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Paradox of Classical Mechanics   Message List  
Reply | Forward Message #189 of 208 |
Re: Paradox of Classical Mechanics

Let imagine observer and two objects (A and B). One object A with simple
movement can move only into one plane. The observer in own frame of reference
sees only this plane also.
Another object B with complicated movement can move in two planes and observer
can see only one of these planes.
The object A has position without movement for observer. The object B has a
movement. The object B has component velocity for each plane. However, observer
can see only one component velocity of objects B . The object A takes momentum
from object B after collision and objects A velocity may be higher than
inspected.
a. The observer can assume the object A has a huge mass. Or if observer knows
the object B mass then he can assume include dark matter for collision process.
b. If frame of reference base on law of momentum conservation then using all
know parameters easy to calculate another plane velocity component of object B
which is invisible for observer. This velocity component for observer has
imaginary character. From the other words, the frame of reference use law of
momentum conservation to readjust another object parameters.


A few words about movement without external forces. The object can rotate on own
center mass without external forces. However, if alternate simple and
complicated movement on object collisions then for observer frame of references
it may possible exchange rotation to translation movement.
Everything Is Relative.




Fri Jul 17, 2009 5:05 am

abelov0927
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Message #189 of 208 |
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http://knol.google.com/k/alex-belov/paradox-of-classical-mechanics-2/1xm\ qm1l0s4ys/9 <http://knol.google.com/k/alex-belov/paradox-of-classical-mechanics-2/1x\...
abelov0927
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Jul 3, 2009
8:34 pm

Hi. I think this is a clue for understanding. The element with zero values of linear velocity on the surface is too small. Base on math the geometrical size of...
abelov0927
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Jul 6, 2009
1:22 am

For this model, à repulsion and à collision comes on different planes. The vertical plane doesn't have any contacts with the rolling body. Otherwise the...
abelov0927
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Jul 11, 2009
8:19 pm

Quote from forum. "Follow by law of momentum conservation V0x(mx(n-1))=V1x(all mass) If discount one element from the ring then and average speed for (n-1) ...
abelov0927
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Jul 15, 2009
4:29 am

Let imagine observer and two objects (A and B). One object A with simple movement can move only into one plane. The observer in own frame of reference sees...
abelov0927
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Jul 17, 2009
6:10 pm

A few philosophy thinks. Collisions may be classified in two groups. Explicit and implicit. 1. Explicit collisions – happens between objects which conducts...
abelov0927
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Jul 17, 2009
6:10 pm

This is a good example is shown transfer between angular and linear momentums. Unfortunately the simulator does not allow giving different angular...
abelov0927
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Jul 20, 2009
10:21 pm

Another good example: Let's repulse a long cylinder inside Isolated System. The repulse should hit the cylinder away from object center mass. This hit energy...
abelov0927
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Jul 22, 2009
2:38 am

Let's solve simple problem. Given a long thin cylinder with length L, radius R and mass M. Case 1. This cylinder takes momentum P into his center mass. Case 2....
abelov0927
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Jul 25, 2009
1:41 am

These thoughts can be used for a rolling body. <http://knol.google.com/k/-/-/1xmqm1l0s4ys/h6o9ht/rollingfriction.jpg> The diagram has shown a rolling disk...
abelov0927
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Jul 8, 2009
8:37 pm

A rolling disk on a straight line surface. <http://knol.google.com/k/-/-/1xmqm1l0s4ys/h6o9ht/rollingfriction.jpg> The diagram has shown a rolling disk on...
abelov0927
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Jul 10, 2009
5:59 pm
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