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Momentum is always conserved |
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| May26-08, 03:53 PM | #1 |
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Momentum is always conserved
I don't understand how I can be at rest and then start walking or when a ball hits the wall it bounces back while the wall get no momentum at all?
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| May26-08, 04:07 PM | #2 |
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As far as I know, conservation of energy underlies conservation of momentum, so therefore if a ball hits a wall and bounces back some of its kinetic energy is converted to other forms such as heat and sound which appear in the wall.
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| May26-08, 04:08 PM | #3 |
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Recognitions:
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In the cases you mentioned there is momentum transfer to the earth (via the wall in the second case). Since you and the ball are a lot less massive than the earth, the velocity effect on the earth is extremely small.
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| May26-08, 04:38 PM | #4 |
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Momentum is always conservedIn either case, momentum is conserved. It's just that the wall is rigidly connected to the ground/Earth and likewise for your walking scenario. Remember that it's mass times velocity to get that momentum figure, so if you have such a large mass, the Earth, it'll have to have an insignificant velocity, essentially, when your tiny mass moves at the given velocity. |
| May26-08, 06:26 PM | #5 |
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So what about that I can walk from rest? How is the momentum conserved here?
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| May26-08, 06:31 PM | #6 |
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Mentor
Blog Entries: 1
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| May26-08, 06:32 PM | #7 |
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When you walk, you push against the earth. Theoretically, this gives it a very slight velocity in the opposite direction, but it's too small to be detected.
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| May26-08, 07:27 PM | #8 |
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here is another way to think about it. think of someone driving a car. the car has momentum. when the car comes to a stop at a stop sign, all the momentum in the car is pushed into the road. this is why you frequently see ripples in the road at places where there are frequent stops. all the momentum must go somehwere so it goes into pushing up the road. momentum is always conserved
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| May26-08, 09:25 PM | #9 |
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![]() Hint: [tex]m_ev_{e,1}+m_pv_{p,1}=m_ev_{e,2}+m_pv_{p,2}[/tex] Do some algebraic manipulation and get this" [tex]v_{1,e}-\frac{m_pv_{p,2}}{M_e}=v_{e,2}[/tex] Now, how did you deduce the earth moves "in the opposite direction?" Something should have yelled to you, wait a minute, that doesnt make sense by the sound of what I just wrote. |
| May26-08, 11:02 PM | #10 |
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Actually, I'm not sorry. You're just an annoying nitpicker. And how do you propose to measure the motion of the earth due to a person walking around upon it? |
| May26-08, 11:04 PM | #11 |
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The initial velocity of the person was set to zero as part of the algebraic manipulation.
Please explain how the earth goes in the 'opposite direction'. |
| May26-08, 11:05 PM | #12 |
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Cyrus,
Ah, I see your point now. I didn't see it at first. Your point is still stupid. I have to specify that the earth is moving before I take a step? Why? What absolute reference frame are you using? |
| May26-08, 11:18 PM | #13 |
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| May26-08, 11:54 PM | #14 |
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Mentor
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Particularly when you are wrong. |
| May27-08, 12:00 AM | #15 |
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If (for an elastic collision) momentum of a ball incident upon a wall is equal and opposite to its resultant momentum, would it be correct to assert that the mass and rigidity of the wall approach infinity?
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| May27-08, 12:01 AM | #16 |
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Ok, sorry if I was rude.
DH, I read what they wrote. They were using a reference frame of the earth being stationary, I did not. In the case where its not stationary, the earth does NOT move backwards. I just showed this using the simple conservation of momentum equation. I have no problems with you stating im wrong, but then show me where my equation is incorrect. |
| May27-08, 12:10 AM | #17 |
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Mentor
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The three conservation laws are related through Noether's theorem. Some quantity is conserved for a system in which the Lagrangian exhibits a symmetry. Energy is conserved if the Lagrangian is temporally symmetric. Linear momentum is conserved if the Lagrangian is symmetric with respect to position. Angular momentum is conserved if the Lagrangian is rotationally symmetric. |
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