Impedance/admittance (acoustic) models for outdoor ground and seafloor

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Discussion Overview

The discussion revolves around the acoustic impedance of seafloor materials compared to terrestrial soils. Participants explore whether seafloor impedance can be modeled as a complex number or if it is typically represented as a real value. The conversation includes references to existing models and research on acoustic impedance in various contexts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants mention mathematical models like Delany-Bazley for calculating impedance of porous materials, noting that these yield complex impedance values.
  • Others clarify that the discussion is focused on acoustic impedance, not electrical impedance.
  • It is suggested that acoustic impedance can be complex if the surface layer has springy properties and mass, which allows for energy storage and phase shifts.
  • Participants express interest in understanding why seafloor impedance is often reported as a real value, questioning if this is due to the incompressibility of water compared to air.
  • References are shared that discuss both real and complex impedance values in different contexts, including water-saturated sand and terrestrial soils.
  • Some participants note that the presence of gas in terrestrial soils may contribute to complex impedance, while seafloor sediments, being saturated with water, lack this energy storage mechanism.

Areas of Agreement / Disagreement

Participants generally agree that seafloor impedance is often represented as a real value, while terrestrial soils can exhibit complex impedance. However, the reasons for this distinction and the conditions under which complex impedance may arise remain contested and unresolved.

Contextual Notes

There are limitations in the discussion regarding the assumptions about the conditions of the materials being analyzed, such as saturation levels and the presence of gases. The implications of these factors on the impedance values are not fully resolved.

bustun
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TL;DR
Can seafloor impedance get a complex value such as ground (porous materials)?
There are some mathematical models (eg Delany-Bazley) to calculate impedance of porous materials and these formulas give complex impedance values as a result. But I could not find any model to be used for seafloor (underwater ground modeling) or I don't know if existing models may be used. I usually got real values for impedances of seafloor.
Are there any physical explanation for seafloor impedance being a real value (not having an imaginary part) or can seafloor impedance also be modeled as a complex number?
Thanks for your help.
 
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I assume you mean electrical impedance.

Yes of course. Line-to-ground capacitance is highly significant for overhead lines and is it much higher for underground or underwater cables.

For large scale power transmission, HVDC has big advantages over AC.

There was a lot of research on sea bottom impedance when trans-Atlantic single-wire telegraphs were first proposed in the 1800s. Would that be helpful to you?
 
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Thanks for your explanation but I mean acoustic impedance.

I apologize for not making it clear.
 
Oops, I also thought you meant electrical transmission line impedance. What does imaginary acoustical impedance mean? Does it mean some transverse component to the normal longitudinal sound transmission?
 
No, as far as I know, it is explained as the phase between pressure and velocity at the ground (or the impedance plane).
 
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berkeman, thank you very much for your help.

I have read the second reference already but the first and third ones are new for me.
These papers are dealing with the subject in detail but as I explained they are gettin real values for seafloor impedance and I am interested into understand if impedance can be a complex value for seafloor.
 
bustun said:
I am interested into understand if impedance can be a complex value for seafloor.
Yeah, I'm only seeing real numbers for the seafloor references like this one:

https://www.sciencedirect.com/topics/engineering/acoustic-impedance

Do you have an example of a reference for regular soil that shows complex values? It may take a non-isotropic medium to generate any phase shift to make the impedance complex...
 
  • #10
Acoustic impedance can be complex if the surface layer is springy and has mass. The storage of energy in the surface as compression of a gas, and the momentum of mass, produce a complex impedance. The self resonant frequency of the layer is important. The complex impedance of the layer is highly frequency dependent near the resonant frequency.
 
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  • #11
Thanks Baluncore for your neat explanation.

Do you have any comment on ground in contact with air having a complex impedance whereas seafloor has real impedance value? Two references are in the following.

https://asa.scitation.org/doi/10.1121/1.2338288
https://www.researchgate.net/publication/321661766_Acoustic_impedance_properties_of_seafloor_sediments_off_the_coast_of_Southeastern_Hainan

Does this have relation with water being denser than air and canceling springy nature of surface layer? (This is just my simple interpretation, I would be pleased to hear yours.)
 
  • #12
bustun said:
Does this have relation with water being denser than air and canceling springy nature of surface layer? (This is just my simple interpretation, I would be pleased to hear yours.)
Fundamentally, it comes down to liquid water being incompressible, while air is compressible.

A terrestrial soil has particles with mass, and unless it is saturated with water, usually contains compressible air between the soil particles.

Sediment on the sea floor is saturated with water, any gas is dissolved or rises to the surface, so there is no energy storage mechanism available to phase shift the acoustic signal energy.
 
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  • #13
As I understand from your explanation, it is normal to expect a real impedance for seafloor layers while terrestrial soil can have a complex impedance.

Thank you very much, your explanations are very helpful.
 
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