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See Pyro look development for information on using the parameters to achieve different flame and smoke looks.
The Smoke Solver is able to perform the basic steps required for a smoke simulation. Pyro Solver (Sparse) extends the functionality of this solver by adding flame simulation along with extra shaping controls.
The essential building blocks of a smoke simulation are the object, solver, and sourcing. The Smoke Object (Sparse) node creates a dynamic object containing the required fields, which are then evolved by the solver as the simulation proceeds. The simplest smoke simulation needs the following data:
densityscalar field that contains where and how much smoke is present;
temperaturescalar field that’s used for buoyancy calculations;
velvector field that captures the instantaneous motion of the smoke.
This solver takes care of ensuring these fields change in a manner consistent
with smoke, but sourcing is responsible for injecting these quantities through
the course of the simulation. For example, you may want to continuously add to
density at the soot source or
temperature to cause hot regions to rise. See
pyro sourcing for more information.
Tools under the Sparse Pyro FX shelf can be used to create setups involving the pyro solver.
By default, this solver operates in sparse mode; that is, the needed
calculations are performed only in the areas of interest, as governed by the
active field. This region is built by looking at the Reference Fields
parameter under the Resizing subtab of the Advanced tab: positive areas
of the specified fields are flagged as active. This intermediate active region
is then dilated to provide a buffer for smoke to expand into. With the
Reference Fields set to
density, for example, the solver will run its
operations near areas which have some soot, thereby concentrating the
computational effort to the smoke’s visible region.
Inactive areas in sparse mode are treated as vacuum that smoke is free to move into. As such, if there are two puffs of smoke blowing at each other, they will be completely invisible to one another until they come sufficiently close for their disjoint active regions to merge.
When Enable Sparse Solving is disabled under the aforementioned tab, the solver will work in dense mode, performing a full global solve everywhere within the domain. With the previous example involving two puffs of smoke, they will be immediately aware of each other’s presence. However, dense mode can be substantially slower in some cases.
You can enable Active Region visualization under the Guides tab of the smoke object to see the active simulation areas.
A smoke object to work on.
When working in sparse mode, Enable Sparse Solving must be enabled on the smoke object.
Nodes attached to this input will be able to use the smoke’s accurate velocity field. The Gas Advect node can be hooked up, for instance, to advect the points of an attached geometry data along with the smoke.
It is not safe to modify the velocity through this input; use the Sourcing or Forces inputs instead.
This input should be used to modify the simulation fields, by sourcing with a Volume Source, for example. It is important to perform any sourcing that affects the active region in sparse mode through this input.
active field at this point is not up-to-date; thus, if you want to
perform an operation that can be done sparsely, it is best to use the
Microsolvers attached to this input will be run before the final pressure
projection. At this point, the
active field can be used as a stencil for
DOPs that support it.
Before the nodes attached to this input are executed, the
is updated to account for any operations that were performed in the
A scaling factor for time inside this solver. 1 is normal speed, greater than 1 speeds up the simulation, while less than 1 slows it down.
A blur factor on the velocity field. A value of 0 allows adjacent voxels to move in different directions without resistance, creating a more chaotic, turbulent look. Higher values of this parameter result in a more coherent velocity field, creating a more flowing look.
Advection-Reflection attempts to inject energy lost due to pressure projection back into the simulation. Enabling this option may exhibit better vortex retainment in the flow.
No reflection is performed; this is the recommended setting for
simulations that involve non-zero goal
divergence, such as explosions.
Performs a single pressure projection per timestep and adds the removed velocity components back at the next step. This option is marginally slower than Disabled, but requires an extra vector field to be carried between timesteps.
Performs two pressure projections and velocity advection passes per timestep. This option is a lot slower than Single-Project, but may yield better results and stability.
Fraction of the projected velocities to re-inject when Advection-Reflection is not set to Disabled. Values near 1 will do a better job of conserving energy, but may result in instabilities.
A blur factor on the temperature field. Higher values diffuse the temperature out further, emulating the spread of heat from hotter to colder areas.
How fast the temperature field cools to zero.
Ambient Temp (K)
Temperature corresponding to value of 0 in the
temperature field (in
Kelvin). This represents the ambient temperature of the environment.
Reference Temp (K)
Temperature corresponding to value of 1 in the
temperature field (in
Kelvin). The temperature range is used to calculate strength of the buoyancy
In general, value of
T in the
temperature field corresponds to a
Ambient Temp (K) + T * (Reference Temp (K) - Ambient Temp (K)).
Hot gas expands, causing it to rise due to lowered density. Acceleration due to buoyancy is calculated using values of the ambient and reference temperatures, as well as the Gravity settings. Value of this parameter is used as a multiplier for the buoyancy force.
Acceleration due to gravity. Stronger gravity results in stronger buoyancy forces.
The direction in which gravity pulls. Hotter gas will tend to rise in the opposite direction.
Use the OpenCL device to accelerate computations.
OpenCL acceleration is currently only supported in dense mode (when Enable Sparse Solving is disabled).
The solver will take at least this many substeps per frame. If you have unusual forces, you may want to increase this parameter for better stability. Increasing this parameter usually makes the simulation run noticeably slower.
The solver will take at most this many substeps per frame.
When Max Substeps is greater than 1, the solver uses this parameter to determine the number of substeps. The condition is that no substep can allow objects to interpenetrate by more than this many voxels. Higher values let the solver take larger substeps, possibly letting smoke pass through colliders.
Quantize to Max Substeps
When enabled, all substeps will divide the frame by Max Substeps. For example, if Max Substeps is set to 4, but the CFL Condition only requires 3 substeps, the solver will take frame steps 0.25, 0.5, and 0.25. This option can be useful for re-using input geometry that has been cached to file at increments of 1/Max Substeps.
Frames Before Solve
Delays the actual simulation this many frames after the object creation. Nodes attached to the Sourcing input will still be executed. This may be needed if some solve nodes can’t be processed before certain initial conditions have been met.
Resize in Full Tiles
When enabled, size changes to the fields will be done in increments of 16 voxels. This is marginally more efficient, but the resultant fields will be larger than necessary.
Resizing is always done in full tiles when Enable Sparse Solving is turned on.
List of fields that determine size of the simulation container. Resizing is done by first computing the bounding box around all voxels of Reference Fields that have a positive value, then expanding this intermediate region by Padding on all sides. This list of fields is also used to build the active region in sparse mode.
Amount of padding to add to the simulation region around the Reference Fields. Padding should be as small as possible, but large enough to ensure that moving smoke does not leave the container within a timestep.
When Enable Sparse Solving is turned on, Padding also controls size of the buffer built into the active region.
By default, the smoke solver will resize
flame (for pyro
only). Additional fields may be resized by specifying them here.
Enable Sparse Solving
Puts the solver in sparse mode, allowing it to perform its computations only in relevant areas.
Enable Sparse Solving must also be enabled on the smoke object for sparse mode to work correctly.
Rule that determines where the fields specified in Fields to Reset are modified.
Fields are not modified anywhere.
Fields are reset in the areas that were previously inactive but are now active.
Fields are reset in the areas that were previously active but are now inactive.
Newly Occupied or Deoccupied
Fields are reset in the areas that changed their activity status in either direction.
Fields to Reset
List of fields to reset, based on the Reset Rule. In the regions where they are modified, these fields are set to their initial value.
A list of forces to scale by the value of the
density field at each voxel.
A list of forces to apply uniformly to all voxels (ignoring their
The algorithm used to perform advection. Semi-Lagrangian is the most basic: it simply traces trajectories through the Velocity Field once to update the Field values. Modified MacCormack carries out an extra tracing step to approximate and compensate for the introduced error; as a result, sharp features of the original field can be better preserved. BFECC performs yet another trace to predict the motion of the estimated error, producing the best results at the highest computational cost.
The error correction steps of Modified MacCormack and BFECC advection may introduce final voxel values that lie outside the range of the original field: this can create negative densities or large velocities, for example. When such values are detected, the final field value depends on the setting of this parameter.
No clamping is performed.
Clamps the value to ensure it lies in the range that would have been seen by Semi-Lagrangian advection.
Falls back to the value predicted by Semi-Lagrangian advection.
Apply a smooth blend between non-clamped and clamped values as the advected field approaches the clamping limit. Particularly with the Revert option, applying a small amount of Blend (0.05-0.1) can reduce grid artifacts in the advected field.
Controls how trajectories are traced through the velocity field. Options in this menu are listed in the order of increasing accuracy and computational cost.
With an appropriate value for the CFL Condition, Forward Euler should be sufficient. Consider using a higher-order Trace Method if you need to use a larger CFL Condition or if you choose to disable that option altogether.
When enabled, trajectory tracing will be done in steps to ensure that the calculated path reflects variations in the velocity field. The step size is governed by the value of this parameter. Particularly, the number of field voxels traveled in each step is equal to the CFL Condition.
Provides a safety limit on the number of steps that can be taken to trace trajectories.
Step limiting will also always apply to velocity advection, even when Use Field Advection Settings for Velocity is disabled.
Max Batch Size
To minimize the cost of tracing paths through the Velocity Field, the target fields are organized into batches (based on their voxel sampling settings), and each batch is advected simultaneously. Enabling this option allows you to limit the number of fields that can be processed in each batch. This is useful for reducing peak memory usage of the advection step.
The batch settings will also always apply to velocity advection, even when Use Field Advection Settings for Velocity is disabled.
By default, the solver will advect
flame (for pyro only). Additional fields may be advected by specifying
Use Field Advection Settings for Velocity
When enabled, Field Advection settings will also be used to advect the velocity field. Turning this option off allows you to change advection settings for velocity.
The remaining settings in this section are the same as the ones listed under Field Advection.
Build Collision Mask
If this option is enabled, the solver will build the
collisionvel fields, allowing automatic interaction between smoke and
Controls how far from the collision objects the relevant fields are to be built. This value is measured in voxels. If disabled, the fields will be initialized everywhere.
Use Point Velocity for Collisions
The local velocity of an affector object is a combination of the angular and linear velocity. However, if the object is deforming and points match frame to frame, the local point velocity can be used as well to estimate the deformation effect.
Use Volume Velocity for Collisions
If an affector object doesn’t have a stable point count, but does have a volume representation, the change in the volume representation can be used as an estimate of deformation velocity.
This does not include any velocity tangential to the volume surface: a conveyor belt will appear to be stationary as the volume remains unchanged frame to frame.
Collide with Non-SDF
Normally, the collision relationship uses the signed distance field for each
object. However, if the object is a different type you can use other ways of
getting its effective signed distance field. If this option is enabled, the
object is examined for a
surface scalarfield, which is treated as a signed
distance field. If a
density field is present, it is treated as a fog
volume with a 0.5 cutoff. If a
Geometry geometry is attached, and it
consists of a single volume, that volume will be treated as a fog volume
(with cutoff of 0.5). However, if its boundary condition is set to SDF, it
will be treated as an SDF.
When enabled, the specified fields will be reset inside the colliders.
Fields to Correct
These fields will be reset inside the colliders when Correct Collisions is turned on.
The degree to which the colliders are affected by smoke is controlled by the value of this parameter. Higher values will increase the effect of pressure forces on the colliders. A value of 0 will prevent any feedback.
Colliders are integrated into the system using a weak coupling approach. The number of projection iterations is controlled by this parameter. Larger values will slow down the simulation, but yield better interaction with collision objects.
Filter Hourglass Modes
Enables filtering of spurious divergent modes that may survive pressure projection when Velocity Sampling on the smoke object is set to Center.
Strength of hourglass filtering. Value of
0 disables the filtering
1 performs full filtering.
Scale by Divergence
Instead of performing the filtering everywhere, it can be selectively applied to voxels where divergence is still detected by turning this option on.
Use Relative Divergence
Similar to Scale by Divergence, this setting applies the filtering with different strength in different places. Instead of pure divergence, however, the quantity used to control filtering strength is the ratio of divergence to speed.
Controls how sensitive filter strength is to the remaining divergence (or divergence relative to speed if Use Relative Divergence is enabled). That is, the relevant quantity is multiplied by this amount before it is used to determine filter strength.
Visualize Filter Strength
When using an adaptive filter (Scale by Divergence turned on), the strength field can be visualized by enabling this option.
Orientation of the cutting plane for visualization.
Relative position of the cutting plane inside the bounding box.
Determines how strength values (which fall between
converted to colors.