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Transformation of propositional calculus statements into integer and mixed integer programs: An approach towards automatic reformulation
A systematic procedure for transforming a set of logical statements or logical conditions imposed on a model into an Integer Linear Progamming (ILP) formulation Mixed Integer Programming (MIP) formulation is presented. An ILP stated as a system of linear constraints involving integer variables and an objective function, provides a powerful representation of decision problems through a tightly interrelated closed system of choices. It supports direct representation of logical (Boolean or prepositional calculus) expressions. Binary variables (hereafter called logical variables) are first introduced and methods of logically connecting these to other variables are then presented. Simple constraints can be combined to construct logical relationships and the methods of formulating these are discussed. A reformulation procedure which uses the extended reverse polish representation of a compound logical form is then described. These reformulation procedures are illustrated by two examples. A scheme of implementation.ithin an LP modelling system is outlined
Why are Fluid Densities So Low in Carbon Nanotubes?
The equilibrium density of fluids under nanoconfinement can differ
substantially from their bulk density. Using a mean-field approach to describe
the energetic landscape near the carbon nanotube (CNT) wall, we obtain
analytical results describing the lengthscales associated with the layering
observed at the fluid-CNT interface. When combined with molecular simulation
results for the fluid density in the layered region, this approach allows us to
derive a closed-form prediction for the overall equilibrium fluid density as a
function of the CNT radius that is in excellent agreement with molecular
dynamics simulations. We also show how aspects of this theory can be extended
to describe water confined within CNTs and find good agreement with results
from the literature
A Universal Molecular-Kinetic Scaling Relation for Slip of a Simple Fluid at a Solid Boundary
Using the observation that slip in simple fluids at low and moderate shear
rates is a thermally activated process driven by the shear stress in the fluid
close to the solid boundary, we develop a molecular-kinetic model for simple
fluid slip at solid boundaries. The proposed model, which is in the form of a
universal scaling relation that connects slip and shear rate, reduces to the
well known Navier-slip condition under low shear conditions, providing a direct
connection between molecular parameters and the slip length. Molecular-dynamics
simulations are in very good agreement with the predicted dependence of slip on
system parameters, including the temperature and fluid-solid interaction
strength. Connections between our model and previous work, as well as
simulation and experimental results are explored and discussed
Statistical Error in Particle Simulations of Hydrodynamic Phenomena
We present predictions for the statistical error due to finite sampling in
the presence of thermal fluctuations in molecular simulation algorithms.
Specifically, we establish how these errors depend on Mach number, Knudsen
number, number of particles, etc. Expressions for the common hydrodynamic
variables of interest such as flow velocity, temperature, density, pressure,
shear stress and heat flux are derived using equilibrium statistical mechanics.
Both volume-averaged and surface-averaged quantities are considered.
Comparisons between theory and computations using direct simulation Monte Carlo
for dilute gases, and molecular dynamics for dense fluids, show that the use of
equilibrium theory provides accurate results.Comment: 24 pages postscript (including 16 figures
Lattice ellipsoidal statistical BGK model for thermal non-equilibrium flows
A thermal lattice Boltzmann model is constructed on the basis of the ellipsoidal statistical Bhatnagar-Gross-Krook (ES-BGK) collision operator via the Hermite moment representation. The resulting lattice ES-BGK model uses a single distribution function and features an adjustable Prandtl number. Numerical simulations show that using a moderate discrete velocity set, this model can accurately recover steady and transient solutions of the ES-BGK equation in the slip-flow and early transition regimes in the small Mach number limit that is typical of microscale problems of practical interest. In the transition regime in particular, comparisons with numerical solutions of the ES-BGK model, direct Monte Carlo and low-variance deviational Monte Carlo simulations show good accuracy for values of the Knudsen number up to approximately 0:5. On the other hand, highly non-equilibrium phenomena characterized by high Mach numbers, such as viscous heating and force-driven Poiseuille flow for large values of the driving force, are more difficult to capture quantitatively in the transition regime using discretizations that have been chosen with computational efficiency in mind such as the one used here, although improved accuracy is observed as the number of discrete velocities is increased
Gas-flow animation by unsteady heating in a microchannel
We study the flow-field generated in a one-dimensional wall-bounded gas layer due to an arbitrary small-amplitude time variation in the temperature of its boundaries. Using the Fourier transform technique, analytical results are obtained for the slip-flow/Navier–Stokes limit. These results are complemented by low-variance simulations of the Boltzmann equation, which are useful for establishing the limits of the slip-flow description, as well as for bridging the gap between the slip-flow analysis and previously developed free-molecular analytical predictions. Results are presented for both periodic (sinusoidal) and nonperiodic (step-jump) heating profiles. Our slip-flow solution is used to elucidate a singular limit reported in the literature for oscillatory heating of a dynamically incompressible fluid
An alternative approach to efficient simulation of micro/nanoscale phonon transport
Starting from the recently proposed energy-based deviational formulation for
solving the Boltzmann equation [J.-P. Peraud and N. G. Hadjiconstantinou, Phys.
Rev. B 84, 2011], which provides significant computational speedup compared to
standard Monte Carlo methods for small deviations from equilibrium, we show
that additional computational benefits are possible in the limit that the
governing equation can be linearized. The proposed method exploits the
observation that under linearized conditions (small temperature differences)
the trajectories of individual deviational particles can be decoupled and thus
simulated independently; this leads to a particularly simple and efficient
algorithm for simulating steady and transient problems in arbitrary
three-dimensional geometries, without introducing any additional approximation.Comment: 4 pages, 2 figure
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