Acoustic impedance in Materials

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Discussion Overview

The discussion revolves around the concept of acoustic impedance in materials, particularly focusing on how the geometry of materials, such as tubular or hollow structures, affects their acoustic properties. Participants explore the implications of density and wave velocity on impedance, as well as the effects of porosity in materials.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant defines acoustic impedance as the product of density and wave velocity in a material and questions whether hollow structures reduce density and impedance compared to solid materials.
  • Another participant suggests that the inquiry may relate to acoustic metamaterials.
  • A later reply clarifies that the question pertains to the impedance relationship of all materials concerning elastic waves, specifically in the context of Hopkinson Bar Design.
  • One participant states that the geometry of a solid does not affect the fundamental properties of density and speed of sound, asserting that these properties are independent of shape.
  • Another participant agrees with the previous point, emphasizing that speed of sound is related to bulk modulus and density, and mentions that porosity leads to increased attenuation due to reflection and refraction.

Areas of Agreement / Disagreement

Participants express differing views on the impact of geometry on acoustic impedance, with some asserting independence from geometry while others question this assumption. The discussion remains unresolved regarding the specific effects of hollow versus solid structures and the role of porosity.

Contextual Notes

Participants reference external resources for further exploration of acoustic impedance, indicating that the discussion may benefit from additional context or definitions related to the properties of materials.

sandon
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Acoustic impedance of material is defined by density multiply by the velocity of waves within the base material.

My question is if i have a tubular or hollow part with a base material, does this count as a reduction of density compared to the base material of the tube or hollow part. Would the impedance of the material be reduced?

Then applying that same logic of tubular/hollowed parts to porous/cellular parts with the base material where the reduction of density can be just as extreme as the tubular/hollowed parts. Would the tubular/hollowed parts have relatively same impedance as the porous/cellular parts?
 
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Paul Colby said:
Are you asking about acoustic Metamaterial
I am asking about all materials' impedance relationship to elastic waves. The purpose is for Hopkinson Bar Design.
 
I see. So your question is how does the acoustic wave impedance differ for propagation along a hollow cylinder versus a solid bar. Interesting question. I have no idea. One could solve (or better look up) the boundary value problem solution for an infinite cylinder and answer the question.
 
sandon said:
Acoustic impedance of material is defined by density multiply by the velocity of waves within the base material.

My question is if i have a tubular or hollow part with a base material, does this count as a reduction of density compared to the base material of the tube or hollow part. Would the impedance of the material be reduced?
In short, no. The density and speed of sound in a material are physics properties, independent of the geometry of the solid. The speed of sound in a material is related to the bulk modulus and density.

http://hyperphysics.phy-astr.gsu.edu/hbase/Sound/souspe2.html
For a discussion on acoustic impedance, see also -
https://www.nde-ed.org/EducationResources/CommunityCollege/Ultrasonics/Physics/acousticimpedance.htm

Porosity in a material is different, since the voids in the material result in reflection and refraction in the material, thus increase the attenuation.
 
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Astronuc said:
In short, no. The density and speed of sound in a material are physics properties, independent of the geometry of the solid. The speed of sound in a material is related to the bulk modulus and density.

http://hyperphysics.phy-astr.gsu.edu/hbase/Sound/souspe2.html
For a discussion on acoustic impedance, see also -
https://www.nde-ed.org/EducationResources/CommunityCollege/Ultrasonics/Physics/acousticimpedance.htm

Porosity in a material is different, since the voids in the material result in reflection and refraction in the material, thus increase the attenuation.
Thanks for your help.
 

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