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Newton's Third Law |
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| Mar14-04, 02:27 PM | #35 |
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Newton's Third Law |
| Mar14-04, 02:31 PM | #36 |
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| Mar14-04, 02:44 PM | #37 |
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| Mar14-04, 02:52 PM | #38 |
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You are completely wrong. What I am asking about is whether there is a causual relationship between the force that A exerts on B and the force B exterts on A. In your explanation there is no causual relation between A and B because the fact that A causes B to move has nothing to do with the fact that B applies an equal and opposite force on A. The only forces producing any kind of movement on B are forces external to B. This is physics 101. |
| Mar14-04, 02:55 PM | #39 |
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| Mar14-04, 02:56 PM | #40 |
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Essentially, you are assuing that a theory's congruence with experiment is suffcient evidence to establish its ontological validity. There are many examples that disprove this view. The most obvious of which is the fact that [from the point of view of the physics community] SR established that Newtonian mechanics does not give accurate predictions at high velocities. I really don't want to get off the topic but this need to be addressed. |
| Mar14-04, 02:58 PM | #41 |
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Why does this basic fact of physics confuse you so much? Have you asked your mom, dad, or one of your teachers to try explaining it to you? |
| Mar14-04, 03:04 PM | #42 |
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It shouldn't matter and you shouldn't need to explain macroscopic things through appeal to the microscopic level. I will be up front with you. I am a Buddhist and there are many things I could bring up that are confirmed experimentally in Buddhism. The reason I don't bring them up is that you are not a Buddhist and my introducing these ideas would be paramount to a Christian quoting the Bible. I am arguing my case purely on logical grounds. My not accepting your introduction of experimental evidence is not a cheap ploy to ignore something that refutes my points. I just don't accept it in the same way you don't accept the experimental results of my view. I think QM is wrong ontologically, although I said it is certainly valueable in so far as it can make correct experimental predictions. If two people are going to debate there needs to be a common accepted ground of terminology. Otherwise, for one, either person could simply make up stuff. Therefore, I hope that we can debate this on the macroscopic level since this post in under classical physics. |
| Mar14-04, 03:08 PM | #43 |
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| Mar14-04, 03:09 PM | #44 |
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I am asking is there a casual relationship between the forces A and B each exert on one another. |
| Mar14-04, 03:14 PM | #45 |
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In addition, there are many refutations of QM in Buddhist literature. The fact is if you can't argue this on classical grounds then you really don't understand it. The reality of the small can not negate the reality of the large. If you are not going to argue this way then then you might as well just leave the argument to those of us who can. |
| Mar14-04, 03:15 PM | #46 |
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| Mar14-04, 03:16 PM | #47 |
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[p-->q]^(~q)-->~p or some such like. It is not possble to argue a case based on "pure logic". Premises have to be chosen to fill in those logical variables, and those premises are bound to be reflective of your worldview. |
| Mar14-04, 04:54 PM | #48 |
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Because this thread has gotten so far off topic, I have split off the philosophical discussion into a thread called Ontology and Logic, located in the Metaphysics and Epistemology Forum.
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| Mar24-04, 12:34 AM | #49 |
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Zero posted:
"When A hits B, does A change speed or direction? Yes. Does B change speed or direction? Yes. Therefore, the speed and direction of A are causally linked to B, and the speed and direction of B are both causally linked to A." What if A & B are charged particles that interact only through their coulomb fields? Suppose that A is suddenly and breifly pushed toward B by some third force. A immediately experiences a new force from B. But B won't experience any change in force for a time x/c where is x is the distance between A & B, and c is the speed of light. It seems that in this case, the force that B exerts on A could be causing the force that A exerts on B, since the B on A force happens first. And during the time interval x/c, the total momentum of A & B is not conserved. Newton didn't know about charged particles and the fact that they're interaction travels at finite speed. But he knew a bit about massive particles that interact through gravity. He defended the absolute validity of his 3rd law by assuming the speed of the gravity interaction was infinite. So the true "classical" answer to this question of whether the force that one of two interacting particles exerts on the other causes the force that the other exerts seems to be no. The interaction appears at the same instant at each one, so neither one could cause the other. The real truth, however, seems to be that the force on the one that moves first is the causer. |
| Mar24-04, 02:31 AM | #50 |
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You mentioned a while back the connection between the 3rd law and momentum conservation. You're right that mechanical momentum conservation requires it, but there are no known forces which actually enforce mechanical momentum conservation!
There are explicit examples in textbooks showing that electromagnetism does not always obey the 3rd law for example. Of course we still like to say that momentum is conserved, but we define it more generally (using the translation invariance that was mentioned above). When you do that, you obtain that the fields themselves carry momentum (and energy). So the sum of the field momentum+mechanical momentum is conserved, but not the mechanical momentum alone. |
| Mar25-04, 03:47 AM | #51 |
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There is probably a better example of Newton's Third Law being violated by classical particles.
Consider two protons. One is travelling North, the other travelling West. Both travel along the same plane. At some point their paths will cross. Let us suppose that Proton A reaches the crossing point first. When Proton B reaches the crossing point, it will exert a magnetic force on Proton A. But Proton A will not exert a force on Proton B, because Proton B is positioned along the path Proton A is travellling. Of course, the problem here is the time delay in which the electromagnetic force propagates. This problem is similar to the whirled string problem, I suppose. |
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