Experimental study of small-amplitude lateral vibrations of an axisymmetric liquid bridge

2007 ◽  
Vol 19 (11) ◽  
pp. 118103 ◽  
Author(s):  
C. Ferrera ◽  
J. M. Montanero
Author(s):  
Kevin D. Murphy ◽  
Lawrence N. Virgin ◽  
Stephen A. Rizzi

Abstract Experimental results are presented which characterize the dynamic response of homogeneous, fully clamped, rectangular plates to narrow band acoustic excitation and uniform thermal loads. Using time series, pseudo-phase projections, power spectra and auto-correlation functions, small amplitude vibrations are considered about both the pre- and post-critical states. These techniques are then employed to investigate the snap-through response. The results for snap-through suggest that the motion is temporally complex and a Lyapunov exponent calculation confirms that the motion is chaotic. Finally, a snap-through boundary is mapped in the (ω, SPL) parameter space separating the regions of snap-through and no snap-through.


2014 ◽  
Vol 27 (1) ◽  
pp. 1-10 ◽  
Author(s):  
Shuo Yang ◽  
Ruquan Liang ◽  
Fusheng Yan ◽  
Taiyin Gao ◽  
Yutao Feng

2000 ◽  
Vol 231 (1) ◽  
pp. 26-31 ◽  
Author(s):  
Olivier Pitois ◽  
Pascal Moucheront ◽  
Xavier Chateau

2015 ◽  
Vol 21 (48) ◽  
pp. 639-644 ◽  
Author(s):  
Osamu KOUCHIYAMA ◽  
Tomoyuki KANDA ◽  
Yasuo TAKENAKA ◽  
Mitsuru MIYAZAKI ◽  
Masahiro NAKAMURA ◽  
...  

1969 ◽  
Vol 36 (4) ◽  
pp. 682-686 ◽  
Author(s):  
Chang-Yi Wang

A rigid rotating cylindrical shaft is vibrating along a diameter in a viscous fluid. Two different cases are investigated through the method of inner and outer expansions. The case of small amplitude vibrations is characterized by the diffusion of vorticity. The coupling of rotation with vibration introduces a normal force, of both inviscid and viscous origins, perpendicular to the direction of oscillation. As rotation increases, the induced steady streaming becomes more skewed and weaker. The case of fast rotation is characterized by the transport of vorticity. Rotation affects both the drag and normal force. The steady torque is increased due to the induction of a steady secondary rotary flow.


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