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Natural frequencies and response of spinning liquid column with apparently sliding contact line
Authors:Prof H F Bauer
Affiliation:(1) Present address: Institut für Raumfahrttechnik, Universität der Bundeswehr München, Werner-Heisenberg-Weg 39, D-W-8014 Neubiberg, Germany
Abstract:Summary The contact line of a liquid with a solid does in many cases—depending on the smoothness of the solid, the viscosity, the surface tension and the excitation force—apparently flow along the solid during oscillations. The influence of this effect upon the natural frequencies, the stability and the response of the system has been investigated at an oscillating and spinning cylindrical liquid column.List of symbols 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, phgr,z cylindrical polar coordinates - t time - u, v, w velocity distribution in rotating liquid - 
$${\text{We}} \equiv \frac{{\varrho a^3 \Omega _0 ^2 }}{\sigma }$$
Weber number - 
$$\bar z_0$$
axial excitation amplitude - 
$$\alpha ^2  = {\text{ 1}} - \frac{{4\Omega _0 ^2 }}{{\Omega ^2 }} > 0$$
elliptic case (OHgr > 2OHgr 0) - 
$$\beta ^2  = {\text{ 1}} - \frac{{4\Omega _0 ^2 }}{{\Omega ^2 }} - 1 > 0$$
hyperbolic case (OHgr > 2OHgr 0) - rhov liquid density - sgr surface tension - zeta liquid surface displacement - PSgr acceleration potential - OHgr 0 rotational speed - OHgr axial forcing frequency - ohgr natural frequency of rotating system - ohgron natural frequency of harmonic axial response
Keywords:
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