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| Tags: basis, relativity |
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#1
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relativity is based on the equivalent principle,
then the developed relativity shows that the equivalent principle is wrong |
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#2
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Neil G wrote:
relativity is based on the equivalent principle, then the developed relativity shows that the equivalent principle is wrong You misunderstand. The equivalence principle states that given a dynamic gravitational field ("real force") in a given geometry you can alter the geometry and alter the dynamic force to yield an equivalent predictive theory. Given this then you can *by convention* choose a geometry in which the dynamic force goes away and in that choice of geometry the gravitational force is just geodesic evolution. It is similar to saying you can set "zero electrostatic potential" to be at any point you like. When doing problems you set the ground of your device to be at zero volts. That is another "relativity principle" namely that voltage is relative and thus it is only meaningful to speak of voltage differences. Setting the ground to be zero volts does not mean the original relativity is wrong, it rather relies implicitly on the relativity principle being right. Otherwise you'd have to worry about whether the ground is "really at zero volts". These choices of convention are loosly refered to as "gauge conditions". There is a deep connection between "equivalence principles" and gauge theories. One is effectively considering a whole class of equivalent models with an explicit group of equivalence transformations (the gauge group). One then insists that physical phenomena which one may predict be independent of the choice of model (choice of gauge). This is how Einstein formulated his field equations. Note however that in the case of gravitation the purely geometric formulation leads some to take geometry too seriously as a physical quality instead of a feature of the formal language. Hence attempts to quantize gravitation by "quantizing geometry". This I believe to be the major flaw of quantum string and 'brane' models inaccurately refered to as "theories". -- Regards, James Baugh |
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#3
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Baugh wrote: Neil G wrote: relativity is based on the equivalent principle, then the developed relativity shows that the equivalent principle is wrong You misunderstand. The equivalence principle states that given a dynamic gravitational field ("real force") in a given geometry you can alter the geometry and alter the dynamic force to yield an equivalent predictive theory. are the "real forces" considered "dynamic gravitational fields"? I thought that there was a huge difference between gravitational and a Newtonian force Given this then you can *by convention* choose a geometry in which the dynamic force goes away and in that choice of geometry the gravitational force is just geodesic evolution. "geodesic evolution" means no Newtonian forces? It is similar to saying you can set "zero electrostatic potential" to be at any point you like. When doing problems you set the ground of your device to be at zero volts. That is another "relativity principle" namely that voltage is relative and thus it is only meaningful to speak of voltage differences. thanks, but I still can't see the connection between the two forces Setting the ground to be zero volts does not mean the original relativity is wrong, it rather relies implicitly on the relativity principle being right. Otherwise you'd have to worry about whether the ground is "really at zero volts". you sounds convincing, but I still can't understand These choices of convention are loosly refered to as "gauge conditions". There is a deep connection between "equivalence principles" and gauge theories. One is effectively considering a whole class of equivalent models with an explicit group of equivalence transformations (the gauge group). One then insists that physical phenomena which one may predict be independent of the choice of model (choice of gauge). I think I begin to understand, thanks This is how Einstein formulated his field equations. Note however that in the case of gravitation the purely geometric formulation leads some to take geometry too seriously as a physical quality instead of a feature of the formal language. Hence attempts to quantize gravitation by "quantizing geometry". This I believe to be the major flaw of quantum string and 'brane' models inaccurately refered to as "theories". -- Regards, James Baugh I understand now, so the "forces" are actually the same type of forces depending on one's point of view, thanks |
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#4
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Baugh wrote:
Note however that in the case of gravitation the purely geometric formulation leads some to take geometry too seriously as a physical quality instead of a feature of the formal language. Hence attempts to quantize gravitation by "quantizing geometry". This I believe to be the major flaw of quantum string and 'brane' models inaccurately refered to as "theories". Don't Feynman lattice spacetimes quantize spacetime also? Isn't the idea of the Planck distance effectively a quantizing of spacetime. I don't think string theory is unique by doing this. Has David Finkelstein told you anything about Tony Smith, a former grad student of his. Smith loves Clifford Algebra just like Finkelstein does. Smith's model kind of looks like bosonic string theory from the top down and SU(5) GUT from the bottom up. John |
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#5
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Neil G wrote:
relativity is based on the equivalent principle, then the developed relativity shows that the equivalent principle is wrong Nice posting. You make an ignorant statement about relativity, then assert that your statement is supported by experiments that you don't cite. With all due respect, you shouldn't be posting here. **** off!!!!! John Anderson |
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#6
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Nice posting. You make an ignorant statement about relativity, then
assert that your statement is supported by experiments that you don't cite. With all due respect, you shouldn't be posting here. **** off!!!!! John Anderson will you ever come with some comments regarding the post you fokin imbecile? do your best, pussy |
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#7
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Let me clearify further. My analogy with regard to electrostatic
potential was aimed at the point of the relativity being broken by fixing an aspect of the theory by convention. This was in response to your claim that the theory contradicted itself in its practice. With regard to the theory of gravity as I described it. The point is that the equivalence principle states that you can either treat gravity as a "real" force or as a pseudo-force or as a hybrad of the two. You can't distinguish between a "real" gravitational force and a pseudo-force due to curvature. (curving time coordinates is equivalent to accelerating the frame.) It is not completely correct to say gravity is "just geometry" rather one should say gravity is indistinguishable from geometry. It is a subtile but possibly important distinction. Take some solution to Einstein's equations, then perturb the geometry but at the same time "add by hand" an additional field of forces in such a way that the combination predicts particles will follow the original paths. You have the same theory with slightly changed metaphysical interpertation. Since it is redundant it is just as well to only work with purely geometric form. But it is by no means an affirmation of metaphysical facts. You can look at the perturbative analysis of gravity waves as an example of a hybrid description of both geometric and dynamic components to the gravitational field. You can also look at it as simply "all geometry" but treated perturbatively which is the usual "interpretation". The point is that neither "interpretation" is a true interpretation. The true interpretation is that test particles will go "that-a-way" in the presence of matter distributions as predicted by the theory. Neil G wrote: Baugh wrote: Neil G wrote: relativity is based on the equivalent principle, then the developed relativity shows that the equivalent principle is wrong You misunderstand. The equivalence principle states that given a dynamic gravitational field ("real force") in a given geometry you can alter the geometry and alter the dynamic force to yield an equivalent predictive theory. are the "real forces" considered "dynamic gravitational fields"? I thought that there was a huge difference between gravitational and a Newtonian force Given this then you can *by convention* choose a geometry in which the dynamic force goes away and in that choice of geometry the gravitational force is just geodesic evolution. "geodesic evolution" means no Newtonian forces? It is similar to saying you can set "zero electrostatic potential" to be at any point you like. When doing problems you set the ground of your device to be at zero volts. That is another "relativity principle" namely that voltage is relative and thus it is only meaningful to speak of voltage differences. thanks, but I still can't see the connection between the two forces Setting the ground to be zero volts does not mean the original relativity is wrong, it rather relies implicitly on the relativity principle being right. Otherwise you'd have to worry about whether the ground is "really at zero volts". you sounds convincing, but I still can't understand These choices of convention are loosly refered to as "gauge conditions". There is a deep connection between "equivalence principles" and gauge theories. One is effectively considering a whole class of equivalent models with an explicit group of equivalence transformations (the gauge group). One then insists that physical phenomena which one may predict be independent of the choice of model (choice of gauge). I think I begin to understand, thanks This is how Einstein formulated his field equations. Note however that in the case of gravitation the purely geometric formulation leads some to take geometry too seriously as a physical quality instead of a feature of the formal language. Hence attempts to quantize gravitation by "quantizing geometry". This I believe to be the major flaw of quantum string and 'brane' models inaccurately refered to as "theories". -- Regards, James Baugh I understand now, so the "forces" are actually the same type of forces depending on one's point of view, thanks -- Regards, James Baugh |
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#8
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Baugh wrote: Let me clearify further. My analogy with regard to electrostatic potential was aimed at the point of the relativity being broken by fixing an aspect of the theory by convention. This was in response to your claim that the theory contradicted itself in its practice. With regard to the theory of gravity as I described it. The point is that the equivalence principle states that you can either treat gravity as a "real" force or as a pseudo-force or as a hybrad of the two. You can't distinguish between a "real" gravitational force and a pseudo-force due to curvature. (curving time coordinates is equivalent to accelerating the frame.) It is not completely correct to say gravity is "just geometry" rather one should say gravity is indistinguishable from geometry. It is a subtile but possibly important distinction. Take some solution to Einstein's equations, then perturb the geometry but at the same time "add by hand" an additional field of forces in such a way that the combination predicts particles will follow the original paths. You have the same theory with slightly changed metaphysical interpertation. Since it is redundant it is just as well to only work with purely geometric form. But it is by no means an affirmation of metaphysical facts. Just a quick input James, been following your posts and I think you're quite smart! You can look at the perturbative analysis of gravity waves as an example of a hybrid description of both geometric and dynamic components to the gravitational field. You can also look at it as simply "all geometry" but treated perturbatively which is the usual "interpretation". The point is that neither "interpretation" is a true interpretation. The true interpretation is that test particles will go "that-a-way" in the presence of matter distributions as predicted by the theory. S Weinberg's writes similiar to James about geometrization of gravitation, and I rarely disagree with SW. however, we have extreme experimental evidence that only 3 spatial dimensions (by testing freedom of movement) exist. Also, that movement requires a real time. I respect James and SW's open mindness but I regard that as a dangerous philosophy. It is dismissive of operations in curved 4D, as being real. We've worked hard to define spacetime and we've measured carefully the effects of gravity on light, like deflection, Shapiro, Pound-Rebka, etc...where light defines our viewpoint. For those reasons, there is no way I'll reconsider the idea of spacetime being an imaginary frame for solving physics problems, spacetime is real. Personally, I don't buy the idea of a slow divorce from reality to suck up some math, on the contrary I would have the logic of math confirmed by Nature, and not the other way around to fit our fantasies...keep that going and we're back to the idiot Catholics who decided creation happened in 4004 BC, and a lot more dummy poop the pope sells to flockies. I meant that paragraph to be severe, because science must retain a firm foot in measureable reality. Everyone reading this post has access to a clock and ruler, and thus we all share spacetime, that non-negotiable. Regards Ken S. Tucker PS: Once again I think Mr. Baugh posts well. |
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#9
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"Baugh" wrote in message ... Let me clearify further. My analogy with regard to electrostatic potential was aimed at the point of the relativity being broken by fixing an aspect of the theory by convention. This was in response to your claim that the theory contradicted itself in its practice. With regard to the theory of gravity as I described it. The point is that the equivalence principle states that you can either treat gravity as a "real" force or as a pseudo-force or as a hybrad of the two. You can't distinguish between a "real" gravitational force and a pseudo-force due to curvature. (curving time coordinates is equivalent to accelerating the frame.) It is not completely correct to say gravity is "just geometry" rather one should say gravity is indistinguishable from geometry. It is a subtile but possibly important distinction. Take some solution to Einstein's equations, then perturb the geometry but at the same time "add by hand" an additional field of forces in such a way that the combination predicts particles will follow the original paths. Baugh I must admit I find your responses fascinating, a bit different, and insightful. Often I read them and think I am not so sure about that - then I think a bit more and say he has a point. But with regard to the above even after thinking about it a bit I am not so sure. I am thinking of Kretchmans objections to the principle of general covariance - he showed it had no physical basis - any law can be put in covariant form Which is why we need to add in the requirement of invariance - namely all the absolute terms appearing in the equations remain unchanged (Ohanian - Gravitation and Space-Time - page 374). Doing what you suggest would seem to violate this requirement - or am I missing something? Thanks Bill You have the same theory with slightly changed metaphysical interpertation. Since it is redundant it is just as well to only work with purely geometric form. But it is by no means an affirmation of metaphysical facts. You can look at the perturbative analysis of gravity waves as an example of a hybrid description of both geometric and dynamic components to the gravitational field. You can also look at it as simply "all geometry" but treated perturbatively which is the usual "interpretation". The point is that neither "interpretation" is a true interpretation. The true interpretation is that test particles will go "that-a-way" in the presence of matter distributions as predicted by the theory. Neil G wrote: Baugh wrote: Neil G wrote: relativity is based on the equivalent principle, then the developed relativity shows that the equivalent principle is wrong You misunderstand. The equivalence principle states that given a dynamic gravitational field ("real force") in a given geometry you can alter the geometry and alter the dynamic force to yield an equivalent predictive theory. are the "real forces" considered "dynamic gravitational fields"? I thought that there was a huge difference between gravitational and a Newtonian force Given this then you can *by convention* choose a geometry in which the dynamic force goes away and in that choice of geometry the gravitational force is just geodesic evolution. "geodesic evolution" means no Newtonian forces? It is similar to saying you can set "zero electrostatic potential" to be at any point you like. When doing problems you set the ground of your device to be at zero volts. That is another "relativity principle" namely that voltage is relative and thus it is only meaningful to speak of voltage differences. thanks, but I still can't see the connection between the two forces Setting the ground to be zero volts does not mean the original relativity is wrong, it rather relies implicitly on the relativity principle being right. Otherwise you'd have to worry about whether the ground is "really at zero volts". you sounds convincing, but I still can't understand These choices of convention are loosly refered to as "gauge conditions". There is a deep connection between "equivalence principles" and gauge theories. One is effectively considering a whole class of equivalent models with an explicit group of equivalence transformations (the gauge group). One then insists that physical phenomena which one may predict be independent of the choice of model (choice of gauge). I think I begin to understand, thanks This is how Einstein formulated his field equations. Note however that in the case of gravitation the purely geometric formulation leads some to take geometry too seriously as a physical quality instead of a feature of the formal language. Hence attempts to quantize gravitation by "quantizing geometry". This I believe to be the major flaw of quantum string and 'brane' models inaccurately refered to as "theories". -- Regards, James Baugh I understand now, so the "forces" are actually the same type of forces depending on one's point of view, thanks -- Regards, James Baugh |
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#10
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Baugh wrote:
With regard to the theory of gravity as I described it. The point is that the equivalence principle states that you can either treat gravity as a "real" force or as a pseudo-force or as a hybrad of the two. You can't distinguish between a "real" gravitational force and a pseudo-force due to curvature. (curving time coordinates is equivalent to accelerating the frame.) It's actually the connection, not the curvature, that is related to "gravitational force". Take some solution to Einstein's equations, then perturb the geometry but at the same time "add by hand" an additional field of forces in such a way that the combination predicts particles will follow the original paths. In general you cannot do that over a finite region. You can always do it at a single point, but that's not sufficient for your needs here. Tom Roberts |
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