On Feb 12, 2006, at 10:30 AM, [EMAIL PROTECTED] wrote:

There's a good bit of chatter on the esoteric portion of the www about the world's waning wobble. Here is the actual data:

http://maia.usno.navy.mil/plot-eop.html

Some attribute this to the Great Rat of Sumatra or the earthquake in that area. But is this a chicken or an egg?

I don't know what the "this" in the above sentence references or what the Great Rat of Sumatra is or what earthquake you reference, so I'm a bit lost here!

This is indeed a neat web site - I wish I had more time right now to look into it:

http://maia.usno.navy.mil/


I will say the length of day (LODS) data is nice evidence for a periodically changing gravimagnetic field. It demonstrates gravimagnetic induction due to a changing gravimagnetic field: dK/ dt. To make sense of the data it seems reasonable to do a Fourier analysis on it (as well as positional data) to look for unexpected influences. It looks like there is 329 day cycle in the positional data, and that period doesn't look familiar offhand.

It looks like a Fourier analysis might account for:

UT2-UT1 = 0.022 Sin(2*pi*T) - 0.012 cos(2*pi*T) - 0.006 sin(4*pi*T) + 0.007 cos(4*pi*T)

where T is in Besselian years, i.e approximately years. However, it is very strange there should are biannual variations.

There is also noted a long term (secular) slowing trend in the Earth's rotation. The web site notes: "The ancient observational data form the basis for estimates of the secular deceleration in the speed of rotation. ... The secular variation of the rotational speed seen by the apparently linear increase in the length of the day is due chiefly to tidal friction. The Moon raises tides in the ocean diminishing the speed of rotation. This effect causes a slowing of the Earth's rotational speed resulting in a lengthening of the day by about 0.0015 to 0.0020 seconds per day per century." I would note there are additional reasons for such a secular trend. These are (a) continual buildup of meteoric dust on the Earth, thus increasing the moment of inertia I and thus decreasing angular velocity, and (b) global warming. It may also be true there is a secular decreasing or increasing of the ambient gravimagnetic field.

Global warming increases the Earth's diameter by crustal expansion. If there were a steel ring about the Earth's equator, and it increased in size by 0.01 percent due to thermal expansion, then, ignoring warping, crunching and crinkling of the band, the Earth's diameter would increase by 0.01/Pi percent. This too thus increases the moment of inertia I_earth and thus decreases angular velocity. I would also point out that secular variations in Earth's moment of inertia cannot be accounted for by atmospheric variation because average wind speed is limited to the speed of sound.

However, the secular trend in angular velocity change appears to be *very very small* when looking at long term data! See:

http://141.74.1.36/MainDisp.csl?pid=95-103

It shows angular velocity lows around 1696, 1752, 1811, 1846, 1887 (small min), 1894, 1902, 1912, 1945, 1993. See Table 1 below.


Yr   dt(Yrs) w_earth(prad/sec)
1696    0    151
1752   56    151.2
1811   59    151.42
1846   35    151.12
1887   41    151.50
1902   15    148.34
1912   10    148.18
1945   33    150.28
1993   48    149.47

Table 1 - Relative minimum angular velocity points



It looks like we should throw out 1902 to get Table 1A.


Yr   dt(Yrs) w_earth(prad/sec)
1696    0    151
1752   56    151.2
1811   59    151.42
1846   35    151.12
1887   41    151.50
1912   25    148.18
1945   33    150.28
1993   48    149.47

Table 1A - Relative minimum angular velocity points

Similarly, we have the maximums in Table 2.


Yr  dt(Yrs) w_earth (prad/sec)


1725    0   151.4
1797   72   152.3
1827   30   152.73
1867   39   153.91
1891   24   151.96
1934   42   151.53
1988   54   150.35

Table 2 - Relative maximum angular velocity points

Combining Tables 1a and 2, and approximating a relative dW/dt the gravimagnetic induction, we have table 3.

Yr   dt(Yrs) W       dW    dW/dt

1696    0    151
1725   29    151.4  +0.40  +13.8
1752   27    151.2  -0.20   -7.4
1797   45    152.3  +0.10   +2.2
1811   14    151.42 -0.88  -62.9
1827   16    152.73 +1.31  +81.9
1846   19    151.12 -1.61  -84.7
1867   21    153.91 +2.79 +132.8
1887   20    151.50 -2.41 -120.5
1891    4    151.96 +0.46 +115.0
1912   21    148.18 -3.78 -180.0
1934   22    151.53 +3.35 +152.2
1945   11    150.28 -1.25 -113.6
1988   43    150.35 +0.07   +1.6
1993    8    149.47 -0.88 -110.0

Table 3 - Extreme angular velocity points

We can see there were some wild ambient gravimagnetic field fluctuation from 1860 to 1945, with a peak around 1912, and it looks like the wild swings in gravimagnetic induction are about to come back.

A wild and unjustified speculation follows! At first glance this gravimagnetic induction data looks like it arises from a pair of mutually orbiting black holes that do not have parallel alignment of their spin axes. Interestingly, a period of about 0.9 years shows up in the polar data at:

http://maia.usno.navy.mil/plot-eop.html

So, the speculation is the Earth local gravimagnetic induction is due to wild variations in Earth's ambient gravimagnetic field due to the mutual torquing of two black holes when in close proximity. Their mutual orbital period is about 40 years, with wild variations in orbital parameters and precession when in close proximity caused by their powerful mutual gravimagnetic influences. An overall cycle of 191 years is due to departure of the black holes from close proximity and thus the powerful mutual gravimagnetic influences, which are a 1/ r^3 effect. It looks like the black holes may have a mutually caused precession rate of about 0.9 years with a beat frequency of about 7 years. It looks like things are heating up between them, and a really big merger event is not far off - within a millennium.

Speculation shield off.

Lots of calculation and modeling are required to make certain sense of the data. Coincidentally, I already have a nice chunk of the computational capability required to do this, but not the time.

Horace Heffner

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