On Friday, December 2, 2022 at 4:53:22 AM UTC-6 [email protected] wrote:

> The definition of the Hubble Constant implies the rate of expansion slows 
> as time advances. I don't see that the two values contradict this 
> conclusion. AG
>
>
The FLRW expansion factor is exp(Hd/c), where Taylor's theorem means 
exp(Hd/c) = 1 + Hd/c + 1/2(Hd/c)^2 + ... . For small distance d we have 
exp(Hd/c) =~ 1 + Hd/c, and for Hd = v this is exp(Hd/c) =~ 1 + v/c. To 
convert this to a time dependent expansion then d = ct.

LC
 

> On Friday, December 2, 2022 at 3:24:35 AM UTC-7 Lawrence Crowell wrote:
>
>> Red shift data from supernovae SN1 give H = 74km/sec-Mpc. The velocity of 
>> a region at distance d is v = Hd. Using the CMB data H = 70km/sec-Mpc. The 
>> two data points appears distinct at a rather high sigma.
>>
>> LC
>>
>> On Friday, December 2, 2022 at 3:15:15 AM UTC-6 [email protected] 
>> wrote:
>>
>>> It's measured about 70 km/sec/megaparsec. This is a direct measurement 
>>> using red shift to measure recessional velocity, and different standard 
>>> candles depending on the distance. So, at a distance of one megaparsec, the 
>>> expansion rate is 70 km/sec; at two megaparsecs the expansion rate is 140 
>>> km/sec; and so on. This suggests the rate of expansion is greater as we go 
>>> back in time; or conversely, that the rate of expansion is slower as we go 
>>> forward in time. How is this reconciled with the 1998 measurements that the 
>>> rate of expansion is actually speeding up? AG
>>
>>

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