Guest Post at Tommaso Dorigo's Blog: Extrinsic Relativity
doing science does not necessarily require a PhD and a desk in a University office, and that ideas and theories are not crackproof or crackpotty, but just right or wrong. (In this connection, he had also published in his blog a great story titled "Cracked Pots" which is well worth reading.) So Tommaso started a series of guest posts at his blog, some from mainstream scientists, some from "alternative theorists" with high academic credentials, and some from "alternative theorists" with no academic credentials, aka "crackpots" (I belong to the third group). He graciously accepted my submission, which he posted on November 16, 2007. This is it.
Contents"Extrinsic" RelativityFirst, let me thank Tommaso for the opportunity to write a guest post for his blog. My name is George Barouxis (aka Gebar), and I am a professional translator from Athens, Greece. This is my translation site where you can see most of the books I have translated into Greek over the years. I also have the "physics bug", and I often build Java applets in order to understand and explain my ideas. So, about those ideas. They concern lowly Special Relativity, but bear with me for a while.
"Proper" Special RelativityLet’s start with some incontrovertible mathematical facts. In the equations of the Lorentz transformation, if we set x’ = 0 we derive the equations of motion for the Moving Body. See derivation here (colored links open in new window): where t’ is the proper time of the Moving Body and T is the time of the Stationary Body. Now, the equation for proper time t’, with some rearranging becomes which is the equation of a circle of increasing radius T if c = 1 (or an ellipse with increasing semiaxes T and cT if c ≠ 1) as shown below: So the Moving Body, if placed on its “proper” position on the graph (the position indicated by its proper time), is always situated on the circumference of this circle of increasing radius T. Let’s see what this means. The usual picture in Special Relativity is this: The Stationary Body is the blue point at x = 0, T = 10, the Moving Body is the red point at x = 6, T = 10, and the Photon is the yellow point at x = 10, T = 10 (this is for a Moving Body with velocity v = 0.6 and for c = 1). The gray axes are the ones calculated for the Moving Body on the basis of the Lorentz transformation. You will notice that the Moving Body is at T = 10, although its proper time, as indicated by the gray number on its left, is t’ = 8. Now, if we place the Moving Body at T = 8, and we add its x and t axis, and the expanding circle of radius T, we get this picture. The red point at x = 6, T = 8 is the Moving Body in its “adjusted” position and the yellow point at x = 10, T = 0 is the Photon in its “adjusted” position. The relationship between the usual Lorentz axes (gray) and the new axes proposed here for the Moving Body (cyan) is this: And this concludes the facts of the case. (You can see a more detailed presentation at my site here, with a Java simulation that among other things shows the formation of the (gray) Lorentz axes by the projection of the (cyan) adjusted Lorentz axes on the x axis of the Stationary Body with the passage of time, as well as algebraic derivations for the above points.) Now the question is what we can make of all this. Quite a few people who have seen this have concluded that I have just come up with a geometric construction or a geometric interpretation of the Lorentz transformation, and they point out that since it predicts the same things as Special Relativity, it probably is just Special Relativity. Well, I have to agree that this is definitely one possible scenario. Let’s see now another one that may prove more interesting and useful.
Extrinsic Definition of the Shape of the Space DimensionFirst we have to talk a bit about spacetime curvature. Now, everybody knows that spacetime in Special Relativity is flat, so we have no curvature there. Spacetime in General Relativity is curved, and curvature in GR is usually described intrinsically, that is without reference to some higher dimensional space within which we imagine our spacetime to be embedded. Here we will use the extrinsic definition of curvature, in the sense of having an equation that gives us the shape of the space dimension. Let’s see how we could go about it. We start with a Stationary Body and its coordinate system, this: This is just a mathematical space. We add the space dimension on which the Stationary Body is situated, like this. This space dimension (orange line) is a straight line perpendicular to the time axis of the Stationary Body, described by a “zero degree” equation of the form t = T. By having T take successive values 1, 2, etc., we can depict the passage of time, through which the space dimension moves “upwards” taking successive positions (time coordinates) at each successive time moment. So at T = 0 it is at the position shown in the graph, at T = 1 it will be at time coordinate 1, etc. If we have a Moving Body with an equation of x = v*t, for v = 0.6 and T = 10 we will have the following picture: The space dimension is at T = 10, and intersecting the “worldline” of the Moving Body, it gives us its position at that time moment. The solution of a system of two simultaneous equations is depicted graphically as the intersection of the graphs of the two equations. The two equations here are the equations of motion in a flat Galilean spacetime:
No curvature here. In such a spacetime the speed of light can be considered infinite. And notice something important, that the orange space dimension coincides with the x axis of the Stationary Body. Essentially, the first equation of motion x = v*T defines the movement of the body in time, and the second equation defines the shape of the space dimension. In this case of a zero degree equation, it is a straight line perpendicular to the time axis of the Stationary Body, so we have no curvature there. The intersection of the two graphs (the solution of the system of simultaneous equations) gives us the position of the Body at each time moment. Now let’s see what happens if we use the equations of motion derived from the Lorentz transformation. Here the equation of the worldline of the Moving Body is the same as previously, but the second equation that gives us the shape of the space dimension is second degree. So instead of a straight line space dimension that moves upwards with the passage of time, we have a cyclic space dimension of radius T that expands “outwards” with the passage of time (reminds you of something?). The intersection of the graph of the Moving Body worldline equation with the graph of the space dimension equation gives us again the position of the Moving Body like this: Now, here we do have curvature, which is extrinsically described by the second equation of motion, the one that gives the proper time of the Moving Body for each point of the space dimension. (This equation defines the shape of the space dimension, essentially how it is embedded in the two dimensional spacetime represented by the whole surface of the graph.) Because we have curvature, the space dimension does not coincide with the x axis of the Stationary Body, and this has some important consequences: although the proper time of the Moving Body is 8 (in the specific case depicted above), we place it at T = 10 (because that’s where our x axis is), and this affects accordingly its worldline like this: This essentially means that we see the projection of the Moving Body on our x axis. This produces the phenomena of Special Relativity as described by the Lorentz transformation, and this may mean that these phenomena are due to the fact that we live in a “spherically” expanding universe but we describe it through a straight linear coordinate system. The usual objection here is that spacetime in Special Relativity is flat, so this can’t be right. Well, spacetime in Special Relativity is definitely flat –after you do the projection mentioned above. Specifically, it is this: You will notice that the darker gray line at T = 10 is straight, so, yes, there is no curvature there. However, this darker gray line is not the space dimension in which the Stationary Body, the Moving Body and the Photon exist. It is just the x axis of the Stationary Body, an abstract mathematical entity with no physical existence. The space dimension here is the expanding cyan circle, and the Moving Body (and its axes) and the Photon get projected on the x axis of the Stationary Body like this: So I do not claim that spacetime in Special Relativity is curved. I claim that there is an underlying curved spacetime, that when is mathematically described through this projection that makes it flat, we have as a result the phenomena of Special Relativity. The difference between the two previous figures is that Figure 10 shows things as they “seem” from the point of view of the coordinate system of the Stationary Body, while Figure 11 shows things as they “really are”, or as they seem from a “higher” point of view that includes the one of Figure 10 and, in a manner of speaking, “explains” them. Let’s take it inversely. If we live in a curved expanding spacetime as shown by General Relativity, we should observe the effects shown in the above graph (if we describe the curved expanding universe extrinsically). And we did observe them, in the MichelsonMorley experiment, which was explained through the Lorentz transformation and Special Relativity. In other words, the effects of Special Relativity are due to the curved expanding universe of General Relativity. But you need the extrinsic description of curvature in order to see this. Now, if we describe the shape of the space dimension extrinsically, we have to specify the dimension in relation to which the space dimension is curved. This is done by the second equation of motion, that defines the shape of the space dimension. We saw above what happens when this equation defines the time coordinate as a function of velocity. The “objects” of our spacetime now have their own “proper” time depending on their velocity, instead of having a universal time that is the same for all, as in the case of a flat Galilean spacetime. Again, if the space dimension is a straight line perpendicular to the time axis, all its points have the same time coordinate. Then the speed of light is infinite and time is absolute. This is a flat Galilean spacetime. If the space dimension is a curve (or even a straight line not perpendicular to the time axis), then different points will have different time coordinates. The speed of light will be finite and time will be relative (the time coordinate of a Moving Body will depend on its velocity). So this is the second scenario I was talking about, the one that says that this is not a geometrical construction or interpretation of the Lorentz transformation, and that the circle defined by the second equation of motion derived by the Lorentz transformation is not just a geometrical construct, it is the space dimension of our spacetime extrinsically defined by that equation. (Let me repeat here that I use the term “extrinsic description of the shape of a dimension” in the sense of having an equation that for each x coordinate of the space dimension gives us its coordinate along another dimension.) So how could one determine which of the two scenarios is the correct one? I am open to suggestions. To be frank, I haven’t worked much in trying to prove that this is a correct description of physical reality and not a geometrical construction. I just treat it as a working hypothesis, and if it’s wrong I expect I will end up at an impasse sooner or later. In the meantime I try to extend its applications in order to see where it will lead me. For instance:
Other applications of the extrinsic definition of the shape of the space dimensionLet me add a few more conjectures that I also treat as working hypotheses, to be expressed mathematically and checked against experimental facts. They are extensions of the basic concept used above, the extrinsic description of the shape or embedding of the space dimension. So in what follows, the aim is again to arrive at the equations of motion, that is, an equation that defines the movement of a particle as a function of time (worldline) and an equation that defines the shape of the space dimension (cyan line) in relation to another dimension, or its embedding in the 2d or 3d space formed by all the dimensions. We talked previously about the shape of the space dimension in relation to the time dimension. This referred to the whole length of the space dimension, as described by the second equation of motion derived by the Lorentz transformation. However, we can also imagine local areas of curvature like this: I think that this will produce gravitation. We see often such pictorial depictions of spacetime curvature produced by gravity, usually with a disclaimer that “this is not how things really are, but it does give some idea of the situation”. This is because spacetime curvature is described intrinsically by General Relativity, while such depictions use an extrinsic representation to make things easier to understand. However, we can very well arrive at a precise extrinsic mathematical description of this spacetime curvature, which will give it a physical, as well as a mathematical, meaning. Spacetime curvature in the picture above has a definite physical meaning if described extrinsically, it is an area of the space dimension that its points have different proper time coordinates that produce the above form in the space dimension (or the form that will produce the acceleration of gravitation as observed in the real world, if this one is wrong). Additionally, some kind of configuration of the space dimension at the apex of this gravity well may represent physically a fundamental particle. This configuration may be a simple or complex loop or other structure that acts as a photon trap, with the spin of the particle being a partial description of the form of this configuration. If at the apex the space dimension doubles upon itself (somehow intersects itself), this “knot” may give the appearance of a “point” particle, while the loop created by this selfintersection will have a non zero size and may allow the point particle to have properties. As we said, when we use the extrinsic description of curvature we specify the dimension in relation to which the space dimension is curved. The above concerns curvature in relation to time. However, we can also imagine the space dimension curving within an additional space or time dimension, and this curvature may represent charge: So the curvature along the t axis represents the mass of the particle, while the curvature along the z axis represents its charge, with the opposite charge being like this: The propagation of a disturbance of the space dimension in relation to this additional space or time dimension, which is produced by the movement of a charged particle, may represent electromagnetic waves, like this. I will not hazard a guess as to how this disturbance may be quantized in respect to the energy it carries, but this may become more obvious if we have a clear (extrinsic) mathematical description that defines its shape as a function of time. Right now an explanation that seems reasonable would be to look at the “pixels” that constitute the space dimension. (In a curved space dimension, different points have different t and z coordinates, but what is the physical size of these “points” along the dimensions of “zlength” and “tlength”, and how is the propagation of a disturbance along such a medium affected by the size of these lengths? There may be some kind of “stair step” there.) Let me point out again that these “working hypotheses” are highly conjectural (meaning I could be wrong). However, even so, they show something important, that when you use the extrinsic definition of the shape of the space dimension your statements acquire physical meaning and this is very useful on many fronts. I appreciate the reasons that made physicists, starting with Einstein himself, to prefer the intrinsic description of curvature. I believe however that the extrinsic description of the embedding of the space dimension can be used at least in a complementary way to the intrinsic description of curvature because it gives physical meaning to our formulations and in this way it can show us more easily where to look, and what to look for. Besides, the Nash embedding theorem may mean that the “transfer of knowledge” between the two descriptions is a legitimate operation. Well, that’s about it. I hope that what I have presented here, although rudimentary (especially on the math side), will at least give some food for thought.
Comments1. Louise  November 16, 2007 Good description of Gebar’s work along with some neat visuals. It is fascinating that the curvature of the Universe, which is predicted by General Relativity, can manifest itself in the local conditions of Soecial Relativity. The possible link between SR and GR makes this work worthy of attention. 2. George Barouxis  November 16, 2007 Hi Louise. You were the first to say there is some merit to this, and the first to comment on this guest post. Thanks for the support . 3. Pioneer1  November 17, 2007 Nice article. Beautiful graphics. Thanks again to the owner of the blog as well. But, you write where t’ is the proper time of the Moving Body and T is the time of the Stationary Body. I object in principle to the assumption of a “Stationary Body.” There is no Stationary Body in nature. Are you using this in a nonprecise so to speak way? I am sure that there is a good explanation but I thought I mention it. 4. George Barouxis  November 17, 2007
Yes, of course. “Stationary” always relatively speaking. In the Galileo and the Lorentz transformation, we have a “Stationary” and a Moving Body or observer or reference system (for instance, the train embankement and the train), and the transformation allows us to compute the coordinates measured for an event by the latter given the coordinates measured for the event by the former (and vice versa). 5. Riccardo Di Sipio  November 17, 2007 I find very intriguing the connection among mass, charge and curvature. To my knowledge, no massless charged particle has ever been observed. This can be accounted by gauge symmetries, of course, but I’m still looking for a clear geometric interpretation of the fact. To me, one thing that does work (at the moment) is the contrast with the experimental observation of a flat universe with \Omega ~ 1. I don’t want to say that your idea is wrong, but just that there might be something very deep behind. 6. George Barouxis  November 17, 2007
The above just offer a way to arrive at such a clear geometric interpretation. I suspect that what will prove (in this “theory”) to determine whether a particle can exist or not (and for how long it will exist) is the stability of the photon trap configuration of the space dimension that constitutes the particle. And of course this will have to be formulated mathematically in order to be able to talk meaninfully about the possible configurations that can exist, their stability and their duration. I am not sure I understand the comment in your second paragraph. Do you mean “one thing that does not work”, meaning that the observation of a flat universe contradicts the curved expanding universe of GR described here? 7. carlbrannen  November 17, 2007 Is there a connection between this and Euclidean Relativity? I think it might be easier for you to read about Euclidean relativity, and to explain the similarities and differences than vice versa. 8. George Barouxis  November 17, 2007 Hi Carl. The main difference is that Euclidean Relativity, if I am not mistaken, makes proper time an altogether different dimension. Here, proper time and coordinate time are the same dimension (that of time), but coordinate time is considered a projection of proper time. I suspect that if what I propose here is the correct version of things, making proper time a different dimension would create a series of impressive but misleading results. I do not know enough about Euclidean Relativity in order to be able to talk about other differences or similarities right away. 9. Riccardo Di Sipio  November 18, 2007 Yes, George. If I don’t go wrong, WMAP and other experiments suggest that the curvature of the universe is globally flat, except for local variations (i.e. close to a BH). 10. George Barouxis  November 18, 2007 Riccardo, here we have to differentiate two things, the local geometry near a mass or a Black Hole and the global geometry of the universe (which is what the WMAP shows). In the first case (the one depicted in figure 12), the curvature of the space dimension in relation to time as depicted affects the worldlines of the objects within the “pointed concave funnel”, and this in its turn affects the distances among the worldlines, making masses approach each other. So here, the curvature in respect to time creates “curvature” in respect to space, in the sense that the Pythagorean theorem would not hold true for such a region. On the other hand, in Figure 9, for instance, we have a depiction of the global geometry of the universe, without taking into consideration the mass of the two bodies. You will notice that the Moving Body traverses the same distance in its “adjusted” and in its “unadjusted” position (in the specific case depicted, x=6 for both). The difference between them is their time. Here the space dimension curves within time only, wordlines are not affected by any local gravitational distortion, so distances are not affected also, and therefore the Pythagorean Theorem would hold true for such a region. That is, this region would appear flat, because it curves solely in respect to time. (This is where the extrinsic description of curvature is helpful.) Perhaps I should point out also that what we term “proper” time is the time that we (being in the position of the Stationary Body) attribute to the Moving Body because we use a linear coordinate system. In a polar coordinate system, both bodies are at the same moment of time (they measure the same age for the “universe”, in the case depicted, 10 seconds). 11. Louise  November 18, 2007 I must agree with Gebar about the spherical expanding Universe of GR. There is more than one way to interpret the CMB (especially if a changing c is involved.) Large objects under the influence of gravity tend to form spheres, and the Universe is very large. 12. Riccardo Di Sipio  November 18, 2007 Ok, I got it. I’m sorry, I’m not a GR and CMB specialist. Thank you for your clear explanation. At this point, I’m wondering if your hypothesis can predict the real curvature or the radius (depending on the shape) of our Universe at a time. I didn’t make any calculation, but it will be no surprises to me if it can imply some kind of c(t) dependence. 13. George Barouxis  November 18, 2007
Neither am I. I can only try to answer this question on the basis of my hypothesis. A GR and CMB specialist most probably would give a completely different answer, and would consider what I present here as nonsense.
Ah, Riccardo, a most interesting but vexing question, to which I have not figured out yet a satisfactory answer. There are two considerations here. The first: In Figure 11 (where T=10) let us imagine that at T=8 a new Photon was emitted by the Stationary Body. If we assume a constant c=1, and that the Photon remains at the time coordinate at which it was emitted, then this Photon at T=10 would be at x=2, and so it will not coincide with the space dimension as depicted there (which for T=8 is at x=6). This would violate the Lorentz transformation. The only way for this not to happen would be (I think, but I am not sure if I remember correctly) if the space dimension was not circular or elliptic but a straight line that met the t axis at such an angle that it would give us the known speed of light. (Before I realized that it violated the Lorentz transformation, I did make this calculation (it is a simple application of the equation of the circle), and the result was that, if the “shape” of the Universe is completely spherical in respect to time, for the speed of light to have the value we observe today (299,792,458 m/s) the age of the Universe would have to be 1,425 billion years, which is off the accepted value approximately by a factor of 10. Intriguing.) The second consideration puts a completely different spin on things. If we calculate the proper time of the Photon through Equation 1b, we see that it is always 0. So, according to this, a Photon emitted at T=0 will remain at T=0 (its proper time would be 0). Furthermore, a Photon emitted, for instance, at T=8, would still remain at T=0 (its proper time again would be 0). Now, this is mandated by the Lorentz transformation. If you try to calculate the proper time of photons, you will get 0. Any other result would violate the Lorentz transformation. Here you can say that the Lorentz transformation breaks down for photons, but this is rather difficult to do because you have neither infinities nor divisions by zero, just a straightforward calculation that results in 0. Or you can accept this result as it is, that is, accept that photons are situated at time moment zero, which would have to be just a moment before the start of time in the universe (the moment of the “Big Bang” would have to be the first moment that was actually greater than zero). Now, this opens up a whole series of new issues (which, to be frank, almost lead us into science fiction or phantasy ). It would mean that when we have a light producing event at T=10, for instance, light starts at x=0, T=0, the origin of the universe (the locus of the Big Bang?) and propagates moving across past time moments. (These may by the longtitudinal waves that Carl Brannen was talking about?). An observer sees this light coming from a specific point of space, but the light has always the same origin, the common origin of all the points of space, the “time center” of the universe. (See, that’s why mainstream physicists don’t work with fundamental issues, so that they don’t have to make a fool of themselves. They leave that to us crackpots . And when they do, they coach it in such obscure mathematical language so that no one will be able to undestand them, except for their colleagues.) Anyway, that is the only interpretation I can come up with about the proper time of photons. If there is any other I would be interested to know.
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