Search results for "Packing"

showing 10 items of 150 documents

Packing a Trunk

2003

We report on a project with a German car manufacturer. The task is to compute (approximate) solutions to a specific large-scale packing problem. Given a polyhedral model of a car trunk, the aim is to pack as many identical boxes of size 4 × 2 × 1 units as possible into the interior of the trunk. This measure is important for car manufacturers, because it is a standard in the European Union.

CombinatoricsPacking problemsMeasure (data warehouse)Linear programmingPolytope modelmedia_common.cataloged_instanceEuropean unionGreedy algorithmInteger programmingAlgorithmTrunkMathematicsmedia_common
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Local dimensions of sliced measures and stability of packing dimensions of sections of sets

2004

Abstract Let m and n be integers with 0 R n to certain properties of plane sections of μ. This leads us to prove, among other things, that the lower local dimension of (n−m)-plane sections of μ is typically constant provided that the Hausdorff dimension of μ is greater than m. The analogous result holds for the upper local dimension if μ has finite t-energy for some t>m. We also give a sufficient condition for stability of packing dimensions of section of sets.

CombinatoricsSection (fiber bundle)Mathematics(all)Packing dimensionDimension (vector space)Plane (geometry)General MathematicsHausdorff dimensionMathematical analysisConstant (mathematics)Stability (probability)MathematicsAdvances in Mathematics
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Quantum Monte Carlo study of high pressure solid molecular hydrogen

2013

We use the diffusion quantum Monte Carlo (DMC) method to calculate the ground state phase diagram of solid molecular hydrogen and examine the stability of the most important insulating phases relative to metallic crystalline molecular hydrogen. We develop a new method to account for finite-size errors by combining the use of twist-averaged boundary conditions with corrections obtained using the Kwee-Zhang-Krakauer (KZK) functional in density functional theory. To study band-gap closure and find the metallization pressure, we perform accurate quasi-particle many-body calculations using the $GW$ method. In the static approximation, our DMC simulations indicate a transition from the insulating…

Condensed Matter - Materials Science540 Chemistry and allied sciencesMaterials scienceCondensed matter physicsBand gapQuantum Monte CarloClose-packing of equal spheresMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesGeneral Physics and Astronomy540 ChemieDensity functional theoryBoundary value problemDiffusion (business)Ground statePhase diagram
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Mode coupling approach to the ideal glass transition of molecular liquids: Linear molecules

1997

The mode coupling theory (MCT) for the ideal liquid glass transition, which was worked out for simple liquids mainly by Gotze, Sjogren, and their co-workers, is extended to a molecular liquid of linear and rigid molecules. By use of the projection formalism of Zwanzig and Mori an equation of motion is derived for the correlators S[sub lm,l[sup (prime)]m[sup (prime)]]([bold q],t) of the tensorial one-particle density rho [sub lm]([bold q],t), which contains the orientational degrees of freedom for l(greater-than)0. Application of the mode coupling approximation to the memory kernel results into a closed set of equations for S[sub lm,l[sup (prime)]m[sup (prime)]]([bold q],t), which requires t…

Condensed Matter::Soft Condensed MatterDipoleQuantum mechanicsMode couplingErgodic theoryEquations of motionLinear molecular geometryHard spheresGlass transitionAtomic packing factorMathematicsPhysical Review E
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Direct observation of a buckling transition during the formation of thin colloidal crystals

2007

We have investigated a colloidal suspension in a thin wedge formed by two glass plates in the presence of a lateral pressure. Starting with a single hexagonal layer, with increasing separation between the glass plates additional layers are added. This process is accompanied by a number of structural transitions necessary to maintain a high packing fraction under the given boundary conditions. Besides the well-known sequence of hexagonal and quadratic phases, we observe two new phases which are identified with the buckling and the rhombic phase recently predicted by other authors.

Condensed Matter::Soft Condensed MatterPhase transitionCrystallographyColloidMaterials sciencegenetic structuresBucklingDirect observationBoundary value problemColloidal crystalComposite materialAtomic packing factorWedge (geometry)
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Brownian dynamics of polydisperse colloidal hard spheres: Equilibrium structures and random close packings

1994

Recently we presented a new technique for numerical simulations of colloidal hard-sphere systems and showed its high efficiency. Here, we extend our calculations to the treatment of both 2- and 3-dimensional monodisperse and 3-dimensional polydisperse systems (with sampled finite Gaussian size distribution of particle radii), focusing on equilibrium pair distribution functions and structure factors as well as volume fractions of random close packing (RCP). The latter were determined using in principle the same technique as Woodcock or Stillinger had used. Results for the monodisperse 3-dimensional system show very good agreement compared to both pair distribution and structure factor predic…

Condensed Matter::Soft Condensed MatterPhase transitionDistribution functionMaterials scienceRandom close packVolume fractionBrownian dynamicsThermodynamicsStatistical and Nonlinear PhysicsHard spheresAtomic packing factorStructure factorMathematical PhysicsJournal of Statistical Physics
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Phase transitions and phase equilibria in spherical confinement

2013

Phase transitions in finite systems are rounded and shifted and affected by boundary effects due to the surface of the system. This interplay of finite size and surface effects for fluids confined inside of a sphere of radius $R$ is studied by a phenomenological theory and Monte Carlo simulations of a model for colloid-polymer mixtures. For this system the phase separation in a colloid-rich phase and a polymer-rich phase has been previously studied extensively in the bulk. It is shown that spherical confinement can strongly enhance the miscibility of the mixture. Depending on the wall potentials at the confining surface, the wetting properties of the wall can be controlled, and this interpl…

Condensed Matter::Soft Condensed MatterQuantum phase transitionsymbols.namesakePhase transitionMaterials scienceCondensed matter physicsPhase (matter)symbolsRadiusWettingAtomic packing factorKelvin equationCritical exponentPhysical Review E
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Frustration of structural fluctuations upon equilibration of shear melts

2002

Abstract We report on the formation of amorphous solids from aquaeous suspensions of charged colloidal spheres. Comprehensive light scattering and microscopic studies show that in these systems the nucleation rate density continuously increases to very high values. At the highest particle densities of 47.5 μm −3 (packing fraction Φ =0.146) an amorphous state is observed of only short range order, finite static shear modulus and frozen long time dynamics. This state is composed of a piling of––as we propose pre-critical––nuclei. Differences from the Hard Sphere case are discussed in some detail. There the arrest of density fluctuations is observed and described by Mode Coupling scenarios. In…

Condensed matter physicsChemistrymedia_common.quotation_subjectNucleationFrustrationHard spheresCondensed Matter PhysicsAtomic packing factorLight scatteringElectronic Optical and Magnetic MaterialsAmorphous solidCondensed Matter::Soft Condensed MatterShear modulusChemical physicsMetastabilityMaterials ChemistryCeramics and Compositesmedia_commonJournal of Non-Crystalline Solids
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Glass transition of hard spheres in high dimensions

2009

We have investigated analytically and numerically the liquid-glass transition of hard spheres for dimensions $d\to \infty $ in the framework of mode-coupling theory. The numerical results for the critical collective and self nonergodicity parameters $f_{c}(k;d) $ and $f_{c}^{(s)}(k;d) $ exhibit non-Gaussian $k$ -dependence even up to $d=800$. $f_{c}^{(s)}(k;d) $ and $f_{c}(k;d) $ differ for $k\sim d^{1/2}$, but become identical on a scale $k\sim d$, which is proven analytically. The critical packing fraction $\phi_{c}(d) \sim d^{2}2^{-d}$ is above the corresponding Kauzmann packing fraction $\phi_{K}(d)$ derived by a small cage expansion. Its quadratic pre-exponential factor is different fr…

Condensed matter physicsStatistical Mechanics (cond-mat.stat-mech)FOS: Physical sciencesGeometryScale (descriptive set theory)Hard spheresCondensed Matter - Soft Condensed MatterAtomic packing factorQuadratic equationExponentSoft Condensed Matter (cond-mat.soft)Glass transitionCritical exponentCondensed Matter - Statistical MechanicsMathematics
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Controlling molecular packing for charge transport in organic thin film devices

2012

Controlling molecular packingSettore CHIM/02 - Chimica Fisica
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