The Hong Kong Polytechnic UniversityDepartment of Aeronautical and Aviation Engineering

ZOOM INTO THE FLOW AT THE WALL.

Boundary Layer & Flow Separation

Explore a laminar boundary layer under a favourable or adverse pressure gradient. Move the probe and inspect the calculated velocity profile.

INTERACTIVE CALCULATED DIAGRAMB · LIVE
Diagram · drag background to pan

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Preparing the calculation…

A · no saved reference

01 / READ THE CHANGE

No slip at the wall

The computed velocity rises from zero at the surface to the local external-flow velocity. Layer thickness is greatly exaggerated in the scene for readability.

02 / READ THE CHANGE

Pressure gradient changes the profile

A decelerating external flow has an adverse pressure gradient. The attached laminar similarity family approaches zero wall shear near its separation limit.

03 / READ THE CHANGE

Stop where the model stops

Below m ≈ −0.0904, this attached solution is unavailable. The page marks separation without fabricating a separated wake or a stall curve.

THE SAME MODEL, CONNECTED VIEWS

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B · solid turquoise   A · dashed amber

Compare A and B

QuantityA · savedB · liveB − AUnit

A remains fixed until saved again. Export includes the model version, settings and plotted data.

Equations, assumptions & sources

Read the balance, then connect each symbol to the model. Open a symbol key for definitions and units. Long equations can be scrolled sideways.

01 · The Falkner–Skan similarity equation

f′′′+ff′′+β(1−f′2)=0 β=2mm+1

Primes denote derivatives with respect to the similarity coordinate η.

Symbols & units
f
Dimensionless stream-function similarity function.
m,β
External-velocity power-law exponent and pressure-gradient parameter; m is not mass in this equation.

02 · No slip at the wall; match the outer flow

f⁡(0)=f′(0)=0 f′(∞)=1

The first condition represents the wall; the second matches the undisturbed outer velocity.

Symbols & units
f′(∞)
Analytical far-field boundary condition. The numerical integration uses a finite similarity domain.

03 · Reconstruct the velocity profile

uUe=f′ η=y(m+1)Ue2νx

The same similarity solution produces the local velocity profile shown above.

Symbols & units
u,Ue
Local streamwise velocity and outer-flow velocity, m/s.
x,y,ν
Along-wall and normal coordinates, m; kinematic viscosity, m²/s. η is dimensionless.

Steady two-dimensional incompressible laminar Falkner–Skan similarity flow with power-law external speed. Numerical shooting to η = 8, step 0.02. Surface display starts at x/L = 0.05 to avoid the leading-edge singularity. No turbulent closure, transition prediction, reattachment or post-stall flow. Reynolds numbers above 500000 are flagged as requiring transition consideration, not asserted to be turbulent.

NASA · boundary layer ↗

Physical relations and teaching sources support the stated concepts. Generic coefficients are explicitly illustrative; they are not measured manufacturer data. Numerical verification is separate from experimental validation. Model version: applied-labs-v1.1.

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