {P}}_{e}}

: excitation strain

M: whole mass (mass inside neck Mo plus finish correction, Mend)

R: whole resistance (radiation loss plus viscous loss)

From the electrical-circuit we all know the next:

The principle cavity resonance parameters are resonance frequency and high quality issue which might be estimated utilizing the parameters defined above (assuming free subject radiation, no viscous losses and leaks, and negligible wall compliance results)

The sharpness of the resonance peak is measured by the standard issue Q of the Helmholtz resonator as follows:

fr{displaystyle f_{r}}

: resonance frequency in Hz

ωr{displaystyle omega _{r}}

: resonance frequency in radians

L: size of neck

L’: corrected size of neck

From the equations above, the next might be deduced:

-The larger the quantity of the resonator, the decrease the resonance frequencies.

-If the size of the neck is elevated, the resonance frequency

Manufacturing of self-sustained oscillations[edit]

The acoustic subject interacts with the unstable hydrodynamic movement above the open part of the cavity, the place the grazing movement is steady. The movement on this part separates from the wall at some extent the place the acoustic and hydrodynamic flows are strongly coupled. [5]

The separation of the boundary layer at the forefront of the cavity (entrance a part of opening from incoming movement) produces sturdy vortices in the principle stream. As noticed in Determine 3, a shear layer crosses the cavity orifice and vortices begin to type as a result of instabilities within the layer at the forefront.

Determine 3

From Determine 3, L is the size of the interior cavity area, d denotes the diameter or size of the cavity size, D represents the peak of the cavity, and

δ{displaystyle delta }

describes the gradient size within the grazing velocity profile (boundary layer thickness).

The speed on this area is characterised to be unsteady and the perturbations on this area will result in self-sustained oscillations contained in the cavity. Vortices will regularly type within the opening area because of the instability of the shear layer at the forefront of the opening.

How are vortices fashioned throughout buffeting?[edit]

As a way to perceive the era and convection of vortices from the shear layer alongside the sunroof opening, the animation under has been developed. At a sure vary of movement velocities, self-sustained oscillations contained in the open cavity (sunroof) shall be predominant. Throughout this time period, vortices are shed on the trailing fringe of the opening and proceed to be convected alongside the size of the cavity opening as strain contained in the cabin decreases and will increase. Move visualization experimentation is one technique that helps acquire a qualitative understanding of vortex formation and conduction.

The animation under, reveals within the center, a facet view of a automotive cabin with the sunroof open. Because the air begins to movement at a sure imply velocity Uo, air mass will enter and go away the cabin because the strain decreases and will increase once more. On the proper hand facet of the animation, a legend reveals a variety of colours to find out the strain magnitude contained in the automotive cabin. On the prime of the animation, a plot of circulation and acoustic cavity strain versus time for one interval of oscillation is proven. The image x shifting alongside the acoustic cavity strain plot is synchronized with strain fluctuations contained in the automotive cabin and with the legend on the appropriate. For instance, each time the x image is positioned on the level the place t=0 (when the acoustic cavity strain is minimal) the colour of the automotive cabin will match that of the minimal strain within the legend (blue).


The perturbations within the shear layer propagate with a velocity of the order of 1/2Uo which is half the imply influx velocity. [5] After the strain contained in the cavity reaches a minimal (blue colour) the air mass place within the neck of the cavity reaches its most outward place. At this level, a vortex is shed at the forefront of the sunroof opening (entrance a part of sunroof within the route of influx velocity). Because the strain contained in the cavity will increase (progressively to pink colour) and the air mass on the cavity entrance is moved inwards, the vortex is displaced into the neck of the cavity. The utmost downward displacement of the vortex is achieved when the strain contained in the cabin can also be most and the air mass within the neck of the Helmholtz resonator (sunroof opening) reaches its most downward displacement. For the remainder of the remaining half cycle, the strain cavity falls and the air under the neck of the resonator is moved upwards. The vortex continues displacing in the direction of the downstream fringe of the sunroof the place it’s convected upwards and outdoors the neck of the resonator. At this level the air under the neck reaches its most upwards displacement.[4] And the method begins as soon as once more.

Methods to determine buffeting[edit]

Move induced checks carried out over a variety of movement velocities are useful to find out the change in sound strain ranges (SPL) contained in the automotive cabin as influx velocity is elevated. The next animation reveals typical auto spectra outcomes from a automotive cabin with the sunroof open at numerous influx velocities. On the prime proper hand nook of the animation, it’s potential to see the influx velocity and resonance frequency equivalent to the plot proven at that immediate of time.


It’s noticed within the animation that the SPL will increase progressively with rising influx velocity. Initially, the degrees are under 80 dB and no main peaks are noticed. As velocity is elevated, the SPL will increase all through the frequency vary till a particular peak is noticed round a 100 Hz and 120 dB of amplitude. That is the resonance frequency of the cavity at which buffeting happens. As it’s noticed within the animation, as velocity is additional elevated, the height decreases and disappears.
On this approach, sound strain degree plots versus frequency are useful in figuring out elevated sound strain ranges contained in the automotive cabin to seek out methods to attenuate them. Among the strategies used to attenuate the elevated SPL ranges achieved by buffeting embrace: notched deflectors, mass injection, and spoilers.

This hyperlink: [1] takes you to the web site of EXA Company, a developer of PowerFlow for Computational Fluid Dynamics (CFD) evaluation.

This hyperlink: [2] is a small information article in regards to the present use of(CFD) software program to mannequin sunroof buffeting.

This hyperlink: [3] is a small trade brochure that reveals the present use of CFD for sunroof buffeting.

[1] Acoustics: An introduction to its Bodily Rules and Purposes ; Pierce, Allan D., Acoustical Society of America, 1989.

[2] Prediction and Management of the Inside Stress Fluctuations in a Move-excited Helmholtz resonator ; Mongeau, Luc, and Hyungseok Kook., Ray W. Herrick Laboratories, Purdue College, 1997.

[3]Affect of leakage on the flow-induced response of automobiles with open sunroofs ; Mongeau, Luc, and Jin-Seok Hong., Ray W. Herrick Laboratories, Purdue College.

[4]Fluid dynamics of a movement excited resonance, half I: Experiment ; P.A. Nelson, Halliwell and Doak.; 1991.

[5]An Introduction to Acoustics ; Rienstra, S.W., A. Hirschberg., Report IWDE 99-02, Eindhoven College of Know-how, 1999.

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