Freitag, 11. November 2016

Dip Day 1519 in Detail

Solving the puzzle of Dip 1519

This post continues the analysis of different dips seen by the Kepler telescope at Boyajian's star (KIC 8462852). To understand the discussion, I recommend to read the analysis of Dip 792, because I use the same basic model.

Again a Starlift model

The very useful starlift model of the last post is reused to understand the very complex signature of the dips around day 1519, as presented in fig 1.

Fig 1: Komplex deep Dip 1519
The dip includes a very deep double dip, with 22% absorption, and a asymmetric basic structure, similar to dip 792.
My idea was, to use the simulated shape of a starlift with "smoke" as described in detail in Dip 792, to understand the shape 1519. Therefore the shape was positioned three times in the time frame with different position in time and different absolute absorption.
The result is shown in fig 2.


Fig 2: A first attempt to reproduce dip 1519

The simulated black line does not reproduce the blue measured values, but some very significant elements are well done. First of all, the double asymmetric main dip fits just perfect. And this was done by simple adding the model of Dip 792 with the same intensity, the factor is in both cases exact 1.0 (one)!
The first deep dip is deeper than the second, the reason is, that the "smoke" of the second dip deepens the first. The numerical distance in time was set to 5h. The length of the starlift beam is 1.50 higher as in dip 792. This also means, that the orbit of the smoke in this simulation is by a factor 1.50 further away as in dip 792. 

To complete the picture, a third starlift beam was introduced 12.5h before the main dip.  
The factor for this dip is 0.36789. Ever seen this number? It is 1/e, but it seems so, that value is by accident similar.
e is the very well known Euler number 2.7182.... the number of natural growth and the mathematical basis for the success of any civilisation. (More about e at wikipedia)

Some Problems

But the simple model does not reproduce the measured line in all parts. In the area A, B and and C, the signal is brighter than it should be. There are two possible explanations:
  1. The starlift beam had some interruptions and so the smoke has some breaks.
  2. The material of the smoke was used for construction and is no longer at this place in the orbit.
If we like solution 2, then it is not to hard to understand bumper D in fig 2. It might be some material in the orbit, it could even be a mirror to power the starlift itself. But this is pure speculation. 
A better solution is given as hard puzzle to the reader.

Thank you for reading and please give me feedback. 
Hopefully a paper, concerning this research is soon completed.

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