"Superball" bouncing between two walls

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SUMMARY

The discussion focuses on the physics of a "Superball" bouncing between two walls, specifically analyzing the motion and forces involved during its transits. Key calculations include the time of collision with the moving wall, represented as t = 2l/(v0 + V), and the derived expressions for velocity and position after multiple bounces. Participants explore the relationship between acceleration, force, and position, ultimately questioning the accuracy of their calculations and assumptions regarding the ball's motion. The conversation emphasizes the importance of correctly defining variables and understanding the dynamics of the system.

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Homework Statement
A "superball" of mass m bounces back and forth between two surfaces with speed v0. Gravity is neglected and the collisions are perfectly elastic.
a. Find the average force F on each wall.
Ans. F = mv0^2 /l
b. If one surface is slowly moved toward the other with speed V <<v0, the bounce rate will increase due to the shorter distance between collisions, and because the ball's speed increases when it bounces from the moving surface. Find F in terms of the separation of the surfaces, x.
(Hint: Find the average rate at which the ball's speed increases as the surface moves.)
Ans. F =(mv0^2/l)(l/x)^3
Relevant Equations
Newtons laws, conservation of momentum and energy.
I have been able to solve part a correctly, but am having some trouble with part b.
I started out calculating values of v and x at various points in time when the ball collides with either wall. I found:

t = 0, v = v0, x = l

t = (l/v0), v = v0, x = l(v0-v)/v0

t = 2l/(v0+V), v = v0 + 2V, x = l(v0-V)/(v0+V)

t = 3l/(v0+2V), v = v0 + 2V, x = l(v0-V)/(v0+2V)

t = 4l/(v0+3V), v = v0 + 4V, x = l(v0-V)/(v0+3V)

t = 5l/(v0 + 4V), v = v0 + 4V, x = l(v0-V)/(v0+4V)

t = 6l/(v0+5V), v = v0 + 6V, x = l(v0-V)/(v0+5V)

Extrapolating from this, one might write for v = v0 + nV, x = l(v0-V)/(v0+(n-1)V), and t = nl/(v0+(n-1)V). Manipulating x = l(v0-V)/(v0+(n-1)V) yields
n = (l-x)(v0-V)/Vx. Substituting this into the expression for v, we have v = v0 + (l-x)(v0-V)/x.

Differentiating this with respect to x should yield a(x), so we have $$a(x) = \frac d {dx} (v_0 + \frac{(l-x)(v_0-V)}{x}).$$

$$a(x) = (v_0 - V) \frac d {dx} (\frac lx -1)$$
$$a(x) = \frac{(V - v_0)l} {x^2}$$

Now, F = ma = m(V - v0)l/x^2.

Letting V - v0 = v0, we have F = -mv0(l/x^2). But this is clearly not the answer indicated. What is the flaw in my solution?
 
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Are you trying to calculate accleleration as a function of ##x## here?
 
I thought that might be the way to calculate the force in terms of x.
 
cpgp said:
t = 2l/(v0+V)
How so?
 
haruspex said:
How so?
Assuming the ball is released at r = 0, it first collides with the moving wall at t = 2l/(v0+V).
 
cpgp said:
Assuming the ball is released at r = 0, it first collides with the moving wall at t = 2l/(v0+V).
Judging from your v=v0 for the second transit, the ball started at the moving end. You got that the first transit takes l/v0. How far is the second transit? How long does that take? What is the total time for those two transits?
 
haruspex said:
Judging from your v=v0 for the second transit, the ball started at the moving end. You got that the first transit takes l/v0. How far is the second transit? How long does that take? What is the total time for those two transits?
The total time for those two transits is 2l/(v0+V). The distance traveled is l(v0-V)/(v0+V).
 
cpgp said:
The total time for those two transits is 2l/(v0+V). The distance traveled is l(v0-V)/(v0+V).
For the second transit you have velocity v0 and distance l(v0-V)/v0. That takes time l(v0-V)/v02. Adding the time of the first transit we have l/v0+l(v0-V)/v02=(l/v0)(1+(v0-V)/v0)=l(2v0-V)/v02

Edit: that was using your second line
t = (l/v0), v = v0, x = l(v0-v)/v0
But I just realized that x is wrong. l(v0-v)/v0 is the distance when it starts the second transit, but it will not have to go that far.
 
Last edited:
haruspex said:
For the second transit you have velocity v0 and distance l(v0-V)/v0. That takes time l(v0-V)/v02. Adding the time of the first transit we have l/v0+l(v0-V)/v02=(l/v0)(1+(v0-V)/v0)=l(2v0-V)/v02

Edit: that was using your second line
t = (l/v0), v = v0, x = l(v0-v)/v0
But I just realized that x is wrong. l(v0-v)/v0 is the distance when it starts the second transit, but it will not have to go that far.
Yes, x is l(v0-V)/(v0+2V).
 
  • #10
cpgp said:
Yes, x is l(v0-V)/(v0+2V).
I don't get that 2.
First transit: dist L, time L/v0
In this time the barrier has advanced VL/v0
Second transit time t, V(L/v0 + t) + v0 t = L
t(v0+V) = L - L(V/v0)
x = v0 t = L(v0-V)/(v0+V)

So what is the total time for the first two transits?

To solve it analytically, define sequences of variables like
vn velocity after n bounces off the moving barrier
tn time between nth and (n+1)th bounce off moving barrier.
Then obtain equations relating successive terms.

At some point, presumably, you should use V<<v0, but avoid doing that too soon as it can lead to a wrong answer.
 
Last edited:
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