This calculator finds the aerodynamic drag force on an object moving through a fluid, using the standard drag equation. Drag is the resistance an object feels as it pushes through air or water, and it grows rapidly with speed, which is why fuel use climbs on the motorway, why cyclists crouch low, and why fast-moving objects are shaped to be streamlined. The drag force depends on four things: the density of the fluid, the speed of the object, its drag coefficient, which captures how streamlined its shape is, and its frontal area, the size of the cross-section it presents to the flow. Crucially, drag rises with the square of the speed, so doubling your speed quadruples the drag force, and the power needed to overcome it, which is force times speed, rises with the cube. This tool computes it. You enter the fluid density, the speed, the drag coefficient and the frontal area, and the calculator returns the drag force in newtons, the dynamic pressure, the power needed to overcome the drag at that speed, and the force in kilograms-force for an everyday sense of scale. The results update as you type. Use it for physics and engineering study, for understanding vehicle and cycling aerodynamics, or for estimating air resistance. The drag force is one half of the fluid density times the speed squared times the drag coefficient times the frontal area. Air at sea level has a density of about 1.225 kilograms per cubic metre, and drag coefficients range from around 0.25 for a sleek car to about 1.0 or more for a flat plate or a cyclist sitting upright. The strong dependence on speed is why aerodynamic efficiency matters most at high speed, and why small reductions in frontal area or drag coefficient can yield meaningful savings.
Drag = half x density x speed² x drag coefficient x area. Drag rises with speed squared; the power to overcome it rises with speed cubed. Air at sea level is ~1.225 kg/m³.
The drag force is one half of the fluid density, times the speed squared, times the drag coefficient, times the frontal area. The dynamic pressure is the half-density-times-speed-squared part. The power needed to overcome the drag at a steady speed is the drag force times the speed, which is why it rises with the cube of the speed.
For a car moving at 30 metres per second with a drag coefficient of 0.3 and a frontal area of 2.2 square metres, in air of density 1.225, the drag force is one half of 1.225 times 900 times 0.3 times 2.2, about 363.83 newtons. The power to overcome it at that speed is force times speed, about 10,915 watts.
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