Lattice Boltzmann collision operators enforcing isotropy and Galilean invariance
A method comprising: simulating, in a lattice velocity set, movement of particles in a volume of fluid, with the movement causing collision among the particles; based on the simulated movement, determining relative particle velocity of a particle at a particular location within the volume, with the relative particle velocity being a difference between (i) an absolute velocity of the particle at the particular location within the volume and measured under zero flow of the volume, and (ii) a mean velocity of one or more of the particles at the particular location within the volume; and determining, based on the relative particle velocity, a non-equilibrium post-collide distribution function of a specified order that is representative of the collision.
1. A method for simulating movement of particles in a volume of fluid by a computer using a lattice velocity set, with the movement causing collisions among the particles, the method comprising:
providing a lattice model having and a lattice velocity set that provides support for hydrodynamic moments;
receiving by one or more computer systems a model of a simulation space including a lattice structure represented as a collection of voxels, and a representation of a physical object, with the voxels having appropriate resolutions to account for surfaces of the physical object;
over a plurality of time increments, and for each time increment,
simulating advection of particles from a first voxel to a subsequent voxel during the time increment; and
simulating interaction of particles within each subsequent voxel during the time increment by applying a lattice post-collide distribution function that is defined in terms of a collision operator of a specified order Galilean invariance in terms of Mach number for the lattice velocity set.
2. The method of claim 1 , wherein the lattice velocity set represents a starting pocket of fluid and a nearby pocket of fluid, and wherein the method further comprises:
determining an effect of the nearby pocket of fluid on the starting pocket of fluid.
3. The method of claim 1 , wherein the lattice post-collide distribution function is a filtered collision operator, and wherein applying the filtered collision operator removes interactions representing non-equilibrium moments.
4. The method of claim 1 , wherein the lattice post-collide distribution function is a filtered collision operator that is based on absolute values of speed or energy represented in the simulation.
5. The method of claim 1 , wherein the lattice post-collide distribution function is a filtered collision operator that is configured to exclude higher order terms that are unsupported by the lattice velocity set.
6. The method of claim 1 , wherein the provided support is first order support for hydrodynamic moments and wherein the specified order Galilean invariance is first order Galilean invariance.
7. The method of claim 1 , wherein the provided support is second order support for hydrodynamic moments and wherein the specified order Galilean invariance is second order Galilean invariance.
8. The method of claim 1 , wherein the lattice model is a lattice Boltzmann model.
9. One or more machine-readable hardware storage devices for simulating movement of particles in a volume of fluid by a computer using a lattice velocity set, with the movement causing collision among the particles, the one or more machine-readable hardware storage devices storing instructions that are executable by one or more processing devices to perform operations comprising:
providing a lattice model having a lattice velocity set that provides support for hydrodynamic moments;
receiving by one or more computer systems a model of a simulation space including a lattice structure represented as a collection of voxels, and a representation of a physical object, with the voxels having appropriate resolutions to account for surfaces of the physical object;
over a plurality of time increments, and for each time increment,
simulating advection of particles from a first voxel to a subsequent voxel during the time increment; and
simulating interaction of particles within each voxel during the time increment by applying a lattice post-collide distribution function that is defined in terms of a collision operator of a specified order Galilean invariance in terms of Mach number for the lattice velocity set.
10. The one or more machine-readable hardware storage devices of claim 9 , wherein the lattice velocity set represents a starting pocket of fluid and a nearby pocket of fluid, and wherein the operations further comprise:
determining an effect of the nearby pocket of fluid on the starting pocket of fluid.
11. The one or more machine-readable hardware storage devices of claim 9 , wherein the lattice post-collide distribution function is a filtered collision operator, and wherein the operations further comprise:
applying the filtered collision operator to remove interactions representing non-equilibrium moments.
12. The one or more machine-readable hardware storage devices of claim 9 , wherein the lattice post-collide distribution function is a filtered collision operator that is based on absolute values of speed or energy represented in the simulation.
13. The one or more machine-readable hardware storage devices of claim 9 , wherein the lattice post-collide distribution function is a filtered collision operator that is configured to exclude higher order terms that are unsupported by the lattice velocity set.
14. The one or more machine-readable hardware storage devices of claim 9 , wherein the provided support is first order support for hydrodynamic moments and wherein the specified order Galilean invariance is first order Galilean invariance.
15. The one or more machine-readable hardware storage devices of claim 9 , wherein the provided support is second order support for hydrodynamic moments and wherein the specified order Galilean invariance is second order Galilean invariance.
16. The one or more machine-readable hardware storage devices of claim 9 , wherein the lattice model is a lattice Boltzmann model.
17. A data processing system for simulating movement of particles in a volume of fluid using a lattice velocity set, with the movement causing collision among the particles, the data processing system comprising one or more processing devices and one or more machine-readable hardware storage devices storing instructions that are executable by the one or more processing devices to perform operations comprising:
providing a lattice model having a lattice velocity set that provides support for hydrodynamic moments;
receiving by one or more computer systems a model of a simulation space including a lattice structure represented as a collection of voxels, and a representation of a physical object, with the voxels having appropriate resolutions to account for surfaces of the physical object;
over a plurality of time increments, and for each time increment,
simulating advection of particles from a first voxel to a subsequent voxel during the time increment; and
simulating interaction of particles within each voxel during the time increment by applying a lattice post-collide distribution function that is defined in terms of a collision operator of a specified order Galilean invariance in terms of Mach number for the lattice velocity set.
18. The data processing system of claim 17 , wherein the lattice velocity set represents a starting pocket of fluid and a nearby pocket of fluid, and wherein the operations further comprise:
determining an effect of the nearby pocket of fluid on the starting pocket of fluid.
19. The data processing system of claim 17 , wherein the lattice post-collide distribution function is a filtered collision operator, and wherein applying the filtered collision operator removes interactions representing non-equilibrium moments.
20. The data processing system of claim 17 , wherein the lattice post-collide distribution function is a filtered collision operator that is based on absolute values of speed or energy represented in the simulation.