Consider the Sprott attractor given by KNXVQUEXYETWOOSGNSBDMHTMCFLNGP

Imagine very many tiny particles, each of them shaped like this attractor. (which is not technically hard to do, just add a prefactor and a postfactor and the attractor can be scaled to any size). One way of thinking about the attractor is a probability distribution in . Suppose that so long as the sum of the probability distributions is less than, I don’t know, to pick a real number at random, say , where is the Euler-Mascheroni constant. These particles will interact in a very odd way compared to a fluid composed of atoms. Which means that you could have many of these particles (let’s assume that we scale it down ). in the same space at once so long as the sum of the probability distributions at a some given point was less than .

We could try a range of sizes, perhaps. What I want to impress on you is how very oddly the fluid particles interact with each other, for they don’t encounter resistance until the sum of the probability distributions of each is , though it would make sense that their rate of movement at a point would depend on the ‘evanesences’ — less evanescent intersecting materials would move through each other more fluidly.