Acoustic Resonance in Fluid-Filled Cavities

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SUMMARY

The discussion focuses on the physics of acoustic resonance in fluid-filled cavities, specifically water-filled spherical balloons. It highlights the use of FEM eigenvalue analysis to determine resonant modes, represented by the equation K-ω²n M = 0, where K and M are stiffness and mass matrices. The conversation emphasizes that boundary conditions, such as Dirichlet (u=0) and Neumann (du/dn=0), significantly affect modal frequencies and shapes. Additionally, it addresses the challenge of finding natural frequencies when the cavity is placed in a different fluid medium, suggesting the use of spherical Bessel functions for accurate modeling.

PREREQUISITES
  • Understanding of FEM eigenvalue analysis
  • Knowledge of boundary conditions in acoustics (Dirichlet and Neumann)
  • Familiarity with spherical Bessel functions
  • Basic principles of acoustic resonance
NEXT STEPS
  • Research FEM eigenvalue analysis techniques for fluid dynamics
  • Study the impact of boundary conditions on modal frequencies
  • Explore the application of spherical Bessel functions in acoustic modeling
  • Investigate methods for calculating natural frequencies in multi-fluid systems
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Researchers, physicists, and engineers working in acoustics, fluid dynamics, and resonance phenomena, particularly those involved in modeling fluid-filled cavities and their interactions with external acoustic sources.

nawidgc
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I am trying to understand the physics of resonance phenomenon. One can find the resonant modes of a water filled spherical cavity either analytically or by using the FEM eigenvalue analysis (K-ω2n M = 0, with K and M being the usual stiffness ans mass matrices in FEM). For the later, we usually set u=0 (Dirichlet bc) or du/dn=0 (Neumann bc) and depending on the boundary condition, the mode shapes and modal frequencies will change.

Let the set of natural frequencies of water filled balloon obtained by this process be denoted as ωn. Now, consider the water balloon to be placed in air and assume I have an acoustic source outside balloon that emits acoustic waves of a frequency that matches with one of the frequencies from the set ωn.

Would this cause the water inside the balloon to resonate at the applied frequency (since it matches with one of its natural frequencies)? My understanding is, once you place the water filled balloon in air, the boundary condition at the interface is no longer u=0 or du/dn=0. So the natural frequencies obtained earlier are no longer correct in this situation.

Alternatively, how can one find the natural frequencies of fluid filled cavities that are embedded inside another fluid with different density and sound speed? Appreciate any comments or answers.
 
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nawidgc said:
I am trying to understand the physics of resonance phenomenon. One can find the resonant modes of a water filled spherical cavity either analytically or by using the FEM eigenvalue analysis (K-ω2n M = 0, with K and M being the usual stiffness ans mass matrices in FEM). For the later, we usually set u=0 (Dirichlet bc) or du/dn=0 (Neumann bc) and depending on the boundary condition, the mode shapes and modal frequencies will change.

Let the set of natural frequencies of water filled balloon obtained by this process be denoted as ωn. Now, consider the water balloon to be placed in air and assume I have an acoustic source outside balloon that emits acoustic waves of a frequency that matches with one of the frequencies from the set ωn.

Would this cause the water inside the balloon to resonate at the applied frequency (since it matches with one of its natural frequencies)? My understanding is, once you place the water filled balloon in air, the boundary condition at the interface is no longer u=0 or du/dn=0. So the natural frequencies obtained earlier are no longer correct in this situation.

Alternatively, how can one find the natural frequencies of fluid filled cavities that are embedded inside another fluid with different density and sound speed? Appreciate any comments or answers.

To find resonance frequencies for external excitation (maximal amplitude at boundary), you basically should replace 0-th order spherical Bessel function j0(r) for 1st order j1(r)
 

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