# Diffusion-Limited Aggregation

Diffusion-limited aggregation creates branched and coral like structures by the process of randomly moving particles that touch and stick to existing stationary particles.

All of the images and movies in this post were created with Visions of Chaos.

Real Life Experiments

If you put an electrodeposition cell into a copper sulfate solution you can get results like the following images.

2D Diffusion-limited Aggregation

DLA is a simple process to simulate in the computer and was one of my first simulations that I ever coded. For the simplest example we can consider a 2D scenario that follows the following rules;

1. Take a grid of pixels and clear all pixels to white.
2. Make the center pixel black.
3. Pick a random edge point on any of the 4 edges.
4. Create a particle at that edge point.
5. Move the particle randomly 1 pixel in any of the 8 directions (N,S,E,W,NE,NW,SE,SW). This is the “diffusion”.
6. If the particle goes off the screen kill it and go to step 4 to create a new particle.
7. If the particle moves next to the center pixel it gets stuck to it and stays there. This is the “aggregation”. A new particle is then started.
Repeat this process as long as necessary (usually until the DLA structure grows enough to touch the edge of the screen).

When I asked some of my “non-nerd” aquaintances what pattern would result from this they all said a random blob like pattern. In reality though the pattern produced is far from a blob and more of a coral like branched dendritic structure. When you think about it for a minute it does make perfect sense. Because the moving particles are all coming from outside the fixed structure they have less of a chance of randomly walking between branches and getting to the inner parts of the DLA structure.

All of the following sample images can be clicked to see them at full 4K resolution.

Here is an image created by using the steps listed above. Starting from a single centered black pixel, random moving pixels are launched from the edge of the screen and randomly move around until they either stick to the existing structure or move off the screen.

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: when they move next to a single stuck particle

The change in this next example is that neighbouring pixels are only checked in the N, S, E and W directions. This leads to horizonal and vertical shaped branching.

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W
Particles stick condition: when they move next to a single stuck particle

There are many alternate ways to tweak the rules when the DLA simulation is running.

Paul Bourke’s DLA page introduces a “stickiness” probability. For this you select a probability of a particle sticking to the existing DLA structure when it touches it.

Decreasing probability of a particle sticking leads to more clumpy or hairy structures.

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: 0.5 chance of sticking when they move next to a single stuck particle

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: 0.1 chance of sticking when they move next to a single stuck particle

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: 0.01 chance of sticking when they move next to a single stuck particle

Another method is to have a set count of hits before a particle sticks. This gives similar results to using a probability.

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has hit stuck particles 15 times

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has hit stuck particles 30 times

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has hit stuck particles 100 times

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has hit stuck particles 1000 times

Another change to experiment with is having a threshold neighbour count random particles have to have before sticking. For example in this next image all 8 neighbours were checked and only 1 hit was required to stick, but the moving particles needed to have at least 2 fixed neighbour particles before they stuck to the existing structure.

The first 50 hits only need 1 neighbour. This build a small starting structure which all the following hits stick to with 2 or more neighbours.

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has 2 or more stuck neighbours

That gives a more clumpy effect without the extra “hairyness” of just adding more hit counts before sticking.

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has 3 or more stuck neighbours

This seems a happy balance to get thick branches yet not too fuzzy ones.

Start configuration: Single centered black pixel
Random pixels launched from: rectangle surrounding existing structure
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has 3 or more stuck neighbours and has hit 3 times

The next two examples launch particles from the middle of the screen with the screen edges set as stationary particles.

Start configuration: Edges of screen set to black pixels
Random pixels launched from: middle of the screen
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has 1 or more stuck neighbours

Start configuration: Edges of screen set to black pixels
Random pixels launched from: middle of the screen
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has 3 or more stuck neighbours

These next three use a circle as the target area. Particles are launched from the center of the screen.

Start configuration: Circle of black pixels
Random pixels launched from: middle of the screen
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has 1 or more stuck neighbours

Start configuration: Circle of black pixels
Random pixels launched from: middle of the screen
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has 2 or more stuck neighbours

Start configuration: Circle of black pixels
Random pixels launched from: middle of the screen
Neighbours checked for an existing pixel: N, S, E, W, NE, NW, SE, SW
Particles stick condition: once a moving particle has 3 or more stuck neighbours

This next image is a vertical 2D DLA. Particles drop from the top of the screen and attach to existing seed particles along the bottom of the screen. Color of sticking particles uses the color of the particle they stick to.

Start configuration: Bottom of screen is fixed particles
Random pixels launched from: top of the screen
Neighbours checked for an existing pixel: S, SE, SW
Particles stick condition: once a moving particle has 1 or more stuck neighbours

Dendron Diffusion-limited Aggregation

Another DLA method is Golan Levin’s Dendron DLA. He kindly provided java source code so I could experiment with Dendron myself. Here are a few sample images.

Hopefully all of the above examples shows the wide variety of 2D DLA possible and the various methods that can produce them. This post was mainly going to be about 3D DLA, but I got carried away trying all the 2D possibilities above.

3D Diffusion-limited Aggregation

DLA can be extended into 3 dimensions. Launch the random particles from a sphere rather than a surroundiong circle. Check for a hit against the 27 possible neighbours for each 3D grid cell.

For these movies I used default software based OpenGL spheres. Nothing fancy. Slow, but still managable with some overnight renders.

In this first sample movie particles stuck once they had 6 neighbours. In the end their are approximately 4 million total spheres making up the DLA structure.

This second example needed 25 hits before a particle stuck and a particle needed 5 neighbours to be considered stuck. This results in a much more dense coral like structure.

A Quick Note About Ambient Occlusion

Ambient occlusion is when areas inside nooks and crannies are shaded darker because light would have more trouble reaching them. Normally to get accurate ambient occlusion you raytrace a hemisphere of rays from the surface point seeing how many objects the rays intersect. The more hits, the darker the shading. This is a slow process. For the previous 3D DLA movies I cheated and used a method of counting how many neighbour particles the current sphere has. The more neighbours the darker the sphere was shaded. This gives a good enough fake AO.

Programming Tip

A speedup some people do not realise is when launching random particles. Use a circle or rectangle just slightly larger than the current DLA structure. No need to start random points far from the structure.

For many years now the ultimate inspiration in DLA for me has been Andy Lomas.

http://www.andylomas.com/aggregationImages.html

His images like this next one are very nice.

Another change Andy uses is to launch the random walker particles in patterns that influence the structure shape as in this next image.

Future Changes

1. More particles. The above 2 movies have between 4 and 5 million particle spheres at the end of the movies. Even more particles would give more natural looking structures like the Andy Lomas examples.

2. Better rendering. Using software (non-GPU) OpenGL works but it is slow. Getting a real ray traced result supporting real ambient occlusion and global illumination would be more impressive.

3. Controlled launching of particles to create different structure shapes other than a growing sphere.

Jason.

# Visions of Chaos is now compatible with High DPI displays

High DPI

Mobile phones and tablets have had nice high DPI displays for a long time now. PC screens have started to catch up and 4K monitors are starting to come down in price and will become the standard in the future.

The good thing about higher DPI screens is that there are many more pixels on the same sized screen so text and images are shown much more clearly.

The bad thing is most applications (especially older programs) are not aware of High DPI scaling settings. If an application does not support scaling Windows just “zooms” the application window to a larger size. This leads to blurry text that most people complain about. So you either set the scaling factor to 100% which leads to tiny text or you live with blurry text.

Over the past few weeks I have been working on making Visions of Chaos high DPI aware. The end result is that it will now run happily on all scale settings and higher 4K monitors without the text being too tiny to read or blown up and blurry. The menus and all text within Visions of Chaos will scale according to your Windows settings and remain smooth and crisp to read.

High DPI in Visions of Chaos

Prior to Visions of Chaos being DPI aware Windows would just scale the output window like in a photo editor app. The following shows how the Visions of Chaos window looks at 150% scaling under Windows 10 on a 4K display.

This leads to the blurred text and the generated image (set to 480×360 pixels in size) is shown onscreen also stretched and blurred to 725 pixels wide.

Here is the same window using the latest version of Visions of Chaos that is DPI aware. The text fonts are scaled to a larger size so they remain crisp and smooth. The fractal image that has been set to 480×360 pixels is exactly 480×360 monitor pixels.

Windows is still playing catch up with higher resolution DPI support, but it will hopefully get better as 4K monitors become the standard. At least you can be confident that Visions of Chaos will continue to be usable and readable at high DPI settings.

Now I can get back to adding new features to Visions of Chaos.

Jason.