time dilation part 4

Time dilation requires a special relationship between CT1 and the "aging" of the higher time states.

Figure 9-TIME DILATION

Referring to Figure 9 we see several ways to approach time Dilation which appears largely related to “which” ct1 sets a higher state passes through.

All quantum points are believed to change at the same rate (hence unlike Einstein, there is no independent time on a quantum level) but in A-Time dilation in Figure 9 the matter particle symbolized by eight circle points on the left is passing through (changing at same rate) 4 ct1 states for the one ct1 state experienced by the one on the right.  This would give a perception of slowed time for the faster moving left spiral than the slower moving right spiral relative to the single ct1 state.

This simplified model ignores that ct4 states pass through millions of ct1 states every second even in the relatively still environment of standing still on the surface of earth, so each one of the circles in Figure 9 representing millions of ct1 states.  What this model indicates is that time is not held in the matter itself, but is instead based on the ct1 states.

The middle figure in Figure 9 shows the catching up effect of time dilation.  Eventually all times must merge under the model. The change must be a change relative to certain ct1 states verses another set.  This may be viewed as shown in the bottom drawing where the similarity or difference between the ct1 states.
Compression indicates that at some point, the amount of change will catch up and that this is the "relative change" that we use in order to have the appearance of manipulating a one change at a time in only one direction can occur.

Similarly, in an “accelerated” ct4 state will, by definition of the solution, combine with more ct1 states in terms of sharing a common solution over a period of time, so that the accelerated ct4 state will have less acceleration relative to any one individual ct state.  Looking to the middle drawing, it can be seen that one, the ‘younger’ ct4 state passes through four ct1 states during a given period of time relative to the other, the “old” ct4 state.  The solution holds that as to any one ct1 state the younger ct4 state has aged less, in this case ¼ less.  This process is happening so quickly (given the 10^-47^th of a second quantum change speed) that it is not easily observed except as a gross function of acceleration.

Figure 10

The most likely mechanism for this is shown in Figure 10 which shows multiple ct1 states intersection with a single ct4 state (along with a ct3 state and unlabled ct2 state) during a given period of time as the “apparently older” because it does not split its “age” with as many ct1 states during a certain number of intersection points which correspond to quantum moments.