| 
 |  | t  |  
| 14 |  
| 13 |  
| 12 |  
| 11 |  
| 10 |  
| 9 |  
| 8 |  
| 7 |  
| 6 |  
| 5 |  
| 4 |  
| 3 |  
| 2 |  
| 1 |  
| 0 |  
 
 | 
| H |  
| 25,81 |  
| 21,05 |  
| 17,76 |  
| 15,06 |  
| 12,74 |  
| 10,72 |  
| 8,94 |  
| 7,35 |  
| 5,94 |  
| 4,66 |  
| 3,52 |  
| 2,50 |  
| 1,57 |  
| 0,74 |  
| 0,00 |  
 
 | 
| H1 |  
| 1,066 |  
| 0,984 |  
| 0,904 |  
| 0,824 |  
| 0,745 |  
| 0,667 |  
| 0,589 |  
| 0,513 |  
| 0,437 |  
| 0,363 |  
| 0,288 |  
| 0,215 |  
| 0,143 |  
| 0,071 |  
| 0,000 |  
 
 | 
  
 | 
The table on the left consists of three columns.
 
- The left column shows the time since the Big Bang in increments of 1 billion lightyears.
 - The middle column "H" shows space expansion in increments of 1 billion lightyears starting from the Big Bang
 - The right column "H1" shows space expansion in increments of 100 million lightyears starting 1400 million years ago from present.
  
The right column shows a clearly linear relation for the first 1 billion years, as described by Hubble's Law. 
The left column shows clearly that also for the function used in this example Hubble's Law is not valid in the first 5 billion years after the Big Bang.  
Figure 2 shows that the speeds involved near the 100% line are much larger than c, assuming that the Cosmological principle applies.
  | 
 
 
 |