Projectile Motion with Air Friction: Parabola or Not?

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SUMMARY

The trajectory of a projectile with air friction does not follow a parabolic path, particularly when air resistance is modeled with a quadratic dependence on velocity. There is no closed-form solution for this scenario; numerical methods or approximations are required. In contrast, a linear dependence of air resistance allows for a closed-form solution. The equations of motion under air resistance yield exponential functions rather than quadratic ones, demonstrating the complexity introduced by air friction.

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  • Understanding of Newton's laws of motion
  • Familiarity with differential equations
  • Knowledge of numerical methods, specifically the forward Euler scheme
  • Basic logarithmic functions for solving equations
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  • Research numerical methods for solving differential equations in physics
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  • Study the effects of air resistance on projectile motion
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kishtik
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How can I find the trajectory of a projectile when not neglecting air friction? Will it still be a parabola?
 
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1. There is no closed form exact solution to this problem if you assume that the air resistance has a quadratic dependence on the velocity.
(You'll need to use either numerical methods or smart approximations)
2. You may find a closed form solution in the case of a linear dependence in velocity of the air resistance.
3. No, the curves will not be parabolas.
 
But how can I use the quadratic formula to find the trajectory?
 
What quadratic formula?
 
no you can't use quadratic formula, since the path taken by the projectile will not be parabolic.
 
Are you talking of solving for the trajectory with qudratic dependency of velocity in air resistance?
If so, use for example a forward Euler scheme with a standard iteration loop to handle the nonlinearity
 
kishtik said:
But how can I use the quadratic formula to find the trajectory?
You dont.
Without air resistance the equations are:
m \frac{d^2 x}{dt^2} = 0
and
m \frac{d^2 y}{dt^2} = -mg
these can be solved by integrating both sides twice(the intitial height and initial velocity are functions of the constants of integration). The solution for x is linear in t and the solution for y is quadratic for t.
with air resistance(proportional to the velocity) the equations are:
m \frac{d^2 x}{dt^2} = -k \frac{dx}{dt}
and
m \frac{d^2 x}{dt^2} = -k \frac{dx}{dt} - mg.
If you solve these you will find exponentials turning up in the solutions, and neither x nor y is quadratic in t. The solution is
x=A+Be^{-kt/m}

y=C+De^{-kt/m}-\frac{mg}{k}t
The initial position is (A+B,C+D). The xcomponent of the initial velocity is -kB/m. The y component of the initial velocity is -kD/m - mg/k. It is somewhat difficult to find y in terms of x, but it can be done by using logarithms as follows:
x-A = Be^{-kt/m}

\frac{x-A}{B} = e^{-kt/m}

ln(x-A)-ln(B) = -kt/m

-\frac{k}{m}(ln (x-A) - ln (B)) = t
now all that's left is to substitute this in the solution for y, to obtain
y=C+D\frac{x-A}{B} +g(ln (x-A) - ln (B))
This clearly is not a parabola.
 

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