Summary
The response of a solidly rotating 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 in the elliptic (Ω>2Ω 0) and hyperbolic frequency range (Ω>2Ω 0).
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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
- \(\bar z_0 \) :
-
axial excitation amplitude
- \(\alpha ^2 = 1 - \frac{{4\Omega ^2 }}{{\Omega ^2 }} > 0\) :
-
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
- Ψ:
-
acceleration potential
- Ω 0 :
-
rotational speed
- Ω:
-
axial forcing frequency
- ω:
-
natural frequency of rotating system
- ω 02n −1:
-
natural frequency of harmonic axial response
References
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Bauer, H. F.: Axial response, transient- and pulse behavior of a cylindrical liquid column in zero gravity. Forschungsbericht Universität der Bundeswehr München, UniBw-WE-9-FB-9-1988.
Bauer, H. F.: Response of a spinning liquid column to axial excitation. Forschungsbericht Universität der Bundeswehr München, UniBw-WE-9-FB-10-1988.
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Bauer, H.F. Response of a spinning liquid column to axial excitation. Acta Mechanica 77, 153–170 (1989). https://doi.org/10.1007/BF01178319
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DOI: https://doi.org/10.1007/BF01178319