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#71
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On Mar 16, 6:12 pm, "Shubee" wrote:
On Mar 16, 5:36 pm, wrote: On Mar 16, 5:06 pm, "Shubee" wrote: On Mar 16, 6:14 am, jem wrote: Shubee wrote: On Mar 15, 7:01 am, jem wrote: Shubee wrote: On Mar 14, 7:45 am, wrote: On Mar 14, 4:07 am, "Shubee" wrote: On Mar 13, 10:17 pm, "Eric Gisse" wrote: On Mar 13, 6:17 pm, "Shubee" wrote: Nonlinear transformations means that the homogenity of space and time is gone. That is only true in chimpanzee relativity. I certainly don't expect alpha male chimps to understand that. And it's obvious that you would have a harder time to learn that. You couldn't even figure out how Hilbert's sixth problem relates to the axiomatization of physics [0][1] [2][3]. If you ever evolve to the point of understanding my high school level formulation titled, The Axiomatization of Physics - Step 1: A Derivation of the Lorentz Transformation [4], you will then discover your mistake. Shubee 0.http://groups.google.com/group/sci.p...sg/fd7ad4b9e1b... 1.http://en.wikipedia.org/wiki/Hilbert%27s_problems 2.http://en.wikipedia.org/wiki/Hilbert's_sixth_problem 3.http://en.wikipedia.org/wiki/Wightman_axioms 4.http://www.everythingimportant.org/r...ty/special.pdf So, , prove that T(T^-1)=I where T is your "nonlinear transform function and I is the identy matrix. Put up or shut up. The transformation does have a group structure*, but it has no more significance than that. In particular, Shooby's claim that, for any function f, the group is "physically indistinguishable" from the Lorentz Group is, like most of what Shooby says, nonsense. * It's a bit easier to verify when the last term in the equation for t' is written as f(x'). Congratulations jem. It sounds like you convinced yourself of the correctness of the claim in exercise 1. You gave a very good hint. You make a very reasonable request. Let me give you a hint: To get the inverse of the nonlinear transformation in exercise 1 of http://www.everythingimportant.org/r...ized.htmmerely exchange x' with x, t' with t and v with -v. The problem is really much easier than it appears. Can you handle this problem, Shooby? Tell us what the constant v "physically" represents. Proper velocity u is defined by eq. (3) in The Axiomatization of Physics - Step 1 and has the clear physical interpretation presented there. In Shubertian physics, the parameter v is only a derived quantity, a function of the proper velocity. The ordinary velocity v is defined by eq. (40) inhttp://www.everythingimportant.org/relativity/special.pdf Bzzt! Sorry, Shooby, only when the function f is constant does v represent the "ordinary velocity" between the reference frames. Got another guess? jem, I don't have to guess. It's obvious that you don't understand my interpretation of equation (1) and equation (2) for the toy universe I call Xi_2. http://www.everythingimportant.org/r...ty/special.pdf Shubee I don't expect that any of my pompous critics could prove the group structure by doing the actual calculation directly but if Tom Roberts or any other capable physicist denies my group structure, then I would be happy to prove that these transformations form a group when I get some time. Note: If anyone wants to prove that my inverse doesn't work, then select any set of constants at random with any arbitrary function and compute the value of the function on those constants and the inverse function of the result. Prove you don't get back to where you started. http://www.everythingimportant.org/r...eneralized.htm Shubee Enough of your BS, calculate T*T^-1. Are you Ken Seto reicarnated? You seem to have the same DNA (idiotic theories and inability to calculate anything). Listen up karandash. Jem already told you that my transformations have a group structure. No he didn't. You are not only inept, you are also a bad liar. I strongly expect that most children who are competent in high school algebra can form the composition of those two functions. So why do you keep avoiding showing your calculations. I asked you about 8 times already : show that T*T^-1=I. Put up or shut the **** up. Even simpler, I figure that it only takes a middle school mathematician to evaluate my function on a random point and the inverse of the image to test my claim. So stop your desperate diversions and do it. If you can't do that yourself, then what are you doing here at sci.physics.relativity? Shubee I am telling you that you are full of ****, this is what I've been doing. Put up, or shut the **** up. |
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#72
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On Mar 16, 6:12 pm, "Shubee" wrote:
On Mar 16, 5:36 pm, wrote: On Mar 16, 5:06 pm, "Shubee" wrote: On Mar 16, 6:14 am, jem wrote: Shubee wrote: On Mar 15, 7:01 am, jem wrote: Shubee wrote: On Mar 14, 7:45 am, wrote: On Mar 14, 4:07 am, "Shubee" wrote: On Mar 13, 10:17 pm, "Eric Gisse" wrote: On Mar 13, 6:17 pm, "Shubee" wrote: Nonlinear transformations means that the homogenity of space and time is gone. That is only true in chimpanzee relativity. I certainly don't expect alpha male chimps to understand that. And it's obvious that you would have a harder time to learn that. You couldn't even figure out how Hilbert's sixth problem relates to the axiomatization of physics [0][1] [2][3]. If you ever evolve to the point of understanding my high school level formulation titled, The Axiomatization of Physics - Step 1: A Derivation of the Lorentz Transformation [4], you will then discover your mistake. Shubee 0.http://groups.google.com/group/sci.p...sg/fd7ad4b9e1b... 1.http://en.wikipedia.org/wiki/Hilbert%27s_problems 2.http://en.wikipedia.org/wiki/Hilbert's_sixth_problem 3.http://en.wikipedia.org/wiki/Wightman_axioms 4.http://www.everythingimportant.org/r...ty/special.pdf So, , prove that T(T^-1)=I where T is your "nonlinear transform function and I is the identy matrix. Put up or shut up. The transformation does have a group structure*, but it has no more significance than that. In particular, Shooby's claim that, for any function f, the group is "physically indistinguishable" from the Lorentz Group is, like most of what Shooby says, nonsense. * It's a bit easier to verify when the last term in the equation for t' is written as f(x'). Congratulations jem. It sounds like you convinced yourself of the correctness of the claim in exercise 1. You gave a very good hint. You make a very reasonable request. Let me give you a hint: To get the inverse of the nonlinear transformation in exercise 1 of http://www.everythingimportant.org/r...ized.htmmerely exchange x' with x, t' with t and v with -v. The problem is really much easier than it appears. Can you handle this problem, Shooby? Tell us what the constant v "physically" represents. Proper velocity u is defined by eq. (3) in The Axiomatization of Physics - Step 1 and has the clear physical interpretation presented there. In Shubertian physics, the parameter v is only a derived quantity, a function of the proper velocity. The ordinary velocity v is defined by eq. (40) inhttp://www.everythingimportant.org/relativity/special.pdf Bzzt! Sorry, Shooby, only when the function f is constant does v represent the "ordinary velocity" between the reference frames. Got another guess? jem, I don't have to guess. It's obvious that you don't understand my interpretation of equation (1) and equation (2) for the toy universe I call Xi_2. http://www.everythingimportant.org/r...ty/special.pdf Shubee I don't expect that any of my pompous critics could prove the group structure by doing the actual calculation directly but if Tom Roberts or any other capable physicist denies my group structure, then I would be happy to prove that these transformations form a group when I get some time. Note: If anyone wants to prove that my inverse doesn't work, then select any set of constants at random with any arbitrary function and compute the value of the function on those constants and the inverse function of the result. Prove you don't get back to where you started. http://www.everythingimportant.org/r...eneralized.htm Shubee Enough of your BS, calculate T*T^-1. Are you Ken Seto reicarnated? You seem to have the same DNA (idiotic theories and inability to calculate anything). Listen up karandash. Jem already told you that my transformations have a group structure. Why aren't you attacking him for agreeing with me?http://groups.google.com/group/sci.p...sg/b0907efe107... I strongly expect that most children who are competent in high school algebra can form the composition of those two functions. Why don't you learn high school math and do it yourself? Even simpler, I figure that it only takes a middle school mathematician to evaluate my function on a random point and the inverse of the image to test my claim. If you can't do that yourself, then what are you doing here at sci.physics.relativity? Shubee 1.Invert the **** that you write at point 1 in this link: http://www.everythingimportant.org/r...eneralized.htm Hint for ****head Shubert: only bijective functions have inverse. 2. Get the matrix of the inverse transformation 3. Calculate T*T^-1 |
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#73
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On Mar 16, 5:33 pm, "Shubee" wrote:
On Mar 16, 6:17 pm, "Eric Gisse" wrote: On Mar 16, 5:12 pm, "Shubee" wrote: [...] Why should anyone care about your approach, shooby? Special relativity is already axiomatic - you add nothing to the theory. Chimpanzee relativity fosters a few misconceptions and The Axiomatization of Physics - Step 1 fixes them all. Shubeehttp://www.everythingimportant.org/relativity/special.pdf But you didn't answer my question, shooby. Why should anyone care? |
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#74
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Shubee wrote:
On Mar 16, 6:14 am, jem wrote: Shubee wrote: On Mar 15, 7:01 am, jem wrote: Shubee wrote: On Mar 14, 7:45 am, wrote: On Mar 14, 4:07 am, "Shubee" wrote: On Mar 13, 10:17 pm, "Eric Gisse" wrote: On Mar 13, 6:17 pm, "Shubee" wrote: Nonlinear transformations means that the homogenity of space and time is gone. That is only true in chimpanzee relativity. I certainly don't expect alpha male chimps to understand that. And it's obvious that you would have a harder time to learn that. You couldn't even figure out how Hilbert's sixth problem relates to the axiomatization of physics [0][1] [2][3]. If you ever evolve to the point of understanding my high school level formulation titled, The Axiomatization of Physics - Step 1: A Derivation of the Lorentz Transformation [4], you will then discover your mistake. Shubee 0.http://groups.google.com/group/sci.p...sg/fd7ad4b9e1b... 1.http://en.wikipedia.org/wiki/Hilbert%27s_problems 2.http://en.wikipedia.org/wiki/Hilbert's_sixth_problem 3.http://en.wikipedia.org/wiki/Wightman_axioms 4.http://www.everythingimportant.org/r...ty/special.pdf So, , prove that T(T^-1)=I where T is your "nonlinear transform function and I is the identy matrix. Put up or shut up. The transformation does have a group structure*, but it has no more significance than that. In particular, Shooby's claim that, for any function f, the group is "physically indistinguishable" from the Lorentz Group is, like most of what Shooby says, nonsense. * It's a bit easier to verify when the last term in the equation for t' is written as f(x'). Congratulations jem. It sounds like you convinced yourself of the correctness of the claim in exercise 1. You gave a very good hint. You make a very reasonable request. Let me give you a hint: To get the inverse of the nonlinear transformation in exercise 1 of http://www.everythingimportant.org/r...eneralized.htm merely exchange x' with x, t' with t and v with -v. The problem is really much easier than it appears. Can you handle this problem, Shooby? Tell us what the constant v "physically" represents. Proper velocity u is defined by eq. (3) in The Axiomatization of Physics - Step 1 and has the clear physical interpretation presented there. In Shubertian physics, the parameter v is only a derived quantity, a function of the proper velocity. The ordinary velocity v is defined by eq. (40) in http://www.everythingimportant.org/r...ty/special.pdf Bzzt! Sorry, Shooby, only when the function f is constant does v represent the "ordinary velocity" between the reference frames. Got another guess? jem, I don't have to guess. It's obvious that you don't understand my interpretation of equation (1) and equation (2) for the toy universe I call Xi_2. You were asked what v represents in your transformation equations, and there isn't any need* to look beyond those equations for the answer. * other than the need to be evasive when you're asked a question whose answer you should know, but don't. http://www.everythingimportant.org/r...ty/special.pdf Shubee I don't expect that any of my pompous critics could prove the group structure by doing the actual calculation directly but if Tom Roberts or any other capable physicist denies my group structure, then I would be happy to prove that these transformations form a group when I get some time. Note: If anyone wants to prove that my inverse doesn't work, then select any set of constants at random with any arbitrary function and compute the value of the function on those constants and the inverse function of the result. Prove you don't get back to where you started. http://www.everythingimportant.org/r...eneralized.htm Shubee |
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#75
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On Mar 17, 5:40 am, jem wrote:
Shubee wrote: On Mar 16, 6:14 am, jem wrote: Shubee wrote: On Mar 15, 7:01 am, jem wrote: Shubee wrote: On Mar 14, 7:45 am, wrote: On Mar 14, 4:07 am, "Shubee" wrote: On Mar 13, 10:17 pm, "Eric Gisse" wrote: On Mar 13, 6:17 pm, "Shubee" wrote: Nonlinear transformations means that the homogenity of space and time is gone. That is only true in chimpanzee relativity. I certainly don't expect alpha male chimps to understand that. And it's obvious that you would have a harder time to learn that. You couldn't even figure out how Hilbert's sixth problem relates to the axiomatization of physics [0][1] [2][3]. If you ever evolve to the point of understanding my high school level formulation titled, The Axiomatization of Physics - Step 1: A Derivation of the Lorentz Transformation [4], you will then discover your mistake. Shubee 0.http://groups.google.com/group/sci.p...sg/fd7ad4b9e1b... 1.http://en.wikipedia.org/wiki/Hilbert%27s_problems 2.http://en.wikipedia.org/wiki/Hilbert's_sixth_problem 3.http://en.wikipedia.org/wiki/Wightman_axioms 4.http://www.everythingimportant.org/r...ty/special.pdf So, , prove that T(T^-1)=I where T is your "nonlinear transform function and I is the identy matrix. Put up or shut up. The transformation does have a group structure*, but it has no more significance than that. In particular, Shooby's claim that, for any function f, the group is "physically indistinguishable" from the Lorentz Group is, like most of what Shooby says, nonsense. * It's a bit easier to verify when the last term in the equation for t' is written as f(x'). Congratulations jem. It sounds like you convinced yourself of the correctness of the claim in exercise 1. You gave a very good hint. You make a very reasonable request. Let me give you a hint: To get the inverse of the nonlinear transformation in exercise 1 of http://www.everythingimportant.org/r...ized.htmmerely exchange x' with x, t' with t and v with -v. The problem is really much easier than it appears. Can you handle this problem, Shooby? Tell us what the constant v "physically" represents. Proper velocity u is defined by eq. (3) in The Axiomatization of Physics - Step 1 and has the clear physical interpretation presented there. In Shubertian physics, the parameter v is only a derived quantity, a function of the proper velocity. The ordinary velocity v is defined by eq. (40) inhttp://www.everythingimportant.org/relativity/special.pdf Bzzt! Sorry, Shooby, only when the function f is constant does v represent the "ordinary velocity" between the reference frames. Got another guess? jem, I don't have to guess. It's obvious that you don't understand my interpretation of equation (1) and equation (2) for the toy universe I call Xi_2. You were asked what v represents in your transformation equations, and there isn't any need* to look beyond those equations for the answer. * other than the need to be evasive when you're asked a question whose answer you should know, but don't. http://www.everythingimportant.org/r...ty/special.pdf Shubee I don't expect that any of my pompous critics could prove the group structure by doing the actual calculation directly but if Tom Roberts or any other capable physicist denies my group structure, then I would be happy to prove that these transformations form a group when I get some time. Note: If anyone wants to prove that my inverse doesn't work, then select any set of constants at random with any arbitrary function and compute the value of the function on those constants and the inverse function of the result. Prove you don't get back to where you started. http://www.everythingimportant.org/r...eneralized.htm Shubee I said very clearly that v is a function of the proper velocity. I also said that these equations describe simple inertial motion. If you proved the group structure, then you know that v adds like ordinary velocity does in chimpanzee relativity. Why isn't that good enough? http://groups.google.com/group/sci.p...3397d03512b7b0 |
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#76
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On Mar 17, 1:33 pm, "Shubee" wrote:
On Mar 17, 5:40 am, jem wrote: Shubee wrote: On Mar 16, 6:14 am, jem wrote: Shubee wrote: On Mar 15, 7:01 am, jem wrote: Shubee wrote: On Mar 14, 7:45 am, wrote: On Mar 14, 4:07 am, "Shubee" wrote: On Mar 13, 10:17 pm, "Eric Gisse" wrote: On Mar 13, 6:17 pm, "Shubee" wrote: Nonlinear transformations means that the homogenity of space and time is gone. That is only true in chimpanzee relativity. I certainly don't expect alpha male chimps to understand that. And it's obvious that you would have a harder time to learn that. You couldn't even figure out how Hilbert's sixth problem relates to the axiomatization of physics [0][1] [2][3]. If you ever evolve to the point of understanding my high school level formulation titled, The Axiomatization of Physics - Step 1: A Derivation of the Lorentz Transformation [4], you will then discover your mistake. Shubee 0.http://groups.google.com/group/sci.p...sg/fd7ad4b9e1b... 1.http://en.wikipedia.org/wiki/Hilbert%27s_problems 2.http://en.wikipedia.org/wiki/Hilbert's_sixth_problem 3.http://en.wikipedia.org/wiki/Wightman_axioms 4.http://www.everythingimportant.org/r...ty/special.pdf So, , prove that T(T^-1)=I where T is your "nonlinear transform function and I is the identy matrix. Put up or shut up. The transformation does have a group structure*, but it has no more significance than that. In particular, Shooby's claim that, for any function f, the group is "physically indistinguishable" from the Lorentz Group is, like most of what Shooby says, nonsense. * It's a bit easier to verify when the last term in the equation for t' is written as f(x'). Congratulations jem. It sounds like you convinced yourself of the correctness of the claim in exercise 1. You gave a very good hint. You make a very reasonable request. Let me give you a hint: To get the inverse of the nonlinear transformation in exercise 1 of http://www.everythingimportant.org/r...ized.htmmerely exchange x' with x, t' with t and v with -v. The problem is really much easier than it appears. Can you handle this problem, Shooby? Tell us what the constant v "physically" represents. Proper velocity u is defined by eq. (3) in The Axiomatization of Physics - Step 1 and has the clear physical interpretation presented there. In Shubertian physics, the parameter v is only a derived quantity, a function of the proper velocity. The ordinary velocity v is defined by eq. (40) inhttp://www.everythingimportant.org/relativity/special.pdf Bzzt! Sorry, Shooby, only when the function f is constant does v represent the "ordinary velocity" between the reference frames. Got another guess? jem, I don't have to guess. It's obvious that you don't understand my interpretation of equation (1) and equation (2) for the toy universe I call Xi_2. You were asked what v represents in your transformation equations, and there isn't any need* to look beyond those equations for the answer. * other than the need to be evasive when you're asked a question whose answer you should know, but don't. http://www.everythingimportant.org/r...ty/special.pdf Shubee I don't expect that any of my pompous critics could prove the group structure by doing the actual calculation directly but if Tom Roberts or any other capable physicist denies my group structure, then I would be happy to prove that these transformations form a group when I get some time. Note: If anyone wants to prove that my inverse doesn't work, then select any set of constants at random with any arbitrary function and compute the value of the function on those constants and the inverse function of the result. Prove you don't get back to where you started. http://www.everythingimportant.org/r...eneralized.htm Shubee I said very clearly that v is a function of the proper velocity. I also said that these equations describe simple inertial motion. If you proved the group structure, then you know that v adds like ordinary velocity does in chimpanzee relativity. Why isn't that good enough?http://groups.google.com/group/sci.p...sg/803397d0351... Hey, for once you are correct, your "paper" belongs to chimpanzee relativity. |
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#77
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Shubee wrote:
On Mar 17, 5:40 am, jem wrote: Shubee wrote: On Mar 16, 6:14 am, jem wrote: Shubee wrote: On Mar 15, 7:01 am, jem wrote: Shubee wrote: On Mar 14, 7:45 am, wrote: On Mar 14, 4:07 am, "Shubee" wrote: On Mar 13, 10:17 pm, "Eric Gisse" wrote: On Mar 13, 6:17 pm, "Shubee" wrote: Nonlinear transformations means that the homogenity of space and time is gone. That is only true in chimpanzee relativity. I certainly don't expect alpha male chimps to understand that. And it's obvious that you would have a harder time to learn that. You couldn't even figure out how Hilbert's sixth problem relates to the axiomatization of physics [0][1] [2][3]. If you ever evolve to the point of understanding my high school level formulation titled, The Axiomatization of Physics - Step 1: A Derivation of the Lorentz Transformation [4], you will then discover your mistake. Shubee 0.http://groups.google.com/group/sci.p...sg/fd7ad4b9e1b... 1.http://en.wikipedia.org/wiki/Hilbert%27s_problems 2.http://en.wikipedia.org/wiki/Hilbert's_sixth_problem 3.http://en.wikipedia.org/wiki/Wightman_axioms 4.http://www.everythingimportant.org/r...ty/special.pdf So, , prove that T(T^-1)=I where T is your "nonlinear transform function and I is the identy matrix. Put up or shut up. The transformation does have a group structure*, but it has no more significance than that. In particular, Shooby's claim that, for any function f, the group is "physically indistinguishable" from the Lorentz Group is, like most of what Shooby says, nonsense. * It's a bit easier to verify when the last term in the equation for t' is written as f(x'). Congratulations jem. It sounds like you convinced yourself of the correctness of the claim in exercise 1. You gave a very good hint. You make a very reasonable request. Let me give you a hint: To get the inverse of the nonlinear transformation in exercise 1 of http://www.everythingimportant.org/r...ized.htmmerely exchange x' with x, t' with t and v with -v. The problem is really much easier than it appears. Can you handle this problem, Shooby? Tell us what the constant v "physically" represents. Proper velocity u is defined by eq. (3) in The Axiomatization of Physics - Step 1 and has the clear physical interpretation presented there. In Shubertian physics, the parameter v is only a derived quantity, a function of the proper velocity. The ordinary velocity v is defined by eq. (40) inhttp://www.everythingimportant.org/relativity/special.pdf Bzzt! Sorry, Shooby, only when the function f is constant does v represent the "ordinary velocity" between the reference frames. Got another guess? jem, I don't have to guess. It's obvious that you don't understand my interpretation of equation (1) and equation (2) for the toy universe I call Xi_2. You were asked what v represents in your transformation equations, and there isn't any need* to look beyond those equations for the answer. * other than the need to be evasive when you're asked a question whose answer you should know, but don't. http://www.everythingimportant.org/r...ty/special.pdf Shubee I don't expect that any of my pompous critics could prove the group structure by doing the actual calculation directly but if Tom Roberts or any other capable physicist denies my group structure, then I would be happy to prove that these transformations form a group when I get some time. Note: If anyone wants to prove that my inverse doesn't work, then select any set of constants at random with any arbitrary function and compute the value of the function on those constants and the inverse function of the result. Prove you don't get back to where you started. http://www.everythingimportant.org/r...eneralized.htm Shubee I said very clearly that v is a function of the proper velocity. And you also said v was the "ordinary velocity", which in general, it's not. In fact the ordinary velocity between two frames may not even be defined (e.g. when f(x) = x/2 and v = c/2). I also said that these equations describe simple inertial motion. Think so? Select two of your crazy-clock reference frames (CC1/CC2), and specify the trajectory in CC1 of the origin of CC2. Unless the clock offset function f is constant, that trajectory isn't going to describe uniform motion, so at least one of those reference frames isn't Inertial. If you proved the group structure, then you know that v adds like ordinary velocity does in chimpanzee relativity. Why isn't that good enough? I have no idea what you think "adds like ordinary velocity" means. In general, v isn't even a velocity in your equations. http://groups.google.com/group/sci.p...3397d03512b7b0 |
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#78
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On Mar 18, 6:00 am, jem wrote:
Shubee wrote: http://www.everythingimportant.org/r...eneralized.htm I said very clearly that v is a function of the proper velocity. And you also said v was the "ordinary velocity", which in general, it's not. In fact the ordinary velocity between two frames may not even be defined (e.g. when f(x) = x/2 and v = c/2). You have to follow my definition (eq. 40), not your definition. I also said that these equations describe simple inertial motion. Think so? Select two of your crazy-clock reference frames (CC1/CC2), and specify the trajectory in CC1 of the origin of CC2. Unless the clock offset function f is constant, that trajectory isn't going to describe uniform motion, so at least one of those reference frames isn't Inertial. Eq. 3 of http://www.everythingimportant.org/r...ty/special.pdf explains very clearly the equation that describes uniform motion in terms of proper velocity in my very general coordinates. If you insist on chimpanzee relativity, then yes, setting x'=0 does give you a confusing function of t in terms of x and f(x). But I am not confused; You are. In general, f(x) isn't invertible or even continuous or measurable so that the best that you can get in general for the point x'=0 is a function that looks like t=h(x). The meaning of this equation for the point x'=0 is that as the origin of CC2 moves through each point x of CC1 as you call it, the local mathematical clock at x will read time t. Naturally, I presuppose a minimal set of axioms in my paper and therefore enjoy emphasizing my trivial law of physics which says that the universe doesn't change physically when arbitrary clock synchronization schemes are used. So exercise 2 still stands. Does my nonlinear group generate an identical physics to Lorentz, as claimed? Here's a fun exercise. In the goofy coordinates of my nonlinear group, let a clock move away at "velocity v" then turn around at some distance and then return at the same speed. Prove the usual time dilation effect. If you proved the group structure, then you know that v adds like ordinary velocity does in chimpanzee relativity. Why isn't that good enough? I have no idea what you think "adds like ordinary velocity" means. In general, v isn't even a velocity in your equations. http://groups.google.com/group/sci.p...sg/803397d0351... |
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#79
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did someone say "variable space" fractally fractionally inclined so
the function varies with permeability and permitivity and not C squared. |
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#80
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Shubee wrote:
On Mar 18, 6:00 am, jem wrote: Shubee wrote: http://www.everythingimportant.org/r...eneralized.htm I said very clearly that v is a function of the proper velocity. And you also said v was the "ordinary velocity", which in general, it's not. In fact the ordinary velocity between two frames may not even be defined (e.g. when f(x) = x/2 and v = c/2). You have to follow my definition (eq. 40), not your definition. How stupid is it to think you can redefine "ordinary velocity"? I also said that these equations describe simple inertial motion. Think so? Select two of your crazy-clock reference frames (CC1/CC2), and specify the trajectory in CC1 of the origin of CC2. Unless the clock offset function f is constant, that trajectory isn't going to describe uniform motion, so at least one of those reference frames isn't Inertial. Eq. 3 of http://www.everythingimportant.org/r...ty/special.pdf explains very clearly the equation that describes uniform motion in terms of proper velocity in my very general coordinates. If you insist on chimpanzee relativity, then yes, setting x'=0 does give you a confusing function of t in terms of x and f(x). But I am not confused; You are. In general, f(x) isn't invertible or even continuous or measurable so that the best that you can get in general for the point x'=0 is a function that looks like t=h(x). The meaning of this equation for the point x'=0 is that as the origin of CC2 moves through each point x of CC1 as you call it, the local mathematical clock at x will read time t. Naturally, I presuppose a minimal set of axioms in my paper and therefore enjoy emphasizing my trivial law of physics which says that the universe doesn't change physically when arbitrary clock synchronization schemes are used. The *description* of the universe changes, i.e. the physics changes. So exercise 2 still stands. Does my nonlinear group generate an identical physics to Lorentz, as claimed? Of course not. Here's a fun exercise. In the goofy coordinates of my nonlinear group, let a clock move away at "velocity v" then turn around at some distance and then return at the same speed. Prove the usual time dilation effect. Considering that any clock that starts in one of your goofy reference frames (i.e. where f isn't constant), and moves away from its starting point at constant velocity v, is never at rest in any of the goofy frames, why don't you have the fun of proving it, and then you can show us your proof. Show it here though - nobody is interested in wading through pages of self-aggrandizing to find anything on your website. Hint: you might want to use a symbol other than "v" for the velocity since "v" also happens to be an indexing parameter used by the goofy transformation. If you proved the group structure, then you know that v adds like ordinary velocity does in chimpanzee relativity. Why isn't that good enough? I have no idea what you think "adds like ordinary velocity" means. In general, v isn't even a velocity in your equations. http://groups.google.com/group/sci.p...sg/803397d0351... |
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