We will solve the problem neglecting the measures of the ball and water resistance.
When the ball reaches the surface of the water, it has a velocity "v=\\sqrt{2gh}" and the time needed to reach water "t_1=\\sqrt{\\frac{2h}{g}}" . When the ball is in water, then it moves with the acceleration directed upwards
"a=\\left(\\frac{\\rho_w}{\\rho}-1\\right)g", where "\\rho_w" is the density of water. The ball stops after the time "t_2=\\frac{v}{a}=\\sqrt{\\frac{2h}{g}}\\frac{1}{\\frac{\\rho_w}{\\rho}-1}" and during this time it passes the distance "s=\\frac{v^2}{2a}=\\frac{h}{\\frac{\\rho_w}{\\rho}-1}". To reach back the water surface the ball needs the time "t_3=\\sqrt{\\frac{2s}{a}}=\\sqrt{\\frac{2h}{g}}\\frac{1}{\\frac{\\rho_w}{\\rho}-1}" . So the total time taken "t=t_1+t_2+t_3=\\sqrt{\\frac{2h}{g}}\\left(1+\\frac{2}{\\frac{\\rho_w}{\\rho}-1}\\right)".
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