Wind tunnels, weather patterns, blood flow, and aerodynamic design
Everything we have built up — velocity fields, the Navier-Stokes equations, boundary layers, turbulence — finds its payoff in real-world engineering and science. Computational Fluid Dynamics (CFD) numerically solves the governing equations on complex geometries, and its applications span virtually every field: aerospace engineers design low-drag aircraft, biomedical engineers model blood flow through arteries, climate scientists simulate global atmospheric circulation, and sports engineers optimize equipment from swim suits to racing cars.
The demos below give you a hands-on taste of three very different application areas. Each one is a simplified 2D model, but the core physics — pressure gradients, viscous forces, continuity, and the Coriolis effect — are the same principles that drive billion-dollar simulations on supercomputers.
A wind tunnel is the classic tool for studying aerodynamic drag and flow separation. Tracer particles flow from left to right around a central body. For a circle, the velocity field uses the exact potential-flow solution (uniform flow + doublet). For other shapes, particles are repelled from the body surface. Behind the object, a turbulent wake forms where flow speed drops and chaotic mixing occurs — this is the primary source of pressure drag. Notice how streamlined shapes (the airfoil) produce far less drag than blunt shapes (the flat plate).
On a rotating planet, air moving toward a low-pressure center is deflected to the right (in the Northern Hemisphere) by the Coriolis force. The result is cyclonic rotation: counterclockwise around a low, clockwise around a high. At low Coriolis values, the pressure gradient force dominates and air flows straight inward. At high values, the Coriolis deflection nearly balances the pressure gradient, producing circular geostrophic flow — the basis of large-scale weather prediction.
Toggle between low and high pressure to see how the spiral direction reverses, and adjust the rotation rate to observe the transition from radial inflow to geostrophic balance.
The cardiovascular system is a pressurized pipe network, and the same continuity equation that governs rivers and pipes applies to arteries. When plaque narrows a vessel (stenosis), the cross-sectional area decreases and the continuity equation A₁v₁ = A₂v₂ requires the blood to accelerate through the constriction. By Bernoulli's principle, this increase in velocity comes at the expense of pressure — creating a pressure drop across the stenosis.
Downstream of the stenosis, the sudden expansion triggers turbulence, elevated wall shear stress, and energy dissipation. In clinical terms, stenosis above 60–70% is considered hemodynamically significant and is a major risk factor for heart attack and stroke.
The fluid dynamics principles you have explored in this module form the foundation of several exciting career paths: