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Calculus1 20 Online
OpenStudy (anonymous):

help!

OpenStudy (anonymous):

OpenStudy (anonymous):

What excatly is your problem?

OpenStudy (anonymous):

As \(y\) components we've got the gravity, which faces downwarts and our toss, which faces upwards: 1) Highest point: For this part we use the fact, that at the highest point the velocity is zero: \[ v_y = v_{0y} - gt = 0 \Rightarrow t = \frac{v_{0y}}{g} \] 2) Maximum height: We've just calculated the time it needs to get to the highest point. Therefore we can plug this time into the formula of position with respect to time:\[ r(t) = \underbrace{r_0}_{72ft} + v_{0y}t - \frac{1}{2}gt^2 \Rightarrow r = r(t) = \underbrace{r_0}_{72ft} + v_{0y} \frac{v_{0y}}{g} - \frac{1}{2}g\left( \frac{v_{0y}}{g}\right)^2 \]\[ = \underbrace{r_0}_{72ft} + \frac{v_{0y}^2}{g} - \frac{1}{2}\frac{v_{0y}^2}{g}\]

OpenStudy (anonymous):

\[t_{up} = \frac{v_{0y}}{g}\] 3) Total time of travel: To solve this we can use two things. - We know the time it takes for the stone to get to it's highes point. - We assume the beach to be at a height of \(h = 0ft\) The stone falling down can be seen as a free fall from a given height \(h_{max}\), we calculated in section 2. The equation for free fall is at follows: \[ r(t_{end}) = h_{max} - \frac{1}{2}gt^2 = \underbrace{\left[ r_0 + \frac{v_{0y}^2}{g} - \frac{1}{2} \frac{v_{0y}^2}{g} \right]}_{h_{max}}- \frac{1}{2}gt^2 \] If we now solve for \(t\) which should give us the time it takes to fall from \(h_{max}\) down to the beach: \[ t = \sqrt{\frac{2h_{max}}{g}} = \sqrt{\frac{2\left[ r_0 + \frac{v_{0y}^2}{g} - \frac{1}{2} \frac{v_{0y}^2}{g} \right]}{g}} \] The total time of travel can now be calculated as: \[ t_{total} = t_{up} + t_{down} = \frac{v_{0y}}{g} + \sqrt{\frac{2\left[ r_0 + \frac{v_{0y}^2}{g} - \frac{1}{2} \frac{v_{0y}^2}{g} \right]}{g}} \]

OpenStudy (anonymous):

4) Velocity at the impact: The impact velocity can now easily be calculated by the time of travelling downwards and the acceleration due to gravity: \[ v_{impact} = - gt_{down} = -g \sqrt{\frac{2\left[ r_0 + \frac{v_{0y}^2}{g} - \frac{1}{2} \frac{v_{0y}^2}{g} \right]}{g}} \]

OpenStudy (anonymous):

I think the formulas should be right that way, but please try to make yourself clear what i did and the physical meaning of each step. If anything is unclear or you find a mistake please don't hesitate to aks.

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