consider a toy universe and galaxies A, B, C, D at three different instants of cosmological times, t = 1, t = 2, and t = 3.
At times t = 1, t = 2, and t = 3, the proper distances to galaxies A, B, C, D are given by the table:
[tex]
\begin{matrix}<br />
& | & A & B & C & D \\<br />
-- & | & - & - & - & - \\<br />
t = 1 & | & 1 & 2 & 3 & 4 \\<br />
t = 2 & | & 4 & 8 & 12 & 16 \\<br />
t = 3 & | & 9 & 18 & 27 & 36<br />
\end{matrix}[/tex]
At times t = 1, t = 2, and t = 3, the recessional speed of galaxies A, B, C, D are given by the table:
[tex]
\begin{matrix}<br />
& | & A & B & C & D \\<br />
-- & | & - & - & - & - \\<br />
t = 1 & | & 2 & 4 & 6 & 8 \\<br />
t = 2 & | & 4 & 8 & 12 & 16 \\<br />
t = 3 & | & 6 & 12 & 18 & 24<br />
\end{matrix}[/tex]
What are the values of the Hubble constant [itex]H[/itex] at the three times? Since [itex]v = H d[/itex], the Hubble constant is given by [itex]H = v/d[/itex]. This give that [itex]H[/itex] equals 2, 1, and 2/3 at times 1, 2, and 3.
Note: 1) at each instant in time, the Hubble constant is constant, i.e., independent of the galaxy used to calculate it; 2) the Hubble constant decreases with time.
What about acceleration or deceleration of the expansion of this universe? During the time interval from [itex]t = 1[/itex] to [itex]t = 2,[/itex] Galaxy A "moves" a distance [itex]\Delta d = 4 - 1 = 3[/itex]. During the later but equal-length interval from [itex]t = 2[/itex] to [itex]t = 3,[/itex] the same galaxy, Galaxy A, "moves" a greater distance, [itex]\Delta d = 9 - 4 = 5[/itex]. This is an indication that the expansion of the universe is accelerating. The fact that this universe is accelerating is independent of which galaxy is used.
This toy model is a Freidman-Robertson-Walker universe that has its scale factor given by [itex]a(t) = t^2.[/itex]