How Does Air Resistance Affect Projectile Motion and Free Fall?

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SUMMARY

The discussion focuses on the impact of air resistance, or drag, on projectile motion and free fall. It highlights the differential equation governing motion with air drag, represented as m(dv/dt) = F - γv², where γ is a drag coefficient dependent on fluid density, cross-sectional area, and drag coefficient (C_d). The equation indicates that as time progresses, velocity approaches a terminal value, demonstrating the significant role of air resistance in determining motion dynamics.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with differential equations
  • Knowledge of fluid dynamics concepts, particularly drag force
  • Basic grasp of projectile motion principles
NEXT STEPS
  • Study the derivation and applications of the drag equation
  • Explore terminal velocity calculations in various fluid environments
  • Investigate the effects of different shapes on drag coefficients (C_d)
  • Learn about numerical methods for solving differential equations in physics
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Students in physics, engineers working on aerodynamics, and anyone interested in the mathematical modeling of motion affected by air resistance.

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Hi, i want to know what are the real effects of air (drag) in the projectile movement and free fall, i mean how drag or air resistance is calculated in both movements, with equations.
 
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The general differential equation for motion with airdrag is (assuming "high" velocity and fluid at rest):

<br /> m\frac{d \vec v}{d t}=\vec F-\gamma v^2<br />

Where F is your "usual" forces, gravity etc and \gamma is a factor that depends on the geometry of your body (shape an cross-sectional area) and the density of the fluid:

<br /> \gamma=\frac{\rho_{fl}A C_d}{2}<br />

You can find more on this term http://en.wikipedia.org/wiki/Drag_equation"

The solution to this equation is that v\sim\tanh t which converges to a constant value as t goes to infinity i. e. there is a terminal velocity.
 
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