floyd0117
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I have a problem where I need to figure out the initial velocity vector \vec{v_0} of a projectile, in order for it to land at the final position \vec{r_f} = x_f\hat{x} + y_f\hat{y} + z_f\hat{z}, from initial position \vec{r_0}.
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The only knowns in the problem are \vec{r_0} and \vec{r_f}. Air resistance is neglected, so the the components of the net force on the projectile are
m\ddot{x} = 0
m\ddot{y} = 0
m\ddot{z} = -mg
So really we can choose any launch angle \phi, and find the necessary |\vec{v}|, or the other way around, to land us at \vec{r_f}. I think it sounds easier to choose a \phi and then find |\vec{v}|. So, I examine the limiting cases...
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Let's say d is the the distance between the initial and final positions in the x-y plane, that is;
d = |x_f\hat{x} + y_f\hat{y}|
and that h is the desired final height, h = z_f.
Then the angle \theta measured form the x-y plane to a line connecting (x_0, y_0 ,z_0) to (x_f, y_f, z_f) is smiply
\theta = \arctan{\dfrac{h}{d}}
So, our limiting cases are:
\phi \rightarrow \theta; |\vec{v_0}| \rightarrow \infty
\phi \rightarrow \dfrac{\pi}{2}; |\vec{v_0}| \rightarrow \infty
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So I can choose any angle between \dfrac{\pi}{2} and \theta, though angles close to those values will necessitate a very large initial velocity. My question is, how do I go from here, to determining |\vec{v_0}|? If I choose a \phi, how do I find a velocity that will get me to \vec{r_f}? It would seem that I need some function of v_0 in terms of both \phi (known, after choosing), and \vec{r_f}. Am I severely over thinknig this?
___
The only knowns in the problem are \vec{r_0} and \vec{r_f}. Air resistance is neglected, so the the components of the net force on the projectile are
m\ddot{x} = 0
m\ddot{y} = 0
m\ddot{z} = -mg
So really we can choose any launch angle \phi, and find the necessary |\vec{v}|, or the other way around, to land us at \vec{r_f}. I think it sounds easier to choose a \phi and then find |\vec{v}|. So, I examine the limiting cases...
____
Let's say d is the the distance between the initial and final positions in the x-y plane, that is;
d = |x_f\hat{x} + y_f\hat{y}|
and that h is the desired final height, h = z_f.
Then the angle \theta measured form the x-y plane to a line connecting (x_0, y_0 ,z_0) to (x_f, y_f, z_f) is smiply
\theta = \arctan{\dfrac{h}{d}}
So, our limiting cases are:
\phi \rightarrow \theta; |\vec{v_0}| \rightarrow \infty
\phi \rightarrow \dfrac{\pi}{2}; |\vec{v_0}| \rightarrow \infty
___
So I can choose any angle between \dfrac{\pi}{2} and \theta, though angles close to those values will necessitate a very large initial velocity. My question is, how do I go from here, to determining |\vec{v_0}|? If I choose a \phi, how do I find a velocity that will get me to \vec{r_f}? It would seem that I need some function of v_0 in terms of both \phi (known, after choosing), and \vec{r_f}. Am I severely over thinknig this?
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