Creeping flow, and the same body with inertia
The exact creeping-flow solution beside a solved field at a Reynolds number where inertia matters. The creeping flow is a mirror image of itself front to back — a photograph of it run backwards is a photograph of it — and the field with inertia has a wake, which is what a direction of time looks like.
5 essays call
creeping-flow. 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 creeping-flow 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.
- The world with no inertia Regimes and numbers
- Whether the droplet turns Regimes and numbers
- How small is small enough Regimes and numbers
- A force without the flow that makes it Viscosity
- A swimmer that cannot go backwards Viscosity