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Boundary layers

How Boundary Layer Thickness Develops Along an Airfoil Surface

HENDOI · 27 October 2026

The boundary layer starts thin at the stagnation point and grows as it travels. A pressure rise makes it grow faster. Thickness, displacement thickness and momentum thickness are three different measures.

Three thicknesses, not one

Air at the wall is at rest relative to the wall. A short distance out, it has rejoined the inviscid speed. That distance is a boundary-layer thickness. Engineers keep three versions, because they answer three questions:

MeasureWhat it asks
δ, the 99% thicknessWhere the speed has essentially recovered. Useful for “how thick is the layer,” and for whether a roughness grain sticks out of it.
δ*, displacement thicknessHow far the outside flow is pushed by the slow fluid. This is the thickness a panel method feels.
θ, momentum thicknessHow much momentum the wall has removed. Skin-friction drag accumulates in θ. The shape factor H = δ*/θ says whether the profile is full and healthy or hollow and near separation.

On a flat plate with no pressure gradient, a laminar layer grows roughly as the square root of the distance from the start, and a turbulent layer grows faster in the streamwise sense but stays fuller. An airfoil is not that plate. The growth rate is set by the pressure field the shape imposed.

What the airfoil does to the growth

Near the stagnation point the layer is thinnest. Around the nose the flow accelerates, the pressure falls, and the layer is held thin and stable. After the suction peak the flow slows, the pressure rises, and the layer thickens quickly. That is why a short, steep recovery separates and a longer recovery may not: the same fluid has to climb the pressure rise, and a tired profile climbs worse. Transition resets the profile. A turbulent layer is fuller, so H drops, even though δ itself usually jumps up because the turbulent layer entrains outer fluid.

A laminar zero-pressure-gradient shape factor is about 2.6. A turbulent layer in mild conditions sits nearer 1.3 to 1.5. When H climbs again under an adverse gradient, separation is close. Integral methods such as Thwaites for a laminar layer, and a turbulent closure after transition, march θ and H along the surface using the edge speed from the outer flow. That march is the boundary-layer half of a VIC or XFOIL-class polar.

What to look at in a result

  • δ* at the trailing edge is the wake’s starting thickness. A large trailing-edge δ* is a drag story and a stall warning.
  • A flat δ* through a strong recovery is suspicious. The layer should be responding to the pressure rise.
  • Compare upper and lower surfaces. At positive angle the upper surface does almost all of the thickening.
  • Do not quote a single “boundary-layer thickness of the airfoil.” Quote the station, the surface, and which of δ, δ* or θ you mean.

The separation lesson explains what happens when the growth runs away. This page is only the growth itself.


Where this sits in the series

In simple words: what this page is for

The boundary layer starts thin at the stagnation point and grows as it travels. A pressure rise makes it grow faster. Thickness, displacement thickness and momentum thickness are three different measures.

This lesson exists because section decisions fail when geometry, method labels and selection reasons are scattered. How Boundary Layer Thickness Develops Along an Airfoil Surface helps you keep a clean trail from shape to polar to choice.

Why the topic matters

Engineers lose time when a title sounds clear but the page only sketches the idea. This article expands How Boundary Layer Thickness Develops Along an Airfoil Surface so you can answer three questions without jargon: what is the idea, when do you use it, and how do you check it in a HENDOI product.

Read the sections above for the core definitions. Use the steps below to move from reading into a real project trail you can share with a teammate.

How to apply this in HENDOI

In practice: create a HENDOI account or log in, open HENFOIL, bring a section in (create, import DAT, or digitize), pass the geometry gate, climb the analysis ladder only as far as the decision needs, then compare and archive. Every calculated number should keep its method label.

When the section choice is ready for the aircraft, continue in HENSYNTH for mission, compliance and trades. Same account. Same plans.

What this page will not claim: a teaching polar or geometry note is not a flight-Re certificate. HENFOIL labels methods so you know what you bought. Tunnel data and professional judgement still sit outside any single software run.

Checklist before you leave this page

  • Can you state the idea of How Boundary Layer Thickness Develops Along an Airfoil Surface in one sentence?
  • Do you know which product owns the next action — HENFOIL or HENSYNTH?
  • Will every number you keep carry a method label or a stored-run source?
  • If you are new here, have you opened Register or Login?

These pages teach the ideas. They are not wind-tunnel data and not a certification analysis. When a number matters, compute it at a stated Reynolds number, Mach number and transition setting, and keep the method label on the result. In HENFOIL that production polar is a VIC polar — see the analysis ladder and the polar field guide.

Both products live

Use this lesson in the HENDOI workspace

This page sits in Boundary layers. HENFOIL and HENSYNTH are both live on one account. These articles are screening lessons — not certification reports.

Live · section

HENFOIL

Turn this lesson into a section you can draw, check, analyse and compare. Run the polar at the Reynolds number of the vehicle. The method name stays on the result.

To Know More

Live · aircraft

HENSYNTH

After the section is chosen, set geometry and mission requirements, run screening, read compliance, synthesize candidates and download or mail the report.

To Know More

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Written by

Sundarapandi Muthupandi, Founder and CEO of HENDOI

This post by

Sundarapandi Muthupandi

Founder & CEO · HENDOI

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