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EXAMPLE 6. THE SHORT PERIOD SUNSPOT CYCLES SYNCHRONIZED WITH THE EARTH DAY.
There are four short period sunspot cycles. These periods are:- 24.011 Earth days, and 32.955 Earth days, and 26.871 Earth days, and 24.142 Earth days. There is also a Sun Oscillation Period of 0.1111111 Earth days.
(A). During 24.011 Earth days, Earth rotates (in relation to the Sun) 24 rotations + a residual angle of 3.96 degrees.
The 32.955 Earth days period “fails” the octant rule.
(B). During 26.871 Earth days, Earth rotates (in relation to the Sun) 26 rotations + a residual angle of 313.56 degrees.
(C). During 24.142 Earth days, Earth rotates (in relation to the Sun) 24 rotations + a residual angle of 51.1 degrees.
(D). During 0.1111111 Earth days, Earth rotates (in relation to the Sun) an angle of 40.0 degrees.
Sample calculation – 24.011 Earth days:- 0.011 x 360 = 3.96 degrees. That is:- 24 rotations of Earth + a residual angle of 3.96 degrees.
When you depict each of these four residual angles as a (single line) radius, the four radiuses look like this:-
When you depict each of these four residual angles as a (single line) radius, the four radiuses look like this:-
The material on this web site is also available in the book Astronomy - The Dishonest Science, by Roger Elliott (available on Amazon)
The material on this web site is also available in the book Astronomy - The Dishonest Science, by Roger Elliott (available on Amazon)
Once again, it is glaringly, blindingly obvious that these residual angles are NOT randomly distributed, as they absolutely SHOULD be if Newtonian Physics alone governed the movements of celestial bodies. (The gravitational field of Earth is insufficiently strong to alter sunspot cycles) Once again, these residual angles all (mysteriously) “hug” the octants. “Something else”, other than Newtonian Physics, is influencing and dictating these sunspot cycles.
The statistical odds against these residual angles “hugging” the octants so closely are in excess of 1 chance in 46.
These odds are calculated in the following manner:-
the largest deviation from an octant is 6.1 degrees (Item C.)
Number of trials = n = 5 and number of successful trials = r = 4 and the probability that any single specific trial will be successful = p = (6.12 x 2 x 8) ÷ 360 = 0.272 and the probability that any single specific trial will be unsuccessful = 1 minus p = 0.728
p(r ≥ 4) = 5C4 x 0.7281 x 0.2724 = 0.019924
+ 5C5 x 0.7280 x 0.2725 = 0.0014888
SUM = 0.0214 or 1 chance in 46. In fact, the odds are longer than this, because some of the deviations from an octant are smaller than 6.12 degrees.
To verify numerical data, go to Appendix 2. Section 1 for all Sun cycles and periods. (Note:- Numerical data verification is only available in the book.)
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