Extracted in late September 2002 from:
West Nile Virus
Latest update 12 May 2008.
Recent changes or additions are in bold.
Key Words: astrobiology, exobiology, gamma-ray bursts, nuclear
photodissociation, solar wind
This page begins with a West Nile Virus arrival date problem,
but migrates to a possible connection between GRB 990510 and a very
unique space weather event..
The null hypothesis in the basic article is that there is no significant
correlation between whatever Venus does and new outbreaks (of unknown
origin) of West Nile Virus. The metric being used in the study is the
time differential between Venus inferior conjunctions and initial cases of
West Nile Virus in geographical regions where surface-to-surface
transmission of the disease from other terrestrial regions is
questionable.
1999 - United States
The first case of West Nile virus in the Western hemisphere has been
reported to have occurred in New York City (two dead crows) on June 29,
1999. The onset may have been about two weeks earlier. According
to a U.S. Government Accounting Office report(1), a veterinarian at Bayside
Veterinary Clinic (New York City area?) found crows with signs of
nervous system disorders in the mid-June to late July 1999 time frame. The
birds were treated. Those that survived were released.
Special Problem
If one chooses to think in terms of extraterrestrial pathogens entering
Earth's upper atmosphere one to two months prior to their
expression at the Earth's surface, then the upper atmosphere
drop-in time frame (for the June 29, 1999 USA WNV bird deaths) would
have been roughly April 29 to May 29. In the middle of that period, the
angle between Venus and Earth, with respect to the sun, would have been
on the order of 70 degrees. At that angle the solar wind should have
blown Venusian particles, biological or otherwise, well clear of the Earth.
See following diagram. This looks like trouble for the Venusian
pathogen hypothesis.
Venus-Sun-Earth angle approx 70 degrees - Normal solar wind.
An unprecedented solar wind disruption took place on May 10, 1999,
which may have some bearing on the interplanetary particle delivery problem.
From late May 10, 1999 to early May 12, 1999, NASA's
ACE and
Wind spacecraft
observed that the density of the solar wind dropped by more than 98
percent. See NASA's article:
The
Day the Solar Wind Disappeared.
This writer speculates that the unusually intense Gamma-Ray Burst
(GRB 990510), which was also detected on May 10, 1999, at about 8:49
universal time (UT), caused the solar wind disruption just mentioned.
The effects of the GRB should have been at least two-fold.
Keep in mind that the GRB radiation flashed through the solar system from
a point near the South Celestial Pole, and that most of the material
density associated with the solar wind is concentrated near the solar
system's equatorial plane. (Click
here
to see a graph of Ulysses spacecraft data regarding solar wind speed as a
function of heliographic latitude.)
The thrust of this paragraph leads to a dead end. The following
paragraph spells out the problem. The primary effect of concern,
would be that the intense light pressure
of the GRB should have imparted a northward impulse to the whole
circumstellar disk of solar wind material. The disk would have
begun levitating, so to speak, generally northward. If the rate of
the northward movement was sufficient, the disk, in its entirety, could
be removed from our line of sight to the sun. In fact, over a 17 hour
period the solar system's equatorial region became nearly devoid
of solar wind particles. (During this period the solar wind speed
in the equatorial plane tapered off to about half its normal value and
the solar wind electrons developed a northerly direction component.)
January 22, 2003 note. The light pressure scenario described above misses
the mark. The upward momentum, supplied by GRB 990510, was much too small
to get the solar wind disk "lifting" accomplished. (Maximum induced upward
velocity of the disk would have been on the order of one centimeter per
second .) That leaves the "other" effect, mentioned in the following
paragraphs, to save (or lose) the day. Quantitative details of that
exercise were "embargoed" until after the Mississippi Academy of Sciences
meeting in Hattiesburg MS on 14 February 2003. The abstract for the
author's presentation is online on page 77 of the [PDF]
Journal
of the Mississippi Academy of Sciences, Volume 48, No. 1,
January 2003. (End of January 22, 2003 note.) [The formerly embargoed
material has been incorporated later on in this article.]
The other effect, which should have occurred much more rapidly, would be
that the majority of all exposed interplanetary atomic nuclei, those
more massive than hydrogen (H1), would tend to get photodissociated
(all the way down to protons and electrons) by the Gamma radiation.
The
NASA
article, referenced above, described a paucity of heavier ions
in the solar wind. (Time frame not stated.)
"According to observations from the ACE spacecraft, the density of
helium dropped to less than 0.1% of its normal value, and heavier ions,
held back by the Sun's gravity, apparently could not escape at all."
. . . On average it takes 4.3 days for ions to travel from the Sun
to the Earth. If the sun had lost its acceleration vigor
at about the same time as the wind density began decreasing, ...
then there should have been some remarkable corresponding
... electromagnetic perturbation in the Sun's appearance
four to five days earler. The author has seen no reference to such an
event. [RSF 07 July 2003 Revised 05 Jul 2007.]
If the GRB photodissociated the heavier nuclei, then it
should have been accomplished within a fraction of a second whenever/wherever the
radiation passed through a given volume of space. Instant plasma!
Comparison of various spacecraft data has probably already resolved that
question.
Consequences of Photodissociation/Disentegration of "Heavy" Nuclei
(Added 24 February 2003.)
This new material was presented at the Mississippi Academy of Sciences
meeting in Hattiesburg Mississippi on 14 February 2003.
According to the author's Emission-Absorption-Scattering (EAS) model of
sub-quantum physics, a neutron consists of a proton with an electron in
a grazing orbit. (This viewpoint might make Heisenberg unhappy,
but it is basically consistent with the 1920's idea of nuclear electrons.)
See
Emission-Absorption-Scattering (EAS) Sub-quantum
Physics and subsidiary articles,
EAS Nuclear Glue and
EAS Neutron Beta Decay.
In the EAS model of a neutron, an electron would orbit a proton at about
0.91 times the speed of light. At this orbit speed the electrical force
between the proton and electron would be equal to and opposite to the
electron's so called orbital centrifugal force.
The orbit radius would be on the order of 1.3 fermis , i.e. 1.3 x 10e-15
meter and the orbital frequency would be on the order of 10e22 Hertz (Hz).
The upper end of the measurable Gamma ray spectrum is also on the
order of 10e22 Hz.
Whenever the frequency of a wavelet of Gamma radiation happens to
approximate the orbiting frequency of a nuclear electron, the Gamma
radiation can electromagnetically pump energy into ...
the electron's orbit. ... This
interaction of Gamma radiation with the orbiting electron can ultimately
lead to the electron's escape from the proton. (This is analogous to
pumping a swing at the proper frequency to make it's oscillations
increase in amplitude.) From the EAS viewpoint, the end result of this
process would be called neutron beta decay.
The average speed for escaping electrons in neutron beta decay should be
on the order of one half the speed of light. (They tend to be slowed the
electrical interaction between the proton and the electron.) Assuming
conservation of linear momentum for neutron decay products, the proton
decay product will have an average speed on the order of
0.5 c / 1737, or roughly 100 km/sec. That speed is about one fourth of
that for the average slow solar wind.
Whenever the neutrons in any given nucleus are induced to undergo beta
decay, then the nucleus itself will rapidly fly apart due to proton-proton
Coulomb repulsion. ( . . . )
It is postulated that extremely high energy Gamma-rays induce nuclear
neutrons to beta decay which leads to explosive photodissociation
of all the remaining nuclear protons.
[Added 7 July 2006.]
GRB 990510 illuminated the solar wind disk from a point near the direction
of the Southern celestial pole. It is speculated that the majority of the
heavier nuclei in the solar wind underwent Gamma-driven
photodissociation, which blew the solar wind apart.
[A sentence about solar wind disk lifting has been removed.]
That the density of the heavier nuclei dropped to less than 0.1 percent of
normal, can be attributed to the dissociation process, rather than
to the Sun's loss of its ability to accelerate the ions above their escape
velocities.
Regardless of what caused the solar wind interruption, it could be useful
to determine whether or not the two-day cessation could have permitted
Venusian particles to jaywalk, so to speak, to Earth, as depicted
in diagram (B).
Solar wind reduction allows jaywalker event? (Revised Diagram)
The present delivery mechanism under consideration is that Venus,
as an electrically charged sphere, accelerated charged microscopic
particles (including microbes) in its upper atmosphere, sufficiently for
them to make the roughly 100 million mile journey to Earth before the
solar wind disk regained its normal density. For this
transfer to work, as stated, the viral particles would have to
be traveling away from Venus at approximately twice the average speed of
the typical solar wind.
. . .
Any jaywalking Venus viruses that reached Earth's upper atmosphere on
around May 13, 1999 could conceivably have been doing their thing,
i.e., initial outbreaks, in the time frame of June 13 to July 13. That's
using the one to two months window mentioned above. The first
reported cases of crows with nervous disorders (birds usually get it
first) occurred in mid-June.
Diagram (C) shows the normal hypothetical delivery geometry for
Venusian particles to Earth. (In this case the August 22, 1999 Venus
inferior conjunction is being shown.) There was a resurgence of
West Nile Virus in the United States in the September-October timeframe.
Normal Venus-to-Earth Delivery System
15-17 June 2003
A talk on this subject was presented in the 10th Annual Conference of
the Natural Philosophy
Alliance (NPA), at the University of Connecticut
at Storrs on 9 June 2003. The following additions to this web article are
made in response to questions and comments raised by the conferees.
It was stated above that nuclear electrons, having orbital frequencies on
the order of 10^22 Hz could be electromagnetically "pumped out of orbit"
by gamma radiation of the same approximate frequency. This means that
an energy audit is in order. The purpose of the audit will be to
see if gamma radiation and accepted binding energy ideas can
account for the disintegration of a significant fraction of the heavier
nuclei in the solar wind. [This paragraph needs some re-write.]
If we consider electromagnetic radiation to be comprised of photons,
the following calculation for gamma photons of frequency 10^22 Hz is
applicable.
Here is a table for binding energies of the lightest nuclides.
Based on energy considerations alone, the hypothetical 41 MeV gamma
photons should be able to totally disassemble any of the light nucleons up
thru Lithium, and cause serious trouble for more massive nuclei.
Then there is the matter of checking the fluence (energy flux per unit
area) for GRB 990510 against the number of candidate nucleons to be
disassembled.
If we restrict ourselves to a very oversimplified scenario by pretending
that the "heavier" nuclei in the solar wind are strictly deuterium
nuclei (one proton + one neutron), we can make a rough estimate of
how many nucleons could be involved in the gamma-induced fission
process. (Fission may not be the most appropriate term.)
The following solar-wind disk relations will be used. Here, we concern
ourselves with the lower half of the disk. (If we get the lower half
moving upward, the top half will follow.)
Keep in mind that the binding energy for a Deuterium nucleus is 2.22 MeV.
We then calculate how much energy GRB 990510 could apply to the problem.
We use the BATSE fluence(2) for radiation above 20 keV.
It appears that, based on energy considerations alone, GRB 990510 could
have induced a total of about eight fission events in the square-centimeter
column of height equal to one-half the thickness of the solar wind disk.
If the numbers above are more-or-less in order, then we cannot apply
accepted energy considerations to the problem of diffusing the
solar wind external to the Sun itself.. That would leave the resonance-like
pumping interaction of Gamma-radiation and hypothetical
orbiting nuclear electrons as an open-ended adventure. (One other
possibility, is that there was no direct en-route connection
between the Gamma-ray Burst and the solar wind perturbation, and that
something did in fact affect the Sun, itself, in some unknown way.)
With regard to the idea that the solar wind disk became less dense
(enroute), another possibility could be that, instead of the disk being
lifted from below, the rapidly disassembled nucleons
may have caused the disk to expand explosively, above and below
the ecliptic, which led to the temporarily rarified solar wind,
which was nearly devoid of nuclei more massive than bare protons.
The normal solar wind speed is about 400 km/sec. At that speed it takes
about one hour to for solar wind perturbations to traverse the 1.5 million
km distance between the L1-region ACE spacecraft and the Earth-region
WIND spacecraft. If the onsets of the solar wind density decreases, as
recorded by these spacecraft, occurred within minutes, or tens of minutes,
of each other, it would be compelling evidence that a Sun-based phenomenon
was NOT the ultimate cause of the disruption.
[The time delay, between the ACE and WIND spacecraft, for a pre-GRB
solar wind perturbation, which started at 07:55 UT on 10 May 1999 (solar
wind speed was approximately 400 km/sec) was, in fact, on the order of
one hour. ACE-WIND delay analysis for perturbations in the hours
immediately following the GRB, are in work. This exposition is
not out of the woods yet. This note, was inserted on 24 June
2003. RSF]
The following graph shows ACE and WIND proton densities before and
after GRB 990510.
. . .
(2) Michael S. Briggs, Robert D. Preece, Jan van Paradijs,
Jean in 't Zand, John Heise, Erik Kuulkers and C. Kouveliotou,
"Wide-Band Spectroscopy of GRB 990510,"
Gamma-Ray Bursts - 5th Huntsville Symposium, (1999) AIP Conference
Proceedings, 526, 125-129.