If v_0 is the initial velocity, then the maximum height of a flight can be calculated as
"H = \\frac{v_{0y}^2}{2g} = \\frac{v_0^2 (\\sin{\\alpha})^2}{2g}" The laws of motion of a projectile along the x- and y-directions can be written as:
"x(t) = v_0 \\cos{\\alpha} \\cdot t,\\\\\ny(t) = v_0 \\sin{\\alpha} \\cdot t - \\frac{g t^2}{2}" Substituting the A and B values (horizontal distance and height) and excluding the time, we obtain:
"t = \\frac{A}{v_0 \\cos{\\alpha}}, \\\\\nB = v_0 \\sin{\\alpha} \\cdot \\frac{A}{v_0 \\cos{\\alpha}} - \\frac{g}{2} \\left( \\frac{A}{v_0 \\cos{\\alpha}} \\right)^2 = A \\tan{\\alpha} - \\frac{g}{2} \\left( \\frac{A}{v_0 \\cos{\\alpha}} \\right)^2" Solving this equation in respect to the initial velocity squared, we derive:
"v_0^2 = \\frac{g A^2}{2 (\\cos{\\alpha})^2 (A \\tan{\\alpha} -B)}" Substituting this value into the initial expession, we conclude:
"H = \\frac{ (A \\tan{\\alpha})^2}{4 (A \\tan{\\alpha} -B)}"
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