Parabolic Path of a Projectile

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The path of a projectile is proven to be parabolic through the equations of motion in both vertical and horizontal directions. In the vertical direction, the equation y(t) = y(0) + v_y(0)t - (1/2)gt^2 describes a parabolic trajectory over time. In the horizontal direction, x(t) = x(0) + v_x(0)t shows constant motion without force, allowing for the substitution of time to express y in terms of x, confirming the parabolic shape. This parabolic path is valid under the assumptions of a flat Earth and constant gravitational field, with no aerodynamic drag. For a spherical Earth and no drag, the trajectory would instead resemble part of an ellipse.
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How do we know, or how can we prove that the path of a projectile is (at least part of) a parabola?
 
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Easily:

In the vertical direction
<br /> F = ma = m\frac{d^2 y}{dt^2} = -mg<br />

Integrated twice we obtain
<br /> y(t) = y(0) + v_y(0)t - \frac{1}{2}gt^2<br />

Which is indeed the equation of a parabola with respect to time.

Now in the x-direction, we have
<br /> x(t) = x(0) + v_x(0)t<br />
since there is no force in this direction. It should be clear that if we re-write y(t) in terms of x(t), by solving for t in the above equation, y(t) will also be a parabola in terms of x.
 
DJ24 said:
How do we know, or how can we prove that the path of a projectile is (at least part of) a parabola?
A parabola occurs under the simplified case of a flat Earth and a constant gravitational field and no aerodynamic drag. For a spherical earth, with no drag, and the equivalent of a point source for gravity, the path is part of an ellipse.
 

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