, the financial support of Region Ile-de-France (SESAME program) and F2M (Fédération 826 Française de Mécanique)

On the effect of coarse aggregate 828 fraction and shape on the rheological properties of self-compacting concrete ,

, Aggregates, vol.24, issue.1, pp.3-6, 2002.

Yield stress and elastic modulus of 831 suspensions of noncolloidal particles in yield stress fluids, J. Rheol, vol.52, issue.1, p.832, 2008. ,

Rheology of non-brownian suspensions, Annual Review of 833 Chemical and Biomolecular Engineering, vol.5, pp.203-228, 2014. ,

Homogenization approach to the behavior of 835 suspensions of noncolloidal particles in yield stress fluids, J. Rheol, vol.52, issue.2, p.836, 2008. ,

Flows of suspen-837 sions of particles in yield stress fluids, J. Rheol, vol.59, pp.1449-1486, 2015. ,

Effect of particle morpho-839 logical parameters on sand grains packing properties and rheology of model mortars ,

, Concr. Res, vol.80, pp.44-51, 2016.

A review of microstructure in concentrated suspensions and its implications for 842 rheology and bulk flow, Rheol. Acta, vol.48, p.909923, 2009. ,

Microstructural theory and the rheology of concentrated 844 colloidal suspensions, J. Fluid Mech, vol.713, pp.420-452, 2012. ,

Shear-induced structure in a concentrated suspension of 846 solid spheres, J. Rheol, vol.24, issue.6, p.847, 1980. ,

Fore-and-aft asymmetry in a concentrated suspension of solid 848 spheres, J. Rheol, vol.31, issue.8, pp.725-732, 1987. ,

The influence of surface roughness on the particle-850 pair distribution function of dilute suspensions of non-colloidal spheres ,

, J. Fluid Mech, vol.339, pp.1-24, 1997.

Experimental signature of the pair-trajectories of rough 853 spheres in the shear-induced microstructure in non-colloidal suspensions, Phys. Rev. Lett, p.854 ,

Microstructure in sheared non-brownian 858 concentrated suspensions, J. Rheol, vol.57, pp.273-292, 2013. ,

Stokesian dynamics simulation of brownian suspen-860 sions, J. Fluid Mech, vol.313, pp.181-207, 1996. ,

Structure, diffusion and rheology of brownian suspensions by 862 stokesian dynamics simulation, J. Fluid Mech, vol.407, p.167200, 2000. ,

Microstructure from simulated brownian suspension flows at large 864 shear rate, Phys. Fluids, vol.14, 1920. ,

Direct investigation of anisotropic 866 suspension structure in pressure-driven flow, Phys. Rev. E, vol.81, p.41403, 2010. ,

Imaging the microscopic structure 868 of shear thinning and thickening colloidal suspensions, Science, vol.333, issue.6047, p.869, 2011. ,

Spatial cooperativity in soft glassy 870 flows, Nature, issue.7200, pp.84-87, 2008. ,

On the 872 application of x-ray microtomography in the field of materials science, Adv. Eng. Mater, vol.873, issue.3, p.539546, 2001. ,

Computed tomography: principles, design, artifacts, and recent advances, vol.875 ,

, , 2009.

A review of x-ray flow visualization with applications to multiphase flows, Journal of Fluids Engineering, vol.877, issue.7, p.74001, 2011. ,

Rhéologie et microstructure des suspensions concentrées non browniennes, 2011. ,

Practical cone-beam algorithm, JOSA A, vol.881, issue.6, pp.612-619, 1984. ,

Preface: Focus on imaging methods in granular physics, Scientific Instruments, vol.884, 2017. ,

URL : https://hal.archives-ouvertes.fr/hal-01534698

Crosssectional imaging of refractiveindexmatched liquidgranular flows ,

, Exp. Fluids, vol.56, p.163, 2015.

Invited article: Refrac-888 tive index matched scanning of dense granular materials, Review of Scientific Instruments, vol.889, p.83, 2012. ,

Accurate detection and complete tracking of large populations of 891 features in three dimensions, Optics Express, vol.17, issue.4685, 2009. ,

Rheology: principles, measurements, and applications, vol.893, 1994. ,

Three-dimensional jamming and flows of soft glassy 895 materials, Nature Materials, vol.9, issue.2, pp.115-119, 2010. ,

Particle migration in concentrated suspensions 897 undergoing squeeze flow, J. Rheol, vol.54, issue.3, pp.563-589, 2010. ,

Spatial resolution characterization of a 899 x-ray microct system, Applied Radiation and Isotopes, vol.94, pp.230-234, 2014. ,

, More and more iterations are needed for convergence at higher solid fractions, but convergence 901 is still obtained for solid fraction as high as 36%. If needed, it should be checked that it still 902 holds for larger solid fractions

Ordering transition of non-brownian suspensions in confined steady 904 shear flow, Phys. Rev. E, vol.81, p.51502, 2010. ,