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http://www.pitt.edu/~jdnorton/teachi...ity/index.html
John Norton (the cleverest Einsteinian): "If one has a disk in special relativity, the geometry of its surface is Euclidean. Say it is ten feet in diameter. That means that we can lay 10 foot long rulers across a diameter. The circumference is pi x 10 feet, which is about 31 feet. That means that we traverse the full circumference by laying 31 rulers round the outer rim of the disk. What if this disk is in rapid uniform rotation and we repeat the measurements? The same ten rulers will measure the diameter. The motion of the disk is always perpendicular to the rulers, so their length is unaffected. That is not so for the rulers laid along the circumference. They lie in the direction of rapid motion. As a result, they shorten and more are needed to cover the full circumference of the disk. The upshot is that we measure the circumference of the disk to be greater than 31 feet, the Euclidean value. In other words, we find that the geometry of is not Euclidean. The circumference of the disk is more than 2pi times its radius. The significance of this thought experiment was great. Through his principle of equivalence, Einstein had found that linear acceleration produces a gravitational field. Now he found that another sort of acceleration, rotation, produces geometry that is not Euclidean." In 1902, in "La Science et l'hypothèse", Henri Poincaré, in order to justify non-Euclidean geometries, presented a parabole. Bidimensional creatures live on a disk. The disk is heated under its center so that the temperature is high at the center and decreases towards the periphery. The creatures use rigid measuring rods in order to determine the geometry of their world. They know nothing about the heater and accordingly discover that the ratio of the circumference and the diameter is greater than pi. The creatures conclude that Euclidean geometry cannot be true on the disk. Albert the Plagiarist and John Norton, the cleverest Einsteinian, are forced to distort the concept of Divine Albert's Divine Length Contraction (rulers do undergo length contraction but parts of the disk covered by them do not) in order to appropriate Poincaré's result. Pentcho Valev |
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John Norton, the cleverest Einsteinan, and his sillier brothers
Einsteinians could solve the famous twin paradox by using the rotating disk: http://www.amazon.com/Relativity-Its.../dp/0486406768 "Relativity and Its Roots" by Banesh Hoffmann, Chapter 5. (I do not have the text in English so I am giving it in French) Banesh Hoffmann, "La relativite, histoire d'une grande idee", Pour la Science, Paris, 1999, p. 126: "Dans un cas, je compare votre horloge a deux des miennes; dans l'autre, vous comparez la mienne a deux des votres; ceci permet a chacun de nous d'observer, sans absurdite, que l'horloge de l'autre est plus lente que la sienne." Translation from French: "In one case, I compare your clock with two of mine; in the other case, you compare my clock with two of yours: this allows each of us to observe, without absurdity, that the clock of the other is slower than his own." The observer referred to by Einstein in the following quotation has two clocks placed on the periphery of a rotating disc, and is going to compare them with a single non-rotating clock (at rest): http://www.bartleby.com/173/23.html Albert Einstein (1879-1955). Relativity: The Special and General Theory. 1920. XXIII. Behaviour of Clocks and Measuring Rods on a Rotating Body of Reference: "An observer who is sitting eccentrically on the disc K' is sensible of a force which acts outwards in a radial direction..." The only difficulty comes from the fact that the two rotating clocks are not inertial. However, by increasing the diameter of the disc while keeping the linear speed of the periphery constant, one can make them virtually inertial. That is, John Norton, the cleverest Einsteinan, and his sillier brothers Einsteinians will make two simple modifications in Einstein's rotating-disc experiment: 1. The non-rotating clock (at rest in K) is no longer placed at the center of the disc; rather, it is outside the disc but close to the rotating periphery where it can be directly compared with passing rotating clocks fixed on the periphery. 2. John Norton, the cleverest Einsteinan, and his sillier brothers Einsteinians will increase the diameter of the disc while keeping the linear speed of the periphery constant. So clocks fixed on the rotating periphery will become virtually inertial. The two modifications will allow John Norton, the cleverest Einsteinan, and his sillier brothers Einsteinians to prove, in accordance with Einstein's 1905 light postulate, both: 1. that rotating clocks run slower than non-rotating clocks. 2. that non-rotating clocks run slower than rotating clocks. Finally, John Norton, the cleverest Einsteinan, and his sillier brothers Einsteinians will see in the dictionary what REDUCTIO AS ABSURDUM means. They may even discover that time dilation is just as absurd as length contraction: http://hyperphysics.phy-astr.gsu.edu.../bugrivet.html Pentcho Valev |
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Slowly but surely the world will realize that the glorious "paradoxes"
that converted Albert the Plagiarist into Divine Albert are in fact absurdities and even idiocies: http://www.personal.leeds.ac.uk/~phl...%20Meeting.htm "Is Frisch right in saying that `theories do not have a tight deductive structure`?.....Are these scientific conflicts and paradoxes cases of inconsistency as logicians understand the term?" Pentcho Valev |
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On Jun 17, 7:22 am, Pentcho Valev wrote:
Slowly but surely the world will realize that the glorious "paradoxes" that converted Albert the Plagiarist into Divine Albert are in fact absurdities and even idiocies: http://www.personal.leeds.ac.uk/~phl...%20Meeting.htm "Is Frisch right in saying that `theories do not have a tight deductive structure`?.....Are these scientific conflicts and paradoxes cases of inconsistency as logicians understand the term?" Pentcho Valev yes |
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On Tue, 17 Jun 2008 04:33:48 -0700 (PDT), Pentcho Valev
wrote: http://hyperphysics.phy-astr.gsu.edu.../bugrivet.html I'd say the solution to this paradox is to distinguish between two kinds of length contraction as follows: I. Suppose the bug and its hole are at rest in 3-space and that the rivet is moving. Then: 1) In the frame of the bug, the Lorentz transform of the length of the rivet represents a genuine length contraction. 2) In the frame of the rivet, the Lorentz transform of the depth of the hole represents only an apparent length contraction--necessary to keep calculations consistent. So the bug is safe in this case. II. Suppose the rivet is at rest in 3-space and the bug and its hole are moving. In this case, the situation is reversed and the bug gets squashed. III. Suppose the bug and rivet are both moving through 3-space. Then: 1) In the frame of the bug, the Lorentz transform of the length of the rivet represents a length contraction that is part genuine and part only apparent. 2) Ditto for the Lorentz transform for the depth of the hole in the frame of the rivet. So in this case the outcome would depend on which is moving faster through 3-space. I don't see any way to resolve this paradox with the spacetime concept. -- Surfer Pentcho Valev |
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On 17 Jun, 08:33, Pentcho Valev wrote:
http://www.pitt.edu/~jdnorton/teachi...s/general_rela... John Norton (the cleverest Einsteinian): "If one has a disk in special relativity, the geometry of its surface is Euclidean. Say it is ten feet in diameter. That means that we can lay 10 foot long rulers across a diameter. The circumference is pi x 10 feet, which is about 31 feet. That means that we traverse the full circumference by laying 31 rulers round the outer rim of the disk. What if this disk is in rapid uniform rotation and we repeat the measurements? The same ten rulers will measure the diameter. The motion of the disk is always perpendicular to the rulers, so their length is unaffected. That is not so for the rulers laid along the circumference. They lie in the direction of rapid motion. As a result, they shorten and more are needed to cover the full circumference of the disk. The upshot is that we measure the circumference of the disk to be greater than 31 feet, the Euclidean value. In other words, we find that the geometry of is not Euclidean. The circumference of the disk is more than 2pi times its radius. The significance of this thought experiment was great. Through his principle of equivalence, Einstein had found that linear acceleration produces a gravitational field. Now he found that another sort of acceleration, rotation, produces geometry that is not Euclidean." In 1902, in "La Science et l'hypothèse", Henri Poincaré, in order to justify non-Euclidean geometries, presented a parabole. Bidimensional creatures live on a disk. The disk is heated under its center so that the temperature is high at the center and decreases towards the periphery. The creatures use rigid measuring rods in order to determine the geometry of their world. They know nothing about the heater and accordingly discover that the ratio of the circumference and the diameter is greater than pi. The creatures conclude that Euclidean geometry cannot be true on the disk. Albert the Plagiarist and John Norton, the cleverest Einsteinian, are forced to distort the concept of Divine Albert's Divine Length Contraction (rulers do undergo length contraction but parts of the disk covered by them do not) *in order to appropriate Poincaré's result. All the relativity paradoxes result in making assumptions at one point about perfect rigidity. Relativity limits rigidity, the speed of sound cannot exceed that of light. This is no exception. A disc moving at relativistic speed will expand because it is elastic. The fucticious light inextensible string must in a relativistic context have a speed of sound = c. In point of fact in real life (the non ideal case) odd things happen when we exceed the speed of sound NOT light. Odd point - a civil war bullet (slower than sound in water) travells further in water than high velocity bullets which all disintegrate. - Ian Parker |
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Ian Parker wrote:
All the relativity paradoxes result in making assumptions at one point about perfect rigidity. Assumptions? perfect rigiidity is what you use to determine a straight line for accurate measurements and without such perfect rigidity and "physical measurements", there is no "physical proof". You have bendy lightwave proof only in anything that uses light beams to measure stuff that is all messed up with gravity and curving of the light. you have a rubber ruler nothing more. ![]() Relativity limits rigidity, the speed of sound cannot exceed that of light. This is no exception. A disc moving at relativistic speed will expand because it is elastic. The fucticious light inextensible string must in a relativistic context have a speed of sound = c. Yes, limit rigidity so the "theory" can not be wrong to itself". ![]() In point of fact in real life (the non ideal case) odd things happen when we exceed the speed of sound NOT light. Very true, but not odd enough that classical stuff, when done correctly, does show "how" it all happens like such. ![]() Odd point - a civil war bullet (slower than sound in water) travells further in water than high velocity bullets which all disintegrate. slow and efficient.. wins the race.. the turtles are everywhere! LOL -- James M Driscoll Jr Spaceman |
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On Jun 17, 12:39*pm, "Spaceman"
wrote: Ian Parker wrote: All the relativity paradoxes result in making assumptions at one point about perfect rigidity. Assumptions? perfect rigiidity is what you use to determine a straight line for accurate measurements and without such perfect rigidity and "physical measurements", there is no "physical proof". You have bendy lightwave proof only in anything that uses light beams to measure stuff that is all messed up with gravity and curving of the light. you have a rubber ruler nothing more. ![]() Relativity limits rigidity, the speed of sound cannot exceed that of light. This is no exception. A disc moving at relativistic speed will expand because it is elastic. The fucticious light inextensible string must in a relativistic context have a speed of sound = c. Yes, limit rigidity so the "theory" can not be wrong to itself". ![]() In point of fact in real life (the non ideal case) odd things happen when we exceed the speed of sound NOT light. Very true, but not odd enough that classical stuff, when done correctly, does show "how" it all happens like such. ![]() Odd point - a civil war bullet (slower than sound in water) travells further in water than high velocity bullets which all disintegrate. slow and efficient.. wins the race.. the turtles are everywhere! LOL -- James M Driscoll Jr Spaceman Actually, the answer is 42. Harry C. |
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On Jun 17, 3:44*pm, john wrote:
On Jun 17, 7:22 am, Pentcho Valev wrote: Slowly but surely the world will realize that the glorious "paradoxes" that converted Albert the Plagiarist into Divine Albert are in fact absurdities and even idiocies: http://www.personal.leeds.ac.uk/~phl...%20Meeting.htm "Is Frisch right in saying that `theories do not have a tight deductive structure`?.....Are these scientific conflicts and paradoxes cases of inconsistency as logicians understand the term?" Pentcho Valev yes W. H. Newton-Smith, The rationality of science, Routledge, London, 1981, p. 229: "A theory ought to be internally consistent. The grounds for including this factor are a priori. For given a realist construal of theories, our concern is with verisimilitude, and if a theory is inconsistent it will contain every sentence of the language, as the following simple argument shows. Let ‘q’ be an arbitrary sentence of the language and suppose that the theory is inconsistent. This means that we can derive the sentence ‘p and not-p’. From this ‘p’ follows. And from ‘p’ it follows that ‘p or q’ (if ‘p’ is true then ‘p or q’ will be true no matter whether ‘q’ is true or not). Equally, it follows from ‘p and not-p’ that ‘not-p’. But ‘not-p’ together with ‘p or q’ entails ‘q’. Thus once we admit an inconsistency into our theory we have to admit everything. And no theory of verisimilitude would be acceptable that did not give the lowest degree of verisimilitude to a theory which contained each sentence of the theory’s language and its negation." The deduction performed by Newton-Smith is unacceptable to a physicist since « from ‘p’ it follows that ‘p or q’ » is not a mathematical deductive argument (see a definition of mathematical deductive argument in http://www.wbabin.net/philos/valev9.pdf ). Still the central idea – that the lowest degree of verisimilitude should be given to an inconsistency – is correct. Pentcho Valev |
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