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Parachute
Parachute
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A parachute is an aerodynamic deceleration device used for the controlled descent, deceleration, or stabilization of a freely falling body through the atmosphere by generating drag. It typically consists of a lightweight, flexible canopy made from durable fabrics such as or , which inflates upon deployment to create a large surface area that increases air resistance. Suspension lines connect the canopy to a harness or that secures the load, whether a , , or , allowing for a safe of around 15-20 miles per hour during landing. The concept of the parachute originated in the late 15th century, when Italian polymath sketched a pyramidal design in his , describing it as a linen-covered wooden frame capable of carrying a person safely from a height. The first practical demonstration occurred in 1783, when French physicist Louis-Sébastien Lenormand jumped from a tree using a device made of two umbrellas, coining the term "parachute" from the French words for "against" and "fall." achieved the first high-altitude descent in 1797, jumping from a hydrogen balloon at 3,200 feet over with a canopy framed by a parasol-like structure, marking the birth of modern parachuting. By 1912, the first parachute jump was performed by U.S. Army Captain Albert Berry from a height of 1,500 feet, paving the way for integration. Parachutes serve diverse applications across military, aerospace, and recreational domains. In military operations, they enable airborne troop insertions, as seen in World War II paratrooper drops, and facilitate supply airdrops for logistics in remote or combat zones using systems like the G-11 cargo parachute for loads up to 5,000 pounds. NASA's missions, such as the Apollo and Orion programs, rely on multi-stage parachute assemblies—including drogue and main canopies up to 116 feet in diameter—to decelerate spacecraft during atmospheric reentry and splashdown. In sports like skydiving, governed by organizations such as the Parachute Association, ram-air parachutes allow precise control and maneuvers, with approximately 3.88 million jumps annually in the U.S. demonstrating a fatality rate of 0.23 per 100,000 jumps as of 2024.

Principles of Operation

Physics of Parachute Descent

The physics of parachute descent is governed primarily by the balance between and aerodynamic drag, which slows the fall to a safe speed. When a parachutist is in freefall, accelerates the body until air resistance balances the weight, reaching . Upon deployment, the parachute increases drag dramatically, reducing this velocity and enabling controlled descent. The primary mechanism is drag force, quantified by the equation Fd=12ρv2CdAF_d = \frac{1}{2} \rho v^2 C_d A, where ρ\rho is air density, vv is the object's velocity relative to the air, CdC_d is the drag coefficient (dependent on shape and porosity), and AA is the projected area of the parachute canopy. This force opposes motion through the air, and at terminal velocity, it equals the gravitational force mgmg, where mm is mass and gg is gravitational acceleration (approximately 9.8 m/s²). Solving for terminal velocity gives vt=2mgρCdAv_t = \sqrt{\frac{2mg}{\rho C_d A}}
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