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path: root/src/shader/code/vertex.glsl
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2019-11-08Update lattice multiple times per frameAdrian Kummerlaender
Controlled by `--lupf` _Lattice updates per frame_ MLUPS are now calculated and displayed. While performance is still bad compared to a optimized GPU implementation (such as [1] or [2]) this improves the situation. [1]: https://tree.kummerlaender.eu/projects/symlbm_playground/ [2]: https://code.kummerlaender.eu/boltzgen/about/
2019-04-28More consistent restrictions of display valuesAdrian Kummerlaender
2019-04-28Experimental visualization of the velocity curlAdrian Kummerlaender
Calculating the curl of our simulated velocity field requires an additional compute shader step. Handling of buffer and shader switching depending on the display mode is implemented rudimentarily for now. Most of this commit is scaffolding, the actual computation is more or less trivial: ``` const float dxvy = (getFluidVelocity(x+1,y).y - getFluidVelocity(x-1,y).y) / (2*convLength); const float dyvx = (getFluidVelocity(x,y+1).x - getFluidVelocity(x,y-1).x) / (2*convLength); setFluidExtra(x, y, dxvy - dyvx); ``` This implements the following discretization of the 2d curl operator: Let $V : \mathbb{N}^2 \to \mathbb{R}^2$ be the simulated velocity field at discrete lattice points spaced by $\Delta x \in \mathbb{R}_{\gt 0}$. We want to approximate the $z$-component of the curl for visualization: $$\omega := \partial_x F_y - \partial_y F_x$$ As we do not possess the actual function $F$ but only its values at a set of discrete points we approximate the two partial derivatives using a second order central difference scheme: $$\overline{\omega}(i,j) := \frac{F_y(i+1,j) - F_y(i-1,j)}{2 \Delta x} - \frac{F_x(i,j+1) - F_x(i,j-1)}{2 \Delta x}$$ Note that the scene shader does some further rescaling of the curl to better fit the color palette. One issue that irks me is the emergence of some artefacts near boundaries as well as isolated "single-cell-vortices". This might be caused by running the simulation too close to divergence but as I am currently mostly interested in building an interactive fluid playground it could be worth it to try running an additional smoothening shader pass to straighten things out.
2019-04-18Bind keys for display toggling, palette scalingAdrian Kummerlaender
2019-04-17Improve color palette of Knudsen criterion modeAdrian Kummerlaender
2019-04-16Add flag to toggle fluid quality displayAdrian Kummerlaender
e.g. check out `./compustream --size 512 128 --open --lups 300 --quality`
2019-04-16Add basic physical scaling and Knudsen quality criterionAdrian Kummerlaender
The paper "Automatic grid refinement criterion for lattice Boltzmann method" [2015] by Lagrava et al. describes a criterion for measuring the local simulation quality using a comparison of the theoretical Knudsen number and the quotient of the cells's non-equilibrium and equilibrium function. While this criterion was developed to enable automatic selection of areas to be refined, it also offers a interesting and unique perspective on the fluid structure. As the criterion requires calculation of the modeled Reynolds-, Mach- and Knudsen-numbers I took the time to set up the basics for scaling the simulation to actually model a physical system. Or rather calculating which physical model is represented by the chosen resolution and relaxation time. [2015]: https://arxiv.org/abs/1507.06767
2019-02-27Test density inflow conditionAdrian Kummerlaender
Seems to be more stable when drawing around. Not that all of this doesn't aim to be accurate in any real world sense.
2019-02-25Add cylinder and dampened inflow to open geometryAdrian Kummerlaender
2019-02-23Store material in fluid buffer and improve visualizationAdrian Kummerlaender
Replaces the density value which is actually not that useful for visualization. Encoding integer values as floats by casting and comparing them using exact floating point comparison is not very safe but works out for now.
2019-02-22Tidy up wall drawing and geometry initializationAdrian Kummerlaender
2019-02-22Improvise interactive wall drawingAdrian Kummerlaender
Internal wall cells need to be disabled to prevent delayed propagation of the reflected populations. This is just quickly thrown together - both the visual drawing and the backend's material handling remain to be improved.
2018-12-19Use GLSL's mix function for color scalingAdrian Kummerlaender
2018-12-18Use pressure as velocity norm display amplifierAdrian Kummerlaender
2018-12-18Purify collide shaderAdrian Kummerlaender
i.e. move fluid vertex placement to appropriate vertex shader. Do not amplify or shift fluid moments in any way prior to passing it to the display pipeline.
2018-12-17Try out velocity norm color mappingAdrian Kummerlaender
2018-12-16Filter weird origin vertexAdrian Kummerlaender
The same thing occurs in computicle. I suspect some initialization / compute shader invokation problem. On the other hand: Why would that happen for the origin vertex and not e.g. the first or last vertex in memory? To be investigated further.
2018-12-16Generate fluid display using geometry shadersAdrian Kummerlaender
This should provide much more flexibility. For our purpose it would be useful if the vertex shader was executed after the geometry shader (to apply the projection matrix) but alas this is not the case. Thus the MVP matrix is applied during geometry construction and the vertex shader only provides density extraction.
2018-12-16Parametrize lattice resolutionAdrian Kummerlaender
2018-12-15Hacky D2Q9 BGK LBM on GPU using GLSL compute shadersAdrian Kummerlaender
Improvised on top of computicles's scaffolding. Works in a world where _works_ is defined as "displays stuff on screen that invokes thoughts of fluid movement".