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| Tags: bang, big, measurement, time |
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#1
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Physicists and astronomers use conventional units of time in speaking
of the Big Bang ("one second after the Big Bang", etc.). But how meaningful are such statements? If time and space are local and depend on the relative velocity of the observer, how can our own local definitions of time (seconds, minutes) be used to describe an interval of "time" during Big Bang conditions? If I were to ask whether the first "second" after the Big Bang was of the same duration as an earth-based second, would it be a meaningful question? |
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#2
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#3
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Wendy Yamamoto:
Physicists and astronomers use conventional units of time in speaking of the Big Bang ("one second after the Big Bang", etc.). But how meaningful are such statements? That depends. Unless something very surprising pops up, what happened on the order of a second is pretty sound. By looking at the current temperature and size of the universe and then extrapolating backwards, it's possible to get much more detailed than one second. We know the strength of the weak and strong interactions and since unification of those forces happens at specific temperatures, it's fairly straight forward to provide a picture of the universe beginning around the first 10^-40 seconds or so. Steven Weinberg's book, "The First Three Minutes" gives a very good and easy to read account of exactly what the title describes. If time and space are local and depend on the relative velocity of the observer, how can our own local definitions of time (seconds, minutes) be used to describe an interval of "time" during Big Bang conditions? Measurements made by different observers can be reconciled because relativity describes the relationship. Essentially, all observers should agree that the universe started at the same time. If I were to ask whether the first "second" after the Big Bang was of the same duration as an earth-based second, would it be a meaningful question? That again depends. If there are no surprises, then presumably a second is a second is a second, at least until you get below 10^-40 (or perhaps 10^-50) seconds or so. At that point, I'm not sure it would be meaningful to think of the universe in those terms. That would be the era of quantum gravity and neither E&M or nuclear forces would have existed. |
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#5
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Because all observers are attached to galaxies, everyone is assumed to
be moving along with the bulk flow matter in an expanding universe. So everyone agrees to the meaning of "cosmic time." http://www.everythingimportant.org/r...multaneity.htm Eugene Shubert |
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#6
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#7
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You say "If there are no surprises, then presumably a second is a
second is a second . . ." But wait. Let's take a conventional illustration of relativity, in which one twin brother leaves earth in a rocket and approaches the speed of light in it. After a few rocket-days, he returns to earth, only to find his earth-twin (and everybody else) greatly aged. This is a trip taken in contemporary time and conditions. Yet a second wasn't a second at all. The seconds were relative. But in this case, I assume a mathematical correlation could easily be drawn between a rocket-second and an earth-second. If I understand you correctly, you are asserting that a similar correlation can be drawn between a Big Bang second and an earth-second using a scale provided by the unity of forces that occurs at a certain "temperature". Has anyone ever done so? I for one would find it quite interesting to learn that the first second after the Big Bang was equivalent to (say) a thousand earth-years --- or whatever the correlation is! |
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#8
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On 8/28/2003 2:59 AM, Wendy Yamamoto wrote:
Let's take a conventional illustration of relativity, in which one twin brother leaves earth in a rocket and approaches the speed of light in it. After a few rocket-days, he returns to earth, only to find his earth-twin (and everybody else) greatly aged. This is a trip taken in contemporary time and conditions. Yet a second wasn't a second at all. Sure it is, when considered LOCALLY. To each twin, for every second along their journey, clocks behave as normal, and at all times a collocated and comoving standard clock will agree with the twin's clock. What relativity requires one to do is abandon the notion of "universal time". Elapsed proper time can VARY for different trajectories, even though standard clocks are used throughout. It really does not make sense to try to fit that into a statement like "a second wasn't a second" -- each second WAS a second, it's just thar your statment makes assumptions about seconds (really "time") that do not hold (in either SR or the real world). The seconds were relative. Not to either twin -- they each observed normal seconds on their own clock. You need to learn to not make global or absolute assumptions. I for one would find it quite interesting to learn that the first second after the Big Bang was equivalent to (say) a thousand earth-years --- or whatever the correlation is! The first second after the big bang (implicitly measured in the conventional way along the trajectory of one of the dust particles) was of the same duration as a second now. The physical conditions during that second were VERY different from the conditions today. Because of that, there is no useful "equivalence" between them. Tom Roberts |
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#9
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Wendy Yamamoto:
You say "If there are no surprises, then presumably a second is a second is a second . . ." Actually, what I meant by surprises was something a little more exotic, but ok... But wait. Let's take a conventional illustration of relativity, in which one twin brother leaves earth in a rocket and approaches the speed of light in it. After a few rocket-days, he returns to earth, only to find his earth-twin (and everybody else) greatly aged. This is a trip taken in contemporary time and conditions. Yet a second wasn't a second at all. The seconds were relative. That was the reason I qualified my statements with: "Measurements made by different observers can be reconciled because relativity describes the relationship. Essentially, all observers should agree that the universe started at the same time." Relativity provides the relationship between the observers which allows them to compare their measurements of the same phenomena. But in this case, I assume a mathematical correlation could easily be drawn between a rocket-second and an earth-second. You are missing the point of relativity. Relativity does not say that those seconds are different. Relativity says that those seconds are the same. What differs is the number of seconds (proper time) which each twin "travels". This is precisely the same relationship as occurs when traversing two different routes between points A and B. One route may be the shortest distance between A and B and the other route may take many twists and turns, so that the elapsed distance on the odometers differs. In that case, one does say that the miles are longer along one route or the other. One says that the miles are the same distance, but the route is longer. In special relativity, the length of the "route" is the elapsed proper time givent by (d\tau)^2 (or (ds)^2 if you prefer), not the coordinate time. If I understand you correctly, you are asserting that a similar correlation can be drawn between a Big Bang second and an earth-second using a scale provided by the unity of forces that occurs at a certain "temperature". Has anyone ever done so? Sure. The unification scale for the electroweak interaction occurs at energy determined by the mass of the W and Z, around a 100 GeV. Estimate the temperature via E = kT and you get a temperature of af about 10^15 K. The situation is not so clearcut for unification with the strong force, but the masses of those gauge boson is presumed to be on the order of 10^16 GeV, which places the temperature at the order of 10^28 K. Gravity is expected to be unified at the energy of the planck mass, which is around 10^19 GeV which is a temperature of about 10^32 K. Now, if you take the planck time to be the time at which gravity separates from the oother three forces, you have a time of 10^-44 seconds. From the temperature and statistical mechanics, you can determine how much the universe would have expanded in order to cool to the temperature at which thestrong interaction separated from the electroweak and then the electromagnetic force separated from the weak force. From this you can determine how large the universe had to be before atoms could form so that the universe becoms transparent to the electromagnetic radiation (e.g. light) that is what we see as the cosmic microwave background radiation. I for one would find it quite interesting to learn that the first second after the Big Bang was equivalent to (say) a thousand earth-years --- or whatever the correlation is! One could speculate about those sorts of things but in reality, it doesn't really make sense to do so. We _define_ a second, so essentially, the value we give for the passage of time is what it means in our terms. The one place such speculation might be considered is during inflation, which is called inflation because in our view of looking at things, the universe expanded much more rapidly than the speed of light, which is how we define a second. It's not clear to me that this definition is really meaningfull during that era and that inflation is more a product of definition than what would be called inflation to "observers" at that era, but that is rather speculative and I haven't looked at inflation enough to see whether the reason it's not clear is simply due to not knowing enough about it for it to be clear. |
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#10
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=?ISO-8859-1?Q?Gy=F6rgy_Szondy?=:
(Bilge) wrote in message ... Wendy Yamamoto: Physicists and astronomers use conventional units of time in speaking of the Big Bang ("one second after the Big Bang", etc.). But how meaningful are such statements? That depends. Unless something very surprising pops up, what happened on the order of a second is pretty sound. By looking at the current temperature and size of the universe and then extrapolating backwards, it's possible to get much more detailed than one second. We know the strength of the weak and strong interactions and since unification of those forces happens at specific temperatures, it's fairly straight forward to provide a picture of the universe beginning around the first 10^-40 seconds or so. Steven Weinberg's book, "The First Three Minutes" gives a very good and easy to read account of exactly what the title describes. If time and space are local and depend on the relative velocity of the observer, how can our own local definitions of time (seconds, minutes) be used to describe an interval of "time" during Big Bang conditions? Measurements made by different observers can be reconciled because relativity describes the relationship. Essentially, all observers should agree that the universe started at the same time. Big Bang assumes that the worldline of all particles started at the same point. Threfore you can observe the univerese from the perspective of any particle (or object) and use its time. You missed the point. What she was asking was in regard to observers who have relative velocities with respect to each other and therfore must reconcile their measurements. Those observers will see the same phenomena differently. That is why I qualified that the way I did. Had I simply left it as you've stated it, I wouldn't have answered the question being asked. That again depends. If there are no surprises, then presumably a second is a second is a second, at least until you get below 10^-40 (or perhaps 10^-50) seconds or so. At that point, I'm not sure it would be meaningful to think of the universe in those terms. That would be the era of quantum gravity and neither E&M or nuclear forces would have existed. Second is measured by clock. Time in General Relativity is also defined by clock. Therefore 3 second is allways the same length of time by definition. What do you define as a clock when there is nothing to use as a standard clock? We use the speed of light, but since light did not exist before electroweak symmetry breaking, this is obviously not a universal definition. One could presume the constant c is more fundamental that the phenomena to which it applies, but I think that can only be justified to a point and I am not sure it can be justified at all prior to the planck time. If general relativity breaks down at the planck time, then I don't think that you have any real means of defining time and distance in any way that resembles the definitions used in general relativity. |
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