Angle for maximum height of ball bounce

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Discussion Overview

The discussion revolves around determining the optimal angle for a ball to achieve maximum height after an elastic bounce, given a fixed kinetic energy and initial height. The participants explore various methods and considerations related to the trajectory and mechanics of the bounce.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants question the definition of "maximum height," suggesting that in a perfectly elastic bounce, the ball returns to its original height regardless of the angle, with the highest point being straight up.
  • One participant raises the importance of friction and spin, asking if the surface is frictionless, which could affect the ball's trajectory.
  • Another participant proposes two methods for calculating the optimal angle: one involving the trajectory's intersection with the surface and the other suggesting a rotation of the system to simplify the problem.
  • A participant expresses difficulty in proceeding with the proposed methods and hints at a potentially easier method.
  • There is a discussion about the mechanical energy of the ball and the conditions under which it can reach maximum height after the bounce, with references to specific equations involving gravitational potential and kinetic energy.
  • Concerns are raised about scenarios where the energy may not be sufficient to reach the vertex of the trajectory, complicating the problem further.
  • One participant outlines a method for solving the angle equation, discussing the manipulation of trigonometric identities and conditions for the determinant of a quadratic equation.

Areas of Agreement / Disagreement

Participants express differing views on the mechanics of the bounce and the conditions necessary for achieving maximum height. There is no consensus on the optimal approach or the implications of energy constraints on the problem.

Contextual Notes

Participants have not resolved assumptions regarding the initial conditions, the impact of energy levels on the trajectory, and the specific definitions of maximum height in the context of elastic bounces.

Final
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There is a ball of mass m. It is at height L (see the picture).
The kinetic energy is fixed (=E). What is the angle a, for which the ball catches up the maximum height after one bounce?
The bounce is elastic.
Thanks,
Final.
 

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Final said:
There is a ball of mass m. It is at height L (see the picture).
The kinetic energy is fixed (=E). What is the angle a, for which the ball catches up the maximum height after one bounce?
The bounce is elastic.
Thanks,
Final.

What do you mean by the "maximum height"? If the bounce is perfectly elastic, then at any angle, the ball will bounce back to the maximum height it reached before the first bounce. What that height is will depend on angle. It would be maximum if the ball is moving straight up.
 
Is it a frictionless surface? If not then you have to take the spin acquired by the ball into account.
 
Yes, it is a frictionless surface.
The ball cannot go straight up, it must bounce.The height depend by the angle... I won't the angle a(E,L) that maximizes the height AFTER the first bounce. What it succeeds before the bounce not interests me.
Thanks,
Final
 
Method I: Write the trajectory of the ball in the form y = y(x) then find where that trajectory intersects the surface (line) y = x. You can then find the slope of the trajectory. You know the angle of incidence will equal the angle of reflection and you can use that as a starting point to calculate a "new trajectory." Find out how high the ball will travel on the new trajectory. It will be function of [itex]\theta[/itex] and you can attempt to maximize the high point of the trajectory with respect to that angle.

Method II: Try rotating your entire system clockwise by 45 degrees. Be sure to rotate gravity too! You can then follow a procedure similar to Method I but your maximization will be with respect to the direction opposite gravity. I don't know if this will simplify your problem (I haven't tried it!) but my first thought is the geometry might be easier.
 
Well,
I have tried both these methods, but my problem is to go on...
Can you solve it?
(I think there is a Method more easy).
Thanks
Final
 
Final said:
There is a ball of mass m. It is at height L (see the picture).
The kinetic energy is fixed (=E). What is the angle a, for which the ball catches up the maximum height after one bounce?
The bounce is elastic.
Thanks,
Final.

Some hints:

The ball has a given mechanical energy mgh + E. It would rise to the maximum height if it moved straight upwards vertically after the first bounce.
When the ball bounces back from the slope the magnitude of its velocity stays the same but the direction changes. The direction of its velocity after having reflected from the slope makes the same angle with the normal of the slope as did the incident velocity, only at the other side of the normal. After reflection, the ball moves vertically upward. What was the direction of its velocity before touching the slope?

ehild
 
Yes, this is easy: the ball must bounce when it is at the vertex of the parabola... the condition is: [tex]2gL + v^2\sin^2{\Theta} - v^2\sin{2\Theta}=0[/tex] (How do you solve this?)
But if the energy is not enough to to catch up the vertex??
Thanks
Final
 
Last edited:
Final said:
Yes, this is easy: the ball must bounce when it is at the vertex of the parabola... the condition is: [tex]2gL + v^2\sin^2{\Theta} - v^2\sin{2\Theta}=0[/tex] (How do you solve this?)
But if the energy is not enough to to catch up the vertex??
Thanks
Final

If the energy is not enough then the problem is just ugly. Apply Tide's method.

OK, I'll think about it.

To solve the equation for [tex]\Theta[/tex] first use that v^2 = 2E/m, rearrange it so as [tex]\sin(2\Theta) =2 \sin(\Theta )\cos(\Theta )[/tex] is alone at one side, take the square of both sides, replace [tex]\cos^2(\Theta) \mbox { by } (1-sin^2(\Theta))[/tex], you get a second order equation for [tex]\sin^2(\Theta)[/tex], find the condition that the determinant must not be negative, and solve.


ehild
 

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