compute ID eflux/grid group-ID mix-ID value1 value2 ...
heatx,heaty,heatz = xyz components of energy flux density tensor
compute 1 eflux/grid all species heatx heaty heatz compute 1 eflux/grid subset species heaty
These commands will dump time averaged energy flux densities for each species and each grid cell to a dump file every 1000 steps:
compute 1 eflux/grid all species heatx heaty heatz fix 1 ave/grid 10 100 1000 c_1[*] dump 1 grid all 1000 tmp.grid id f_1[*]
Define a computation that calculates components of the energy flux density vector for each grid cell in a grid cell group. This is also called the heat flux density vector, and is based on the thermal velocity of the particles in each grid cell. The values are tallied separately for each group of species in the specified mixture, as described in the Output section below. See the mixture command for how a set of species can be partitioned into groups.
Only grid cells in the grid group specified by group-ID are included in the calculations. See the group grid command for info on how grid cells can be assigned to grid groups.
The values listed above rely on first computing and subtracting the center-of-mass (COM) velocity for all particles in the group and grid cell from each particle to yield a thermal velocity. This thermal velocity is used to compute the components of the energy flux density vector, as described below. This is in contrast to some of the values tallied by the compute grid temp command which simply uses the full velocity of each particle to compute a momentum or kinetic energy density. For non-streaming simulations, the two results should be similar, but for streaming flows, they will be different.
The results of this compute can be used by different commands in different ways. The values for a single timestep can be output by the dump grid command.
The values over many sampling timesteps can be averaged by the fix ave/grid command. It does its averaging as if the particles in the cell at each sampling timestep were combined together into one large set of particles to compute the formulas below.
Note that the center-of-mass (COM) velocity that is subtracted from each particle to yield a thermal velocity for each particle, as described below, is also computed over one large set of particles (across all timesteps), in contrast to using a COM velocity computed only for particles in the current timestep, which is what the compute sonine/grid command does.
Note that this is a different form of averaging than taking the values produced by the formulas below for a single timestep, summing those values over the sampling timesteps, and then dividing by the number of sampling steps.
Calculation of the energy flux density is done by first calcuating the center-of-mass (COM) velocity of particles for each group with a grid cell. This is done as follows:
COMx = Sum_i (mass_i Vx_i) / Sum_i (mass_i) COMy = Sum_i (mass_i Vy_i) / Sum_i (mass_i) COMz = Sum_i (mass_i Vz_i) / Sum_i (mass_i) Cx = Vx - COMx Cy = Vy - COMy Cz = Vz - COMz Csq = Cx*Cx + Cy*Cy + Cz*Cz
The COM velocity is (COMx,COMy,COMz). The thermal velocity of each particle is (Cx,Cy,Cz), i.e. its velocity minus the COM velocity of particles in its group and cell.
The heatx, heaty, heatz values compute the components of the energy flux density vector due to particles in the group as follows:
heatx = 0.5 * fnum/volume Sum_i (mass_i Cx Csq) heaty = 0.5 * fnum/volume Sum_i (mass_i Cy Csq) heatz = 0.5 * fnum/volume Sum_i (mass_i Cz Csq)
Note that if particle weighting is enabled via the global weight command, then the volume used in the formula is divided by the weight assigned to the grid cell.
This compute calculates a per-grid array, with the number of columns equal to the number of values times the number of groups. The ordering of columns is first by values, then by groups. I.e. if momxx and momxy values were specified as keywords, then the first two columns would be momxx and momxy for the first group, the 3rd and 4th columns would be momxx and momxy for the second group, etc.
This compute performs calculations for all flavors of child grid cells in the simulation, which includes unsplit, cut, split, and sub cells. See Section 6.8 of the manual gives details of how SPARTA defines child, unsplit, split, and sub cells. Note that cells inside closed surfaces contain no particles. These could be unsplit or cut cells (if they have zero flow volume). Both of these kinds of cells will compute a zero result for all their values. Likewise, split cells store no particles and will produce a zero result. This is because their sub-cells actually contain the particles that are geometrically inside the split cell.
Grid cells not in the specified group-ID will output zeroes for all their values.
The array can be accessed by any command that uses per-grid values from a compute as input. See Section 6.4 for an overview of SPARTA output options.
The per-grid array values will be in the units of energy flux density = energy-velocity/volume units.
Styles with a kk suffix are functionally the same as the corresponding style without the suffix. They have been optimized to run faster, depending on your available hardware, as discussed in the Accelerating SPARTA section of the manual. The accelerated styles take the same arguments and should produce the same results, except for different random number, round-off and precision issues.
These accelerated styles are part of the KOKKOS package. They are only enabled if SPARTA was built with that package. See the Making SPARTA section for more info.
You can specify the accelerated styles explicitly in your input script by including their suffix, or you can use the -suffix command-line switch when you invoke SPARTA, or you can use the suffix command in your input script.
See the Accelerating SPARTA section of the manual for more instructions on how to use the accelerated styles effectively.
compute grid, compute thermal/grid, compute pflux/grid, fix ave/grid, dump grid