Article View: sci.physics
Article #1056Re: ORTHODOX SPECIAL RELATIVITY
From: Mcirvin
Date: Mon, 10 Aug 1992 21:45
Date: Mon, 10 Aug 1992 21:45
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6195 bytes
crb7q@kelvin.seas.Virginia.EDU (Cameron Randale Bass) writes: >In article <1992Aug10.184700.3204@sbcs.sunysb.edu> rscott@csws1.ic.sunysb.edu (Robert Scott) writes: >> [claim that SR follows from signal delays] > It is not this simple. It is not just that there are 'speed of > light delays'. That was perfectly understandible in terms of > a fixed propagational ether. It is that the speed of light > appears to be the same no matter what your motion (or relative motion > with respect). The interesting thing about this idea is that even though the space as modeled in the program has an "ether" (coordinates are presumably stored internally in some absolute frame), objects made entirely of formations of robots exchanging signals behave in a Lorentz-invariant way, and the speed of light appears to be the same in all frames, provided that you use measuring equipment available within the program's physics: measure time with a canonical pair of robots bouncing a signal, etcetera. > Restrict signals to the speed of light all you want, but you need > the Lorentz covariance to actually model relativity. How do > you suggest programming this without using the SR framework? Reread his post: he's putting it in by denying his robots, which are the only particles in the model world's physics, any knowledge of quantities that aren't Lorentz invariant. The *kinematics* of SR will indeed emerge if you only use systems of robots as clocks, meter sticks, etcetera. The only real problem is that this is a model of insufficient generality to show how SR intrudes into real-world phenomena, without the added specification that c should look the same in all frames no matter what measuring devices you use-- but that's more an issue of interpreting the program than of writing it. The model also doesn't really address the full complexity of SR *dynamics*, but one can model such things as collisions by giving the robots appropriate instructions. >>4. SELECT A NEW VELOCITY, SPECIFIED AS THE VELOCITY THAT WOULD BE >>NEEDED TO TRAVEL FROM EVENT X TO EVENT Y, WHERE X AND Y ARE AFFINE >>COMBINATIONS OF THE POINTS OF ORIGIN OF PREVIOUSLY RECEIVED MESSAGES. >>IF X=Y OR IF THE SPECIFIED VELOCITY IS LIGHT-SPEED OR GREATER, THEN THE >>COMMAND IS IGNORED. > Event Y already occurred? How would one reach an event that > had already happened? The robot isn't going to go *to* event Y, it's going to have the *velocity* corresponding to the interval between X and Y. This is a means of specifying velocities that is completely Lorentz invariant. > What you have here sounds very much (though in a confused > fashion) like galilean relativity with lightspeed delays. I think > that you will find, to your misfortune, that you either have > a preferred frame or light (or messages) does not travel > at a single speed with respect to all observers. Look again, keeping in mind that the only clocks and meter sticks you can use are formations of robots. Don't be fooled by the all-caps (note to Robert Scott: on Usenet people will read your posts more carefully and take you more seriously if you use lower case). >>IT HAS ONE EXTRA DIMENSION, CONSISTING OF THE GROUP OF >>UNIFORM EXPANSIONS OF SPACE-TIME ABOUT AN ARBITRARY REFERENCE POINT. >>NEVERTHELESS, I STILL THINK THAT THE EXPERIENCE OF LIVING IN THIS SORT >>OF VIRTUAL WORLD CONVEYS ALMOST ALL OF THE FLAVOR OF WHAT SPECIAL >>RELATIVITY IS LIKE. THE EXTRA EXPANSION SYMMETRY IS VERY EASY TO >>UNDERSTAND (DESPITE THE RARITY OF TRUE EXPANSION SYMMETRY IN NATURE, AS >>ILLUSTRATED FOR EXAMPLE BY GALILEO'S ANALYSIS OF WHY IT IS UNHEALTHY >>FOR AN ANIMAL FOR IT TO GROW TOO BIG), AND ONCE YOU'VE GOTTEN USED TO > > You are confusing the existence of a symmetry of the underlying > equations (space, etc.) with a symmetry of objects that exist > in the space. He's not. He's talking about a symmetry that physics may or may not possess, and such things as scaling relations in nature do rely intimately on the symmetry. Suppose dilation symmetry really did exist in nature: then a physical evolution enlarged in space and time by a constant factor would still be an allowable physical evolution, and lots of things having to do with objects would be different. Matter of a given composition could possess any density, and objects could be structurally sound at any size provided that the matter were scaled appropriately. There could be tiny civilizations made of incredibly dense versions of ordinary matter. The nonexistence of dilation symmetry in real physics is what prohibits all this. Personally I'd be all for giving the robots proper-time clocks. That would both get rid of the extra symmetry and also imply some Lorentz-invariant physics independent of the exchange of light-speed signals, such as we have in real life. Many SR-kinematic phenomena can indeed be made to follow from the kind of model Robert Scott is talking about. It's a little misleading to say that it follows entirely from signal delays, since you additionally have to base all physics upon the transmission of the signals. It's better to say that it follows from the intrinsically Lorentz-invariant nature of the model he's constructed. I would also argue that the treatment of SR from a geometric viewpoint is ultimately simpler than thinking in terms of a model where all physics consists of signal transmission. Nevertheless, a program like the one he's described would illustrate relativistic kinematics in a novel way. -- Matt McIrvin, professional gradgrind, amateur Usenet drifter
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Path: arc1-ca.pugleaf.net!sparky!uunet!dtix!darwin.sura.net!wupost!kuhub.cc.ukans.edu!husc-news.harvard.edu!husc8!mcirvin From: mcirvin@husc8.harvard.edu (Mcirvin) Newsgroups: sci.physics Subject: Re: ORTHODOX SPECIAL RELATIVITY Message-ID: <mcirvin.713483129@husc8> Date: 10 Aug 92 21:45:29 GMT References: <1992Aug10.184700.3204@sbcs.sunysb.edu> <1992Aug10.202618.1433@murdoch.acc.Virginia.EDU> Lines: 111 Nntp-Posting-Host: husc8.harvard.edu