Projectile Motion with Air Resistance

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SUMMARY

This discussion focuses on calculating projectile motion while accounting for air resistance, a complex aspect of physics. The fundamental equation of motion without drag is derived from F=ma, specifically m(d²x/dt²) = Fg. When incorporating air resistance, the equation becomes m(d²x/dt²) = Fg - D(d x/dt)², where D represents the drag coefficient influenced by the object's shape and the fluid properties. Simplifications such as Stokes' drag can be applied to make the equations more manageable.

PREREQUISITES
  • Basic calculus understanding
  • Familiarity with differential equations
  • Knowledge of forces in physics, specifically F=ma
  • Understanding of drag forces and coefficients
NEXT STEPS
  • Study the derivation of projectile motion equations with air resistance
  • Learn about Stokes' drag and its applications in fluid dynamics
  • Explore numerical methods for solving differential equations
  • Investigate the impact of different drag coefficients on projectile trajectories
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High school students studying physics, educators teaching projectile motion, and anyone interested in the effects of air resistance on motion.

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Guys, Hello,
I am a high school student who has just started basic calculus and would like to know how to find the motion of the projectile taking air resistance into account. (The range, time, etc)(I have learned about projectile motion without air resistance) Please help me.
 
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Accounting for air resistance in ballistic flight is complex. The equation of motion without drag comes from the solution of a differential equation F=ma or:
m\frac{d^2\mathbf{x}}{dt^2} = \mathbf{F}_g
It is simple in the case of projectile motions without air resistance near the Earth's surface because the force is constant. Once you throw drag in there you have the force as a typically complicated function of the velocity. There are certain simplifications one can make. In Stokes' drag one assumes the drag force is proportionate to the velocity (and of course in the opposite direction) this keeps the equation linear:
m\frac{d^2 \mathbf{x}}{dt^2} = \mathbf{F}_g - D \frac{d \mathbf{x}}{dt}^2
where D is the drag coefficient which depends on the properties of the fluid (air) and the shape and size of the object.

See: http://en.wikipedia.org/wiki/Drag_(physics)"
 
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