Maximizing Horizontal Range of a Projectile

8 replies · 4K views · last reply
Science Advisor
Homework Helper
Education Advisor
Insights Author
Messages
1,262
Reaction score
755
Attachments
  • Projectile diagram: a ball launched at speed v0 at angle θ0 above horizontal from the top of a tower of height h, landing a horizontal distance R away on the ground; handwritten heading reads θ0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.8 KB · Views: 358
  • Projectile diagram: a ball launched at speed v0 at angle θ0 above horizontal from the top of a height h, following a red parabolic path to ground, with horizontal range R marked; header reads θ0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.7 KB · Views: 274
  • Handwritten diagram of a projectile launched at speed v0 and angle θ0 above horizontal from the top of a tower of height h, landing a horizontal distance R away on the ground, with the heading θ0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.8 KB · Views: 305
  • Projectile diagram: a ball launched at speed v0 at angle theta0 above horizontal from the top of a building of height h, landing a horizontal distance R away on the ground; heading reads theta0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.8 KB · Views: 267
  • Diagram of a projectile launched at angle θ0 with speed v0 from the top of a vertical height h, following a red arc that lands at horizontal range R; heading reads θ0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.7 KB · Views: 284
  • Handwritten diagram of a projectile launched at speed v0 and angle θ0 above horizontal from the top of a block of height h, landing a horizontal distance R away on the ground; heading reads θ0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.8 KB · Views: 247
  • Handwritten diagram of a projectile launched at speed v0 at angle θ0 from the top of a block of height h, landing at horizontal range R; heading reads θ0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.8 KB · Views: 256
  • Handwritten diagram of a projectile launched at speed v0 and angle theta0 above the horizontal from the top of a block of height h, landing a horizontal distance R away; the heading reads theta0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.8 KB · Views: 240
  • Diagram of a projectile launched at angle θ0 with speed v0 from the top of a vertical cliff of height h, its red parabolic path landing at horizontal range R; heading reads θ0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.7 KB · Views: 258
  • Handwritten diagram of a projectile launched at speed v0 and angle theta0 above the horizontal from the top of a block of height h, landing a horizontal distance R away on the ground; the heading reads theta0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.8 KB · Views: 232
  • Handwritten diagram of a projectile launched at speed v0 and angle theta0 from the top of a block of height h, landing at horizontal range R; the heading reads theta0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    6.8 KB · Views: 370
  • Handwritten sketch of a projectile launched at speed v0 and angle θ0 above horizontal from the top of a vertical height h, landing a horizontal distance R away; the heading reads θ0 = ? for R = Rmax.
    Maximum-Range-diagram-1.jpg
    5.1 KB · Views: 498
Last edited by a moderator:
  • Like
Likes   Reactions: vanhees71 and Greg Bernhardt
Thanks for posting. An error, perhaps, and a question, I extend. 1] In the 3rd equation right hand side, the first term should be $$R~tan(\theta)$$ and NOT $$v_0~R~tan(\theta) ~.$$ 2] In Method 2, should your definitions of ##\alpha## be $$sin(\alpha) = \frac{h}{R'} , where $$ $$R' = \sqrt{h^2+R^2}~,$$ and ##R## is defined as in your figure?
 
  • Like
Likes   Reactions: neilparker62 and vanhees71
Thanks for the correction - have updated as per your suggestion. Please let me know if there's anything still unclear.
 
Diagram of a projectile path: a boy at left throws a rock in a dotted parabolic arc over a rectangular building, with a 15.0 m horizontal distance marked along the ground and a vertical arrow labelled h showing the building's height.

I attempted solving this problem using @kuruman 's equation ##|\vec{v_i} \times \vec{v_f}|=Rg## in Method 3. Wolfram Alpha choked on it - readers might find it interesting to figure out why ?

Wolfram Alpha input interpretation solving (18.3 cos(57°), 18.3 sin(57°)) × (18.3 cos(57°), −1√((18.3 sin(57°))² + −1×2×9.81h)) = −15×9.8 for h, with result stating no solutions exist.
 
I am a Mathematica person myself so I put the two kinematic equations in x and y and asked it to solve for the time of flight tf and the height h. It worked fine (see below). I don't understand WA code well enough to ascertain what you are doing with it.

Mathematica input cell NSolve[{18.3 Cos[57°] tf == 15, 18.3 Sin[57°] tf - 0.5*9.8*tf^2 == h}, {tf, h}] with output {{tf -> 1.50498, h -> 11.9996}}.
 
  • Like
Likes   Reactions: vanhees71
Don't go conventional - just trust your own method! WA choked and it wasn't because your method or WA is at fault! The 'code' I put in was quite simple - it asked WA to solve the vector equation directly. What you have above is the solution provided on the kinematics webpage here and your vector technique shows it up as wrong!
 
neilparker62 said:
Don't go conventional - just trust your own method! WA choked and it wasn't because your method or WA is at fault! The 'code' I put in was quite simple - it asked WA to solve the vector equation directly. What you have above is the solution provided on the kinematics webpage here and your vector technique shows it up as wrong!
I don't see why the WA 'code' is a vector equation. I can see the two-dimensional vector on the left side but the right-hand side looks like a scalar and why is it negative? Also, I don't know about WA, but Mathematica does not accept 2-d vector cross products. For 2-d vectors, a third component must be set to zero.

I think the proper way to use the equation directly in WA is to ask it to solve the equation $$\sqrt{\left[v_0(\cos\theta, \sin\theta,0) \times (v_0\cos\theta,-\sqrt{v_{0}^2\sin^2\theta-2g\Delta h},0)\right]\cdot \left[v_0(\cos\theta, \sin\theta,0) \times (v_0\cos\theta,-\sqrt{v_{0}^2\sin^2\theta-2g\Delta h},0)\right]} =gR.$$The LHS is the square root of the dot product of the cross product with itself, i.e. the magnitude. It is set equal to ##gR##, a positive quantity.

I tried this with Mathematica. The numerical NSolve befuddled it. However, I got the expected result with cautionary messages when I used FindRoot and gave it an approximate value for ##\Delta h##.
 
WA is fine with 2D vector cross products. eg (ai + bj) x (ci + dj) would be entered as {a,b} cross {c,d}. The output is negative because i x -j is negative. On entry you need to make sure the ##v_f## vector is pointing downwards because the projectile is landing on the roof. It has passed (or should have passed) the maximum point of the trajectory. The reason WA chokes is not because it is wrong nor that your vector equation is wrong but because 15m is on the wrong side of the axis of symmetry - the projectile is still heading upward at that point. See following parametric graph of the projectile motion:

https://www.desmos.com/calculator/fwage30bpg