Regime
Set by the squeeze number — whether the gas in the film has time to leave it
Every figure drawn under this hypothesis — 27 of them — with the essay each one belongs to and the generator that drew it.
27 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 damper that turns into a spring — a trapped isothermal film — σ large enough that no gas leaves in a cycle · bearing-film
- The heat of a squeeze leaves across the gap — air in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ as stated · bearing-film · hero
- The heat of a squeeze leaves across the gap — air in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ as stated · bearing-film
- The heat of a squeeze leaves across the gap — air in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ as stated · bearing-film
- The heat of a squeeze leaves across the gap — air in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ as stated · bearing-film
- The heat of a squeeze leaves across the gap — air in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ as stated · bearing-film
- The heat of a squeeze leaves across the gap — air in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ as stated · bearing-film
- The heat of a squeeze leaves across the gap — air in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ as stated · bearing-film
- The gas sets a squeeze film's loss, not its stiffness — gas in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ swept from 0.1 to 100 atm · bearing-film · hero
- The gas sets a squeeze film's loss, not its stiffness — gas in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ swept from 0.1 to 100 atm · bearing-film
- The gas sets a squeeze film's loss, not its stiffness — gas in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ swept from 0.1 to 100 atm · bearing-film
- The gas sets a squeeze film's loss, not its stiffness — gas in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ swept from 0.1 to 100 atm · bearing-film
- The gas sets a squeeze film's loss, not its stiffness — gas in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ swept from 0.1 to 100 atm · bearing-film
- The gas sets a squeeze film's loss, not its stiffness — gas in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ swept from 0.1 to 100 atm · bearing-film
- The gas sets a squeeze film's loss, not its stiffness — gas in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ swept from 0.1 to 100 atm · bearing-film
- The gas sets a squeeze film's loss, not its stiffness — gas in a thin gap, walls at a fixed temperature; squeeze number and ωh²/κ swept from 0.1 to 100 atm · bearing-film
- A damper that turns into a spring — air at 20 °C, µ = 18.1 µPa·s, isothermal — the film is thin and inertia is absent · bearing-film
- A damper that turns into a spring — air at 20 °C, µ = 18.1 µPa·s, isothermal — the film is thin and inertia is absent · bearing-film
- A damper that turns into a spring — air at 20 °C, µ = 18.1 µPa·s, isothermal — the film is thin and inertia is absent · bearing-film
- A damper that turns into a spring — a trapped isothermal film at 20 kHz — no gas leaves in a cycle · bearing-film
- A levitator lifts by its amplitude, not its gas — gas trapped in a 20 µm gap at 20 kHz, squeeze number 18 to 85 across 1 and 3 atm · bearing-film
- A levitator lifts by its amplitude, not its gas — gas in a thin gap, walls at a fixed temperature; squeeze number 55 to 85, so the gas is trapped · bearing-film · hero
- A levitator lifts by its amplitude, not its gas — gas in a thin gap, walls at a fixed temperature; squeeze number 55 to 85, so the gas is trapped · bearing-film
- A levitator lifts by its amplitude, not its gas — gas in a thin gap, walls at a fixed temperature; squeeze number 55 to 85, so the gas is trapped · bearing-film
- A levitator lifts by its amplitude, not its gas — gas in a thin gap, walls at a fixed temperature; squeeze number 55 to 85; ωh²/κ as dialled · bearing-film
- A levitator lifts by its amplitude, not its gas — gas in a thin gap, walls at a fixed temperature; squeeze number 55 to 85, so the gas is trapped · bearing-film
- A levitator lifts by its amplitude, not its gas — gas in a thin gap, walls at a fixed temperature; squeeze number 55 to 85, so the gas is trapped · bearing-film