The effect of wall depletion on the rheology of microfibrillated cellulose water suspensions by optical coherence tomography

Rheology of microfibrillated cellulose (MFC) water suspensions was characterized with a rotational rheometer, augmented with optical coherence tomography (OCT). To the best of the authors’ knowledge, this is the first time the behavior of MFC in the rheometer gap was characterized by this real-time imaging method. Two concentrations, 0.5 and 1 wt% were used, the latter also with 10−3 and 10−2 M NaCl. The aim was to follow the structure of the suspensions in a rotational rheometer during the measurements and observe wall depletion and other factors that can interfere with the rheological results. The stepped flow measurements were performed using a transparent cylindrical measuring system and combining the optical information to rheological parameters. OCT allows imaging in radial direction from the outer geometry boundary to the inner geometry boundary making both the shear rate profile and the structure of the suspension visible through the rheometer gap. Yield stress and maximum wall stress were determined by start-up of steady shear and logarithmic stress ramp methods and they both reflected in the stepped flow measurements. Above yield stress, floc size was inversely proportional to shear rate. Below the yield stress, flocs adhered to each other and the observed apparent constant shear stress was controlled by flow in the depleted boundary layer. With higher ionic strength (10−2 M NaCl), the combination of yield stress and wall depletion favored the formation of vertical, cylindrical, rotating floc structures (rollers) coupled with a thicker water layer originating at the suspension—inner cylinder boundary at low shear rates.

[1]  R. J. Kerekes,et al.  Flocculation of cellulose fibres: new comparison of crowding factor with percolation and effective-medium theories , 2009 .

[2]  J. Ntalikwa Determination of surface charge density of α-alumina by Acid - base titration , 2007 .

[3]  J. R. Abbott,et al.  A constitutive equation for concentrated suspensions that accounts for shear‐induced particle migration , 1992 .

[4]  Juha Salmela,et al.  Flocculated flow of microfibrillated cellulose water suspensions: an imaging approach for characterisation of rheological behaviour , 2012, Cellulose.

[5]  C. Gaillard,et al.  Rheological behaviour and microstructure of microfibrillated cellulose suspensions/low-methoxyl pectin mixed systems. Effect of calcium ions , 2012 .

[6]  C. Kasai,et al.  Real-Time Two-Dimensional Blood Flow Imaging Using an Autocorrelation Technique , 1985, IEEE 1985 Ultrasonics Symposium.

[7]  Jari Vartiainen,et al.  Health and environmental safety aspects of friction grinding and spray drying of microfibrillated cellulose , 2011 .

[8]  Peter J. Scales,et al.  The bucket rheometer for shear stress-shear rate measurement of industrial suspensions: social capital and wellbeing among Iraqi women refugees in rural Victoria , 2007 .

[9]  Hiroyuki Yano,et al.  Optically Transparent Composites Reinforced with Networks of Bacterial Nanofibers , 2005 .

[10]  J. Desbrières,et al.  Rheological characterization of cellulosic microfibril suspensions. Role of polymeric additives , 2001 .

[11]  S. Berot,et al.  Rheological characterization of microfibrillated cellulose suspensions after freezing , 2010 .

[12]  U. Björkman The metarheology of crowded fibre suspensions , 2006 .

[13]  Antti I. Koponen,et al.  Rheological characterization of micro-fibrillated cellulose fibre suspension using multi scale velocity profile measurements , 2013 .

[14]  Daisuke Tatsumi,et al.  Effect of Fiber Concentration and Axial Ratio on the Rheological Properties of Cellulose Fiber Suspensions , 2002 .

[15]  K. R. Sandberg,et al.  Microfibrillated cellulose, a new cellulose product: properties, uses, and commercial potential , 1983 .

[16]  Juha Salmela,et al.  Flocculation of microfibrillated cellulose in shear flow , 2012, Cellulose.

[17]  David V. Boger,et al.  Yield Stress Measurement for Concentrated Suspensions , 1983 .

[18]  D. V. Boger,et al.  Direct Yield Stress Measurement with the Vane Method , 1985 .

[19]  David Plackett,et al.  Microfibrillated cellulose and new nanocomposite materials: a review , 2010 .

[20]  R. J. Kerekes,et al.  Characterization of fibre flocculation regimes by a crowding factor , 1992 .

[21]  B. Derakhshandeh,et al.  The apparent yield stress of pulp fiber suspensions , 2010 .

[22]  Howard A. Barnes,et al.  A review of the slip (wall depletion) of polymer solutions, emulsions and particle suspensions in viscometers: its cause, character, and cure , 1996 .

[23]  Ulf Björkman,et al.  Floc dynamics in flowing fibre suspensions , 2005 .

[24]  D. V. Boger,et al.  Avoiding slip in pulp suspension rheometry , 2012 .

[25]  Tom Lindström,et al.  Deswelling of hardwood kraft pulp fibers by cationic polymers , 1990 .

[26]  M. Hubbe,et al.  COLLOIDAL STABILITY AND AGGREGATION OF LIGNOCELLULOSIC MATERIALS IN AQUEOUS SUSPENSION: A REVIEW , 2008 .

[27]  E. Lasseuguette,et al.  Rheological properties of microfibrillar suspension of TEMPO-oxidized pulp , 2008 .

[28]  Local transient rheological behavior of concentrated suspensions , 2011, 1111.6795.

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

[30]  Hirofumi Ono,et al.  1H Spin–Spin Relaxation Time of Water and Rheological Properties of Cellulose Nanofiber Dispersion, Transparent Cellulose Hydrogel (TCG) , 2004 .

[31]  R. Hill Elastic modulus of microfibrillar cellulose gels. , 2008, Biomacromolecules.

[32]  D. Cheng Yield stress: A time-dependent property and how to measure it , 1986 .

[33]  H. Liimatainen,et al.  FIBRE FLOC MORPHOLOGY AND DEWATERABILITY OF A PULP SUSPENSION: ROLE OF FLOCCULATION KINETICS AND CHARACTERISTICS OF FLOCCULATION AGENTS , 2009 .

[34]  G. W. Blair The importance of the sigma phenomenon in the study of the flow of blood , 1961 .

[35]  Janne Laine,et al.  Effect of polymer adsorption on cellulose nanofibril water binding capacity and aggregation , 2008, BioResources.

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

[37]  G. W. Blair The importance of the sigma phenomenon in the study of the flow of blood , 1958 .

[38]  R. J. Kerekes,et al.  Rheology of pulp fibre suspensions: A critical review , 2011 .

[39]  Martin A. Hubbe,et al.  FLOCCULATION AND REDISPERSION OF CELLULOSIC FIBER SUSPENSIONS: A REVIEW OF EFFECTS OF HYDRODYNAMIC SHEAR AND POLYELECTROLYTES , 2007 .

[40]  Satoshi Miyaguchi,et al.  Optically transparent wood-cellulose nanocomposite as a base substrate for flexible organic light-emitting diode displays , 2009 .

[41]  Pirjo Pietikäinen,et al.  Effect of cationic polymethacrylates on the rheology and flocculation of microfibrillated cellulose , 2011 .

[42]  M. Österberg,et al.  Interaction between water-soluble polysaccharides and native nanofibrillar cellulose thin films , 2011, BioResources.