Answer:
y = [tg α] *x - [1/2 g/ (v0 ²cos²(α))]* x² , which describes a parabolic path
Explanation:
since
x = (v0 cos(α))t
where x represents horizontal distance covered by the projectile
and
y = (v0 sin(α))t −(1/2) gt^2
where y represents vertical distance, we can replace the parameter t in order to have a function of coordinates, then
x = (v0 cos(α))t → x /(v0 cos(α))= t
replacing t in the equation of y
y = (v0 sin(α))t −(1/2) gt^2 = (v0 sin(α))x/(v0 cos(α)) −(1/2) g[x/(v0 cos(α))]² =
[sin(α) /cos(α)]* x - 1/2 g x²/(v0 cos(α))² = [tg α] *x - [1/2 g/ (v0 ²cos²(α))]* x²
therefore
y = [tg α] *x - [1/2 g/ (v0 ²cos²(α))]* x²
since tg α= constant=C1 , [-1/2 g/ (v0 ²cos²(α))]= constant=C2 , then
y = C1*x + C2* x²
which describes a parabolic path