Oscillation frequency of 2D circular drop in an ambient environment

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SUMMARY

The natural oscillating frequencies of a 2D circular drop of liquid in an ambient environment are discussed, referencing Prosperetti's 1979 work. The dimensionless frequency for such a drop is defined as λ_n = √(n(n-1)(n+1)). The discussion highlights the challenges of modeling 2D systems, particularly the zero values for surface area, volume, and mass, which complicate the analysis. The correct equations for droplets and bubbles are differentiated, with a specific focus on the droplet's behavior as outlined in equation 28 of the referenced material.

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Hi PF!

Do you know what the natural oscillating frequencies are for a 2D circular drop of liquid in an ambient environment (negligible effects)?

Prosperetti 1979 predicts the frequencies for both a spherical drop and bubble here at equations 5b and 6b. There must be a simpler circular 2D extension, right?

Much appreciated!
 
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The problem with a 2D model is that the terms for the surface area, volume and mass are all zero.
 
Baluncore said:
The problem with a 2D model is that the terms for the surface area, volume and mass are all zero.
A 2D circle for sure exists. I read somewhere that the dimensionless frequency is ##\lambda_n = \sqrt{n(n-1)(n+1)}##. I know for sure one exists: just can't recall the circular bubble and drop exactly.
 
For completeness, I just now read and it seems what I posted in post 3 is correct for a droplet (not a bubble). This is directly given in equation 28 here. Still unsure about the bubble.
 
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