The range of a projectile fired up the side of a mountain?

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Discussion Overview

The discussion revolves around determining the optimal angle of projection, \(\theta\), for maximizing the range of a projectile fired up the side of a mountain with a constant slope, \(\phi\). Participants explore various approaches to model the projectile's motion and calculate the maximum range, while neglecting air resistance.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant suggests starting with the formula \(x_{max}=\frac{v_0^2 \sin 2\alpha}{g}\) but expresses uncertainty about its applicability to the mountain scenario.
  • Another participant questions the relevance of the initial formula and proposes calculating the projectile's distance in terms of \(\phi\), \(\theta\), and \(v_0\) to find the maximum range.
  • A different participant recommends finding the equation of the parabola representing the projectile's path and its intersection with the mountain slope to determine the maximum range.
  • Another approach involves using normal and tangential components of motion relative to the mountainside to derive the time at which the projectile's position is again zero.
  • One participant describes forming a triangle to represent the distance traveled up the mountain and provides a detailed mathematical expression for the distance as a function of time, leading to a condition for maximum distance.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the best approach to solve the problem, with multiple competing views and methods presented throughout the discussion.

Contextual Notes

Participants express uncertainty regarding the applicability of certain formulas and the assumptions underlying their calculations. The discussion involves various mathematical steps that remain unresolved.

cj
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Another question pertaining to a lab that I have to setup...

The range of a projectile fired up the side of a mountain?

At the base of a mountain with a constant slope of
[tex]\phi[/tex], a projectile is fired from a cannon oriented
at an angle of [tex]\theta[/tex].

What [tex]\theta[/tex] will result in the maximum range up the
side of the mountain?

What is this maximum range??

- air resistance can be neglected.

---
As a starting point I'm looking at

[tex]x_{max}=\frac{v_0^2sin2\alpha}{g}[/tex]

But am not clear about next steps.
 
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This is a classic problem.

That said, it's not at all clear that your formula applies to this situation. Perhaps it's easier to calculate the distance the projectile travels in terms of [tex]\phi[/tex],[tex]\theta[/tex] and [tex]v_0[/tex] and then find the maximum?
 
Yes, this is the line of thinking I was considering -- but came to a dead-end.

NateTG said:
This is a classic problem.

That said, it's not at all clear that your formula applies to this situation. Perhaps it's easier to calculate the distance the projectile travels in terms of [tex]\phi[/tex],[tex]\theta[/tex] and [tex]v_0[/tex] and then find the maximum?
 
Find the equation for the parabola with the correct slope (y as a function of x).
Find the intersection of this parabola with the straight line representing the mountain slope (i.e, find the x-coordinate of the point of intersection).

alternatively, write the equations of motion in terms of normal and tangential components to the mountainside. Determine the time at which the projectile's normal position is again 0.

Anyhow, once you've found this, you may find an equation for distance as a function of the angle that can be maximized.
 
Last edited:
Form a triangle so that you have the slope representing the distance traveled up the mountain.
(u cos theta) t is horizontal distance (theta = angle between initial velocity vector,u, and horizontal) and 1/2 gt ^ 2 is vertical distance on triangle.

distance up mountain = sqrt [ (1/2gt ^2)^ 2 + (u cos theta)^2 t ^ 2]

Since distance up mountain is a function of time:
for maximum distance up mountain

d(distance)/ dt = 0

so d/dt sqrt [ (1/2gt ^2)^ 2 + (u cos theta)^2 t ^ 2]= 0

If phi is angle of mountain slope, then
tan phi = vertical of triangle/ horizontal of triangle
tan phi = 1/2 gt ^ 2 / ( u cos theta) t
so 1/2 gt^2 = (u cos theta) t x tan phi
u cos theta = (1/2 gt)/tan phi

so d/dt sqrt [ (1/2gt ^2)^ 2 + (1/2 gt) ^2/ (tan phi)^2 t ^ 2]= 0
d/dt sqrt [ 1/4 g^2 x t^4 + 1/4g^2 x t^2/ (tan phi)^2 t^2 ]= 0

for constant phi we can evaluate d/dt.


( differentiation can be done using u substitution and chain rule)

substituting the theta and phi for t in the differentiated expression
will give maximum distance projectile travels up mountain.
 
Last edited:

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