t 0 sWall -Visibility -Gust - m/s
Visibility below 200 m: real-world advice is to pull off the road, switch lights off and wait it out.
Drag to orbit, wheel or pinch to zoom. Brown parcels are dust carried by the cold outflow; each one stands for a share of the dust mass, so density equals concentration. Sky and fog dim with the visibility computed at the town.

Haboob Dust Wall

A cold downdraft spreads as a gravity current across a 3 km desert domain towards a small town.

Run

Presets

Storm

Live readings

Visibility at the town

Dust concentration vs height at the town

Why sand moves before dust

Experiments

Run an experiment to compare the model with theory.

Independent checks (live)

The science

The wall. Rain-cooled air sinks and spreads along the ground as a density current. Its front moves at Uf = Fr √(g' h) with reduced gravity g' = g ΔT / T and Froude number Fr ≈ 1.07 (Benjamin 1968; Simpson 1999). A deficit of 8 K and 1.5 km depth gives about 21 m/s. The head lifts air at the nose, which is why the wall rolls upward.

Lifting sand. Wind stress is the friction velocity u* = κ U10 / ln(10/z0). Grains move when u* exceeds the threshold u*t = √[A(γ/(ρad) + ρp g d/ρa)] (Shao and Lu 2000; A = 0.0123, γ = 1.65e-4 N/m). The cohesion term makes 10 µm dust far harder to lift than 100 µm sand: dust is mostly released by the impacts of saltating sand. Saltation flux (Kawamura): Q = C (ρa/g)(u* - u*t)(u* + u*t)2, C ≈ 2.78, so Q grows roughly as u*³.

Dust. Emission is F = α Q with an efficiency α that is an illustrative, tunable number (real values depend on soil crust and clay content and span orders of magnitude). Parcels random-walk vertically with K = κ u* z (1 - z/H), settle at the Stokes speed ws = (ρp - ρa) g d² / (18 μ) corrected for finite Reynolds number, and are lifted in the head. In steady turbulence the profile follows the Rouse law, C ∝ ((H - z)/z)Ro with Ro = ws/(κ u*).

Visibility. Extinction β = 3 Qext C / (2 ρp d) with Qext ≈ 2 and Koschmieder's law V = 3.912/β (2 % contrast threshold).

Simplifications, stated honestly. Two-dimensional wind field prescribed from the current depth (no solved Navier-Stokes), one grain size for transport and one for suspension, no coagulation or electrostatics, no moist processes, no recycling of the cold pool, uniform soil, and the dust parcels are a Monte-Carlo sample (about 7000, so the concentration at the town has sampling noise of a few percent). Constants such as C, A, γ, Fr and α are typical literature values and should be treated as order-of-magnitude. Real haboobs also carry lobes and clefts and last hours.

Educational model. Terrain, buildings and palms were modelled in Blender and baked to textures; the dust is simulated live.

Made with 🟠 Blender · Three.js