Perturbation theory of parametrically driven capillary waves at low viscosity

1997 ◽  
Vol 351 ◽  
pp. 301-344 ◽  
Author(s):  
PER LYNGSHANSEN ◽  
PREBEN ALSTRØM

We present a critical review of the Hamiltonian and the Lagrangian theories of pattern formation in driven capillary waves at low viscosity and high aspect ratio. We construct a Hamiltonian perturbation theory in the spirit of Milner's (1991) formulation, and derive the amplitude equations and their coefficients relevant at the onset of surface waves. Our presentation is detailed, and we carefully point out the differences between our results for the nonlinear coefficients and the results obtained by others. From our standing wave analysis we find that the square pattern is subcritical. Among the supercritical standing wave patterns, we find that the eightfold quasi-crystalline pattern, observed by Christiansen et al. (1992) and by Bosch (1995), is more stable than both rolls and hexagons. We outline the high-aspect-ratio experimental results obtained so far, and discuss them in the light of the theory.

CIRP Annals ◽  
2012 ◽  
Vol 61 (1) ◽  
pp. 479-482 ◽  
Author(s):  
Yasuhiro Takaya ◽  
Masaki Michihata ◽  
Terutake Hayashi ◽  
Taisuke Washitani

2020 ◽  
Vol 17 (4) ◽  
pp. 1003-1012 ◽  
Author(s):  
Andrew Claypole ◽  
James Claypole ◽  
Alex Holder ◽  
Tim C. Claypole ◽  
Liam Kilduff

BioResources ◽  
2020 ◽  
Vol 16 (1) ◽  
pp. 16-18
Author(s):  
Martin A. Hubbe

Conventional rheological tests can be difficult to carry out in the case of suspensions of nanofibrillated cellulose (NFC). Such suspensions tend to migrate away from the walls of a rheometer device, leaving a low-viscosity layer. The very high aspect ratio of typical nanofibrillated cellulose particles favors formation of tangled clusters. But application of hydrodynamic shear can cause fragmentation of those clusters. It is proposed in this essay that some focus be placed on the fragments of entangled clusters of NFC and interactions between them at their fractured surfaces. The condition of near-uniform, defect-free structures of nanocellulose spanning the volume within a sheared suspension might be regarded as an unlikely circumstance. Isaac Newton started with a very simple equation to start to understand rheology. It is proposed that a similarly bold and simplified approach may be needed to account for the effects of broken entangled clusters of NFC on flow phenomena, their assessment, and their consequences related to industrial processes.


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