"Superball" bouncing between two walls

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The discussion centers on solving the motion of a superball bouncing between two walls, with a focus on calculating velocity, distance, and time during its bounces. Initial calculations for various points in time reveal relationships between velocity and position, leading to a derived formula for acceleration as a function of position. Participants identify errors in the distance calculations for the second transit and clarify the total time for the first two transits. The conversation emphasizes the importance of accurately defining variables and equations to analyze the ball's motion effectively. The thread concludes with a suggestion to define sequences for velocity and time to facilitate further analysis.
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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.
 
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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).
 
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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.
 
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