A bit of time

I am deathly ill with my inner problem, the world is broken into pieces and I'm nauseously destabilized.  I worked at the office and care barely remember the work although it was productive enough to use.  If this post spins out of control, it will come back in control eventually.

Time is defined in this post consistent with the others but with slightly more detail.

The next post will discuss the subext of these transition where you eliminate relative ct1 substitution even though your subsequent states are made up of parts where the substitutions are required.  For this reason, you must limit ct1 substitution to 1 or essentially one in transitional states, to get to ct2 and ct2 approaches the limit of 1 to get to ct3 and so on resulting from the equations to give the force limit characteristics that we use when discussing these for differential equations.

The transition for jumping ct states is achieved by reducing the solution order to one of the preceding states between the next to one and it looks like this:

It begins with Positive/negative/positive/negative/positive/negative or -1^n.  This creates a pre-space environment where there is no space between solutions because there is no space.  What remains is solution order.

One thing that this drawing shows is that there are many way to arrive at this solution, but the -1^n is observed so it is likely that the building block of ct0 is built by -1^n.

The next step is where you create space ct0-ct1 which is theorized as a pairing two opposite charges and putting the pre-space ct0 between the two paired sets. In effect you are adding a non-space between solutions for space to create the next level, geometry.

For ct1 to follow this pattern, you must have one ct1 coming in on one side at a1 and one going out on the other side at aa2 for the photon shown.  

The movement of trading states up to the point of the transition out for ct2 will give waves their length.  but at this point we are only looking at a photon and this gives them their speed, one ct1 in to move forward, one ct1 going out to keep the photon in place.

They may break by making this exchange at some other point, eg aa1, presumably. which would change the direction of the photon or dissipate it as a ct1 solution is introduced somewhere which pushes the ct1 out of its orbit, creating a curved set of points, magnetism.

If more than one ct1 intervenes at the ends there is no effect, but in the middle, it turns the ct2 into a transitional state.

This limit as the spacing approach is made to one (not zero) of the prior state compression occurs.  Time is nothing more than the difference between ct1 substitution and the other substitutions that take place as a result of the ct1 substitution being limited by compression.

This idea will be expanded on in the next few chapters.

The initial sketch of this is preserved.

There are some permutations to this but the general idea of time is that it is the absence of ct1 substitution in ct2 and higher solutions relative to higher state solutions.  Since all states are made by ct1 substitutions, this ratio appears most likely and it is a matter of solution order.

As one type transitions to the next compression level (gradually or otherwise) you get another dimension and a higher level of substitution.

It is a linear issue.   Ct1 separation is reduced to 1, creating a first dimensional ratio, ct2 separation is reduced to 1 creating a second dimensional ratio (2 to 3); and so on until you have the three observed and one indirectly observed spatial ratios.