Three equations, and the set they never leave
The Lorenz trajectory at r = 28, projected on x and z, after the transient has been discarded. It never repeats, never leaves, and never crosses itself in three dimensions. The Lyapunov exponent printed beside it is measured on this system by separating a nearby pair, so the claim of sensitive dependence is a computation.
5 essays call
lorenz-truncation. The drawing above is what it returns with no arguments at all; every
call below passes it something, because a placement that passes nothing draws whichever member
of the family the generator happens to default to rather than the one its essay argues about.
It is also the blast radius. Changing lorenz-truncation changes every figure listed here
at once, and on this site it may change what they assert as well as what they show —
which is what has to be rebuilt and looked at before the change is believed.
Where it is called
What each of these essays asks for instead of the defaults is on the regime index, which reads the parameters back out of the finished figures rather than out of the placements.
- A threshold with a closed form Transition and turbulence
- Three numbers left of a fluid Transition and turbulence
- A millionth is enough Transition and turbulence
- The randomness that is not in the equations What is taught wrongly
- The truncation that cannot carry three times the heat Transition and turbulence