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| ====== Research ====== | ====== Research ====== |
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| For most of my scientific life I worked on Granular Fluids. While real granular particles like sand, gravel, pills, cereals or coffee beans come in all sorts of shapes and are usually quite irregular, as a theoretician I exclusively use spherical (or disk shaped) particles. I prefer to solve problems with pen and paper (and the occasional help of Gradshteyn and Maple) but I also burn a lot of CPU time running and analyzing event driven molecular dynamics simulations. | For most of my scientific life I worked on Granular Fluids but I also have fun with bacteria and the occasional spin model. While real granular particles like sand, gravel, pills, cereals or coffee beans come in all sorts of shapes and are usually quite irregular, as a theoretician I exclusively use spherical (or disk shaped) particles. I prefer to solve problems with pen and paper (and the occasional help of Gradshteyn and Maple) but I also burn a lot of CPU time running and analysing event driven molecular dynamics simulations. Bacteria, I found, are much more complicated than hard spheres. Still I try to tackle them with simple models. |
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| | ===== Granular Rheology ===== |
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| | Developing constitutive equations for granular fluids is quite challenging. Many attempts have been made starting with the granular Boltzmann equation or similar approaches from the realm of rarefied gases. Unfortunately, granular flows mostly involve high densities and deformation rates far beyond the linear response regime. By exploiting slow relaxation close to the granular glass transition (see below) I could generalize the //Integration Through Transients//((Fuchs & Cates [[https://doi.org/10.1122/1.3119084|J. Rheol.]] **53**, 957 (2009) )) (ITT) approach to granular fluids. For the rich phenomenology |
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| | * see [[res:Granular Rheology]] |
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| ===== The Granular Glass Transition ===== | ===== The Granular Glass Transition ===== |
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| Experiments by Durian //et al.// ((Abate & Durian, [[http://dx.doi.org/10.1103/PhysRevE.74.031308|PRE]] **74**, 031308 (2006) )) indicated that densely packed fluidized granular systems may be in a glassy state. I managed to generalize the so called //Mode Coupling Theory// ((Götze, //Complex dynamics of glass-forming liquids: A mode-coupling theory//, OUP Oxford, 2009)) of the glass transition (that had been developed for equilibrium fluids) to the far from equilibrium stationary state of a driven granular fluid. The result is: It works, it makes nontrivial predictions and there is a granular glass transition | Experiments by Durian //et al.//((Abate & Durian, [[http://dx.doi.org/10.1103/PhysRevE.74.031308|PRE]] **74**, 031308 (2006) )) indicated that densely packed fluidized granular systems may be in a glassy state. I managed to generalize the so called //Mode Coupling Theory//((Götze, //Complex dynamics of glass-forming liquids: A mode-coupling theory//, OUP Oxford, 2009)) of the glass transition (that had been developed for equilibrium fluids) to the far from equilibrium stationary state of a driven granular fluid. The result is: It works, it makes nontrivial predictions and there is a granular glass transition |
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| * see [[res:Granular Glass Transition]] | * see [[res:Granular Glass Transition]] |
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| | ===== Trail-Mediated Microbial Interaction ===== |
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| | A number of micro-organisms leave sticky trails while moving around on surfaces. In turn they react to the presence of trails, effectively using them as a means to communicate((Zhao //et al.// [[http://dx.doi.org/10.1038/nature12155|Nature]] **497**, 388 (2013) )). I could show that trail-mediated self-interactions significantly alter the single particle dynamics and eventually lead to a localization transition. Collectively, we found, trail-mediated interactions to facilitate colony formation in //Pseudomonas aeruginosa// |
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| | * see [[res:Trail-Mediated Interaction]] |
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| | ===== Fluidized Beds ===== |
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| | For the development of new measurement techniques for granular fluids it is useful to have efficient and faithful simulation tools. We are exploring the capabilities of a novel hybrid event-driven code((Fiege & Zippelius [[https://doi.org/10.1088/1742-6596/759/1/012001|J. Phys. Conf. Ser.]] **759**, 012001 (2016) )) to simulate bubbling fluidized beds by cross-validating the numerical results with experimental measurements. |
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| | * see [[res:Fluidized Beds]] |
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| ===== Rough Granular Particles ===== | ===== Rough Granular Particles ===== |
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| For simplicity, granular particles are most often assumed to be smooth. I.e., the slide past each other with zero friction. In reality this is certainly not the case. Frictional particles have a number of surprising features. E.g., there is no equipartition between rotational and translational degrees of freedom ((Luding, Huthmann, McNamara, Zippelius, [[http://dx.doi.org/10.1103/PhysRevE.58.3416|PRE]] **58**, 3416 (1998) )) and with an extremely long calculation, we could show that the axis of rotation and the direction of flight of a rough particle are correlated. | For simplicity, granular particles are most often assumed to be smooth. I.e., the slide past each other with zero friction. In reality this is certainly not the case. Frictional particles have a number of surprising features. E.g., there is no equipartition between rotational and translational degrees of freedom((Luding, Huthmann, McNamara, Zippelius, [[http://dx.doi.org/10.1103/PhysRevE.58.3416|PRE]] **58**, 3416 (1998) )) and with an extremely long calculation, we could show that the axis of rotation and the direction of flight of a rough particle are correlated. |
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| * see [[res:Rough Spheres]] | * see [[res:Rough Spheres]] |
| * see [[res:Granular Mixtures]] | * see [[res:Granular Mixtures]] |
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| [[wr:main]] | [[shear:literature]] |