The dawn of astronomy: A study of the temple-worship and mythology of the ancient EgyptiansLockyer, Norman, Sir
Religion
The dawn of astronomy: A study of the temple-worship and mythology of the ancient Egyptians
Lockyer, Norman, Sir
Astronomy, Egyptian; Sun -- Mythology; Sun worship; Temples -- Egypt
A diagram will show what will happen under these conditions. If we take
first the points at which the axis, instead of being inclined towards
the sun, is inclined at right angles to it, it is perfectly obvious
that we shall get a condition of things in which the movement of the
earth on its axis will cause the dark side of the earth and also the
light side represented by the side nearest to the sun, both being of
equal areas, to extend from pole to pole; so that any place on the
earth rotating under those conditions will be brought for half a period
of rotation into the sunlight, and be carried for half a period of the
rotation out of the sunlight; the day, therefore, will be of the same
length as the night, and the days and nights will therefore be equal
all over the world.
We call this the time of the equinoxes; the nights are of the same
length as the day in both these positions of the earth with regard to
the sun.
[Illustration: EARTH AND SUN AT THE EQUINOXES.]
In the next figure we have the other condition. Here the earth's axis
is inclined at the greatest angle of 23°½, towards, and away from,
the sun. If I take a point very near the north pole, that point will
not, in summer, be carried by the earth's rotation out of the light,
and a part equally near the south pole will not be able to get into
it. These are the conditions at and near two other points called the
solstices.
[Illustration: EARTH AND SUN AT THE SOLSTICES.]
On each of these globes I have drawn a line representing the overhead
direction from London. If we observe the angle between the direction of
the zenith and that to the sun in winter we find it considerable; but
if we take the opposite six-monthly condition we get a small angle.
In other words, under the first condition the sun at noon will be far
from the zenith of London, we shall have winter; and in the other
condition the sun will be as near as it can be to the zenith at noon,
we shall have summer. These two cases represent the two points in the
earth's orbit at which the sun has the greatest declination south and
north. With the greatest north declination the sun will come up high,
appear to remain at the same height above the horizon at noon for a
day or two, as it does at our summer solstice, and then go down again;
at the other point, when it has the greatest southern declination, it
will go down to the lowest point, as it does in our winter, stop, and
come up again--that is, the sun will stand still, so far as its height
above the horizon at noon is concerned, and the Latin word solstice
exactly expresses that idea. We have, then, two opposite points in the
revolution of the earth round the sun at which we have equal altitudes
of the sun at noon, two others when the altitude is greatest and least.
[Illustration: DIAGRAM SHOWING POSITION OF THE SUN IN RELATION TO THE
ZENITH OF LONDON AT THE NORTHERN WINTER SOLSTICE.]
Public-domain text, read in full here on John Shaqi.
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