Summary
The response of a solidly rotating anchored finite liquid column consisting of frictionless liquid is subjected to axial harmonic excitation. The response of the free liquid surface elevation and velocity distribution has been determined analytically in the elliptic (Ω>2Ω 0) and hyperbolic frequency range (Ω>2Ω 0). For the liquid surface displacement the response has been evaluated numerically as a function of the forcing frequencyΩ/2Ω 0. In addition the first natural stuck-edge frequency has been determined and compared with the slipping case.
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Abbreviations
- a :
-
radius of liquid bridge
- h :
-
length of liquid bridge
- I 0,I 1 :
-
modified Besselfunctions
- J 0,J 1 :
-
Besselfunctions
- p :
-
liquid pressure
- r, ϕ,z :
-
cylindrical polar coordinates
- t :
-
time
- u, v, w :
-
velocity distribution in rotating liquid
- \(We \equiv \frac{{\varrho a^3 \Omega _0 ^2 }}{\sigma }\) :
-
Weber number
- z0 :
-
axial excitation amplitude
- \(\alpha ^2 = 1 - \frac{{4\Omega _0 ^2 }}{{\Omega ^2 }} > 0\) :
-
elliptic case (Ω>2Ω 0)
- \(\beta ^2 = \frac{{4\Omega _0 ^2 }}{{\Omega ^2 }} - 1 > 0\) :
-
hyperbolic case (Ω>2Ω 0)
- ϱ:
-
liquid density
- σ:
-
surface tension
- ζ:
-
liquid surface displacement
- Φ:
-
acceleration potential
- Ω 0 :
-
rotational speed
- Ω:
-
axial forcing frequency
- ω:
-
natural frequency of rotating system
- ω0n :
-
natural frequency of harmonic axial response
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Bauer, H.F. Axi-symmetric natural frequencies and response of a spinning liquid column under strong surface tension. Acta Mechanica 90, 21–35 (1991). https://doi.org/10.1007/BF01177396
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DOI: https://doi.org/10.1007/BF01177396