Effect of fibrils on curvature- and rotation-induced hydrodynamic stability

Flow of a suspension of water and nano-fibrillated cellulose (NFC) in a curved and rotating channel is studied experimentally and theoretically. The aim is to investigate how NFC affects the stability of the flow. This flow is subject to a centrifugal instability creating counter-rotating vortices in the flow direction. These rolls can be both stabilised and destabilised by system rotation, depending on direction and velocity of the rotation. Flow visualisation images with pure water and an NFC/water suspension are categorised, and stability maps are constructed. A linear stability analysis is performed, and the effect of fibrils is taken into account assuming straight fibrils and constant orientation distributions, i.e., without time-dependent flow-orientation coupling. The results show that NFC has a less stabilising effect on the primary flow instability than indicated from the increase in viscosity measured by a rotary viscometer, but more than predicted from the linear stability analysis. Several unknown parameters (the most prominent being fibril aspect ratio and the interaction parameter in the rotary diffusion) appear in the analysis.

[1]  N. Phan-Thien,et al.  A new constitutive model for fibre suspensions: flow past a sphere , 1991 .

[2]  J. Ericksen Transversely isotropic fluids , 1960 .

[3]  R. Sureshkumar,et al.  Centrifugal instability of semidilute non-Brownian fiber suspensions , 2002 .

[4]  G. B. Jeffery The motion of ellipsoidal particles immersed in a viscous fluid , 1922 .

[5]  Øyvind Weiby Gregersen,et al.  Rheological Studies of Microfibrillar Cellulose Water Dispersions , 2011 .

[6]  G. Batchelor,et al.  The stress system in a suspension of force-free particles , 1970, Journal of Fluid Mechanics.

[7]  J. Azaiez Linear stability of free shear flows of fibre suspensions , 2000, Journal of Fluid Mechanics.

[8]  S. Edwards,et al.  The Theory of Polymer Dynamics , 1986 .

[9]  P. Henrik Alfredsson,et al.  Curvature- and rotation-induced instabilities in channel flow , 1990, Journal of Fluid Mechanics.

[10]  David V. Boger,et al.  The flow of fiber suspensions in complex geometries , 1988 .

[11]  M J Alava,et al.  Modeling the viscosity and aggregation of suspensions of highly anisotropic nanoparticles , 2012, The European physical journal. E, Soft matter.

[12]  Satish C. Reddy,et al.  A MATLAB differentiation matrix suite , 2000, TOMS.

[13]  G. Batchelor,et al.  The stress generated in a non-dilute suspension of elongated particles by pure straining motion , 1971, Journal of Fluid Mechanics.

[14]  Suresh G. Advani,et al.  The Use of Tensors to Describe and Predict Fiber Orientation in Short Fiber Composites , 1987 .

[15]  W. R. Dean Fluid Motion in a Curved Channel , 1928 .

[16]  C. Petrie,et al.  The rheology of fibre suspensions , 1999 .

[17]  Kentaro Abe,et al.  Review: current international research into cellulose nanofibres and nanocomposites , 2010, Journal of Materials Science.

[18]  Lin Jianzhong,et al.  Hydrodynamic instability of fiber suspensions in channel flows , 2004 .

[19]  O. Ikkala,et al.  Enzymatic hydrolysis combined with mechanical shearing and high-pressure homogenization for nanoscale cellulose fibrils and strong gels. , 2007, Biomacromolecules.

[20]  A. B. Metzner,et al.  Drag reduction in the turbulent flow of fiber suspensions , 1974 .

[21]  Glenn H. Fredrickson,et al.  The hydrodynamic stress in a suspension of rods , 1990 .

[22]  C. L. Tucker,et al.  Orientation Behavior of Fibers in Concentrated Suspensions , 1984 .