Age | Commit message (Collapse) | Author |
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Nothing too crazy here, the speed= setting still controls the
speed in lieu of something driving the tap.
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This is too aggressive and produces some undesirable visible
artifacts on the periphery, especially for slow-moving
small-size fields.
In such scenarios the elements near the edges would be
excessively pruned when the direction wandered off-screen, then
leaving an overly sparse region when the direction inevitably
wandered back.
This is still an issue but it's far less prominent when only
clipping to the flow field boundaries... since the FOV doesn't
quite encompass the edges of the flow field. Now the elements
can survive wandering a bit off-screen, and re-enter.
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This is a first stab at colorizing the output.
The flow field now has two v3f_t datums per cell, direction and
color.
It's a bit pastel-y and color choice/palettes definitely needs
work, at least some gamma correction would make sense.
But I kind of like the pastel look actually, some of the
combinations start looking very 80s aesthetic.
A good way to watch flow's possibilities is:
--module=rtv,channels=flow,duration=10,context_duration=10,caption_duration=0 \
--video=sdl,fullscreen=on --defaults --go
The long-ish duration really gives a chance to get into the
groove of things before switching
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Simplify ff_new() failure path by using ff_free(), also make
ff_free() more ergonomic by returning NULL.
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This is kind of a particle system, where the particles are pushed
around through a 3D vector space treated as a flow field.
No physics are being simulated here, it's just treating the flow
field as direction vectors that are trilinearly interpolated when
sampled to produce a single direction vector. That direction
vector gets applied to particles near it.
To keep things interesting the flow field evolves by having two
distinct flow fields which the simulation progressively
alternates sampling from. For every frame, both flow fields are
sampled for every particle, but how much weight is given to the
influence of one vs. the other varies by a triangle wave over
time. When the weight is biased enough to one of the flow fields
near a peak/valley in the triangle wave, the other gets
re-populated while its influence is negligible, also
interpolating its new values with 25% influence from the active
field.
The current flow field population routine is completely random.
Yet there's a surprising amount of emergent order despite being
totally randomized direction vectors.
Currently supported settings include:
size= the width of the 3D flow field cube in direction vectors
(the number of vectors is size*size*size)
count= the number of particles/elements
speed= how far a particle is moved along the current sample's
direction vector
This was first implemented in 2017, but sat unfinished in a topic
branch for myriad reasons. Now that rototiller has much more
robust settings infrastructure, among other things, it seemed
worth finishing this up and merging.
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