Understanding and predicting viscous, elastic, plastic flows

被引:67
作者
Cheddadi, I. [1 ,2 ,3 ,4 ]
Saramito, P. [1 ,2 ]
Dollet, B. [3 ,4 ,5 ,6 ]
Raufaste, C. [3 ,4 ,7 ]
Graner, F. [3 ,4 ,8 ,9 ]
机构
[1] Univ J Fourier Grenoble I, Lab Jean Kuntzmann, UMR 5524, F-38041 Grenoble 09, France
[2] CNRS, F-38041 Grenoble 09, France
[3] Univ J Fourier Grenoble I, Lab Spectrometrie Phys, UMR 5588, F-38402 St Martin Dheres, France
[4] CNRS, F-38402 St Martin Dheres, France
[5] Univ Rennes 1, Inst Phys Rennes, UMR 6251, F-35042 Rennes, France
[6] CNRS, F-35042 Rennes, France
[7] Univ Oslo, NO-0316 Oslo, Norway
[8] Inst Curie, CNRS, BDD, UMR 3215, F-75248 Paris 05, France
[9] INSERM, U 934, F-75248 Paris 05, France
关键词
CONSTITUTIVE EQUATION; 2-DIMENSIONAL FLOW; UNIFORM-FLOW; MODEL; FOAM; RHEOLOGY; SHEAR; PATTERNS; SOAP;
D O I
10.1140/epje/i2011-11001-4
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Foams, gels, emulsions, polymer solutions, pastes and even cell assemblies display both liquid and solid mechanical properties. On a local scale, such "soft glassy" systems are disordered assemblies of deformable rearranging units, the complexity of which gives rise to their striking flow behaviour. On a global scale, experiments show that their mechanical behaviour depends on the orientation of their elastic deformation with respect to the flow direction, thus requiring a description by tensorial equations for continuous materials. However, due to their strong non-linearities, the numerous candidate models have not yet been solved in a general multi-dimensional geometry to provide stringent tests of their validity. We compute the first solutions of a continuous model for a discriminant benchmark, namely the flow around an obstacle. We compare it with experiments of a foam flow and find an excellent agreement with the spatial distribution of all important features: we accurately predict the experimental fields of velocity, elastic deformation, and plastic deformation rate in terms of magnitude, direction, and anisotropy. We analyse the role of each parameter, and demonstrate that the yield strain is the main dimensionless parameter required to characterize the materials. We evidence the dominant effect of elasticity, which explains why the stress does not depend simply on the shear rate. Our results demonstrate that the behaviour of soft glassy materials cannot be reduced to an intermediate between that of a solid and that of a liquid: the viscous, the elastic and the plastic contributions to the flow, as well as their couplings, must be treated simultaneously. Our approach opens the way to the realistic multi-dimensional prediction of complex flows encountered in geophysical, industrial and biological applications, and to the understanding of the link between structure and rheology of soft glassy systems.
引用
收藏
页数:15
相关论文
共 55 条
[1]   Uniform flow of viscoelastic fluids past a confined falling cylinder [J].
Afonso, Alexandre ;
Alves, Manuel A. ;
Pinho, Fernando T. ;
Oliveira, Paulo J. .
RHEOLOGICA ACTA, 2008, 47 (03) :325-348
[2]   An experimental investigation of negative wakes behind spheres settling in a shear-thinning viscoelastic fluid [J].
Arigo, MT ;
McKinley, GH .
RHEOLOGICA ACTA, 1998, 37 (04) :307-327
[3]   An elasto-visco-plastic model for immortal foams or emulsions [J].
Benito, S. ;
Bruneau, C. -H. ;
Colin, T. ;
Gay, C. ;
Molino, F. .
EUROPEAN PHYSICAL JOURNAL E, 2008, 25 (03) :225-251
[4]  
Bingham EC, 1922, Fluidity and plasticity, V2
[5]   Kinetic Theory of Plastic Flow in Soft Glassy Materials [J].
Bocquet, Lyderic ;
Colin, Annie ;
Ajdari, Armand .
PHYSICAL REVIEW LETTERS, 2009, 103 (03)
[6]   First-principles constitutive equation for suspension rheology [J].
Brader, J. M. ;
Cates, M. E. ;
Fuchs, M. .
PHYSICAL REVIEW LETTERS, 2008, 101 (13)
[7]   Glass rheology: From mode-coupling theory to a dynamical yield criterion [J].
Brader, Joseph M. ;
Voigtmann, Thomas ;
Fuchs, Matthias ;
Larson, Ronald G. ;
Cates, Michael E. .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 2009, 106 (36) :15186-15191
[8]  
Cantat I., 2010, MOUSSES STRUCTURE DY
[9]   Tensorial constitutive models for disordered foams, dense emulsions, and other soft nonergodic materials [J].
Cates, ME ;
Sollich, P .
JOURNAL OF RHEOLOGY, 2004, 48 (01) :193-207
[10]   Numerical modelling of foam Couette flows [J].
Cheddadi, I. ;
Saramito, P. ;
Raufaste, C. ;
Marmottant, P. ;
Graner, F. .
EUROPEAN PHYSICAL JOURNAL E, 2008, 27 (02) :123-133