- #71
twofish-quant
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Drakkith said:Perhaps I am mistaken, as I don't have a good grasp of the math of all this, but isn't the accelerating universe model the "best fit" to the data?
I don't think this is a good way of thinking about the problem. Since "best fit" really means nothing. The problem is that the reasoning is circular. In order to have a "best fit" you have to have a model of the problem which is a problem if you don't understand what is going on. If you don't have a model for what is going on, then how can you tell if one fit is "better" than another?
One reason I'm arguing with RUTA is that I do think we would have a serious problem if cosmologists were doing what he thinks they are doing, but they aren't.
What is better is to look at the data, go through all of the possible explanations, and then see which ones are excluded and which ones are allowed. As you get more data, the number of viable explanations goes down.
Would assuming that DL=(1+z)Dp is true only for small Dp be a less reasonable assumption than assuming it is true for all values?
Doesn't matter. The problem is that when you are dealing with unexpected data, there is no basis for figuring out what is a "reasonable assumption." So what you do is to assume that you've got the relationship wrong, and then see what happens.
In fact, what happens is that you end up with a Taylor expansion, and for small z, the first term is (1+z)Dp.
Do we have any real reason for believing that?
GR says that DL *isn't* (1+z)Dp for curved spacetime. However GR also puts some limits into what the relationship between DL and Dp can be.