Conservation of momentum - trampoline

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SUMMARY

The discussion centers on the conservation of momentum and energy in the context of a trampoline jump, specifically analyzing Joe's drop from a height of 3 meters. The force exerted by the trampoline is modeled as F = kx, where k represents the spring constant. Participants agree that while momentum is not conserved when considering Joe alone due to external forces like gravity and the normal force from the trampoline, it is conserved when the Earth is included in the system. Additionally, real-world factors such as energy loss to heat and sound are acknowledged as limitations of the model.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with the concepts of potential energy (mgh) and kinetic energy
  • Knowledge of elastic potential energy and spring constants (F = kx)
  • Basic grasp of momentum as a vector quantity
NEXT STEPS
  • Explore the implications of energy loss in real-world trampoline physics
  • Study the effects of air resistance on jumping dynamics
  • Investigate different spring constants in various trampoline designs
  • Learn about momentum conservation in closed systems versus open systems
USEFUL FOR

Students studying physics, particularly those focusing on mechanics, as well as educators and anyone interested in the practical applications of energy and momentum conservation in sports and recreational activities.

Pottesur
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English isn't my main language, so I apologize in advance if something is unclear.

We are leaving air resistance out of this problem!

1. Homework Statement

We are going to describe the force F from the trampoline on the Joe as F = kx, k is a spring constant. This is a model.

1. Joe drops from a window at 3 meters above the trampoline, hits the trampoline with stiff legs, and bounces back up. How high up does Joe go now?

2. Based on your own experience with trampolines: is this model a good model for vertical trampoline jumping? Are there any sides to the model which are particularly weak?

3. Is momentum (size and direction) conserved when Joe hits the trampoline?

Homework Equations

The Attempt at a Solution


1. Conservation of energy. Joe will have potential energy as he drops because of gravity (mgh), which will transfer to kinetic energy as he falls towards the trampoline. When he hits the trampoline, the kinetic energy will be zero and the energy will be stored as elastic potential energy in the springs. He bounces back up to three meters when the elastic potential energy is released to kinetic energy.

2. Wouldn't some of the energy in "the real world" be lost to heat and/or sound? And the spring constant is probably different from trampoline to trampoline. Not quite sure what the right answer here is.

3. This is where I've really been struggling, particularly with what I am supposed to view as my system. If I look at Joe as the system, momentum is not conserved because there are external forces acting on him, right? When he is in mid-air gravity is acting on him, and when he hits the trampoline there is a normal force acting on him. Are both these forces considered external forces? But if I look at velocity, and conservation of energy, his velocity will be the same just before and after the jump. But because they differ in direction, is this also a reason momentum isn't conserved? Or is it a consequence of external forces acting on Joe? What if I consider the person and the Earth as a system, is momentum then conserved?

I am finding momentum quite hard to understand. Hopefully someone here can help me out :)
 
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Pottesur said:
English isn't my main language, so I apologize in advance if something is unclear.

We are leaving air resistance out of this problem!

1. Homework Statement

We are going to describe the force F from the trampoline on the Joe as F = kx, k is a spring constant. This is a model.

1. Joe drops from a window at 3 meters above the trampoline, hits the trampoline with stiff legs, and bounces back up. How high up does Joe go now?

2. Based on your own experience with trampolines: is this model a good model for vertical trampoline jumping? Are there any sides to the model which are particularly weak?

3. Is momentum (size and direction) conserved when Joe hits the trampoline?

Homework Equations

The Attempt at a Solution


1. Conservation of energy. Joe will have potential energy as he drops because of gravity (mgh), which will transfer to kinetic energy as he falls towards the trampoline. When he hits the trampoline, the kinetic energy will be zero and the energy will be stored as elastic potential energy in the springs. He bounces back up to three meters when the elastic potential energy is released to kinetic energy.

2. Wouldn't some of the energy in "the real world" be lost to heat and/or sound? And the spring constant is probably different from trampoline to trampoline. Not quite sure what the right answer here is.

3. This is where I've really been struggling, particularly with what I am supposed to view as my system. If I look at Joe as the system, momentum is not conserved because there are external forces acting on him, right? When he is in mid-air gravity is acting on him, and when he hits the trampoline there is a normal force acting on him. Are both these forces considered external forces? But if I look at velocity, and conservation of energy, his velocity will be the same just before and after the jump. But because they differ in direction, is this also a reason momentum isn't conserved? Or is it a consequence of external forces acting on Joe? What if I consider the person and the Earth as a system, is momentum then conserved?

I am finding momentum quite hard to understand. Hopefully someone here can help me out :)

You have analysed the issue fairly well. You noticed that momentum is a vector, so has a direction. That's good. Therefore, Joe's momentum is reversed by a trampoline jump.

Yes, if you include the Earth, then momentum of the Joe-Earth system is conserved.
 
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Hello Pottessur, ##\qquad## :welcome: ##\qquad## !

your english is excellent.
1. agree
2. agree. And different spring constants ##k## can easily be accommodated
3. agree. If you want momentum conservation, all the forces have to be within the system

[edit] slow typist. PeroK was a lot faster :smile: .
 
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Pottesur said:
momentum quite hard to understand
If it helps: the time derivative of momentum is force $$\vec {\bf F} = {d\vec{{\bf p}}\over dt}$$
 
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Ahh, thank you guys so much for your feedback! I really appreciate it. I now have a bit more confidence in myself, haha :biggrin:
 
Pottesur said:
When he hits the trampoline, the kinetic energy will be zero
Well, not straightaway. It is gradually converted to elastic PE.
Pottesur said:
the spring constant is probably different from trampoline to trampoline.
Yes, but that is not a flaw in the model. The model encompasses that possibility.
Pottesur said:
Wouldn't some of the energy in "the real world" be lost to heat and/or sound?
Yes, heat mostly, but how would you have to amend the F=kx model?
There's also air resistance.
 

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