Maximize the distance of projectile on a hill

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Homework Help Overview

The problem involves determining the optimal angle from the horizontal at which an athlete should throw a rock from the peak of a hill that slopes downward at a specific angle. The goal is to maximize the horizontal distance the rock travels.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants discuss the derivation of equations related to projectile motion and the relationship between the launch angle and the slope of the hill. There are attempts to differentiate the expression for horizontal distance to find the angle that maximizes it. Some participants question the implications of the slope on the expected maximum distance angle.

Discussion Status

Several participants have provided insights into the relationship between the launch angle and the slope angle, with some suggesting that the derived angle is a general solution. There is ongoing exploration of how to express the distance in terms of the slope angle, and some participants have offered guidance on interpreting the results.

Contextual Notes

There is a focus on understanding the implications of the slope on the projectile's range, and participants are considering how to relate the angles mathematically. The discussion reflects a mix of theoretical exploration and practical application of the derived relationships.

Mr Davis 97
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Homework Statement


An athlete stands at the peak of a hill that slopes downward uniformly at angle ##\phi##. At what angle ##\theta## from the horizontal should they throw a rock so that it has the greatest range?

Homework Equations


SUVAT equations and trig relations

The Attempt at a Solution



I found the following three equations:

##y = v_0 \sin \theta t - \frac{1}{2} g t^2##
##t = \frac{x}{v_0 \cos \theta}##
##y = -x \tan \phi##

I combined all of these to find the final horizontal position x:

##x = \frac{v_0^2}{g}(\sin 2 \theta + 2 \tan \phi \cos^2 \theta)##
We need to maximize ##x## with respect to ##\theta##, so we take the first derivative and set it to ##0##.

##\frac{dx}{d \theta} = 2 \cos 2 \theta + 2 \tan \phi (2 \cos \theta) (- \sin \theta) = 0##

##\tan 2 \theta = \frac{1}{ \tan \phi}##

So this is what I end up with, but I am not sure what to do next... Any ideas?

Edit: I played with it a little more and found that ##\theta = \frac{1}{2} (90 - \phi)##, but I am not quite sure how to use this to find the angle that gives the maximum distance.
 
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Mr Davis 97 said:

Homework Statement


An athlete stands at the peak of a hill that slopes downward uniformly at angle ##\phi##. At what angle ##\theta## from the horizontal should they throw a rock so that it has the greatest range?

Homework Equations


SUVAT equations and trig relations

The Attempt at a Solution



I found the following three equations:

##y = v_0 \sin \theta t - \frac{1}{2} g t^2##
##t = \frac{x}{v_0 \cos \theta}##
##y = -x \tan \phi##

I combined all of these to find the final horizontal position x:

##x = \frac{v_0^2}{g}(\sin 2 \theta + 2 \tan \phi \cos^2 \theta)##
We need to maximize ##x## with respect to ##\theta##, so we take the first derivative and set it to ##0##.

##\frac{dx}{d \theta} = 2 \cos 2 \theta + 2 \tan \phi (2 \cos \theta) (- \sin \theta) = 0##

##\tan 2 \theta = \frac{1}{ \tan \phi}##

So this is what I end up with, but I am not sure what to do next... Any ideas?
You know tan(2θ). What is θ then? (Imagine a numerical value for tan(Φ). How would you calculate θ? )
 
Your analysis shows that the angle to get maximum distance depends on the slope ... if you expect the max distance angle to be independent of the slope, then you have made a mistake somewhere.

Note: what do they mean by "range"?
 
Mr Davis 97 said:
##\theta = \frac{1}{2} (90 - \phi)##, but I am not quite sure how to use this to find the angle that gives the maximum distance.

That was an excellent solution. And that is the answer. You have found ##\theta## in terms of ##\phi##.

What you have is called a general solution to the problem: you have established a direct relationship between the two variables.

Now, if you know or measure ##\phi## for a given slope, you can calculate the required ##\theta##. You could then calculate the range, ##x##, using these values.

Alternatively, you could go back to your equation:

##x = \frac{v_0^2}{g}(\sin 2 \theta + 2 \tan \phi \cos^2 \theta)##

And, using some trig, express ##x## entirely as a function of ##\phi## using ##\theta = \frac{1}{2} (90 - \phi)##

That would give you a general solution for the maximum possible range, ##x##, in terms of ##\phi##.
 
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Mr Davis 97 said:
##\tan 2 \theta = \frac{1}{ \tan \phi}##
So this is what I end up with, but I am not sure what to do next... Any ideas?
Yes, I have an idea - you're done, essentially!
To finish up,
tan(2θ) = cot(φ)
2θ = tan-1[cot(φ)]
& I'll leave the rest to you! :-)
Well done.

EDIT: and yes I see that θ = 1/2 (90 - φ) is equivalent and better.
 
PeroK said:
That was an excellent solution. And that is the answer. You have found ##\theta## in terms of ##\phi##.

What you have is called a general solution to the problem: you have established a direct relationship between the two variables.

Now, if you know or measure ##\phi## for a given slope, you can calculate the required ##\theta##. You could then calculate the range, ##x##, using these values.

Alternatively, you could go back to your equation:

##x = \frac{v_0^2}{g}(\sin 2 \theta + 2 \tan \phi \cos^2 \theta)##

And, using some trig, express ##x## entirely as a function of ##\phi## using ##\theta = \frac{1}{2} (90 - \phi)##

That would give you a general solution for the maximum possible range, ##x##, in terms of ##\phi##.

Awesome! I'll try to remember that in the future, that the solution might just be a symbolic relationship rather than numerical.
 

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