Regime
Set by the Brinkman number — the heat a shear makes against the heat conducted away
Every figure drawn under this hypothesis — 45 of them — with the essay each one belongs to and the generator that drew it.
45 figure placements state this regime. The strip along the foot of every figure names two things — the model that produced it and the regime it holds in — and this listing is read back out of the finished drawing rather than from what produced it.
- A lost steady state still holds the film — an exponential viscosity law; walls held at their temperature · shear-heat · hero
- A lost steady state still holds the film — an exponential viscosity law; walls held at their temperature · shear-heat
- A lost steady state still holds the film — an exponential viscosity law; walls held at their temperature · shear-heat
- A lost steady state still holds the film — an exponential viscosity law; walls held at their temperature · shear-heat
- A lost steady state still holds the film — an exponential viscosity law; walls held at their temperature · shear-heat
- A lost steady state still holds the film — an exponential viscosity law; walls held at their temperature · shear-heat
- A lost steady state still holds the film — an exponential viscosity law; walls held at their temperature · shear-heat
- A lost steady state still holds the film — an exponential viscosity law; walls held at their temperature · shear-heat
- A motor turns the runaway into a jump — an exponential viscosity law; walls held at their temperature; drive droop k against the cold film's resistance · shear-heat · hero
- A motor turns the runaway into a jump — an exponential viscosity law; walls held at their temperature; drive droop k against the cold film's resistance · shear-heat
- A motor turns the runaway into a jump — an exponential viscosity law; walls held at their temperature; drive droop k against the cold film's resistance · shear-heat
- A motor turns the runaway into a jump — an exponential viscosity law; walls held at their temperature; drive droop k against the cold film's resistance; switched on from rest · shear-heat
- A motor turns the runaway into a jump — an exponential viscosity law; walls held at their temperature; drive droop k against the cold film's resistance · shear-heat
- A motor turns the runaway into a jump — an exponential viscosity law; walls held at their temperature; drive droop k against the cold film's resistance · shear-heat
- A motor turns the runaway into a jump — an exponential viscosity law; walls held at their temperature; drive droop k against the cold film's resistance · shear-heat
- The film that heats itself — steady laminar films, constant properties — no temperature feedback yet · shear-heat · hero
- The film that heats itself — steady laminar films, constant properties — no temperature feedback yet · shear-heat
- The film that heats itself — an exponential viscosity law, steady conduction to walls at a fixed temperature · shear-heat
- A motor turns the runaway into a jump — an exponential viscosity law; walls at fixed temperature; load ramped at 0.004 per diffusion time · shear-heat
- A rotor's inertia slows the jump and cannot make it ring — exponential viscosity law, as in Nahme's film; k = 0.04; M is spin-up time over diffusion time · shear-heat · hero
- A rotor's inertia slows the jump and cannot make it ring — exponential viscosity law, as in Nahme's film; k = 0.04; M is spin-up time over diffusion time · shear-heat
- A rotor's inertia slows the jump and cannot make it ring — exponential viscosity law, as in Nahme's film; k = 0.04; M is spin-up time over diffusion time · shear-heat
- A rotor's inertia slows the jump and cannot make it ring — exponential viscosity law, as in Nahme's film; k = 0.04; M is spin-up time over diffusion time · shear-heat
- A rotor's inertia slows the jump and cannot make it ring — exponential viscosity law, as in Nahme's film; k = 0.04; M is spin-up time over diffusion time · shear-heat
- A rotor's inertia slows the jump and cannot make it ring — exponential viscosity law, as in Nahme's film; k = 0.04; M is spin-up time over diffusion time · shear-heat
- A slow sensor makes the bearing cycle — exponential viscosity law, as in Nahme's film; k = 0.04, stall group 2, derating 0.22 per unit · shear-heat · hero
- A slow sensor makes the bearing cycle — exponential viscosity law, as in Nahme's film; k = 0.04, stall group 2, derating 0.22 per unit · shear-heat
- A slow sensor makes the bearing cycle — exponential viscosity law, as in Nahme's film; k = 0.04, stall group 2, derating 0.22 per unit · shear-heat
- A slow sensor makes the bearing cycle — exponential viscosity law, as in Nahme's film; k = 0.04, stall group 2, derating 0.22 per unit · shear-heat
- A slow sensor makes the bearing cycle — exponential viscosity law, as in Nahme's film; k = 0.04, stall group 2, derating 0.22 per unit · shear-heat
- A slow sensor makes the bearing cycle — exponential viscosity law, as in Nahme's film; k = 0.04, stall group 2, derating 0.22 per unit · shear-heat
- A warm bush stops the bearing hunting — exponential viscosity law; droop 0.04, stall group 2; cusp at droop 0.0738 · shear-heat · hero
- A warm bush stops the bearing hunting — exponential viscosity law; droop 0.04, stall group 2, derating 0.22; cusp at droop 0.0738 · shear-heat
- A warm bush stops the bearing hunting — exponential viscosity law; droop 0.04, stall group 2, derating 0.22; cusp at droop 0.0738 · shear-heat
- A warm bush stops the bearing hunting — exponential viscosity law; droop 0.04, stall group 2, derating 0.22; cusp at droop 0.0738 · shear-heat
- A warm bush stops the bearing hunting — exponential viscosity law; droop 0.04, stall group 2; cusp at droop 0.0738 · shear-heat
- A warm bush stops the bearing hunting — exponential viscosity law; droop 0.04, stall group 2, derating 0.22; cusp at droop 0.0738 · shear-heat
- A warm bush stops the bearing hunting — exponential viscosity law; droop 0.04, stall group 2, derating 0.22; cusp at droop 0.0738 · shear-heat
- The film that heats itself — an exponential viscosity law — the fold is Frank–Kamenetskii's 0.8785 · shear-heat
- The film that heats itself — an exponential viscosity law — the fold is Frank–Kamenetskii's 0.8785 · shear-heat
- A rotor's inertia slows the jump and cannot make it ring — δₛ = 1; exponential viscosity law, as in Nahme's film; k = 0.04; M is spin-up time over diffusion time · shear-heat
- A rotor's inertia slows the jump and cannot make it ring — δₛ = 1; exponential viscosity law, as in Nahme's film; k = 0.04; M is spin-up time over diffusion time · shear-heat
- The film that heats itself — steady laminar Couette flow, constant properties — Br = 8 on the rise itself · shear-heat
- The film that heats itself — steady laminar Couette flow, constant properties — Br = 8 on the rise itself · shear-heat
- A warm bush stops the bearing hunting — exponential viscosity law; housing time 300 film diffusion times; film on 40 points · shear-heat