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22nd July 2013 |
09:30 to 11:00 |
E Knobloch |
Localized structures in fluid flows |
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22nd July 2013 |
11:15 to 12:00 |
M Shearer |
Surfactants and Thin Liquid Layers 1 |
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22nd July 2013 |
14:00 to 14:45 |
M Shearer |
Surfactants and Thin Liquid Layers 1 |
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22nd July 2013 |
15:00 to 16:30 |
R Kamien |
Topological defects in crystals and liquid crystals 1 |
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23rd July 2013 |
09:30 to 10:15 |
L Pismen |
Bridging the scales near the contact line 1 |
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23rd July 2013 |
10:15 to 11:00 |
U Thiele |
Gradient dynamics formulations of thin film equations |
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23rd July 2013 |
11:15 to 12:00 |
D Holm |
Geometric approach to modelling complex fluids 1 |
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23rd July 2013 |
14:00 to 14:45 |
D Holm |
Geometric approach to modelling complex fluids 1 |
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23rd July 2013 |
15:00 to 16:30 |
I Stewart |
Introduction to liquid crystal continuum theory: statics and dynamics |
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24th July 2013 |
09:30 to 11:00 |
E Knobloch |
Localized structures in fluid flows |
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24th July 2013 |
11:30 to 13:00 |
L Biferale |
Lattice Boltzmann Methods for multi-phase turbulent flows |
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25th July 2013 |
09:30 to 11:00 |
I Stewart |
Introduction to liquid crystal continuum theory: statics and dynamics |
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25th July 2013 |
11:15 to 12:00 |
D Holm |
Geometric approach to modelling complex fluids 2 |
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25th July 2013 |
14:00 to 14:45 |
D Holm |
Geometric approach to modelling complex fluids 2 |
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25th July 2013 |
15:00 to 16:30 |
J Ward |
Fluid dynamic approaches to modelling bacterial biofilms growth |
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26th July 2013 |
09:30 to 11:00 |
R Kamien |
Topological defects in crystals and liquid crystals 2 |
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26th July 2013 |
11:15 to 12:00 |
L Pismen |
Bridging the scales near the contact line 2 |
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26th July 2013 |
14:00 to 14:45 |
L Pismen |
Bridging the scales near the contact line 3 |
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26th July 2013 |
15:00 to 16:30 |
U Thiele |
Depinning transitions and deposition patterns |
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29th July 2013 |
09:30 to 11:00 |
AD Rey |
Mechanics and Thermodynamics of Nematic Shape Equations |
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29th July 2013 |
11:15 to 12:00 |
F Gay-Balmaz |
An introduction to the variational principles and Poisson brackets for complex fluids |
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29th July 2013 |
14:00 to 14:45 |
F Gay-Balmaz |
Equivalent theories of liquid crystals |
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29th July 2013 |
15:00 to 16:30 |
S Kalliadasis |
Recent progress on the moving contact line problem |
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30th July 2013 |
09:30 to 11:00 |
T Ratiu |
Geometric approach to the Hamiltonian and Lagrangian formulation of complex fluids |
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30th July 2013 |
11:15 to 12:00 |
J Toner |
Fish gotta swim, birds gotta fly, I gotta do Feynmann graphs 'till I die: A hydrodynamic theory of flocking 1 (Part 1) |
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30th July 2013 |
14:00 to 14:45 |
J Toner |
Fish gotta swim, birds gotta fly, I gotta do Feynmann graphs 'till I die: A hydrodynamic theory of flocking 1 (Part 2) |
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30th July 2013 |
15:00 to 16:30 |
A Bertozzi |
Particle laden thin films: theory and experiment |
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31st July 2013 |
09:30 to 11:00 |
J Feng |
Computation of complex fluid flows |
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31st July 2013 |
11:30 to 13:00 |
R Golestanian |
Hydrodynamic Coordination at Low Reynolds Number |
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1st August 2013 |
09:30 to 11:00 |
Y Kevrekidis |
Equation-free approach to deriving effective macroscopic equations for complex interacting systems |
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1st August 2013 |
11:15 to 12:00 |
AD Rey |
Capillary Models for Liquid Crystal Fibers, Membranes, Films, and Drops |
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1st August 2013 |
14:00 to 14:45 |
AD Rey |
Capillary Models for Liquid Crystal Fibers, Membranes, Films, and Drops (Part 2) |
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1st August 2013 |
15:00 to 16:30 |
J Yeomans |
Swimming at low Reynolds number |
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2nd August 2013 |
09:30 to 11:00 |
T Ratiu |
Geometric approach to the Hamiltonian and Lagrangian formulation of complex fluids |
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2nd August 2013 |
11:30 to 13:00 |
J Toner |
Fish gotta swim, birds gotta fly, I gotta do Feynmann graphs 'till I die: A hydrodynamic theory of flocking 2 ¯ |
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