a) The maximum height the projectile will reach after it's launched from the height "h":
"H=h+\\frac{(v_0\\text{ sin}\\theta)^2}{2g}=\\frac{2gh+(v_0\\text{ sin}\\theta)^2}{2g}."
And this will take time
"t_1=\\frac{v_0\\text{ sin}\\theta}{g}."
Then it will fall back to the ground during
"t_2=\\sqrt{\\frac{2H}{g}}=\\frac{\\sqrt{2gh+(v_0\\text{ sin}\\theta)^2}}{g}." Meanwhile the projectile will move forward with constant velocity
"v_x=v_0\\text{ cos} \\theta," and of course it will cover the range
"R=v_x(t_1+t_2)=\\\\=\\frac{v_0\\text{ cos} \\theta}{g}(v_0\\text{ sin}\\theta+\\sqrt{2gh+(v_0\\text{ sin}\\theta)^2})." b) Substitute "h=0" and get simple relation for the horizontal range:
"R(0)=\\frac{v_0^2\\text{ sin} (2\\theta)}{g}." c) That is the answer to this problem.
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