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#41
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Dear George Dishman:
"George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news rxMe.57073$E95.48764@fed1read01...Dear George Dishman: "George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news:7hLLe.36643$E95.9310@fed1read01... Dear George Dishman: "George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news:81xLe.35947$E95.12374@fed1read01... Dear George Dishman: "George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news:YsdLe.25309$E95.8692@fed1read01... ... going to attempt some deft trimming ... More trimmed throughout. Think of a pool table. It would be easy to define x and y axes and calculate the motion of the balls using Newtonian mechanics - no problems. We could also use polar coordinates (r, theta) with the origin at the centre of the table. Now every time a ball passes through the origin, theta becomes undefined. That is a coordinate problem only though, the actual motion of the balls must be the same whichever choice of coordinate system we make. Right. Now is spacetime, or the underlying reality that has the features we recognize as spacetime, the billiard table, the coordinates, or some mixture of both? Good question, this is perhaps where differing understanding of the terminology can cause problems. By "spacetime" I mean the underlying reality, the billiard table. We have invented a number of ways of labelling that mathematically in the form of coordinates such as Schwarzschild, Eddington-Finkelstein and Kruskal but the are only coordinates, ways of quantifying locations and times. OK. Space and time are irretrievably bound, which is the strong suite of GR. "That which works" out here, doesn't at/near an event horizon. It isn't just mathematics, it is a requirement of the model. No, that's not true. The failure at the horizon is purely mathematical as for the pool table example, the failure at the singularity is physical. Consider that the sources that are the most active astrophysically, are black holes (with companions). Indeed, but the radiation and jets are produced in the accretion disk outside the horizon. So it isn't quite "mathematical", then is it? Physically, the Universe (and the BH) are attempting to solve the "immovable object/irresistable force" problem. Now consider the definition of "singularity". The event horizon *is* a singularity. No? No. The singularity is at the centre, there is nothing unusual physically at the horizon. It *is* a singularity in Schwarzchild coordinates. I quote from Wikipedia a.. mathematical singularity - a point where a mathematical function goes to infinity or is in certain other ways ill-behaved. It is also a point where all functions meet. a.. gravitational singularity - an infinity occurring in an astrophysical model, involving infinite curvature (a mathematical singularity) in the space/time continuum, namely a black hole. What is unusual at the horizon is that light cannot ever propagate away from it. In all coordinate choices, this is true. ... No, from what I have seen, some coordinate systems stop at the horizon while other don't, but there is no physical effect there in the GR model. Look again. A very large number of sources cite how you never actually get to see anything fall into the event horizon. GR very much says that what you measure, does not include the inside of the event horizon. Ever. Yes, that's true but if you look at a spacetime diagram showing light cones, it is obvious why that occurs and it doesn't involve a singularity. It does involve a singularity, George. As defined by the English language. A "singularity" is not always just a "point". ... He made assumptions, assumptions not evident without mining his pages. Ah now that's different and very interesting. Can you give me a pointer to what you found? ... adding the link back in for posterity ... URL:http://casa.colorado.edu/~ajsh/schw.shtml It isn't what I found, George. Read my sentence again. It is that I didn't find "what assumptions the pretty pictures are based on", in the infinte variations of how that can be expressed in the English language. I still read it as saying that you _did_ find assumptions but that you had to 'mine his pages' to do so. I could only have been clearer had I added the sentence: "Which I did not do." There is window dressing, but he construction details of the manequins, might be there somewhere, but I did not find it. Likely it was numerical simulation of the equations of GR direct. Exactly, the only 'assumptions' were the other stars he included in the hypothetical system. The ray tracing I believe is pure GR without any simplifications at all. I don't know how he did a "Schwarzchild" solution across the event horizon. Yet that is the suggestion. Only the choices of "simplifying assumptions" are (perhaps) omitted, so only Andrew knows. Even he URL:http://casa.colorado.edu/~ajsh/home.html ... I don't see a path to the answer. Neither did I which is why I asked where in the pages you had found them. I think I'd rather kill my hypothesis with logic (integrating over the surface) rather than use someone else's assumptions to try and do it. I am very uncomfortable with his assumption that we could fall at c... for example. Relative to what? Relative to an observer at infinity, that's not an assumption but derived from the theory. Really? Is that c at the infinite observer's location, or c at the local curvature to the faller? 'c' is just a number, a universal constant. AIUI the speed is greater than c relative to the infinite observer but it is zero relative to the falling observer of course (you did say "we could fall at c"). I got my b*tt chewed too. Light would pass the falling observer at exactly c. The "infinite observer" sees that over a path that passes through an area of space with "high curvature", the "flight time" is longer than if there were less curvature. So c_nonlocal (better: c_path_average) No, it would be better to say "speed_path_average" since c is just a constant, 299792458m/s. Yes, sloppy talk does no one any good. would appear to decrease, as observed by an infinite observer. "Shapiro time delay" is an observation fully in agreement with GR. So what does it mean to say that we "infinite observers" can say stuff about physics beyond the *singularity* that is the event horizon? David, the event horizon is *not* a singularity, only certain coordinate system have an *artificial* singularity on that surface. That is the root of all our disagreements I think. It is how the word is defined, George. You (and most other mainstreamers) place the singularity "at the center", even though this is not physically meaningful in *this* Universe. Yet in my hypothesis, the only singularity is the severance of one spacetime, adjoint to another (essentially identical?) spacetime. The mass/energy only "reports to a different boss, on a different form". What the external Universe calls "an infintely dense central singularity", the insiders call "an approaching infinitely-diffuse, cold future". We will evaporate before that will complete, of course. This is why the r axis is referred to as "timelike". So time has a different letter in that region, it is still time. It *is* still time, but it is not outer-time. It is not related to external-time, except perhaps to be orthogonal to it. Again, this is just the model, I know. I don't want to sound as though I'm laying down the law but I think you need to stop and make some enquiries. AIUI, it isn't the model, it is the coordinates. Physically time outside the horizon and time inside are the same, it is only when you get to the singularity at the centre that the physics fails. Then we can agree to disagree. I'll stop offering it, and do some studying. If no one champions this, in 10 or 20 years (when/if I can go back to school), maybe I'll take up the gauntlet again. I have been trying to find something on this and this is the best I have found so far: http://math.ucr.edu/home/baez/RelWWW/wrong.html#holes Note the bullet list below the Penrose diagram "The Schwarzschild solution 'changes signature' at the event horizon. This is incorrect--- this is a common student misconception which arises from misunderstanding the nature of the coordinate singularity in the Schwarzschild chart for the external region at r = 2m." Note that his comment applies "for the external region"... No, his comment is that the existence of a change of signature is incorrect. He explains that this "arises from misunderstanding the nature of the coordinate singularity ... for the external region" The entire bullet point applies to the external region. I disagree, it seems clear it to me it refers to a signature change at the boundary between the regions. Are you familar with German, George? No, but it isn't written in German. The structure of English is not the same. But it is close... NOT! ;) Are you aware of the importance of the "sequence" of the word "nicht" in a sentence, and how it applies to the meaning of the sentence? At the end of that "sentence" is the phrase: Schwarzschild chart for the external region at r = 2m. He says two things, first; "The Schwarzschild solution 'changes signature' at the event horizon. This is incorrect --- this is a common student misconception ..." That seems quite clear. Then he gives the explanation for the source of the misunderstanding: "... which arises from misunderstanding the nature of the coordinate singularity in the Schwarzschild chart for the external region at r = 2m." To rephrase it, 'People incorrectly think there is a change between inside and outside because they fail to understand the problem with the coordinate system used outside.' Note he specifically says it is a *coordinate* singularity. Understood. Disagree. Move on. It is, as you point out, a modelling problem, with a model *that* cannot be applied to r = 2m, just as you cannot apply Lorentz contraction/dilation to any object (massive or not) travelling at c. No, I think it is a coordinate problem, not a model problem. The balls don't fall off the table. They start a new table, since the table only exists because there are balls on it. As I say though, I'll let it go. I can't prove it. They are still just coordinates, nothing more. Tell that to strong X-ray sources. Tell that to objects that evaporate by quantum mechanical means. They are coordinates that work really well here in "mostly flatland". The model says that "something might happen if"... Have you no curiosity? This isn't about curiosity or the lack thereof, I think you are building your views on a trivial misunderstanding of the GR model. I hear your words, but mine have been labelled. Mine is an interpretation based on GR models/coordinate choices. One that is potentially falsifiable. If the inside of the BH forms a separate Universe, the we can look around/back and know what that internal Universe might look like. I don't hold that this Universe is unique, or at least self-sufficient. snip quoted text The same objects, will provide multiple specular images. And this is still outside the event horizon. Interesting but as you say those were for an external observer and external sources. Do you think they get *more* pure, or make more "sense" on the inside? I think the form of the distortion will vary but that's all, you still get a distorted view of sources lying on your past light cone. Our past lightcone stops at the Big Bang. Some MODELS of the Universe suggest that the same might be true of someone infalling across an event horizon. Isn't it worth a look? (Geez, I'm sounding like Uncle Al, only not as smart.) Yes, it is worth looking but we need to correctly understand what the models say. We understand what the models say. Internal time is NOT directly correlated to external time, by all metrics than we can yet apply to BHs. So see how far that can take us to understanding "The Beginning". ... Kruskal has his name on his choice of coordinates. He chose them because he wanted to make a prediction (or solve) to the inside of the event horizon. Predictions are *enabled* by models, and mathematics. Exactly, and a method of defining coordinates that doesn't suffer from the pool table effect is something that enable predictions to be made over a greater range, but the predictions themselves come from the physical model. And predictions are to be... - experimentally verified. Right? Not in this case, we cannot observe the inside as much as we would like to. .... unless, the Big Bang *is* inside. You have misunderstood Chris' page, I believe. All the pages I have seen refer to the "radius" as "timelike" inside the BH, regardless of coordinate system. Are there two times? No, I think the latter 'r' referes to past versus future, that's all, but see Tom's reply. "We can't know." is not very satisfying to me. It seems that "we can look" is far superior. Tough. Either we can or we can't, that is determined by reality, not our preference. Understanding whether we can or not is the best we can do. So why do you have a preference for one model over another? I am not offering "new physics", I am offering that our Universe is not unique in the scheme of things. And my hypothesis is potentially falsifiable. What is raising the question of a non-closed Universe? Without dark energy, GR gives some simple solutions for an expanding universe: 1) Density greater than the critical value means spatially and temporally finite so we have a closed universe and a big crunch. Expansion slows and reverses. A photon created at t=0 gets exactly half way across the universe when the crunch arrives. Which doesn't work too well, since we have photons arriving in all directions from even ~300,000 y after the Big Bang. Why is that relevant, there wasn't a centre as you know. Let's see. We can determine the temperature of the CMBR a "billion years ago" by observing processes in distant stars. You have arrived at 4300 6300 LY actually but never mind. I hope to hold that number. light years for the thickness of the CMBR. Seems to me like we are still receiving light that has travelled more than once around the size of that early Universe, Age now is 13.7 billion years. Hypothetically, if we were in a closed universe currently at maximum volume, the crunch would be at 27.4 billion years. In that case GR said it would take a photon precisely 54.8 billion years to get back to where it was created after going "once round". The cosmological constant changes all that though. even though it may no longer be able to make it around the size of the Universe now. So the stated condition "A photon created at t=0 gets exactly half way across the universe when the crunch arrives." is obviously not met in this Universe. Currently a closed universe seems highly unlikely as we have discussed. Agreed. You asked me "why" and I was answering that. I wonder why they feel that space would contract again in such a short time? Why do you think it would be a short time? http://www.astro.ucla.edu/~wright/flatness.gif Red is closed, green and black are open. 4300 light years thick. Went opaque "in an instant". My figure of 6300 LY would suggest it was opaque at 372,700 years and transparent at 379,000 years. "In an instant" doesn't seem inappropriate in cosmological terms. .... but it does to a mechanical engineer! Is the "thickness" being the same order of magnitude as the global "quench" meaningful? The FRW metric has the Universe collapse again, but after many billions of years. Exactly. But it does not "solve" a spacetime that has "chunks" of mass in it. But then it too is "just a MODEL". Any solution to the equations is "just a model", the trick is to find one that matches all we can observe and then have it tell us about things we can never see. That's my kind of "what if ...". But that isn't science, George. snip Other than the dark energy contribution, you will find many argue it is precisely that, the remnant kinetic motion from t=0. The sum of that kinetic energy and gravitational potential energy is zero in many of the GR models. However, our "expansion velocity" is much higher than our kinetic motion wrt the Universe at large. Again you seem to be thinking of expansion as a motion away from a centre. No. There is nothing special in "the direction we are moving away from" kinetically, at 300 km/sec. We are moving away from the CMBR with a (sort of) gamma of 1079... which is NOT kinetic motion. I just don't use the language the way experienced do. OK, and perhaps I also mis-used it in trying to understand you. We can measure the dipole moment of the CMBR anisotropy .... and the Universe et al... and call that a motion relative to locally co-moving coordinates. I think of that like the proper motion of a star within our galaxy. The z of the CMBR can be thought of as produced by motion of the source away from us but it can also be considered as similar to gravitational redshift or a stretching of the wavelength of the photon while it was travelling through space that was being stretched. That sucked when Paul Lutus was feeding it to me. A photon, once emitted, can be absorbed or scattered. It cannot be "stretched". The red shift of supernovae duration is similarly red shifted to its emission spectra. The light emitted is characteristic of the process that emitted it, the local curvature in which is was emitted, the global curvature of the Universe that emitted it, the global curvature of the Universe that detected/absorbed it, and the local curvature of the detector. Nothing was "stretched", any more than it is between the Earth's surface and the GPS satellites, or between the surface of the Sun and here. Ignoring my 'proper motion' part, the kinetic motion and the "expansion velocity" are one and the same. I think that I will stick with Ned Wright's defintion, wherein "kinetic motion" is kept separate form expansion. "Let each man lay his dead according to his own fashion." When is the last time you asked "what if"? Frequently, for example in reading Alan Guth's paper on this subject. That's different to finding out how to interpret an existing 'what if'. http://www.arxiv.org/abs/astro-ph/0301199 OK. Here are mine... "What if we find structures the same age as the CMBRM?" Then the observed nature of those structures is what we should base our hypotheses on if we are to approach this scientifically. Good. Do you agree they *could* be observable... to say some 500,000 years after the BB... *IF* they existed? "What if we find heavy elements in excess of what can be explained in standard Big Bang theory, the same age as the CMBRM?" Then the measured relative abundances are what we should base our hypotheses on if we are to approach this scientifically. I like to be proactive... I like the scientific method. I can't reconcile that statement with your disallowing certain models of GR. But that isn't my problem. No, "at those temperatures" means at the temperature necessary to produce the obserevd H/He/Li mix regardless of whether it happened in our universe or the container. This is where I am trying to fabricate some "breathing room". But you aren't, you are removing the only mechanism we know capable of producing what we see. I *think* I'm trying to offer an alternative, George. What is your alternative explanation for the ~24% observed ratio of He/H not involving the conventional plasma? As I have said, I cannot disallow such a plasma. I am only trying to offer an alternative to said plasma, and it (my hypothesis) will have a spectrum yet-to-be-determined. I suspect, as you figured out, a time-integrated external-history will include a good deal of the BH's own "failed evaporation"... including the bitter end. And as I've said, I might by some stretch of the imagination be right, and there still be a "Universe filling, opaque plasma". Then if that rips down matter back to protons then it wouldn't be an alternative. They keep talking about "recombination", and BHs do tend not to stay one size... as they ingest matter. It could start out as a shredder, and end up as a flocculation pond (very slow agitation, that enables agregation of molecules into skimmable or sinkable structures) snip Our hole could have formed in an early Universe, and our hole could have consumed its companion(s) early on too. Or we could have shredded whatever we got first... somehow I want to believe we are much bigger than this. Bigger than infinite? Do you really mean you want to believe there an "outside" which is older than this? See Guth. No, I want to believe in an outside that is disjoint-in-time from us. Then that is 'new physics' No, it isn't. It is a choice of model. And it is potentially observable/falsifiable. What I meant by "much bigger than this" is, I think we have too much mass evident today, to have made a small BH as a "youth". Too much??? There is only 4% of the critical density as baryonic matter and even dark matter only brings it up to about a third of what is required. Consider a young Universe, some 6300 ly "across", with mass sufficient to achieve a "curvature coefficient" of 1079 (compared to today). That may be a small beginning, but it no less massive. But I guess we had to start somewhere. ;) I just need spectrum data... the Sun, and some of the full sky surveys that mapped the CMBR... which will not do a good job with individual spectral lines most likely. Do you have some ideas where I can look? The Sun isn't going to be much use, you need spectra for everything from white dwarfs to red giants and you need to know the mix visible in the container universe from our location within it and their ages. These should be written into spectrum data near the plane of the Milky Way, in the CMBR data... assuming that is available since it is "contaminated". For the CMBR, use this link http://lambda.gsfc.nasa.gov/product/...prod_table.cfm Yes. This would be good (as a start) for a free BH, or one near our position in a "largely spiral" galaxy. Then I need to come up with a spectrum for a BH consuming a companion, and to somehow infer the influx to the BH at the center of our own galaxy. If I'm going to prepare several "broths" best to use many available spices. or Google for "firas data products". It should be on the Lambda site but that seems to be down at the moment. Thanks George. I seem to be wearing on your nerves. So I will try not to respond more than once a week. That way the "potential irritation" level is down. It takes me about an hour to key this all in, and I hope it doesn't take you nearly this long to reply. (Although a *lot* of thought goes into your responses.) David A. Smith |
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#42
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Dear Geroge Dishman,
"George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news rxMe.57073$E95.48764@fed1read01...Dear George Dishman: "George Dishman" wrote in message ... Just a note, I found some of what we were discussing. No, from what I have seen, some coordinate systems stop at the horizon while other don't, but there is no physical effect there in the GR model. I found the relevant part he http://casa.colorado.edu/~ajsh/schwp.html "The Schwarzschild spacetime geometry appears ill-behaved at the horizon, the Schwarzschild radius (vertical red line). However, the pathology is an artefact of the Schwarzschild coordinate system. Spacetime itself is well- behaved at the Schwarzschild radius, as can be ascertained by computing the components of the Riemann curvature tensor, all of whose components remain finite at the Schwarzschild radius." I understand what you are saying, George. Now try these: URL:http://www.aleph.se/Trans/Global/Omega/baby.txt URL:http://math.ucr.edu/home/baez/PUB/generichole URL:http://math.ucr.edu/home/baez/gr/oz1.html There is window dressing, but he construction details of the manequins, might be there somewhere, but I did not find it. Likely it was numerical simulation of the equations of GR direct. Only the choices of "simplifying assumptions" are (perhaps) omitted, so only Andrew knows. There is a list on this page under "Caveats" http://casa.colorado.edu/~ajsh/approach.html Yes. He supposedly had a Schwarzchild solution that he was able to map across the event horizon. A nice trick. Then he claims that we "fall at c". And yet, this seems to be what is at hand. David A. Smith |
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#43
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"N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news:yUwOe.124442$E95.97537@fed1read01... Dear Geroge Dishman, "George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news rxMe.57073$E95.48764@fed1read01...Dear George Dishman: "George Dishman" wrote in message ... Just a note, I found some of what we were discussing. No, from what I have seen, some coordinate systems stop at the horizon while other don't, but there is no physical effect there in the GR model. I found the relevant part he http://casa.colorado.edu/~ajsh/schwp.html "The Schwarzschild spacetime geometry appears ill-behaved at the horizon, the Schwarzschild radius (vertical red line). However, the pathology is an artefact of the Schwarzschild coordinate system. Spacetime itself is well- behaved at the Schwarzschild radius, as can be ascertained by computing the components of the Riemann curvature tensor, all of whose components remain finite at the Schwarzschild radius." I understand what you are saying, George. Now try these: URL:http://www.aleph.se/Trans/Global/Omega/baby.txt David, is there a way to get rid of the "URL:" part, it breaks the link in Outlook Express because the text is no longer a URL if you put "URL" in front. Anyway, from that link I see: A. The formation of a black hole creates "baby universe," the final singularity of the black hole tunnelling right on through to the initial "big bang" singularity of the new universe thanks to quantum effects. The phrase "the final singularity of the black hole" refers to the point at the centre and confirms what I have been saying. Later it says: "The fact that the entropy of a black hole is (at least under certain circumstances) proportional to the area of its event horizon is a curious relationship between general relativity, quantum field theory and statistical mechanics that many people believe to pointing somewhere, but unfortunately nobody is sure where. Part of the reason is that the standard derivations are somewhat indirect, and the event horizon is not a physical object, so the sense in which it is the locus of entropy is difficult to understand." Again "the event horizon is not a physical object" agrees with my view. URL:http://math.ucr.edu/home/baez/PUB/generichole URL:http://math.ucr.edu/home/baez/gr/oz1.html There is window dressing, but he construction details of the manequins, might be there somewhere, but I did not find it. Likely it was numerical simulation of the equations of GR direct. Only the choices of "simplifying assumptions" are (perhaps) omitted, so only Andrew knows. There is a list on this page under "Caveats" http://casa.colorado.edu/~ajsh/approach.html Yes. He supposedly had a Schwarzchild solution that he was able to map across the event horizon. A nice trick. No trick needed, nothing changes at the horizon. Then he claims that we "fall at c". And yet, this seems to be what is at hand. Imagine a duck swimming up river at 5m/s in a stream that narrows approaching a weir. As the stream narrows, the water moves faster. If the duck starts where the water flows at 4m/s it will escape but if it starts where it is 6m/s it will move towards the weir ever faster until it goes over. A singularity occurs if the width of the stream gets to zero at the weir as the speed becomes infinite, but nothing happens to the water (or the duck) where the flow is 5m/s. George |
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#44
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"N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news:6twOe.124437$E95.51864@fed1read01... Dear George Dishman: "George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news rxMe.57073$E95.48764@fed1read01...Dear George Dishman: Severly trimmed again. No, that's not true. The failure at the horizon is purely mathematical as for the pool table example, the failure at the singularity is physical. Consider that the sources that are the most active astrophysically, are black holes (with companions). Indeed, but the radiation and jets are produced in the accretion disk outside the horizon. So it isn't quite "mathematical", then is it? I don't see your point, the matter in the jets never gets nearer than r=3m while the horizon is at r=2m. Physically, the Universe (and the BH) are attempting to solve the "immovable object/irresistable force" problem. No, it's more like the gravitational slingshot of a probe round a planet, it only passes nearby. Now consider the definition of "singularity". The event horizon *is* a singularity. No? No. The singularity is at the centre, there is nothing unusual physically at the horizon. It *is* a singularity in Schwarzchild coordinates. I quote from Wikipedia a.. mathematical singularity - a point where a mathematical function goes to infinity or is in certain other ways ill-behaved. It is also a point where all functions meet. OK, that says it is "mathematical", i.e. has no physical significance. a.. gravitational singularity - an infinity occurring in an astrophysical model, involving infinite curvature (a mathematical singularity) in the space/time continuum, namely a black hole. OK, that could refer to the centre though there is nothing in the context to differentiate. What is unusual at the horizon is that light cannot ever propagate away from it. In all coordinate choices, this is true. Yep, ask the duck if there is a ripple on the water at it's point of no return (see my other post). Yes, that's true but if you look at a spacetime diagram showing light cones, it is obvious why that occurs and it doesn't involve a singularity. It does involve a singularity, George. As defined by the English language. A "singularity" is not always just a "point". Sorry, I should have made the distincton between mathematical and physical. There is window dressing, but he construction details of the manequins, might be there somewhere, but I did not find it. Likely it was numerical simulation of the equations of GR direct. Exactly, the only 'assumptions' were the other stars he included in the hypothetical system. The ray tracing I believe is pure GR without any simplifications at all. I don't know how he did a "Schwarzchild" solution across the event horizon. Yet that is the suggestion. Indeed, it is possible and retains discrete images because the GR model does not include any physical change at the horizon. No, it would be better to say "speed_path_average" since c is just a constant, 299792458m/s. Yes, sloppy talk does no one any good. Me too, see above. would appear to decrease, as observed by an infinite observer. "Shapiro time delay" is an observation fully in agreement with GR. So what does it mean to say that we "infinite observers" can say stuff about physics beyond the *singularity* that is the event horizon? David, the event horizon is *not* a singularity, only certain coordinate system have an *artificial* singularity on that surface. That is the root of all our disagreements I think. It is how the word is defined, George. I'm not sure of the exact technical definition but "the boundary of the region from which light cannot escape" is probably close. You (and most other mainstreamers) place the singularity "at the center", even though this is not physically meaningful in *this* Universe. At the centre, many measures become infinite in a way that is independent of coordinates, the theory blows up and you have a singularity in the model. There is no such occurence at the horizon though some coordiante systems fail. Yet in my hypothesis, the only singularity is the severance of one spacetime, adjoint to another (essentially identical?) spacetime. IMHO, that would be "new physics" since this doesn't happen in GR. The mass/energy only "reports to a different boss, on a different form". What the external Universe calls "an infintely dense central singularity", the insiders call "an approaching infinitely-diffuse, cold future". We will evaporate before that will complete, of course. This is why the r axis is referred to as "timelike". So time has a different letter in that region, it is still time. It *is* still time, but it is not outer-time. It is not related to external-time, except perhaps to be orthogonal to it. Again, this is just the model, I know. I don't want to sound as though I'm laying down the law but I think you need to stop and make some enquiries. AIUI, it isn't the model, it is the coordinates. Physically time outside the horizon and time inside are the same, it is only when you get to the singularity at the centre that the physics fails. Then we can agree to disagree. I think that's best, I doubt we will resolve this here but please note I am not rejecting any aspect of GR, just your interpretation of it. If it turns out your version is correct, I will happily acknowledge being enlightened. big snip I don't hold that this Universe is unique, or at least self-sufficient. Nor am I claiming that (or otherwise), see my comments on Guth. Yes, it is worth looking but we need to correctly understand what the models say. We understand what the models say. Internal time is NOT directly correlated to external time, by all metrics than we can yet apply to BHs. That is where we have agreed to disagree. "We can't know." is not very satisfying to me. It seems that "we can look" is far superior. Tough. Either we can or we can't, that is determined by reality, not our preference. Understanding whether we can or not is the best we can do. So why do you have a preference for one model over another? I don't exclude or prefer any model, other than perhaps being skeptical of "non-trivial topology" without convincing evidence, I don't like the idea of the universe being a Klein Bottle! I am not offering "new physics", I am offering that our Universe is not unique in the scheme of things. And my hypothesis is potentially falsifiable. That isn't contentious, it is only your idea of a physical singularity at the event horizon that I consideer to be "new physics" as I believe it is in contradiction to GR. What is raising the question of a non-closed Universe? Without dark energy, GR gives some simple solutions for an expanding universe: 1) Density greater than the critical value means spatially and temporally finite so we have a closed universe and a big crunch. Expansion slows and reverses. A photon created at t=0 gets exactly half way across the universe when the crunch arrives. Which doesn't work too well, since we have photons arriving in all directions from even ~300,000 y after the Big Bang. Why is that relevant, there wasn't a centre as you know. Let's see. We can determine the temperature of the CMBR a "billion years ago" by observing processes in distant stars. You have arrived at 4300 6300 LY actually but never mind. I hope to hold that number. light years for the thickness of the CMBR. Seems to me like we are still receiving light that has travelled more than once around the size of that early Universe, Age now is 13.7 billion years. Hypothetically, if we were in a closed universe currently at maximum volume, the crunch would be at 27.4 billion years. In that case GR said it would take a photon precisely 54.8 billion years to get back to where it was created after going "once round". The cosmological constant changes all that though. even though it may no longer be able to make it around the size of the Universe now. So the stated condition "A photon created at t=0 gets exactly half way across the universe when the crunch arrives." is obviously not met in this Universe. Currently a closed universe seems highly unlikely as we have discussed. Agreed. You asked me "why" and I was answering that. Then I still don't understand why you said "Which doesn't work too well, since we have photons arriving in all directions from even ~300,000 y after the Big Bang". They were produced everywhere so would be arriving from all directions even 1s after the bang. My figure of 6300 LY would suggest it was opaque at 372,700 years and transparent at 379,000 years. "In an instant" doesn't seem inappropriate in cosmological terms. ... but it does to a mechanical engineer! Is the "thickness" being the same order of magnitude as the global "quench" meaningful? What do you mean by "global 'quench'"? The FRW metric has the Universe collapse again, but after many billions of years. Exactly. But it does not "solve" a spacetime that has "chunks" of mass in it. But then it too is "just a MODEL". Any solution to the equations is "just a model", the trick is to find one that matches all we can observe and then have it tell us about things we can never see. That's my kind of "what if ...". But that isn't science, George. Isn't it? Basing our extrapolations on models derived from observation instead of philosophy or religion seems to me to be precisely what science is about. The z of the CMBR can be thought of as produced by motion of the source away from us but it can also be considered as similar to gravitational redshift or a stretching of the wavelength of the photon while it was travelling through space that was being stretched. That sucked when Paul Lutus was feeding it to me. It is a standard way of expressing it. I'm not keen myself but I think the three descriptions are effectively equivalent while appearing different in the same sense as wave/particle duality. A photon, once emitted, can be absorbed or scattered. It cannot be "stretched". The red shift of supernovae duration is similarly red shifted to its emission spectra. The light emitted is characteristic of the process that emitted it, the local curvature in which is was emitted, the global curvature of the Universe that emitted it, the global curvature of the Universe that detected/absorbed it, and the local curvature of the detector. Nothing was "stretched", any more than it is between the Earth's surface and the GPS satellites, or between the surface of the Sun and here. I hear your assertion. Ignoring my 'proper motion' part, the kinetic motion and the "expansion velocity" are one and the same. I think that I will stick with Ned Wright's defintion, wherein "kinetic motion" is kept separate form expansion. "Let each man lay his dead according to his own fashion." Can you give me a pointer to this in his tutorial, I wasn't aware he used the terms. I'll search later but if you have bookmarked the section it would save me some time. "What if we find structures the same age as the CMBRM?" Then the observed nature of those structures is what we should base our hypotheses on if we are to approach this scientifically. Good. Do you agree they *could* be observable... to say some 500,000 years after the BB... *IF* they existed? They should be visible after 379,000 years if they existed then. I am hoping we will see Pop III novae with the next generation scopes but they are expected to be around z=20. If super-massive BHs preceded galaxy formation, we might see quasars even earlier. "What if we find heavy elements in excess of what can be explained in standard Big Bang theory, the same age as the CMBRM?" Then the measured relative abundances are what we should base our hypotheses on if we are to approach this scientifically. I like to be proactive... I like the scientific method. I can't reconcile that statement with your disallowing certain models of GR. That's because I don't believe I am, I think you are inventing "new science" when to suggest a physical singularity where none exists in GR. If you want to talk about the Cauchy horizon, that would be another matter, but I know little of that. What is your alternative explanation for the ~24% observed ratio of He/H not involving the conventional plasma? As I have said, I cannot disallow such a plasma. I am only trying to offer an alternative to said plasma, Yes, I understand that, but how does your alternative produce that elemental ratio? and it (my hypothesis) will have a spectrum yet-to-be-determined. I suspect, as you figured out, a time-integrated external-history will include a good deal of the BH's own "failed evaporation"... including the bitter end. And as I've said, I might by some stretch of the imagination be right, and there still be a "Universe filling, opaque plasma". Then if that rips down matter back to protons then it wouldn't be an alternative. They keep talking about "recombination", It is a misnomer, it should be just "combination", it's a bit of an in-joke actually. and BHs do tend not to stay one size... as they ingest matter. It could start out as a shredder, and end up as a flocculation pond (very slow agitation, that enables agregation of molecules into skimmable or sinkable structures) snip Our hole could have formed in an early Universe, and our hole could have consumed its companion(s) early on too. Or we could have shredded whatever we got first... somehow I want to believe we are much bigger than this. Bigger than infinite? Do you really mean you want to believe there an "outside" which is older than this? See Guth. No, I want to believe in an outside that is disjoint-in-time from us. Then that is 'new physics' No, it isn't. I'll continue to disagree on that. It is a choice of model. And it is potentially observable/falsifiable. What I meant by "much bigger than this" is, I think we have too much mass evident today, to have made a small BH as a "youth". Too much??? There is only 4% of the critical density as baryonic matter and even dark matter only brings it up to about a third of what is required. Consider a young Universe, some 6300 ly "across", with mass sufficient to achieve a "curvature coefficient" of 1079 (compared to today). Lots of confusion there, the optical thickness of the period of recombination was 6300 ly but that happened at 380,000 years so the part of the universe which is _currently_ observable might have been 760,000 LY across and the whole universe would have been billions of light years across or perhaps infinite. The universe appears to be flat and would have been then too. The figure of 1079 is the redshift compared to today, not the curvature. That may be a small beginning, but it no less massive. It still held only 4% of the required matter in baryonic form. But I guess we had to start somewhere. ;) I just need spectrum data... the Sun, and some of the full sky surveys that mapped the CMBR... which will not do a good job with individual spectral lines most likely. Do you have some ideas where I can look? The Sun isn't going to be much use, you need spectra for everything from white dwarfs to red giants and you need to know the mix visible in the container universe from our location within it and their ages. These should be written into spectrum data near the plane of the Milky Way, in the CMBR data... assuming that is available since it is "contaminated". For the CMBR, use this link http://lambda.gsfc.nasa.gov/product/...prod_table.cfm Yes. This would be good (as a start) for a free BH, or one near our position in a "largely spiral" galaxy. I intended that as a good start for the CMBR after the removal of all stars. You need individual stellar spectra separately. A free BH has no spectrum since it is black ! Then I need to come up with a spectrum for a BH consuming a companion, Try Cyg X1 and to somehow infer the influx to the BH at the center of our own galaxy. It appears to be in a relatively clear region so is invisible. If I'm going to prepare several "broths" best to use many available spices. or Google for "firas data products". It should be on the Lambda site but that seems to be down at the moment. Thanks George. I seem to be wearing on your nerves. Not at all, though I think we have done the singularity thing to death. So I will try not to respond more than once a week. That way the "potential irritation" level is down. It takes me about an hour to key this all in, and I hope it doesn't take you nearly this long to reply. This one took about the same and I haven't looked up any new references for you. I spent another half hour or so reading the John Baez pages but I don't count that as I learn from them anyway. (Although a *lot* of thought goes into your responses.) Thanks, it's nice to know you appreciate it. I could tell you do the same and while we may disagree I hope you feel you benefit as much as me from reading the cited resources. best regards George |
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Dear George Dishman:
"George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news:yUwOe.124442$E95.97537@fed1read01... Dear Geroge Dishman, "George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news rxMe.57073$E95.48764@fed1read01...Dear George Dishman: "George Dishman" wrote in message ... Just a note, I found some of what we were discussing. No, from what I have seen, some coordinate systems stop at the horizon while other don't, but there is no physical effect there in the GR model. I found the relevant part he http://casa.colorado.edu/~ajsh/schwp.html "The Schwarzschild spacetime geometry appears ill-behaved at the horizon, the Schwarzschild radius (vertical red line). However, the pathology is an artefact of the Schwarzschild coordinate system. Spacetime itself is well- behaved at the Schwarzschild radius, as can be ascertained by computing the components of the Riemann curvature tensor, all of whose components remain finite at the Schwarzschild radius." I understand what you are saying, George. Now try these: URL:http://www.aleph.se/Trans/Global/Omega/baby.txt David, is there a way to get rid of the "URL:" part, it breaks the link in Outlook Express because the text is no longer a URL if you put "URL" in front. I intentionally add the URL:, so that Outlook Express and other readers will correctly form long links. Oh well... FWIW the links work for me. Anyway, from that link I see: A. The formation of a black hole creates "baby universe," the final singularity of the black hole tunnelling right on through to the initial "big bang" singularity of the new universe thanks to quantum effects. The phrase "the final singularity of the black hole" refers to the point at the centre and confirms what I have been saying. Later it says: "The fact that the entropy of a black hole is (at least under certain circumstances) proportional to the area of its event horizon is a curious relationship between general relativity, quantum field theory and statistical mechanics that many people believe to pointing somewhere, but unfortunately nobody is sure where. Part of the reason is that the standard derivations are somewhat indirect, and the event horizon is not a physical object, so the sense in which it is the locus of entropy is difficult to understand." Again "the event horizon is not a physical object" agrees with my view. But nothing else did, nor did it it in any particular talk about the production of an inner Universe due to a choice of metric. However, it is not important. I think it is a good question if the event horizon is even *in* this Universe. You can't measure it, you can never get information from it, you can only determine the mass that the BH contains and *infer* its position as the "asymptote" from which infalling objects might ever get light out to you. The last stable physical state not involving Steve Willner's "new physics" is well outside the event horizon. I am not asking if the event horizon is a physical object, only if it would appear to be so at the instant of the Big Bang, *from the inside*. But you know this... URL:http://math.ucr.edu/home/baez/PUB/generichole URL:http://math.ucr.edu/home/baez/gr/oz1.html There is window dressing, but he construction details of the manequins, might be there somewhere, but I did not find it. Likely it was numerical simulation of the equations of GR direct. Only the choices of "simplifying assumptions" are (perhaps) omitted, so only Andrew knows. There is a list on this page under "Caveats" http://casa.colorado.edu/~ajsh/approach.html Yes. He supposedly had a Schwarzchild solution that he was able to map across the event horizon. A nice trick. No trick needed, nothing changes at the horizon. Yes, trick needed. Schwarzchild is singular at the event horizon, as we have covered ad nauseum. Yet he managed to achieve a continuous presentation... maybe it is well behaved on either side of the EH. Then he claims that we "fall at c". And yet, this seems to be what is at hand. Imagine a duck swimming up river at 5m/s in a stream that narrows approaching a weir. As the stream narrows, the water moves faster. If the duck starts where the water flows at 4m/s it will escape but if it starts where it is 6m/s it will move towards the weir ever faster until it goes over. A singularity occurs if the width of the stream gets to zero at the weir as the speed becomes infinite, but nothing happens to the water (or the duck) where the flow is 5m/s. The analogies are fine George. Unfortunately, *to whom* does the infalling person appear to fall at c? Presumably a stationary observer, but there are on possible stationary observers inside the photon sphere, much less inside the event horizon. So what use are the words, what meaning can they convey where the context is not part of this Universe (except though total mass, total charge, total angular moementum)? David A. Smith |
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Dear George Dishman: "George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news:6twOe.124437$E95.51864@fed1read01... Dear George Dishman: "George Dishman" wrote in message ... "N:dlzc D:aol T:com (dlzc)" N: dlzc1 D:cox wrote in message news rxMe.57073$E95.48764@fed1read01...Dear George Dishman: Severly trimmed again. No, that's not true. The failure at the horizon is purely mathematical as for the pool table example, the failure at the singularity is physical. Consider that the sources that are the most active astrophysically, are black holes (with companions). Indeed, but the radiation and jets are produced in the accretion disk outside the horizon. So it isn't quite "mathematical", then is it? I don't see your point, the matter in the jets never gets nearer than r=3m while the horizon is at r=2m. My point is that the first singularity is the event horizon. It is physically not located *in* this Universe. The fact that any infalling matter starts boiling away due to collisions, even though the source of the colliding particles is (most commonly) the same companion, just adds support to my non-specular arrival of light to the inside. Physically, the Universe (and the BH) are attempting to solve the "immovable object/irresistable force" problem. No, it's more like the gravitational slingshot of a probe round a planet, it only passes nearby. .... and nearby ... and nearby ... Now consider the definition of "singularity". The event horizon *is* a singularity. No? No. The singularity is at the centre, there is nothing unusual physically at the horizon. It *is* a singularity in Schwarzchild coordinates. I quote from Wikipedia a.. mathematical singularity - a point where a mathematical function goes to infinity or is in certain other ways ill-behaved. It is also a point where all functions meet. OK, that says it is "mathematical", i.e. has no physical significance. As with any English word, it has many meanings. The event horizon meets this constraint as well. b.. gravitational singularity - an infinity occurring in an astrophysical model, involving infinite curvature (a mathematical singularity) in the space/time continuum, namely a black hole. OK, that could refer to the centre though there is nothing in the context to differentiate. "a black hole" is really clear George. It doesn't try to differentiate to "internal structure", only for what we *can* see (in some sense). It clearly doesn't refer to the center, and I didn't even write it. What is unusual at the horizon is that light cannot ever propagate away from it. In all coordinate choices, this is true. Yep, ask the duck if there is a ripple on the water at it's point of no return (see my other post). So the event horizon *is* a physical singularity, if not a physical object. Yes, that's true but if you look at a spacetime diagram showing light cones, it is obvious why that occurs and it doesn't involve a singularity. It does involve a singularity, George. As defined by the English language. A "singularity" is not always just a "point". Sorry, I should have made the distincton between mathematical and physical. There is nothing physical about the inside of BH, George. So the only flashlight we have to view the caverns where Injun Joe hid, is via mathematics. Some mathematics indicates that we might see the inside of an event horizon at the beginning of our Universe... namely the Big Bang. There is window dressing, but he construction details of the manequins, might be there somewhere, but I did not find it. Likely it was numerical simulation of the equations of GR direct. Exactly, the only 'assumptions' were the other stars he included in the hypothetical system. The ray tracing I believe is pure GR without any simplifications at all. I don't know how he did a "Schwarzchild" solution across the event horizon. Yet that is the suggestion. Indeed, it is possible and retains discrete images because the GR model does not include any physical change at the horizon. Not and use "Schwarzchild", unless it is well behaved on either side of the event horizon. Like as not, he did not use anything Schwarzchild for the "dive into the BH" animations. So we don't know what he did use. And it is not important, because it is "only mathematics", right George? No, it would be better to say "speed_path_average" since c is just a constant, 299792458m/s. Yes, sloppy talk does no one any good. Me too, see above. You pretty much kick *ss. would appear to decrease, as observed by an infinite observer. "Shapiro time delay" is an observation fully in agreement with GR. So what does it mean to say that we "infinite observers" can say stuff about physics beyond the *singularity* that is the event horizon? David, the event horizon is *not* a singularity, only certain coordinate system have an *artificial* singularity on that surface. That is the root of all our disagreements I think. It is how the word is defined, George. I'm not sure of the exact technical definition but "the boundary of the region from which light cannot escape" is probably close. See both defintions of singularity above, and the various pages you have shown me that Schwarzchild is singular at the EH. "The singularity at the center" is a non-sequitur, if you don't agree that mathematics is our road in-and-out. Some of those roads describe *our* Universe, and the "singularity at the center" as a very diffuse, cold future. You (and most other mainstreamers) place the singularity "at the center", even though this is not physically meaningful in *this* Universe. At the centre, many measures become infinite in a way that is independent of coordinates, the theory blows up and you have a singularity in the model. There is no such occurence at the horizon though some coordiante systems fail. They *all* fail, George. You yourself use the word "measure". How would you measure that which can only reliably return your signal after the black box has evaporated? The English language is really slippery, I know. But our grandiose posturings: - about how this Unvierse must be unique, - the BH must be some sort of cosmic garbage disposal, - that our continguous-reality-that-passes-for-spacetime must have a separate life of its own, and extend "recognizeably" even down into this garbage disposal, - and violate all the conservation laws just so that we can be sure that there is a "singularity at the center", is simply too much for me to believe. Yet in my hypothesis, the only singularity is the severance of one spacetime, adjoint to another (essentially identical?) spacetime. IMHO, that would be "new physics" since this doesn't happen in GR. GR is a theory, which means it has mathematics associated with it, and not as some sort of unwarranted "apendage". It has solutions for BHs. All of the solutions (that I have seen) that do an adequate job of describing massive structures, do so by either blending or replacing external space with internal time. .... This is why the r axis is referred to as "timelike". So time has a different letter in that region, it is still time. It *is* still time, but it is not outer-time. It is not related to external-time, except perhaps to be orthogonal to it. Again, this is just the model, I know. I don't want to sound as though I'm laying down the law but I think you need to stop and make some enquiries. AIUI, it isn't the model, it is the coordinates. Physically time outside the horizon and time inside are the same, it is only when you get to the singularity at the centre that the physics fails. Then we can agree to disagree. I think that's best, I doubt we will resolve this here but please note I am not rejecting any aspect of GR, just your interpretation of it. If it turns out your version is correct, I will happily acknowledge being enlightened. Well, it has been "fun", in some sense. I don't expect to be right. But I do expect me to ask the question, as clearly as possible, and defend the right for the question to "exist". .... Yes, it is worth looking but we need to correctly understand what the models say. We understand what the models say. Internal time is NOT directly correlated to external time, by all metrics than we can yet apply to BHs. That is where we have agreed to disagree. OK. "We can't know." is not very satisfying to me. It seems that "we can look" is far superior. Tough. Either we can or we can't, that is determined by reality, not our preference. Understanding whether we can or not is the best we can do. So why do you have a preference for one model over another? I don't exclude or prefer any model, other than perhaps being skeptical of "non-trivial topology" without convincing evidence, I don't like the idea of the universe being a Klein Bottle! Worse than that. A potentially infinite series of such bottles. Personally, I think it ends at step two, and "where we came from" and "where our black holes lead" is to one-and-the-same Universe, primarily anti-matter, and opposite tendency to chirality. But, that is for another life... I am not offering "new physics", I am offering that our Universe is not unique in the scheme of things. And my hypothesis is potentially falsifiable. That isn't contentious, it is only your idea of a physical singularity at the event horizon that I consideer to be "new physics" as I believe it is in contradiction to GR. Only if you consider spacetime to be "physical" is there a "physcial singularity" at the event horizon. Since: - there is no spacetime without matter/energy, - you cannot interact directly with any matter/energy starting at (really before) the event horizon, - any infall is already *NOT* in this Universe... only the gestalt is evident, - the population must therefore have its own physics, which I fully expect to be the Pauli exclusion principle, conservation of momenergy, and so on. I don't expect "new physics", I only expect continuation of *known* physics. And like those that don't want to believe that the reality-dressed-like-spacetime actually binds time to space, I see you wanting to believe that all such reality continues "unbroken" inside the event horizon. And we will agree to disagree. What is raising the question of a non-closed Universe? Without dark energy, GR gives some simple solutions for an expanding universe: 1) Density greater than the critical value means spatially and temporally finite so we have a closed universe and a big crunch. Expansion slows and reverses. A photon created at t=0 gets exactly half way across the universe when the crunch arrives. Which doesn't work too well, since we have photons arriving in all directions from even ~300,000 y after the Big Bang. Why is that relevant, there wasn't a centre as you know. Let's see. We can determine the temperature of the CMBR a "billion years ago" by observing processes in distant stars. You have arrived at 4300 6300 LY actually but never mind. I hope to hold that number. light years for the thickness of the CMBR. Seems to me like we are still receiving light that has travelled more than once around the size of that early Universe, Age now is 13.7 billion years. Hypothetically, if we were in a closed universe currently at maximum volume, the crunch would be at 27.4 billion years. In that case GR said it would take a photon precisely 54.8 billion years to get back to where it was created after going "once round". The cosmological constant changes all that though. even though it may no longer be able to make it around the size of the Universe now. So the stated condition "A photon created at t=0 gets exactly half way across the universe when the crunch arrives." is obviously not met in this Universe. Currently a closed universe seems highly unlikely as we have discussed. Agreed. You asked me "why" and I was answering that. Then I still don't understand why you said "Which doesn't work too well, since we have photons arriving in all directions from even ~300,000 y after the Big Bang". They were produced everywhere so would be arriving from all directions even 1s after the bang. And how they could have NOT been aroud the early Universe *at least once*, when it took ~300,000 years to get to a size of 6300 ly. Maybe I'm being too Newtonian about it... My figure of 6300 LY would suggest it was opaque at 372,700 years and transparent at 379,000 years. "In an instant" doesn't seem inappropriate in cosmological terms. ... but it does to a mechanical engineer! Is the "thickness" being the same order of magnitude as the global "quench" meaningful? What do you mean by "global 'quench'"? What was completed by "379,000 years". The plasma was quenched to a normal matter state. If we were expanding compressed air as an analogy, it the point at which water vapor (as opposed to steam) would form. The FRW metric has the Universe collapse again, but after many billions of years. Exactly. But it does not "solve" a spacetime that has "chunks" of mass in it. But then it too is "just a MODEL". Any solution to the equations is "just a model", the trick is to find one that matches all we can observe and then have it tell us about things we can never see. That's my kind of "what if ...". But that isn't science, George. Isn't it? Basing our extrapolations on models derived from observation instead of philosophy or religion seems to me to be precisely what science is about. Models involve mathematics, George. The z of the CMBR can be thought of as produced by motion of the source away from us but it can also be considered as similar to gravitational redshift or a stretching of the wavelength of the photon while it was travelling through space that was being stretched. That sucked when Paul Lutus was feeding it to me. It is a standard way of expressing it. I'm not keen myself but I think the three descriptions are effectively equivalent while appearing different in the same sense as wave/particle duality. But it requires that the photon give up some of its energy, yet retain the vector portion of its mometum entirely intact. We don't know how to do that. A photon, once emitted, can be absorbed or scattered. It cannot be "stretched". The red shift of supernovae duration is similarly red shifted to its emission spectra. The light emitted is characteristic of the process that emitted it, the local curvature in which is was emitted, the global curvature of the Universe that emitted it, the global curvature of the Universe that detected/absorbed it, and the local curvature of the detector. Nothing was "stretched", any more than it is between the Earth's surface and the GPS satellites, or between the surface of the Sun and here. I hear your assertion. It is just a lot longer to say... ;) Ignoring my 'proper motion' part, the kinetic motion and the " |