Andereck C. D., Liu S. S. & Swinney H. L.
1986
Flow regimes in a circular Couette system with independently rotating cylinders. J. Fluid Mech.
164, 155–183.

Babler M. U., Biferale L., Brandt L., Feudel U., Guseva K., Lanotte A. S., Marchioli C., Picano F., Sardina G. & Soldati A.
2015
Numerical simulations of aggregate breakup in bounded and unbounded turbulent flows. J. Fluid Mech.
766, 104–128.

Biferale L., Meneveau C. & Verzicco R.
2014
Deformation statistics of sub-Kolmogorov-scale ellipsoidal neutrally buoyant drops in isotropic turbulence. J. Fluid Mech.
754, 184–207.

Byron M., Einarsson J., Gustavsson K., Voth G., Mehlig B. & Variano E.
2015
Shape-dependence of particle rotation in isotropic turbulence. Phys. Fluids
27 (3), 035101.

Chaffey C. E. & Brenner H.
1967
A second-order theory for shear deformation of drops. J. Colloid Interface Sci.
24 (2), 258–269.

Chevillard L. & Meneveau C.
2013
Orientation dynamics of small, triaxial-ellipsoidal particles in isotropic turbulence. J. Fluid Mech.
737, 571–596.

Cox R. G.
1969
The deformation of a drop in a general time-dependent fluid flow. J. Fluid Mech.
37 (03), 601–623.

Cristini V., Blawzdziewicz J., Loewenberg M. & Collins L. R.
2003
Breakup in stochastic Stokes flows: sub-Kolmogorov drops in isotropic turbulence. J. Fluid Mech.
492, 231–250.

Dabiri S., Lu J. & Tryggvason G.
2013
Transition between regimes of a vertical channel bubbly upflow due to bubble deformability. Phys. Fluids
25 (10), 102110.

Eaton J. K & Fessler J. R.
1994
Preferential concentration of particles by turbulence. Intl J. Multiphase Flow
20, 169–209.

Eckhardt B., Grossmann S. & Lohse D.
2000
Scaling of global momentum transport in Taylor–Couette and pipe flow. Eur. Phys. J. B
18 (3), 541–544.

Eckhardt B., Grossmann S. & Lohse D.
2007a
Fluxes and energy dissipation in thermal convection and shear flows. Europhys. Lett.
78 (2), 24001.

Eckhardt B., Grossmann S. & Lohse D.
2007b
Torque scaling in turbulent Taylor–Couette flow between independently rotating cylinders. J. Fluid Mech.
581, 221–250.

Elghobashi S.
1994
On predicting particle-laden turbulent flows. Appl. Sci. Res.
52 (4), 309–329.

Frankel N. A. & Acrivos A.
1970
The constitutive equation for a dilute emulsion. J. Fluid Mech.
44 (01), 65–78.

van Gils D. P. M., Narezo Guzman D., Sun C. & Lohse D.
2013
The importance of bubble deformability for strong drag reduction in bubbly turbulent Taylor–Couette flow. J. Fluid Mech.
722, 317–347.

Girimaji S. S. & Pope S. B.
1990
Material-element deformation in isotropic turbulence. J. Fluid Mech.
220, 427–458.

Grossmann S., Lohse D. & Sun C.
2016
High Reynolds number Taylor–Couette turbulence. Annu. Rev. Fluid Mech.
48, 53–80.

Guido S., Minale M. & Maffettone P. L.
2000
Drop shape dynamics under shear-flow reversal. J. Rheol.
44 (6), 1385–1399.

Guido S. & Villone M.
1998
Three-dimensional shape of a drop under simple shear flow. J. Rheol.
42 (2), 395–415.

Hinze J. O.
1955
Fundamentals of the hydrodynamic mechanism of splitting in dispersion processes. AIChE J.
1 (3), 289–295.

Johnson P. L. & Meneveau C.
2015
Large-deviation joint statistics of the finite-time Lyapunov spectrum in isotropic turbulence. Phys. Fluids
27 (8), 085110.

Kolmogorov A. N.
1949
On the disintegration of drops in a turbulent flow. Dokl. Akad. Nauk SSSR
66, 30.

Lu J., Fernández A. & Tryggvason G.
2005
The effect of bubbles on the wall drag in a turbulent channel flow. Phys. Fluids
17 (9), 095102.

Lu J. & Tryggvason G.
2008
Effect of bubble deformability in turbulent bubbly upflow in a vertical channel. Phys. Fluids
20 (4), 040701.

Lund T. S. & Rogers M. M.
1994
An improved measure of strain state probability in turbulent flows. Phys. Fluids
6 (5), 1838–1847.

Maffettone P. L. & Minale M.
1998
Equation of change for ellipsoidal drops in viscous flow. J. Non-Newtonian Fluid Mech.
78 (2), 227–241.

Magnaudet J. & Eames I.
2000
The motion of high-Reynolds-number bubbles in inhomogeneous flows. Annu. Rev. Fluid Mech.
32 (1), 659–708.

Marchioli C., Fantoni M. & Soldati A.
2010
Orientation, distribution, and deposition of elongated, inertial fibers in turbulent channel flow. Phys. Fluids
22 (3), 033301.

Marchioli C. & Soldati A.
2015
Turbulent breakage of ductile aggregates. Phys. Rev. E
91 (5), 053003.

Maxey M. R. & Riley J. J.
1983
Equation of motion for a small rigid sphere in a nonuniform flow. Phys. Fluids
26 (4), 883–889.

Minale M.
2008
A phenomenological model for wall effects on the deformation of an ellipsoidal drop in viscous flow. Rheol. Acta
47 (5–6), 667–675.

Minale M.
2010
Models for the deformation of a single ellipsoidal drop: a review. Rheol. Acta
49 (8), 789–806.

Mortensen P. H., Andersson H. I., Gillissen J. J. J. & Boersma B. J.
2008
On the orientation of ellipsoidal particles in a turbulent shear flow. Intl J. Multiphase Flow
34 (7), 678–683.

Ni R., Kramel S., Ouellette N. T. & Voth G. A.
2015
Measurements of the coupling between the tumbling of rods and the velocity gradient tensor in turbulence. J. Fluids Mech.
766, 202–225.

Njobuenwu D. O. & Fairweather M.
2015
Dynamics of single, non-spherical ellipsoidal particles in a turbulent channel flow. Chem. Engng Sci.
123, 265–282.

Ostilla-Mónico R., Huisman S. G., Jannink T. J. G., Van Gils D. P. M., Verzicco R., Grossmann S., Sun C. & Lohse D.
2014a
Optimal Taylor–Couette flow: radius ratio dependence. J. Fluid Mech.
747, 1–29.

Ostilla-Mónico R., van der Poel E. P., Verzicco R., Grossmann S. & Lohse D.
2014b
Boundary layer dynamics at the transition between the classical and the ultimate regime of Taylor–Couette flow. Phys. Fluids
26 (1), 015114.

Ostilla-Mónico R., van der Poel E. P., Verzicco R., Grossmann S. & Lohse D.
2014c
Exploring the phase diagram of fully turbulent Taylor–Couette flow. J. Fluid Mech.
761, 1–26.

Ostilla-Mónico R., Stevens R. J. A. M., Grossmann S., Verzicco R. & Lohse D.
2013
Optimal Taylor–Couette flow: direct numerical simulations. J. Fluid Mech.
719, 14–46.

Ostilla-Mónico R., Verzicco R. & Lohse D.
2015
Effects of the computational domain size on direct numerical simulations of Taylor–Couette turbulence with stationary outer cylinder. Phys. Fluids
27 (2), 025110.

Parsa S., Calzavarini E., Toschi F. & Voth G. A.
2012
Rotation rate of rods in turbulent fluid flow. Phys. Rev. Lett.
109 (13), 134501.

Perlekar P., Biferale L., Sbragaglia M., Srivastava S. & Toschi F.
2012
Droplet size distribution in homogeneous isotropic turbulence. Phys. Fluids.
24 (6), 065101.

van der Poel E. P., Ostilla-Mónico R., Donners J. & Verzicco R.
2015
A pencil distributed finite difference code for strongly turbulent wall-bounded flows. Comput. Fluids
116, 10–16.

Rallison J. M.
1984
The deformation of small viscous drops and bubbles in shear flows. Annu. Rev. Fluid Mech.
16 (1), 45–66.

Shin M. & Koch D. L.
2005
Rotational and translational dispersion of fibres in isotropic turbulent flows. J. Fluid Mech.
540, 143–173.

Spandan V., Ostilla-Mónico R., Verzicco R. & Lohse D.
2016
Drag reduction in numerical two-phase Taylor–Couette turbulence using an Euler–Lagrange approach. J. Fluid Mech.
798, 411–435.

Stone H. A.
1994
Dynamics of drop deformation and breakup in viscous fluids. Annu. Rev. Fluid Mech.
26 (1), 65–102.

Taylor G. I.
1932
The viscosity of a fluid containing small drops of another fluid. Proc. R. Soc. Lond.
138, 41–48.

Taylor G. I.
1934
The formation of emulsions in definable fields of flow. Proc. R. Soc. Lond.
146, 501–523.

Tryggvason G., Dabiri S., Aboulhasanzadeh B. & Lu J.
2013
Multiscale considerations in direct numerical simulations of multiphase flows. Phys. Fluids
25 (3), 031302.

de Tullio M. D., Nam J., Pascazio G., Balaras E. & Verzicco R.
2012
Computational prediction of mechanical hemolysis in aortic valved prostheses. Eur. J. Mech. (B/Fluids)
35, 47–53.

Vananroye A., Van Puyvelde P. & Moldenaers P.
2011
Deformation and orientation of single droplets during shear flow: combined effects of confinement and compatibilization. Rheol. Acta
50 (3), 231–242.

Verzicco R. & Orlandi P.
1996
A finite-difference scheme for three-dimensional incompressible flows in cylindrical coordinates. J. Comput. Phys.
123 (2), 402–414.