We may assume an arbitrary angle between the horizontal and the initial velocity vector.
Let the x-axis be directed from the player to the goal post. The x-coordinate after the time t will be
"x(t) = x_0 + v_0\\cos\\alpha\\cdot t = v_0\\cos\\alpha\\cdot t."
The total time of the flight of a ball will be twice the time of the movement to the maximum height (the point in which the vertical component of the velocity becomes 0, so "v_0\\sin\\alpha - gt = 0" ).
"t = 2 \\cdot \\dfrac{v_0\\sin\\alpha - 0}{g} = \\dfrac{2v_0\\sin\\alpha}{g}."
Therefore,
"x(t) = v_0\\cos\\alpha \\cdot \\dfrac{2v_0\\sin\\alpha}{g} = \\dfrac{v_0^2\\cdot\\sin2\\alpha}{g}" .
The maximum value of "\\sin2\\alpha" is 1, so the maximum distance will be "\\dfrac{v_0^2}{g} \\approx 10\\,\\mathrm{m}."
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