Projectile motion of two balls off a cliff

Click For Summary
The discussion focuses on the projectile motion of two balls thrown from a cliff, one at an angle above the horizontal and the other below. The original poster struggles to calculate the individual ranges, mistakenly arriving at zero due to incorrect application of equations. Participants suggest drawing diagrams to visualize the problem and emphasize the importance of understanding the physics behind the kinematic equations rather than just plugging in numbers. They highlight that the time of flight differs for each throw, which affects the range calculations, and clarify that the problem specifically asks for the difference in ranges, not the individual ranges themselves. Understanding the relationship between the angles and velocities is crucial for solving the problem correctly.
tellmesomething
Messages
449
Reaction score
68
Homework Statement
1. Two balls are projected from the top of a cliff with equal initial speed u. One starts at angle θ
above the horizontal while the other starts at angle θ below. Difference in their ranges is
Relevant Equations
Non
Screenshot_2024-11-23-17-39-07-609_com.miui.notes.jpg

This is just the object which is thrown theta angle below rhe horizontal. I fail to understand how to get the individual range of this. I tried but I am getting zero, can someone point out what is wrong in my method

So ##R=ucos\theta*t ##
##\frac{h}{R}=tan\theta##
Therefore ##h=Rtan\theta##
We know that ##H=usin\theta*t+\frac{1}{2}gt^2##
So ##Rtan\theta=\frac{R}{ucos\theta}[usin\theta +\frac{1}{2}g\frac{R}{ucos\theta}]##
As you can see we get
##usin\theta=usin\theta+\frac{1}{2}g\frac{R}{ucos\theta} ##

So R=0

What is wrong here
 
Physics news on Phys.org
tellmesomething said:
Homework Statement: 1. Two balls are projected from the top of a cliff with equal initial speed u. One starts at angle θ
above the horizontal while the other starts at angle θ below. Difference in their ranges is
Relevant Equations: Non

View attachment 353821
This is just the object which is thrown theta angle below rhe horizontal. I fail to understand how to get the individual range of this. I tried but I am getting zero, can someone point out what is wrong in my method

So ##R=ucos\theta*t ##
##\frac{h}{R}=tan\theta##
Therefore ##h=Rtan\theta##
We know that ##H=usin\theta*t+\frac{1}{2}gt^2##
So ##Rtan\theta=\frac{R}{ucos\theta}[usin\theta +\frac{1}{2}g\frac{R}{ucos\theta}]##
As you can see we get
##usin\theta=usin\theta+\frac{1}{2}g\frac{R}{ucos\theta} ##

So R=0

What is wrong here
The projectile moves in a parabola. The angle ##\theta## is only the initial angle.
 
  • Like
Likes Steve4Physics and erobz
tellmesomething said:
Homework Statement: 1. Two balls are projected from the top of a cliff with equal initial speed u. One starts at angle θ
above the horizontal while the other starts at angle θ below. Difference in their ranges is
Relevant Equations: Non

View attachment 353821
This is just the object which is thrown theta angle below rhe horizontal. I fail to understand how to get the individual range of this. I tried but I am getting zero, can someone point out what is wrong in my method

So ##R=ucos\theta*t ##
##\frac{h}{R}=tan\theta##
Therefore ##h=Rtan\theta##
We know that ##H=usin\theta*t+\frac{1}{2}gt^2##
So ##Rtan\theta=\frac{R}{ucos\theta}[usin\theta +\frac{1}{2}g\frac{R}{ucos\theta}]##
As you can see we get
##usin\theta=usin\theta+\frac{1}{2}g\frac{R}{ucos\theta} ##

So R=0

What is wrong here
Your diagram doesn't seem to make sense for the problems neither do your kinematic models?

I would start by writing the range of each projectile after I drew two diagrams for comparison. Begin with the projectile that is projected above horizontal. Solve the system of kinematic equations for it, what do you get for its range?

P.S. after I did that, I realized I could satisfy both scenarios with the same equation by seeing the sign properties of the trig functions with regards to ##\theta## and ## -\theta## arguments.
 
Last edited:
@tellmesomething, avoid using different symbols (h and H) for the same quantity.

It looks like you are sticking numbers into equations and doing the algebra without fully understanding the physics – dangerous! Here’s a possible approach:

1) For the upwards throw, note that the initial vertical component of velocity is usin⁡θ upwards. And for the downwards throw, it is usin⁡θ downwards.

2) Use the above to find the time-of-flight for each throw. The times are different. (The times aren’t affected by the horizontal component of motion.)

3) The horizontal component of velocity for both throws is ucos⁡θ so, knowing the times, you can now find the two ranges.

Edit: It's worth noting that there is a quick method to solve the problem. This depends on the fact that the time-difference between the throws can easily be found - if you can spot the 'trick'.
 
Last edited:
  • Like
Likes Lnewqban and erobz
tellmesomething said:
...
This is just the object which is thrown theta angle below rhe horizontal. I fail to understand how to get the individual range of this.
But you are not asked to calculate the range of the downwards thrown ball; the problem asks for the difference in the ranges of both balls.

If you draw an imaginary horizontal line at the same altitude of the common point of throw (Two balls are projected from the top of a cliff with equal initial speed u), at what angle and velocity the ball that was thrown upwards would cross that line in its way down? (no calculation is needed to answer that question).
 
  • Like
Likes haruspex and Steve4Physics
Thread 'Chain falling out of a horizontal tube onto a table'
My attempt: Initial total M.E = PE of hanging part + PE of part of chain in the tube. I've considered the table as to be at zero of PE. PE of hanging part = ##\frac{1}{2} \frac{m}{l}gh^{2}##. PE of part in the tube = ##\frac{m}{l}(l - h)gh##. Final ME = ##\frac{1}{2}\frac{m}{l}gh^{2}## + ##\frac{1}{2}\frac{m}{l}hv^{2}##. Since Initial ME = Final ME. Therefore, ##\frac{1}{2}\frac{m}{l}hv^{2}## = ##\frac{m}{l}(l-h)gh##. Solving this gives: ## v = \sqrt{2g(l-h)}##. But the answer in the book...

Similar threads

Replies
4
Views
2K
  • · Replies 24 ·
Replies
24
Views
2K
  • · Replies 7 ·
Replies
7
Views
1K
  • · Replies 38 ·
2
Replies
38
Views
2K
  • · Replies 9 ·
Replies
9
Views
496
Replies
1
Views
1K
Replies
8
Views
1K
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 18 ·
Replies
18
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K