He claimed that he was able to find the times of sunspot maxima for
every cycle back to A.D. 300, as well as many of the 11-year cycles back
to 649 B.C. He reports that the earliest known reference to a sunspot is
due to Theophrastus of Athens (ca. 370-290 B.C.), a student of Aristotle.
Chinese records of sunspots date from about 28 B.C. to A.D. 1638. From
his data, Schove found that the average period for a sunspot cycle is
11.11 years with individual cycles ranging in length from 9 to 14 years.
He also confirmed the so-called Maunder minimum in the latter half of
the seventeenth century when sunspots were virtually absent. Recent
speculation about the Maunder minimum involves the theory that the sun
is shrinking.
When it comes to ancient observations of the aurora in the Bible,
Schove interprets the following passages as sightings of the aurora:
Jeremiah 1:13: And the word of the LORD came unto me the second
time, saying, What seest thou? And I said, I see a seething pot; and
the face thereof is toward the north.
14 Then the LORD said unto me, Out of the north an evil shall break
forth upon all the inhabitants of the land.
Ezekiel 1:4: And I looked, and, behold, a whirlwind came out of the
north, a great cloud, and a fire infolding itself, and a brightness was
about it, and out of the midst thereof as the colour of amber, out of the
midst of the fire.
Zechariah 1:8: I saw by night, and behold a man riding upon a red
horse, and he stood among the myrtle trees that were in the bottom;
and behind him were there red horses, speckled, and white.
To interpret these as references to the aurora is stretching it, especially
Zechariah 1:8 where the phenomenon is described as a man on a red
horse standing among the myrtle trees. A seething pot? maybe, but it
should say a seething sky, instead, to be more correct. To interpret the
seething pot as an aurora would require human corruption of the text and
a low view of inspiration. As for the whirlwind in Ezekiel 1:4,
whirlwinds are common in the Mid-East, so why not take it at face value?
Besides, all of these are prophetic visions and, as visions, are not required
to have any physical substance.
Other historic references to the aurora seem more realistic.
Anaximenes provides us with the earliest known Greek account in the
sixth century B.C. Anaxagoras (ca. 500 B.C.) and Aristotle (387-322
B.C.) also wrote about the aurora. Among the Romans who reported
aurorae are Cicero (106-43 B.C.), Livy (59 B.C.-A.D. 17) and Seneca (4
B.C.-A.D. 65). The latter describes an event in A.D. 37 when the people
in Rome thought that the colony of Ostia was on fire. During most of the
night, the heaven appeared to be illuminated by a faint light resembling
thick smoke. At low latitudes, aurorae are often red in color.
It is generally thought that aurorae do not occur at the equator, but on
September 25, 1909, aurorae were seen at Singapore (1°N) and Batavia
(6°S). On May 13, 1921, aurorae were sighted at Samoa (14°S) and Tongatabu
(21°S). So aurorae may be seen from any point on the earth.
Properties of the Solar Wind
The solar wind is a collection of electrons and protons which started
out as hydrogen atoms but which were stripped apart by the heat of the
solar corona (some 10,000,000 degrees) and ejected at speeds ranging
from 300 to 600 kilometers per second. When they reach the earth, the
temperature of the solar wind is between 18,000 and 180,000 degrees
Fahrenheit (10,000 to 100,000 degrees Kelvin or Celsius) and there are
from 1 to 30 protons or electrons per cubic centimeter (20 to 600 per
cubic inch).
Figure 1: The Magnetosphere and its plasmic parts and
currents.2
Since the protons and electrons are free from each other, the plasma,
as the solar wind is called, is highly conductive. As a result, it retains
part of the sun's magnetic field and is subject to the earth's magnetic
field, too. The earth's field acts as an obstacle to the solar wind and the
effect is to deform and compress the terrestrial field's lines of force. The
deformation results in the construction of a boundary between the solar
wind and the earth's field, which boundary is called the magnetopause
(Figure 1). The magnetopause begins about 40,000 miles (64,000 km)
from the earth in the direction toward the sun and extends more than
2,000,000 miles (3,200,000 km) in the downwind direction. Also,
since the speed of the solar wind is about 10 times the speed of sound
near the earth, a shock wave (akin to a sonic boom) is permanently in
place upstream from the magnetopause. The shock slows down the solar
wind and heats it up to a temperature of over a million degrees Kelvin
(1.8 million Fahrenheit). The shocked, slowed gas then flows over the
magnetosphere where, in the process, a small fraction is trapped and becomes
part of the gas in the reservoir called the plasma sheet. The temperature
there ranges is from 20 million to 200 million degrees Fahrenheit
(10 to 100 million Kelvins).
The plasma sheet is not a simple sheet in form. Instead, it is shaped
more like that of a glass tube at the end of which some gigantic glass
blower has started to blow a bubble. Yet the bubble's end looks like a
pair of pincers pinching the earth near its poles (Figure 1). It is from
these pincers that electrons rain down from the plasma sheet into the
earth's upper atmosphere to produce the aurorae. During solar storms,
the plasma sheet moves closer to the earth, causing the aurora to move
closer and closer to the equator. That motion stops at the edge of yet
another collection of particles called the plasmasphere. The plasmasphere
is the upward extension of the earth's ionosphere and is composed
of ionized atoms (atoms stripped of one or more of their electrons),
mainly hydrogen, from the earth's atmosphere. Compared to the plasma
sheet, the plasmasphere is cold and dense.
The plasmasphere is in the shape of a doughnut (toroid) with the earth
filling the hole in the middle. It has a sharp upward boundary called the
plasmapause, which is caused by a wind in the magnetosphere which at
that point sweeps away particles faster than the ionosphere produces
them. The shape of that boundary is dictated by the earth's magnetic
field. On the average it is 20,000 miles (30,000 km) from the earth at the
equator, and it reaches the top of the atmosphere at about 63 degrees
north and south latitudes. These are the auroral latitudes.
Although the densities may not sound like much, the pinching effect
of the plasmasphere can produce dramatic currents. One of the greatest
magnetic storms occurred on September 1, 1859. It was observed in
Honolulu, Cuba, Jamaica, Guadalupe and, in the southern hemisphere at
Santiago and Sydney. The solar flare which spawned it was the first ever
observed, being visible as a white spot on the face of the sun, an extremely
rare event. The storm disrupted telegraph communications in
France where isolated cables would spark to grounded objects brought
near the wire. Elsewhere, the storm aided communication. For example,
the telegraph between Boston and Portland ran for two hours without a
battery, using only the current induced by the storm.
Conclusion
At this point there is nothing inherently geocentric or even creationistic
about the aurorae. Perhaps the reference to stretching the heavens as a
curtain in Isaiah 40:22 refers, in part, to the aurorae; but I doubt it.
Others have speculated that the center of the aurorae, above the magnetic
poles of the earth, are the sides of the north referred to in Isaiah 14:13,
but I doubt that, too; for Psalm 48:2 relates those sides to mount Zion and
the city of the great King. Future generations may find the solar wind
and the magnetosphere to be a useful source of energy; but for the time
being it is still a pristine phenomenon untouched by human hands.
NOTES AND REFERENCES
1
Schove, D. J., 1955. The Sunspot Cycle, 649 B.C. to A.D. 2000, J.
of Geophys. Rsrch., 60:127-156.
___________, 1962. Auroral Numbers Since 500 B.C., J. of the
British Astron. Assoc., 72:30.
___________, and P.-Y. Ho, 1967. Chinese Records of Sunspots
and Aurorae in the Fourth Century A.D., J. of the American Oriental
Society, 87:105.
2
The reference to this figure has been lost, but the figure is from page
39 of the 11 January 1974 issue of Science, (Vol. 183). The complete
reference may be found there.