|
1 Granular Fluids: From Everyday Life to the Lab |
|
|
1 | (18) |
|
1.1 The Granular "States" |
|
|
1 | (2) |
|
|
3 | (10) |
|
|
3 | (1) |
|
|
4 | (4) |
|
|
8 | (5) |
|
1.3 Granular Versus Active Fluids |
|
|
13 | (6) |
|
|
15 | (4) |
|
2 Boltzmann Equation: A Gas of Grains |
|
|
19 | (34) |
|
|
19 | (10) |
|
2.1.1 Elastic Smooth Hard Spheres |
|
|
21 | (1) |
|
2.1.2 Statistics of Hard Spheres Collisions |
|
|
22 | (3) |
|
|
25 | (2) |
|
|
27 | (2) |
|
2.2 The Boltzmann Equation |
|
|
29 | (12) |
|
2.2.1 Liouville and Pseudo-Liouville Equations |
|
|
29 | (3) |
|
2.2.2 The BBGKY Hierarchy |
|
|
32 | (3) |
|
2.2.3 The Boltzmann Hierarchy and the Boltzmann Equation |
|
|
35 | (1) |
|
2.2.4 Collision Invariants and H-theorem |
|
|
36 | (2) |
|
2.2.5 The Maxwell Molecules |
|
|
38 | (1) |
|
2.2.6 The Enskog Correction |
|
|
39 | (2) |
|
2.3 The Boltzmann Equation for Granular Gases |
|
|
41 | (12) |
|
2.3.1 Average Energy Loss |
|
|
41 | (1) |
|
|
42 | (2) |
|
2.3.3 The Homogeneous Cooling State |
|
|
44 | (2) |
|
2.3.4 Inelastic Maxwell Molecules |
|
|
46 | (1) |
|
|
47 | (3) |
|
2.3.6 Looking for a "Granular" H-theorem |
|
|
50 | (1) |
|
|
51 | (2) |
|
3 Hydrodynamics: A Sea of Grains |
|
|
53 | (28) |
|
3.1 Granular Kinetic Theory |
|
|
53 | (9) |
|
3.1.1 A Sketch of the Chapman-Enskog Approximation Method |
|
|
54 | (1) |
|
3.1.2 Densities and Fluxes |
|
|
55 | (1) |
|
3.1.3 Equations for the Densities |
|
|
56 | (1) |
|
3.1.4 Chapman-Enskog Closure |
|
|
57 | (4) |
|
|
61 | (1) |
|
3.2 Critiques of Granular Hydrodynamics |
|
|
62 | (4) |
|
3.3 Applications of Granular Hydrodynamics |
|
|
66 | (7) |
|
3.3.1 Linear Stability Analysis of the Homogeneous Cooling State |
|
|
66 | (2) |
|
3.3.2 A Solvable Case: Granular Sedimentation in 2D |
|
|
68 | (3) |
|
|
71 | (1) |
|
3.3.4 Other Instabilities of Granular Hydrodynamic |
|
|
72 | (1) |
|
3.4 Fluctuating Hydrodynamics |
|
|
73 | (8) |
|
3.4.1 Simple Models of Noise |
|
|
74 | (3) |
|
3.4.2 Deriving the Fluctuations from the Kinetic Equation |
|
|
77 | (2) |
|
|
79 | (2) |
|
4 Tracer's Diffusion: Swimming Through the Grains |
|
|
81 | (16) |
|
|
81 | (4) |
|
4.1.1 Decoupling the Gas from the Tracer |
|
|
82 | (1) |
|
4.1.2 The Transition Rate |
|
|
83 | (2) |
|
|
85 | (4) |
|
4.2.1 Langevin Equation for the Tracer |
|
|
87 | (2) |
|
4.3 Non-Markovian Tracer's Diffusion |
|
|
89 | (1) |
|
4.4 The Granular Brownian Ratchet |
|
|
90 | (7) |
|
|
91 | (2) |
|
4.4.2 Other Methods, Models and Experiments |
|
|
93 | (1) |
|
|
94 | (3) |
|
5 The Arrow of Time: Past and Future of Grains |
|
|
97 | (12) |
|
5.1 Equilibrium from a Dynamical Perspective |
|
|
97 | (4) |
|
5.1.1 The Case of Markov Processes |
|
|
98 | (1) |
|
|
98 | (1) |
|
5.1.3 Observables Related to Entropy Production |
|
|
99 | (2) |
|
5.2 The Case of the Granular Intruder |
|
|
101 | (5) |
|
5.2.1 The Paradox of the Large Mass Limit |
|
|
101 | (1) |
|
|
102 | (1) |
|
|
103 | (1) |
|
5.2.4 Coupling with the Fluid: Non-equilibrium Re-established |
|
|
104 | (2) |
|
5.3 Time-Reversal in Fluctuating Hydrodynamics |
|
|
106 | (3) |
|
|
107 | (2) |
Conclusion and Perspectives |
|
109 | (2) |
Appendix A Expansion of the First Two Moments of the Transition Rates for Large Mass of the Tracer |
|
111 | (6) |
Index |
|
117 | |