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Basic Hubbles Law Concepts. |
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| Jan12-13, 04:37 AM | #1 |
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Basic Hubbles Law Concepts.
Okay so if I'm correct, Hubbles red-shift relationship was first established via expecting a doppler shift - a change in the observed wavelength (perspective of reciever at the time of reception) with respect to that emitted (perspective of the emitter), caused solely due to the respective motion between the two bodies.
However the cosmological red-shift was then dedcuded via the fact that a correlation between the distant of the galaxy and the recession velocity was sufficiently significant. My questions are: - Is it correct that if the red-shift was solely down to the doppler shift, such a correlation would not be expected following the cosmological principle - all red-shifts observed, if data is collected on a wide enough scale would cancel due to the isotropy and homogenity tof the universe? -However, I also thought that Ho was determined via taylor expansion, and so assuming sufficiently small distances/redshifts , such that all terms can be neglected expect the first one giving arise to the linear relationship. But these two seem to contradict one another? Thanks very much anyone who can shed some light on this. |
| Jan12-13, 03:17 PM | #2 |
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It is true that Hubble assumed v = cz in interpreting redshifts as velocities, and arriving at Hubble's law. I would have to refresh my memory by running some numbers, but I think the redshifts out to which v = cz is a valid approximation still correspond to cosmological distance scales, much larger than the distances at which the Hubble flow begins to dominate over peculiar motions. That's why his assumption worked (meaning that he was able to draw the right conclusion: Hubble's Law). That's also my explanation for why there is no "contradiction" of the type you were worried about. EDIT: This doesn't seem like homework, so I'm moving it to the Cosmology discussion forum. |
| Jan12-13, 06:21 PM | #3 |
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| Jan13-13, 03:28 AM | #4 |
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Basic Hubbles Law Concepts.If the Universe is not expanding or contracting and not perfectly homogenous then matter tends to gather together into a point. The expansion prevents this. |
| Jan13-13, 03:54 AM | #5 |
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| Jan13-13, 01:05 PM | #6 |
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However, if your ice cream scoop were too small, you'd find that the two scoops might differ quite drastically in matter distribution. This is because the universe is fairly inhomogenous on small scales. You look and you see a galaxy cluster "over here", and a giant void with no galaxies "over there." Clearly, there are dramatic variations in the density of matter on these scales. In the very early universe, all the matter was in the form of a very smooth (i.e. mostly homogeneous) gas with some mean density. However, the gas was not perfectly homogenous. There were tiny fluctuations in the density. Maybe the gas was slightly over-dense "here", and slightly under-dense "there." These variations were the key to why there is structure in the universe today, because they grew under their own gravity to form gravitationally-bound structures (stars, galaxies, and clusters of galaxies). If there had been no such variations, then all the matter in the universe would still be in the form of a smooth, featureless gas today, and we wouldn't exist. Anyway, the peaks in the density distribution of matter are the places where there are now clusters of galaxies: the largest gravitationally-bound structures in the universe. On scales smaller than this, things are quite inhomogeneous, and the velocity of objects relative to each other is a result of local conditions e.g. since there is inhomogeneity, maybe locally there is some large central mass concentration whose gravity is affecting everything else, like the Great Attractor, or the central cD galaxy in a cluster. Galaxies in a cluster are bound to each other, meaning none will escape, but they buzz around the centre of the cluster like bees in a bee hive, interacting gravitationally in complex ways. So, for an astronomer in one of those galaxies, the other ones in his local universe would probably have a statistically pretty random distribution of Doppler shifts, since he is looking on a spatial scale where things are gravitationally-bound, and so the peculiar motions of those galaxies dominate over the Hubble flow. This is true in our Local Group: the Andromeda galaxy is blueshifted. This is what I was talking about when I referred to peculiar motions, and it is probably the case in both the static and non-static universe scenarios. I would be willing to believe that, ignoring expansion, peculiar motions would be minimal between extremely large matter structures in the universe (e.g. galaxy superclusters and the great "walls" and "voids" in the sponge-like large-scale structure) due to the large scale homogeneity. |
| Jan24-13, 11:08 PM | #7 |
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@ Cepheid #2: We have an FAQ about this: http://www.physicsforums.com/showthread.php?t=508610
I read the above referenced thread referred to in your post here (#2). Not to be picayune, but the following phrase in that thread is not an accurate statement: The expansion of the universe was originally discovered by Hubble... I think it would be more accurate to state there that: The expansion of the universe was predicted by the models developed by de Sitter and LaMaitre, and the data reported by Slipher, Hubble and others indicating a systematic red shift in the spectra of light received from galaxies proportional to their distance from us was accepted as confirming the expansion predicted by these models. Anyway, for what its worth. |
| Jan26-13, 11:53 AM | #8 |
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binba.....posts:
A simple reply is that these two proposals/observations are 'backwards'... in other words, the opposite is actually true. You are in good company however: Even Einstein at first thought the universe was STATIC!!! Even after HE developed general relativity. It was Hubble's observations that distant galaxies were receding from us in all directions that caused Einstein to rethink his "biggest blunder"....that the universe was actually expanding. A homogeneous and isotropic universe expands. That's the basis of the FLRW metric...the distance measure. Isoptropic and homogeneous assumptions mean that there is a uniform gravitational curvature that leads to redshift. A SIMPLIFIED way to BEGIN thinking about this classically is to maybe consider that once you start rolling down a hill of steady incline you don't stop....gravity in general keeps you moving along. If friction is high enough,sure you might stop. In the universe, that 'friction' might have been analogous to the attractive force of gravity. But Einsteins initial instinct was wrong: such gravitational attraction is NOT sufficient for a static universe, nor to stop cosmological expansion. As far is is currently known expansion will continue for all time. Cephid's second post explains very well how our cosmological model is NOT precise.....the primordial expansion 'gas' was not perfectly smooth...nor is our universe today....but over large enough scales and with the use of fine tuned observation measures in our model, we think the FLRW cosmological model does give accurate predictions. The explanations here are pretty good...even without studying all the math: Friedmann–Lemaître–Robertson–Walker metric http://en.wikipedia.org/wiki/Friedma...3Walker_metric |
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