Bungee jumping and Conservation of energy

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Homework Help Overview

The discussion revolves around a bungee jumping scenario involving conservation of energy principles. The problem presents an equation relating the length of the bungee cord to the maximum acceleration experienced by the jumper, prompting participants to evaluate its physical reasonableness under specific conditions.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the implications of setting maximum acceleration to specific values, questioning the physical meaning of the derived equation and its limits. There is discussion about the conditions under which the cord begins to stretch and the relationship between free fall and the bungee cord's behavior.

Discussion Status

The conversation is ongoing, with participants providing insights and raising questions about the assumptions made in the problem. Some suggest the need for limit considerations in evaluating the equation, while others express confusion regarding the implications of certain values for the length of the cord.

Contextual Notes

Participants note that the jumper comes to a halt just before hitting the ground, which complicates the interpretation of free fall and the stretching of the cord. There is also mention of the need to justify the conditions under which the equation holds true.

solarcat
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Homework Statement


A person is bungee jumping from the top of a cliff with height H. The un-stretched length of the bungee rope is L. The person comes to a stop just before hitting the ground. The length of the cord is equal to H(amax-g)/(amax+g), where amax is the maximum acceleration upward right before the person hits the ground. Show this equation is physically reasonable by evaluating it when amax = g and amax = infinity.

Homework Equations


Conservation of energy

The Attempt at a Solution


amax = g
L = H(g-g)/(g+g) = 0
This means that the cord starts stretching right as the person jumps.
amax = infinity
L = (infinity -g)/(infinity+g)*H = H
If the length of the cord is equal to H, the cord never starts stretching.
If the cord never starts stretching, then the jumper is always in free-fall, and the acceleration is equal to g. Then shouldn't the results be the other way around?
 
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solarcat said:
The length of the cord is equal to H(amax-g)/(amax+g),
It's not clear which length that refers to, but you seem to have interpreted it correctly.
solarcat said:
This means that the cord starts stretching right as the person jumps.
Yes, but why should that correspond to amax=g? I don't think it is at all obvious, but in order to satisfy the question there needs to be some justification.
solarcat said:
evaluating it when ... amax = infinity.
Bad question. It should say as amax tends to infinity, and likewise you need to use limits in the answer. You cannot validly write:
solarcat said:
L = (infinity -g)/(infinity+g)*H = H

solarcat said:
If the cord never starts stretching, then the jumper is always in free-fall
You are given that the jumper does come to a halt just before hitting the ground, so it cannot be all free fall.
 
haruspex said:
It should say as amax tends to infinity, and likewise you need to use limits in the answer. You cannot validly write: L = (infinity -g)/(infinity+g)*H = H
OK, fair enough. But I have also derived the equation amax = k/m(H-L) - g. This is because when the cord starts stretching, the net force on the jumper ma = Ft-mg. a is maximized when Ft (tension) is greatest, which would be when the cord is stretched the most, which would be at the bottom. Then
m*amax = k(H-L) - mg
amax = (k/m)(H-L) - mg
(infinity + mg) (m/k) = H-L
Smaller values of L result in larger values of amax, and the length can't be negative... But I'm confused, because also, the elastic potential energy at the bottom should equal the initial potential energy, mgH.
So mgH = 1/2 k (H-L)^2
mgH/(H-L) = 1/2 k (H-L)
2mgH(H-L) = k (H-L)
2gH/(H-L) = (k/m)(H-L)
From the last equation, amax + mg = (k/m)(H-L)

amax + mg = 2gH/(H-L)
As amax gets larger and larger, the denominator should get smaller, so H-L = 0 --> H = L

And I'm still not sure why L = H(g-g)/(g+g) = 0
 
Last edited:
solarcat said:
(infinity + mg) (m/k) = H-L
This illustrates the need to treat it as a limits problem. That equation tells you that as amax tends to infinity k tends to infinity, but it does not tell you the relationship between those two trends, so it does not indicate what happens to H-L.
solarcat said:
amax + mg = 2gH/(H-L)
That can be turned into the equation you were given. By eliminating k it does allow you to see what happens to H-L.
solarcat said:
And I'm still not sure why L = H(g-g)/(g+g) = 0
I guess you mean you do not see a simple reason why amax=g should correspond to L=0. Maybe you can reason that L=0 means this will be SHM across the entire height H. What would that tell you about the relationship between acceleration at the top and acceleration at the bottom?
 

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