Throwing a ball from atop a hill

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In summary: Maybe I'll think about that later.In summary, a boy stands on a hill that slopes uniformly downward at angle ##\phi##, and he wants to know at what angle ##\theta## he should throw a rock to achieve the greatest range. By rotating the reference frame so the hill is horizontal, the slope can be factored into the acceleration, making the position and velocity equations easier to work with. Setting the vertical component of velocity equal to zero gives half the total flight time, which can then be plugged into the horizontal component of the distance equation to find the optimal angle ##\theta## for a given angle ##\phi##. However, if the frame is rotated an arbitrary angle, the resulting equation for ##\theta## will
  • #1
swevener
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Homework Statement


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

Homework Equations


##\mathbf{s} = \mathbf{v}_0 t + \frac{1}{2} \mathbf{a} t^2##

##\mathbf{v} = \mathbf{v}_0 + \mathbf{a} t##

The Attempt at a Solution


First I tilted the reference frame so the sloping hill is horizontal and the initial velocity is at an angle ##\theta + \phi## from the ground. This makes the acceleration ##\mathbf{a} = g \sin(\phi) \hat{\imath} - g \cos(\phi) \hat{\jmath}##. So position is given by
[tex]\mathbf{s} = \left[ v_0 t \cos(\theta + \phi) + \frac12 g t^2 \sin(\phi) \right] \hat{\imath} + \left[ v_0 t \sin(\theta + \phi) - \frac12 g t^2 \cos(\phi) \right] \hat{\jmath}.[/tex] Taking the derivative with respect to time,
[tex]\mathbf{v} = \left[ v_0 \cos(\theta + \phi) + g t \sin(\phi) \right] \hat{\imath} + \left[ v_0 \sin(\theta + \phi) - g t \cos(\phi) \right] \hat{\jmath}.[/tex]Setting the vertical component of velocity equal to zero gives half the total flight time:
[tex]t_{\text{max}} = \frac{v_0 \sin(\theta + \phi)}{g \cos(\theta)}.[/tex] Plugging ##2 t_{\text{max}}## into the horizontal component of ##\mathbf{s}## gives the distance traveled:
[tex]\begin{align}s_x (2 t_{\text{max}}) &= v_0 \frac{2 v_0 \sin(\theta + \phi)}{g \cos(\phi)} \cos(\theta + \phi) + \frac12 g \sin(\phi) \frac{4 v_0^2 \sin^2(\theta + \phi)}{\cos^2(\phi)} \\
&= \frac{2 v_0^2}{g \cos(\phi)} [ \sin(\theta + \phi) \cos(\theta + \phi) + \sin^2(\theta + \phi) \tan(\phi) ].\end{align}[/tex]
To find the optimal ##\theta## for a given ##\phi##, take
[tex]\begin{align}\frac{\text{d}}{\text{d} \theta} s_x (2 t_{\text{max}}) = 0 &= \cos(\theta + \phi) \cos(\theta + \phi) - \sin(\theta + \phi) \sin(\theta + \phi) + 2 \sin(\theta + \phi) \cos(\theta + \phi) \tan(\phi) \\
&= \cos^2(\theta + \phi) - \sin^2(\theta + \phi) + \sin(2(\theta + \phi)) \tan(\phi) \\
&= \cos(2(\theta + \phi)) + \sin(2(\theta + \phi)) \tan(\phi).\end{align}[/tex] A bit of algebra gives
[tex]\tan(2(\theta + \phi)) = - \cot(\phi),[/tex] which results in an equation for ##\theta##
[tex]\theta = \frac12 \arctan(-\cot(\phi)) - \phi.[/tex]
Now, the book's hint was that when ##\phi## is 60º, ##\theta## should be 15º. My equation spits out -75º, which has the slight problem of meaning the boy would be throwing the rock through the hill. So my question is why am I off by 90º? Did I make a mistake in my math somewhere? Does it have to do with rotating my reference frame? :frown:
 
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  • #2
well -75 degrees seems suspiciously like 15 degrees

so your book says it slopes down at 60 degrees so should you be using -60 degrees?

I would try to solve it without the rotation to see if things work out.
 
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  • #3
It seems to me my equation should be spitting out 15º, not 15º - 90º.
 
  • #4
jedishrfu said:
so your book says it slopes down at 60 degrees so should you be using -60 degrees?

I would try to solve it without the rotation to see if things work out.

Using -60º just gives me +75º. I've played with all the signs; the only answer that (sort of) works out is the one I got.

And solving the problem without the frame rotation is all kinds of unpleasant.
 
  • #5
swevener said:
And solving the problem without the frame rotation is all kinds of unpleasant.
Not really.
Flight time t, hor dist x, vert dist y (measuring positive downwards), accn a, initial velocity u at θ above horizontal:
-ut sin(θ) + at2/2 = y = x tan(ϕ) = ut cos(θ)tan(ϕ)
at/2u = tan(ϕ)cos(θ) + sin(θ)
xa/u2 = 2tan(ϕ)cos2(θ) + 2 sin(θ)cos(θ) = tan(ϕ)(cos(2θ)+1) + sin(2θ)
For max x:
tan(ϕ)(-2sin(2θ)) + 2cos(2θ) = 0
tan(ϕ) = cot(2θ)
ϕ = π/2 - 2θ
 
  • #6
haruspex said:
Not really.

Well, it was the way I was trying to do it, but if anything I've learned that I tend to overcomplicate things.

Anyway, I figured out the problem was my rotated frame. I plugged the ##2 t_{\text{max}}## I got above into the unrotated horizontal component of the distance equation and got the same equation haruspex did. Though I still don't know why rotating my frame an arbitrary angle offset my answer by exactly 90º.
 

FAQ: Throwing a ball from atop a hill

How does the height of the hill affect the distance the ball travels?

The height of the hill affects the distance the ball travels due to the increased potential energy of the ball at the top of the hill. The higher the hill, the more potential energy the ball has, allowing it to travel farther when thrown.

Does the angle at which the ball is thrown from the hill make a difference?

Yes, the angle at which the ball is thrown from the hill does make a difference. The optimal angle for maximum distance is 45 degrees, as it allows for a balance between the vertical and horizontal components of the ball's velocity.

How does the weight of the ball affect its trajectory when thrown from a hill?

The weight of the ball does not significantly affect its trajectory when thrown from a hill. As long as the ball is thrown with enough force to overcome the force of gravity, its weight will not have a major impact on its trajectory.

What is the relationship between the speed of the ball and the height of the hill?

The speed of the ball is directly related to the height of the hill. The higher the hill, the greater the potential energy of the ball, which can be converted into kinetic energy as the ball rolls down the hill. This results in a higher speed for the ball when it reaches the bottom of the hill.

How does air resistance affect the distance the ball travels when thrown from a hill?

Air resistance can have a significant impact on the distance the ball travels when thrown from a hill. The higher the hill, the longer the ball is in the air and the more time it has to be affected by air resistance, which can decrease its distance. However, the effect of air resistance is relatively small and can be minimized by throwing the ball with greater force.

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