One layer, and the four others inside and outside it
The velocity profile over a flat plate, and the temperature profile in the same layer at four Prandtl numbers: a liquid metal at 0.01, air at 0.71, water at 7 and a heavy oil at 100. The equations differ by one number and the profiles differ by a factor of twenty in thickness. At Pr = 1 the two are the *same function* — not similar, identical, to eight decimal places — because the equations and the conditions are then the same, which is what every statement called a Reynolds analogy rests on.
7 essays call
thermal-layer. 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 thermal-layer 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 other layer, and the one number that separates them Regimes and numbers
- The wall that heats itself Compressible flow
- The skin that lags the flight Compressible flow
- The thermometer that heats itself Compressible flow
- Three readings, and the one each answer leans on Compressible flow
- The gradient the heat never hears Compressible flow
- The heat the eddies do not carry Regimes and numbers