Regime
Boundary-layer theory — Re large enough that the layer is thin, and the number cancels
Every figure drawn under this hypothesis — 69 of them — with the essay each one belongs to and the generator that drew it.
69 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 finite force from an infinite speed — external flow going as a power of distance · bl-profile
- A guess with a constant in it — flat plate, no pressure gradient · bl-profile
- A layer that is an integral of everything upstream — the two distributions above, up to the station · how-long-viscosity-remembers
- A layer with a kink in it — the last profile has zero slope at the wall · bl-profile
- A limit nothing reaches — a stated closure for the first, the exact similarity solution for the second · overlap-layer
- Ask for the pressure, and see what shape that is — external flow going as a power of distance · bl-profile
- Drag in the theory that forbids it — external flow going as a power of distance · bl-profile
- Every mode decays and it grows anyway — U = 30 m/s in air — transition placed at Re_x = 3e+6, observed · plate-friction
- Faster than the wind that drives it — chord Reynolds number 10⁶, laminar · drag-split
- How many things a flow must be told — flat plate, no pressure gradient · bl-profile
- How much uphill a layer can take — external flow going as a power of distance · bl-profile · hero
- How much uphill a layer can take — the last profile has zero slope at the wall · bl-profile
- How much uphill a layer can take — external flow going as a power of distance · bl-profile
- How much uphill a layer can take — flat plate, no pressure gradient · bl-profile
- How thick is thin — flat plate, no pressure gradient · bl-profile · hero
- How thick is thin — flat plate, no pressure gradient · bl-profile
- How thick is thin — the last profile has zero slope at the wall · bl-profile
- How thick is thin — flat plate, no pressure gradient · bl-profile
- How thick is thin — laminar, zero pressure gradient, ν = 10⁻⁵ m²/s at U = 1 m/s · bl-profile
- The air a wing does not carry — flat plate, no pressure gradient · bl-profile
- The air a wing does not carry — laminar, zero pressure gradient, ν = 10⁻⁵ m²/s at U = 1 m/s · bl-profile
- The air a wing does not carry — Re_x = 2.0e+6 — laminar, zero pressure gradient · bl-profile
- The air a wing does not carry — laminar similarity solutions — β from 1 to separation at −0.1988 · bl-profile
- The air a wing does not carry — flat plate, no pressure gradient · bl-profile
- The body the outer flow actually sees — laminar, zero pressure gradient, ν = 10⁻⁵ m²/s at U = 1 m/s · bl-profile · hero
- The body the outer flow actually sees — laminar, zero pressure gradient, ν = 10⁻⁵ m²/s at U = 1 m/s · bl-profile
- The body the outer flow actually sees — flat plate, no pressure gradient · bl-profile
- The body the outer flow actually sees — external flow going as a power of distance · bl-profile
- The body the outer flow actually sees — flat plate, no pressure gradient · bl-profile
- The cheapest way to stay up — flat plate, one side, no pressure gradient · drag-split
- The cheapest way to stay up — chord Reynolds number 10⁶, laminar · drag-split
- The cheapest way to stay up — chord Reynolds number 10⁶, laminar · drag-split
- The cost of going turbulent — U = 30 m/s in air — transition placed at Re_x = 5e+5, observed · plate-friction
- The layer that stops growing — U = 30 m/s in air — transition placed at Re_x = 5e+5, observed · plate-friction
- The number that is an answer — a laminar flat-plate boundary layer — Pr from 10⁻⁵ to 10³ · regime-collapse · hero
- The number that is an answer — a laminar flat-plate boundary layer — Blasius, Pr from 0.01 to 100 · regime-collapse
- The number that is an answer — a laminar flat-plate boundary layer — Pr from 10⁻⁵ to 10³ · regime-collapse
- The number that is an answer — a laminar flat-plate boundary layer — the exponent, not the coefficient · regime-collapse
- The number that is an answer — a laminar flat-plate boundary layer — Pr from 10⁻⁵ to 10³ · regime-collapse
- The number that is an answer — a laminar flat-plate boundary layer — the exponent, not the coefficient · regime-collapse
- The number that is an answer — a laminar flat-plate boundary layer, Pr from 10⁻⁵ to 10³ · regime-collapse
- The number that is not a number — U = 30 m/s in air — transition placed at Re_x = 5e+5, observed · plate-friction
- The number that is not a number — U = 30 m/s in air — transition placed at Re_x = 1e+5, observed · plate-friction
- The number that is not a number — U = 30 m/s in air — transition placed at Re_x = 3e+6, observed · plate-friction
- The skin that lags the flight — turbulent, Pr = 0.71 — the friction is a one-seventh-power correlation at Re_x = 10⁷ · thermal-layer · hero
- The skin that lags the flight — turbulent, Pr = 0.71 — the friction is a one-seventh-power correlation at Re_x = 10⁷ · thermal-layer
- The skin that lags the flight — turbulent, Pr = 0.71 — the friction is a one-seventh-power correlation at Re_x = 10⁷ · thermal-layer
- The skin that lags the flight — turbulent, Pr = 0.71 — the friction is a one-seventh-power correlation at Re_x = 10⁷ · thermal-layer
- The skin that lags the flight — turbulent, Pr = 0.71 — the recovery factor is 0.84 and the friction a correlation · thermal-layer
- The skin that lags the flight — turbulent, Pr = 0.71 — the recovery factor is 0.84 and the friction a correlation · thermal-layer
- The skin that lags the flight — turbulent, Pr = 0.71 — the friction is a one-seventh-power correlation at Re_x = 10⁷ · thermal-layer
- The solution that keeps its nonlinear term — water, nu = 10⁻⁶ m²/s; a disc at 100 rad/s, radius 0.2 m · oscillating-wall
- The solutions stop being chosen — U = 30 m/s in air — transition placed at Re_x = 5e+5, observed · plate-friction
- The third thickness — Re_x = 2.0e+6 — laminar, zero pressure gradient · bl-profile · hero
- The third thickness — Re_x = 2.0e+6 — laminar, zero pressure gradient · bl-profile
- The third thickness — laminar similarity solutions — β from 1 to separation at −0.1988 · bl-profile
- The third thickness — laminar, zero pressure gradient, ν = 10⁻⁵ m²/s at U = 1 m/s · bl-profile
- The third thickness — flat plate, no pressure gradient · bl-profile
- The two drags a wing pays — flat plate, one side, no pressure gradient · drag-split
- The two drags a wing pays — chord Reynolds number 10⁶, laminar · drag-split
- The wall that shakes — flat plate, no pressure gradient · bl-profile
- The wall that shakes — flat plate, no pressure gradient · bl-profile
- The wind a swept wing feels — laminar boundary layer — incompressible, on an infinite wing yawed at 35° · swept-wing · hero
- The wind a swept wing feels — laminar boundary layer — incompressible, on an infinite wing yawed at 35° · swept-wing
- The wind a swept wing feels — laminar boundary layer — incompressible, on an infinite wing yawed at 35° · swept-wing
- The wind a swept wing feels — laminar boundary layer — incompressible, on an infinite wing yawed at 45° · swept-wing
- Where the heat of a drag is made — Re_x = 2.0e+6 — laminar, zero pressure gradient · bl-profile
- Where the straight line stops — external flow going as a power of distance · bl-profile
- Where vorticity comes from — flat plate, no pressure gradient · bl-profile