Volumenpackungen nach SAE J1100

We present new algorithms to approximate the discrete volume of a polyhedral geometry using boxes defined by the US standard SAE J1100. This problem is NP-hard and has its main application in the car design process. The algorithms produce maximum weighted independent sets on a so-called conflict graph for a discretisation of the geometry. We present a framework to eliminate a large portion of the vertices of a graph without affecting the quality of the optimal solution. Using this framework we are also able to define the conflict graph without the use of a discretisation. For the solution of the maximum weighted independent set problem we designed an enumeration scheme which uses the restrictions of the SAE J1100 standard for an efficient upper bound computation. We evaluate the packing algorithms according to the solution quality compared to manually derived results. Finally, we compare our enumeration scheme to several other exact algorithms in terms of their runtime. Grid-based packings either tend to be not tight or have intersections between boxes. We therefore present an algorithm which can compute box packings with arbitrary placements and fixed orientations. In this algorithm we make use of approximate Minkowski Sums, computed by uniting many axis-oriented equal boxes. We developed an algorithm which computes the union of equal axis-oriented boxes efficiently. This algorithm also maintains the Minkowski Sums throughout the packing process. We also extend these algorithms for packing arbitrary objects in fixed orientations.

Crystal phases and glassy dynamics in monodisperse hard ellipsoids

We have performed Monte Carlo and molecular dynamics simulations of suspensions of monodisperse, hard ellipsoids of revolution. Hard-particle models play a key role in statistical mechanics. They are conceptually and computationally simple, and they offer insight into systems in which particle shape is important, including atomic, molecular, colloidal, and granular systems. In the high density phase diagram of prolate hard ellipsoids we have found a new crystal, which is more stable than the stretched FCC structure proposed previously . The new phase, SM2, has a simple monoclinic unit cell containing a basis of two ellipsoids with unequal orientations. The angle of inclination is very soft for length-to-width (aspect) ratio l/w=3, while the other angles are not. A symmetric state of the unit cell exists, related to the densest-known packings of ellipsoids; it is not always the stable one. Our results remove the stretched FCC structure for aspect ratio l/w=3 from the phase diagram of hard, uni-axial ellipsoids. We provide evidence that this holds between aspect ratios 3 and 6, and possibly beyond. Finally, ellipsoids in SM2 at l/w=1.55 exhibit end-over-end flipping, warranting studies of the cross-over to where this dynamics is not possible. Secondly, we studied the dynamics of nearly spherical ellipsoids. In equilibrium, they show a first-order transition from an isotropic phase to a rotator phase, where positions are crystalline but orientations are free. When over-compressing the isotropic phase into the rotator regime, we observed super-Arrhenius slowing down of diffusion and relaxation, and signatures of the cage effect. These features of glassy dynamics are sufficiently strong that asymptotic scaling laws of the Mode-Coupling Theory of the glass transition (MCT) could be tested, and were found to apply. We found strong coupling of positional and orientational degrees of freedom, leading to a common value for the MCT glass-transition volume fraction. Flipping modes were not slowed down significantly. We demonstrated that the results are independent of simulation method, as predicted by MCT. Further, we determined that even intra-cage motion is cooperative. We confirmed the presence of dynamical heterogeneities associated with the cage effect. The transit between cages was seen to occur on short time scales, compared to the time spent in cages; but the transit was shown not to involve displacements distinguishable in character from intra-cage motion. The presence of glassy dynamics was predicted by molecular MCT (MMCT). However, as MMCT disregards crystallization, a test by simulation was required. Glassy dynamics is unusual in monodisperse systems. Crystallization typically intervenes unless polydispersity, network-forming bonds or other asymmetries are introduced. We argue that particle anisometry acts as a sufficient source of disorder to prevent crystallization. This sheds new light on the question of which ingredients are required for glass formation.