Summary
For a solidly rotating viscous cylindrical liquid column of finite length the response to axial synchronous, counter- and one-sided excitation is determined for anchored contact lines at the disc-rim. For a rotating column additional responses of inertial waves (hyperbolic range) appear forΩ < 2Ω 0, while in the elliptic rangeΩ < 2Ω 0 the sloshing response occurs. The various responses for the free surface displacement have been numerically evaluated. Only in the one-sided exitation case all resonance peaks appear, while for synchronous excitation only the odd resonances and for counter-excitation only the even resonance peaks occur.
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Abbreviations
- a :
-
radius of column
- h :
-
length of liquid bridge
- I n :
-
modified Bessel function
- p :
-
liquid pressure
- r, φ,z :
-
cylindrical polar coordinates
- t :
-
time
- u, v, w :
-
velocity distribution
- \(We = \frac{{\varrho a^3 \Omega o^2 }}{\sigma }\) :
-
Weber number
- z 0 :
-
excitation amplitude
- ϱ:
-
liquid density
- σ:
-
surface tension
- \(\sigma ^ * = \frac{{\sigma a}}{{\varrho v^2 }}\) :
-
surface tension parameter
- \(Oh = \frac{1}{{\sqrt {\sigma ^ * } }}\) :
-
Ohnesorge number
- ζ:
-
liquid surface displacement
- \(v = \frac{\eta }{\varrho }\) :
-
kinematic viscosity
- Ω 0 :
-
rotational speed
- \(\omega _0 = \frac{{\Omega _0 a^2 }}{v}\) :
-
dimensionless rotational speed
- Ω:
-
forcing frequency
- \(\Omega ^ * = \frac{{\Omega a^2 }}{v}\) :
-
dimensionless forcing frequency
- \(\bar \Omega = \frac{\Omega }{{\sqrt {\frac{\sigma }{{\varrho a^3 }}} }}\) :
-
dimensionless forcing frequency for non-viscous liquid
- λa=Λ:
-
root of bi-cubic Eq.(33)
- \(\chi _n = \frac{{n\pi a}}{h}\) :
-
root of bi-cubic Eq.(33)
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Bauer, H.F., Eidel, W. Viscous response of an anchored spinning liquid column to various axial excitations. Acta Mechanica 116, 153–170 (1996). https://doi.org/10.1007/BF01171427
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DOI: https://doi.org/10.1007/BF01171427